This is only a preview of the May 2026 issue of Silicon Chip. You can view 44 of the 112 pages in the full issue, including the advertisments. For full access, purchase the issue for $10.00 or subscribe for access to the latest issues. Items relevant to "Power Amp Clipping Indicator":
Items relevant to "Simple LC Meter":
Items relevant to "WiFi Alarm Monitor":
Articles in this series:
Items relevant to "μDCC Decoder":
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MAY 2026
ISSN 1030-2662
05
9 771030 266001
The VERY BEST DIY Projects!
$14 00* NZ $14 90
INC GST
INC GST
AMPLIFIER
CLIPPING
INDICATOR
protect your loudspeakers from being overdriven
Analog Computers
how they differ from digital computers, and are they making a comeback?
microDCC Decoder
our smallest decoder yet
Despite its size, it has two 100mA function outputs and sound output
Rosehill Gard
e
3 – 4 June 2 ns Event Centre
026, see pag
e 40
Contents
Vol.39, No.05
May 2026
16 Analog Computers, Part 1
Nowadays computing is pretty much all digital, so have we moved on
from analog computers; or might they come back? We look at what makes
analog computers unique, with historical and modern day examples.
By Dr David Maddison, VK3DSM
Technology feature
Analog Computers
Page 16
40 Electronex 2026
The Electronex exhibition is back in Sydney this year, to be held at Rosehill
Gardens Event Centre on the 3rd and 4th of June.
By Various Authors
Trade exhibition showcase
76 Power Electronics, Part 7
In this series of articles, we explore the principles of power electronics.
This month, we cover resonant converters and soft switching, and how
switching losses can be a greater problem at higher frequencies.
By Andrew Levido
Electronic design
Page 62: compact and simple
¬C Meter
82 Installing a CB Radio in your Car
Here’s how to neatly fit your own CB radio in a car, which can be very useful
when driving on country roads.
By Julian Edgar
Automotive / radio feature
90 BrisbaneSilicon ELM11 Board
The ELM11 is an affordable development board that uses the LUA
programming language and is designed in Australia.
Review by Tim Blythman
Microcontroller development board
30 Power Amp Clipping Indicator
Protect your loudspeakers from being overdriven and possibly destroyed
with our Clipping Indicator. It can reduce the signal level applied to an
amplifier, protecting the speakers, and can be built-in or standalone.
By John Clarke
Audio project
62 Simple LC Meter
Using just 20 parts, this tiny LC meter can measure inductances from
<10nH to around 100mH and capacitances from <10pF to about 1μF. It’s
powered from a single AA cell and is housed in a 3D-printed case.
By Andrew Woodfield
Test & measurement project
69 WiFi Alarm Monitor
This project is ideal for checking up on the elderly. It monitors both an
alarm condition (like a burglar alarm going off) and daily activity. It can then
send a remote alert to a device like a phone or an email address.
By Kenneth Horton
Monitoring project
84 μDCC Decoder
Our previous DCC Decoder was a small design at 23 × 14mm, but we
thought we could one-up it and make it even smaller. This microDCC
(μDCC) Decoder measures 18 × 12mm and even has sound output.
Part 7 by Tim Blythman
Model train project
Page 69
WiFi
Alarm
Monitor
2
Editorial Viewpoint
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Classic mains power indicators
I was interested to see the Mains Power LED Indicator
in the February 2026 issue (siliconchip.au/Article/19655).
I have a similar indicator in my workshop with a story
attached to it. I wanted a wide-angle, long-lasting indicator lamp to remind me if I had forgotten to switch off the
main workshop power.
Some years ago, I visited Alcatraz (the historic prison
island near San Francisco) and was surprised to see a gigantic, very aged-looking neon lamp on an old fuse and switchboard that was still glowing, probably since the 1930s. I
knew that most American panel lamps with these sorts
having clear or coloured glass lenses were made by Dialco.
Later, when I was looking on eBay for a Dialco glass-lens
panel lamp for another project, I stumbled across one of
the exact same gigantic neon indicator lamps as the one I
saw at Alcatraz. So I put it in a painted and labelled diecast box with a panel line IEC connector to feed it with an
extension cord from the main power feed board and hung
it on the wall (see the attached photo).
It reminds me not to spend too much time in the workshop, too!
Dr Hugo Holden, Buddina, Qld.
Sourcing good-quality axial electrolytic caps
I have not yet had to replace the main power supply filter caps in my Tektronix 2465B oscilloscopes, featured in
the Vintage Electronics column last month. However, I did
some research. It is a little difficult to find axial capacitors
of suitable size, capacitance and voltage values these days.
A large neon indicator lamp put in a diecast box to imitate
the look of the lamps found in Alcatraz.
4
Silicon Chip
I eventually discovered some amazing suitable replacements that are available from AliExpress. I bought some
for evaluation in my workshop, and they passed with flying colours, with extremely low leakage values. They are
genuine parts (not fakes), likely left over from an automotive manufacturing contract.
They are EPCOS Sikorel military-specification style
parts with astonishingly high temperature and high pulse
current ratings (they can even be shorted without damage,
not that you should do it!). I have attached a photo below.
They are excellent parts, and I hardly ever say that about
electrolytic capacitors.
It is worth looking up the specifications of these Sikorel
capacitors, which come in many values and sizes; there are
many on AliExpress for sale. I bought enough of these to
replace the original parts in my vintage oscilloscope, if or
when they fail. Some of the parts available include:
• AliExpress 1005009581483411 (270μF 200V; what I
bought)
• AliExpress 1005009559895645 (10μF 100V)
• AliExpress 1005010449425160 (680μF 75V)
• AliExpress 1005010433682158 (470μF 75V)
• AliExpress 1005007864314700 (680/1000/1800μF
40V)
• AliExpress 1005010745748467 (470/1000μF 35V)
Dr Hugo Holden, Buddina, Qld.
Interesting method of replacing SMDs
I was interested to read David Coggins letter on page 4
of the March 2026 issue. His experiences largely mirrored
These EPCOS Sikorel electrolytic capacitors have
extremely high temperature and current ratings.
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Above: to remove the PIC on one of Silicon Chip’s RGB
LED Analog Clock kits, Richard Verrall used a small
cut-off disc from an angle grinder to sever the pins. The
remaining solder was then easily removed.
Right: the voltage (cyan) and current (yellow) waveforms
using a current clamp and the HV Isolating Probe.
mine. I bought two RGB LED Analog Clock kits, one having the GPS module and the other with WiFi capability.
The first kit functioned as expected. I then assembled
the second clock kit, but got a very garbled light display.
So I ordered another PIC and found a satisfactory way to
remove the existing unit by using a very small cut-off disc
to sever the device’s legs.
It looks like a mess, but surprisingly, the remains of the
legs could be desoldered and removed. The board then
cleaned up better than expected. I ordered some new programmed PICs, hoping they might resolve the impasse!
Richard Verrall, Taroona, Tas.
Comment: it isn’t hard to remove these chips using a lowcost hot air rework station. Still, it’s good to know there’s
another method.
We’ve had a few people now report that their problems
with the Clock kit went away after replacing the PIC. So it
seems increasingly likely that a bad batch of PICs made
its way into the kits. We always verify the flash contents
after programming them, so it should not be a problem in
their programming.
Reactive current fools master/slave power board
Silicon Chip readers may be interested in this problem
we had with a new LG OLED TV.
We have been using a master/slave power board with
our TV to turn off all the accessories (DVD, sound bar,
Xbox etc) to save standby power when we are not using
the TV. When we replaced the TV with an LG OLED type,
the master/slave power board stopped working, remaining on all the time.
I used one of those plug-in power meters to see what was
going on. It showed the TV was drawing 0.22A in standby
but only using 0.3W! No wonder the power board was confused. When switched on, it used around 0.7A and 150190W depending on the picture brightness.
I had a look at the voltage and current waveforms on an
oscilloscope (see the photo at upper right) using a current
clamp and a High Voltage Isolating Probe (January 2015
issue; siliconchip.au/Article/8244). Sure enough, the current
was a sinewave close to 90° out of phase with the voltage.
It is a stepped sinewave with about 19 steps per cycle,
presumably being generated by the power factor correction (PFC) circuit in the TV’s switch-mode power supply,
but I was surprised it was so high at 52VA of reactive voltamps in standby.
6
Silicon Chip
I remembered I had the USB Sensing Mains Switch project (January 2009; siliconchip.au/Article/1271) around
somewhere. After a long search, I found it and substituted
it for the master/slave power board. I used one of the USB
outlets on the TV to trigger it. It worked a treat and reduced
my standby power from 19W to 1.5W.
The flat tops on the mains voltage in the scope grab are
real! They are not from overloading my probe.
Mike Hammer, Mordialloc, Vic.
Keep wires straight for surge protection!
Well done to Ian Ashford for presenting the Solar Panel
Protector and Optimiser project in the March 2026 issue
(siliconchip.au/Article/19824).
I am sure it will find many uses in domestic and alternative supply installations. However, I would like to point
out something that surprised me when looking at the pictures of the installation. All the Earthing conductors were
wound into coils.
I teach electrotechnology to electrical apprentices at
TAFE and sadly, this habit has been passed down from
old-timers to the current-day apprentices, and I have to
correct them on it. Referring to Appendix F (Surge protection devices in AS/NZS3000), Clause F1.2.5 states:
Conductors used to connect a surge protection device to
both the line, via the overcurrent protective device, and to
the main earthing or neutral conductor should be consistent with the current rating of the backup fuse or circuit
breaker but should be not less than 6mm2, be as short and
direct as possible and with no loops.
The idea of surge protection as outlined in Ian’s article is to shunt the surge current to Earth via the lowest
impedance path possible. Placing extra turns in the Earth
conductors makes them become inductors, albeit of a very
small value. This small inductance can still have a very
high initial impedance due to the extremely fast rise time
of the surge voltage waveform.
Lenz’s law then comes into play.
This fast rise time coupled with the massive amount
of current will create a huge amount of magnetic flux.
Induced back-EMF is proportional to the number of turns
in the coil multiplied by the change in flux value divided
by the time it takes for that flux to change. This back-EMF
could make the Earth conductor appear as an open circuit initially.
This would then defeat the purpose of installing surge
Australia's electronics magazine
siliconchip.com.au
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With so many cameras, computers and effects, things can get busy fast! The
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All models have built in hardware streaming engine for live streaming via its
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Use Professional Video Effects
ATEM Mini is really a professional broadcast switcher used by television stations.
This means it has professional effects such as a DVE for picture in picture effects
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protection. Once again, it is a great project, but it is good
practice to keep the wiring short and direct.
Geoff Coppa, Toormina, NSW.
Computer evolution over the last 30 years
It was interesting to see the photo of the IBM XT computer on page 26 of the February 2026 issue of Silicon Chip.
That was my first PC, after having an Apple IIe, Commodore 64 & 128, Amstrad 64 & 128, Amiga 500, Macintosh
etc, most of which I picked up at tip shops and op shops.
I got the IBM XT at the local tip shop. It was missing a
video card. I also picked up some other junk: monitors,
video cards and the like. After trying different video cards
and a couple of monitors, I got the XT working.
It had a 10MB MFM hard drive, two 360-kilobyte floppy
drives and a green monochrome monitor. It was running
DOS 3.3; I used XTGold as the file manager. I still have
that PC sitting on a shelf in my shed, unused for decades.
After that I had a 286, 386 and then 486 with DOS 6.22
and Windows 3.1. I also had several Macintoshes: the P1,
P2, P3 and P4 with CRT monitors, 4:3 LCD monitors and
then 16:9 LCD monitors. Then came Windows 95, 98, 98SE,
2000 and XP.
Most of that hardware came from tip shops and a computer shop that I was collecting the ‘junk’ from – old hardware that customers no longer needed when they upgraded.
Then I switched to laptops instead of desktop machines,
with dual-core i3s, i5s, i7s running Windows 7, 10, 11 and
now Linux.
Advances in technology lead to unusable hardware; with
Windows 11 not supported on so many devices, we can
expect to see many more people switching to Linux with
the end of support for Windows 10. Fortunately, Linux
runs well on old dual-core devices, so that may save a lot
of old hardware from the scrap heap.
Bruce Pierson, Dundathu, Qld.
Comment: Windows 11 updates have caused a lot of
problems lately, making staying on Windows 10 feel like
dodging a bullet! There’s nothing wrong with many of those
“obsolete” computers except that Microsoft has decided
not to support them anymore.
Flashing Mains LED Indicator suggestion
Thanks for the Mains Power LED Indicator project (February 2026; siliconchip.au/Article/19655); I’ve built similar circuits without a zener diode. I recently built a mains-
powered, DIAC-based LED flasher for my pool pump setup,
as I often forget to switch the pool pump timer/electrics
back to normal from pause mode after pool maintenance.
When I read your article, I thought your design had the
potential for an updated version, with an onboard slide
switch to choose between always-on or flash mode.
Ciril Kosorok, Mount Druitt, NSW.
Transistor-assisted ignition circuit improvements
I refer to your Serviceman’s Log entry in November 2025
on a transistor-assisted ignition unit repair by Bruce Pierson (siliconchip.au/Article/19230). I recall building several of them ‘back in the day’; in fact, I still run one on a
1950 Rolls Royce Silver Dawn. A couple of simple modifications to the original circuit to improve performance and
efficiency may be of some interest to others. My revised
circuit is shown overleaf.
8
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
A revised circuit of the Transistor Ignition from Electronics Australia December 1979. The changes include an added
BC548 transistor, 10W resistor and a 27nF capacitor between the collector and emitter of Q4.
Firstly, adding a transistor (BC548) from the base to the
emitter of the BUX80, in conjunction with a 10W resistor
from the emitter of Q2 to ground, forces the main switching
transistor to switch off much faster. It does this by pulling
the base to the emitter instead of simply removing the base
drive to the BUX80, giving a quicker switch-off time, therefore producing a faster and more vigorous spark.
The original 220nF points capacitor value is a compromise. Too low and all the stored coil energy makes a mini
arc welder across the points. Too high means too much
energy being absorbed by the capacitor with little remaining to create a healthy spark. When a transistor is doing
the hard work of switching, we can get away with a significantly smaller value capacitor in this position.
A value of 27nF results in a significantly more energetic spark and with a faster rise time. A faster rise time
means less time for the spark to be potentially bled away
from a dirty/fouled spark plug. More spark energy has to
be a good thing!
I found that removing one of the three 2.7W resistors supplying base current to the BUX80 still enabled that transistor to saturate to around 0.25V.
J. B. Upper Caboolture, Qld.
Comment: that design was from a long time ago (47
years!). Our latest ignition systems utilise an IGBT as the
switching element. As you point out, the points capacitor really needs to be selected for the best compromise
between wear on the points and spark energy. The ideal
value depends on the ignition coil, mechanical arrangement for the points and engine type (low-revving, high-
revving etc).
Lilienfeld’s patents in the 1920s and 1930s, plus Heil in
1934) were theoretical or non-functional.
However, there is another possibility, often called the
“lost transistor”: the Adams Crystal Amplifier from 1933,
created by a 13-year-old New Zealander, Robert Adams.
He used crystals like chalcopyrite and iron pyrite to create this device. It was essentially like a cat’s whisker diode
(which was in common use at the time) but with an additional point contact added.
It demonstrated the potential of solid-state amplification.
He regarded his invention as “obvious” and thus unpatentable. Unlike the Bell Labs device, it was not properly
documented, published in scientific journals, or patented.
SC
Dr David Maddison, Toorak, Vic.
Who really invented the transistor?
The Bell Labs point-contact transistor, developed by
Bardeen, Brattain and Shockley in 1947, is widely recognised as the first working transistor. Earlier attempts (eg,
10
Silicon Chip
This may be the first transistor, invented by a 13-yearold New Zealand boy in 1933. Source: https://memorial.
bellsystem.com/belllabs_transistor1.html
Australia's electronics magazine
siliconchip.com.au
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Part 1 by Dr David Maddison, VK3DSM
Analog Computers
An analog computer at Lewis Flight Propulsion Laboratory in 1949 – https://w.wiki/HRcx
These days, we are surrounded by digital computers, but computing wasn’t always
performed with binary numbers. Analog computers were used extensively in the
past, and possibly will also be in the future.
T
oday, what most people think of as
a computer is a digital computer, like
a laptop or smartphone. However,
digital computers weren’t the first and
aren’t the only kinds of computers.
The first electronic digital computer
was built in 1946. Called ENIAC, it
filled a room – see Fig.1. One of its jobs
was to compute artillery trajectories.
The Moore School of Electrical Engineering at the University of Pennsylvania developed an alternative: a simple
analog differential analyser, a type of
mechanical analog computer (Fig.2).
It performed the same task with gears
and shafts in a much smaller space,
foreshadowing a rivalry that has lasted
nearly 100 years.
Some analog computers are very
ancient indeed. Originally, all analog
computers were mechanical, but in
the 1940s, electronic analog computers were developed. They are easier to
develop than mechanical designs and
more reliable. They have some advantages compared to digital computers.
Unlike digital computers, which
represent information using discrete
16
Silicon Chip
binary states (0 or 1), or quantum
computers, which use discrete qubits
that can be in a superposition of the
0 and 1 states, an analog computer
can represent and process a continuum of values, using something like
a voltage or current. That gives it an
almost infinite number of distinguishable states within the physical range.
Analog computers started to become
obsolete in the late 1950s with the
rise of transistors and early digital
machines, accelerating through the
1970s as microprocessors like the
Intel 4004 (1971) made digital computers scalable and affordable. However, analog computers remained in
some niches (eg, flight simulators)
into the 1980s.
By the 1970s, mechanical and electronic analog computers had become
largely obsolete, replaced by faster,
more precise digital systems. However, they are now making a comeback
in various forms, where their ability
to electronically represent a continuum can bypass digital computer bottlenecks.
Australia's electronics magazine
This article will concentrate on
describing traditional analog computers, their uses, and covering their history. A follow-up article next month
will look at the current and future uses
of analog computers and state-of-theart technology.
Differences between analog
and digital computers
An electronic analog computer cannot do everything a digital computer
can do, but it can excel in certain realtime simulations of physical systems,
where it can have superior speed and
efficiency.
Because an analog computer deals
with continuous values, its accuracy
and repeatability are inferior to a digital computer. Analog computers typically have a calculation error in the
0.1-1% range.
Traditional electronic analog computers were programmed by physically rewiring a patch panel – see Fig.3.
This same method was used on some
of the earliest digital computers, such
as ENIAC, the Harvard Mark I and the
siliconchip.com.au
Colossus computer for cryptographic
key settings.
In modern analog and mixed-signal
systems, the physical patch panel has
largely been replaced by digital configuration interfaces (SPI, I²C, USB
etc) that program field-programmable
analog arrays (FPAAs), memristor crossbars, floating-gate arrays or
switched-capacitor circuits, making
it easier to change their configuration.
Where analog computers excel
Traditional analog computing excels
at real-time simulations of continuous
physical phenomena, such as the flight
dynamics of aircraft.
More recently, its ability to map
physical variables directly onto continuously variable electrical signals
(voltages, currents, or resistances)
has made analog hardware extremely
attractive for mimicking biological
neural networks.
They can perform the massive
matrix-vector multiplications required
in AI pattern recognition and sensory
processing with far greater energy efficiency than conventional digital chips.
This dramatic power consumption
advantage, often by a factor of 1001000 times for similar workloads, is
the primary driver behind the current resurgence of interest in analog
and analog-inspired computing techniques.
Figs.1: the ENIAC electronic digital computer circa 1947-1955. Like the one
shown in Fig.2, it could compute artillery trajectories, but the analog computer
was smaller and more efficient at the time. Source: https://penntoday.upenn.
edu/news/worlds-first-general-purpose-computer-turns-75
Where digital computers excel
Digital computing excels in precision, repeatability and accuracy,
as intermediate and final values are
represented by precise mathematical
values, not analog properties, which
cannot be precisely or reproducibly
represented.
Also, digital computers can run a
huge array of software from word processing to video editors to databases
and everything else imaginable; analog computers usually perform much
more specific tasks.
Digital computers can also store vast
amounts of data and programs and
with results reproducible between different computers, and are not subject
to subtle hardware variations between
platforms.
The digital computer is a practical
realisation of Alan Turing’s Universal
Turing Machine (UTM) — a theoretical device capable of computing any
function that is algorithmically computable.
siliconchip.com.au
Fig.2: a mechanical analog computer circa 1942-1945.
Fig.3: a Comdyna GP-6 (user manual: siliconchip.au/link/acag) made for
educational purposes. Its prominent patch panel is set up to solve the simple
equation x’’ + x’ = 0 representing a certain case of pure viscous damping.
Source: www.glennsmuseum.com
Australia's electronics magazine
May 2026 17
In contrast, real-world analog computers built in the 20th century were
not universal in the Turing sense
because they could only efficiently
solve specific classes of problems
(mainly differential equations) and
lacked the ability to simulate arbitrary computation without exponential growth in hardware.
However, Claude Shannon proved
in 1941 that a theoretical model he
called the General Purpose Analog
Computer (GPAC), built from ideal
integrators, adders, multipliers and
constant units, is equivalent in computational power to a Universal Turing
Machine and can therefore compute
any computable real function (to arbitrary precision, given unlimited time
and perfect components).
While Shannon proved that a theoretically ideal GPAC is as powerful
as a UTM, no physical GPAC can ever
be implemented exactly because real
electronics cannot provide infinite
precision, infinite range or perfect
components, making true analog universality practically unattainable.
Despite this, special-purpose analog
computers remain extremely useful.
What analog computers do
Traditional analog computers of the
past could emulate physical systems,
such as:
• Aerospace and flight dynamics to
model aerodynamic forces, pitch, roll,
yaw and jet engine inlet control, such
as on the SR-71, which used a hydraulic analog computer.
• Aquifer simulation.
• Astronomical or planetary motion
Fig.4: a reproduction of the back of
the Antikythera mechanism. Source:
https://w.wiki/HRct
18
Silicon Chip
(eg, the Antikythera mechanism and
many later planetariums).
• Automotive automatic transmissions; for more on this, see our article
on “Fluid logic, Fluidics and Microfluidics” in August 2019 (siliconchip.
au/Article/11762).
• Ballistics and trajectory analysis.
• Chemical reaction simulation.
• Convective flow simulation.
• Damped mechanical system simulation (eg, vehicle suspensions).
• Economic modelling (as in the
MONIAC hydraulic computer).
• Electronic circuits.
• Flight simulation.
• Fluid dynamics simulation.
• Heat transfer simulation.
• Hydraulic and fluid networks,
such as the flow of fluids through complex pipe networks in chemical plants,
water supplies or sewerage systems.
• Medical monitoring.
• Nuclear reactor kinetics; modelling thermal and neutron flux.
• Oscillating systems like massspring-dampers.
• Power-grid analysis.
• Radioactive decay simulation.
• Tide prediction.
• Temperature and industrial process control.
Analog computer history
The history of analog computers
can be divided into two main eras,
the ‘classic’ and ‘modern’ eras. The
classic era is:
• Up until the 1940s, mechanical
and electro-mechanical computers
dominated. They were expensive and
slow to configure.
Fig.5: a reproduction of the front of
the Antikythera mechanism. Source:
https://w.wiki/HRcs
Australia's electronics magazine
• During the 1940s and 1950s,
valves and electronic analog computers appeared and began to dominate.
The K2-W valve op amp module was
introduced in 1953.
• During the 1960s and 1970s, transistorised op-amp based computers
became inexpensive and were used
in engineering education and industry. This was the peak of analog computing in the classic era.
• From the 70s onward, digital computers dominated, with analog computers continuing only in niche areas.
In the modern ‘revival’ era, from
around 2020 onward, the focus of analog computers is on energy-efficient AI
inference engines and AI matrix-vector
multiplications.
Such analog or mixed-signal chips
are being produced by companies like
Imec (from 2020), Mythic (from 2021),
Lightmatter (from 2022), Aspinity &
SynSense (from 2023), ACCEL & IBM
(from 2024), Anabrid (from 2025),
as well as Encharge, Microsoft and
Peking University.
Mechanical analog computers
Here is a list of some of the important mechanical analog computers:
Antikythera mechanism (200BCE)
The first known specialised
mechanical analog computer was the
Antikythera mechanism (Figs.4 & 5)
made between 200BCE and 80BCE
and discovered at the bottom of the
Mediterranean Sea in 1901. It is a complex geared mechanism (the details
of which can be seen at https://w.
wiki/HRcu) that was used to predict
Fig.6: Lord Kelvin’s tide predicting
machine. Source: https://w.wiki/HRcv
siliconchip.com.au
Fig.7: a replica of the Difference Engine located at the Computer History Museum
in Mountain View, California. The first complete one is located in London’s
Science Museum. Source: www.flickr.com/photos/jitze1942/4305143894/
Fig.8: a Norden Bombsight. Source:
https://w.wiki/HRcw
astronomical positions and eclipses
decades in advance.
A neat interactive example of a partial reconstruction can be viewed at
siliconchip.au/link/acaq
It is a remarkable achievement of
science and engineering that has been
subject to intense study ever since its
discovery. With X-ray tomography
in 2005, it became possible to read
its inscriptions and determine other
details. It is estimated to have had at
least 37 gears.
An Australian YouTuber went
through much of the manufacturing
process using the same tools and materials the ancients would have had (see
https://siliconchip.au/link/aca0).
mechanical integrators (six in the initial version) driven by electric motors,
shafts and gears to solve complex differential equations. It was originally
built to model power transmission networks, but it quickly proved invaluable for problems in physics, ballistics, seismology and more, dramatically reducing calculation times from
months to hours.
Slide rule (1622)
English clergyman William Oughtred invented the slide rule around
1622, shortly after John Napier introduced the logarithms on which it was
based, in 1614. Slide rules were in use
until around 1972, when they were
replaced by calculators.
Planimeter (1814, 1854)
A planimeter is a form of specialised mechanical analog computer for
measuring areas on a map or plan. It
is a continuous mechanical integrator,
hence an analog computer. A tracer is
moved around the boundary enclosing an area, and the area is computed.
siliconchip.com.au
The first known planimeter was
invented in 1814 by J. M. Hermann;
the most popular design, still in use
today, was invented by Jacob Amsler
in 1854.
The Difference Engine (1822)
Charles Babbage completed his Difference Engine 0, a mechanical computer to produce mathematical tables,
in 1822. This and Babbage’s subsequent work were brilliant, but suffered
from enormous mechanical complexity and funding problems. Some of his
designs were only completed in recent
years (see Fig.7).
Tide predictor (1872)
Lord Kelvin developed a tide predicting analog computer (Fig.6).
Machines based on this design and
built by Arthur Doodson are credited
with the accurate tide predictions that
were vital for the D-Day Normandy
landings in 1944.
Differential Analyzer (1931)
American engineer Vannevar Bush,
along with Harold Hazen, unveiled
their groundbreaking Differential Analyzer at MIT in 1931. It was a massive
mechanical analog computer, often
regarded as one of the first advanced
computing devices of the modern era.
It was a room-sized machine
using interconnected wheel-and-disc
Australia's electronics magazine
Norden bombsight (1931)
The Norden Mark XV bombsight
(Fig.8) was a mechanical analog computer used during WW2 by the USAAF
and US Navy, and into the Korean
and Vietnam wars. Its purpose was to
calculate when to drop bombs to hit
a target on the ground. It was one of
the most expensive programs of WW2,
costing about half that of the Manhattan Project.
E6-B flight computer (1940)
This circular slide rule was used for
flight planning. It has been replaced
by electronic devices today, but is
still in use for flight training, in aviation exams and for backup purposes
in case electronic devices fail.
Electronic and hydraulic
analog computers
We will now look at some significant
early analog computers. Some hydraulic computers will be included among
May 2026 19
Table 1: equivalent hydraulic and electrical concepts
Concept
Electrical
Hydraulic
Voltage
Pressure
Current
Flow rate
Electric charge
Fluid quantity
Path for ‘current’ flow
Wire
Pipe
Impedance
Resistor
Constriction in pipe
Energy storage
Capacitor
Bladder on diaphragm
Inertia
Inductor
Turbine/paddle wheel
Current flows in one
direction
Diode
One-way valve
Signal amplification
Transistor
Pressure-actuated valve
Constant source
Voltage or current
source
Pump w/ or w/o
feedback control
the electronic ones, as they operate on
analogous principles – see Table 1.
solving inhomogeneous differential
equations.
AC Network Analyzer (1929)
This was an electronic or electromechanical analog computer first built by
MIT’s Harold Locke Hazen under the
leadership of Vannevar Bush. It was
designed to study large-grid AC power
systems and complex power flows
in real time. The computer included
components like phase-shifting transformers, inductors/gyrators, variable
resistors, capacitors and adjustable
loads.
It was essentially a scale model of
a large grid electrical system. It was
programmed by physically wiring
circuits on patch panels and reading results with meters. This type of
machine was used extensively from
1929 to the 1960s. To reduce the size
of transformers, these machines were
run at a much higher frequency than
the 50/60Hz of real-world networks.
It was a special-purpose analog computer and a predecessor of the later
general-purpose op-amp-based electronic analog computers of the 1950s.
It does not seem to be regarded as an
electronic analog computer by most
commentators, but this author thinks
it is. It is not to be confused with the
1931 Differential Analyzer, also built
under Bush’s influence.
V-2 Guidance Computer (1941)
Despite the AC Network Analyzer
above, the first generally-accepted
electronic analog computer is considered to be the German Mischgerät
V-2 guidance computer designed by
Helmut Hölzer, used for rocket guidance.
It was a single-purpose computer
comprising resistors, capacitors and
valve amplifiers. It differentiated voltages from yaw, roll and pitch gyroscopes to sense the rocket’s divergence from the original orientation of
the gyroscopes, deriving the rate of
divergence. This was converted to correcting voltages that controlled servos
for the steering vanes located in the
rocket exhaust.
It was a much cheaper, lighter and
better-performing solution than competing methods. It did not use op
amps, but influenced later US analog computers, as the technology
and Hölzer himself were brought to
America after the war under Operation Paperclip.
Water Integrator (1936)
The Water Integrator (Fig.9) was a
hydraulic computer invented by Russian Vladimir Lukyanov; versions of
such hydraulic computers were in
use in the USSR until the 1980s. In
the 1930s, the original machine was
the only one in the USSR capable of
20
Silicon Chip
M9 Gun Director (1943)
Bell Labs’ M9 Gun Director was a
specialised electronic analog computer developed in the USA. It worked
with the SCR-854 radar, which provided real-time range and direction
data. It solved trigonometric equations, computed firing solutions and
then transmitted aiming data such as
azimuth, elevation and fusing time
directly to gun servo motors.
Apart from target speed, direction
and range, it took into account wind,
Australia's electronics magazine
Fig.9: a version of the 1-IGL-1-3 Water
Integrator hydraulic analog computer.
Source: Polymus – siliconchip.au/
link/acar
air pressure, shell velocity and gun
parallax. It achieved a high success
rate in England against German V-1
flying bombs and German aircraft,
reducing the number of shells needed
to shoot down a target from thousands
to around 100.
The M9 was the first electronic analog computer that contained circuits
fulfilling the function of operational
amplifiers, the foundation of later electronic analog computers, but which
had not yet been named as such (see
the PDF at siliconchip.au/link/aca1).
The M9 laid the foundation for
future integrated radar and fire control computers, including defensive
weapons like the Phalanx CIWS still
in use today, including by Australia.
Project Cyclone (1946)
A family of computers was developed by Reeves Instrument Corporation for the US Navy – see Fig.10. More
than 60 REAC (Reeves Electronic Analog Computer) machines were built
and placed in various institutions.
Seven models were produced between
1947 and 1965. This family of computers is credited with proving that
there was a viable commercial market
for computers.
ANACOM (1946, 1948)
The Westinghouse ANACOM solved
problems in grid-scale power systems,
such as lightning surges on transmission lines, plus mechanical design
problems, oil flow and many others
(see Fig.11). It was in use until 1991.
It was under constant development
and, by the 1980s, it was under the
control of a digital computer to set
up the initial starting conditions for
siliconchip.com.au
Fig.10: a 1965 sales brochure for the REAC 600 from Reeves. Source: https://archive.org/details/TNM_REAC_600_
computer_system_-_Reeves_1965_20180302_0183/page/n1
problems being solved. It was probably
the longest-lasting conventional analog computer used into the digital age.
(like Philbrick’s K2-W) became widely
used, and more advanced machines
took over.
model of the computer shown in the
image; it may have been a REAC 100,
released in 1947. The REAC 100 had
18 op amps, 10 integrators, 10 summers, 10 inverters, 25 potentiometers
and five servo-multipliers.
GEDA (1947)
REAC (1949)
The Goodyear Electronic DifferREAC (see the lead photo) was an
ential Analyzer was developed for
analog computer at Lewis Flight Prothe Goodyear Aircraft Corporation to
pulsion Laboratory (now the John
MONIAC (1949)
solve differential equations for missile
H. Glenn Research Center), in Ohio.
The MONIAC was a hydraulic comguidance simulations. It was released
NASA did not clearly identify the puter that used water and fluid logic
commercially in 1949.
instead of electricity and elecGEDA used valve-based
tronic components for its calhigh-gain DC amplifiers staculations. It was invented by
bilised by a unique commuNew Zealander Bill Phillips.
tator system (a rotary switch
Its purpose was to model the
that periodically rebalanced
national economic processes
amplifier inputs to reduce
of the United Kingdom. We
drift), similar to the system
described it in the August
used in modern ‘chopper
2019 issue, on page 21.
stabilised’ op amps. GEDA
systems typically had 20-85
RCA Typhoon (1951-1952)
amplifiers configured as inteThe RCA-designed Project
grators, summers, multipliers
Typhoon was one of the largetc, via patch panels.
est electronic analog computThey were used for missile
ers ever built (see Fig.14). It
trajectory simulation, flight
was designed for the US Navy
dynamics, control systems
to be used in solving complex
and even early war-gaming.
differential equations for the
They were superseded by the Fig.11: the Westinghouse ANACOM (ANAlog COMputer). development of ships, submamid-1950s as true op amps
rines, aircraft and missiles. It
Source: www.researchgate.net/figure/fig1_220494419
siliconchip.com.au
Australia's electronics magazine
May 2026 21
Operational amplifiers
An operational amplifier (op amp) is an extremely high-gain differential-voltagecontrolled amplifier. When negative feedback is added, typically via a few resistors
and capacitors, it can be made to perform addition, subtraction, integration,
voltage inversion or other mathematical operations with almost zero error.
The op amp is the workhorse of the analog computer, with two inputs (+ and −)
and one output. Its name comes from its original use, performing mathematical
operations in electronic analog computers, but now it has many other uses. It
was the basic computing element of all electronic analog computers of the
1950s to the 1970s.
The term operational amplifier was coined in 1947 by John Ragazzini, but the
first practical commercially available op amp was the Philbrick GAP/R K2-W,
released in 1953 (Fig.12). The first truly ‘modern’ op amp was the μA741 IC,
released in 1968 and still in production (see Fig.13). Other classic op amps that
came later include the TL071/2/4, LM324/358, NE5532/4, LM833 and OP07.
For more details, see our article on The History of the Op Amp in the August
2021 issue (siliconchip.au/Article/14987).
required a staff of nine engineers and
mathematicians, plus six technicians.
It had 100 dials and 6,000 plug-in
connections. Its output devices were
two Electronic Associates Variplotters, 18 GE recording voltmeters and
a 3D trajectory indicator. It had 4000
valves, 450 precision DC amplifiers, a
bank of polystyrene capacitors for 80
simultaneous integrations, hybrid step
multipliers and a power consumption
of 46kW.
Special circuitry was designed to
achieve accuracies of 0.001%; the
power supply was regulated to that
tolerance as well.
Convair Analog Computer (1953)
It was used for stress analysis of aircraft, and flight simulation, including
a cockpit simulator. It had 8500 valves,
reportedly occupied several floors and
was one of the largest analog computers ever made – see siliconchip.au/
link/acas
K2-W (1953)
The first commercially available,
modular, standardised op amp was
George A. Philbrick’s K2-W valve module, released in 1953 (some say 1952)
– see Fig.12. It was manufactured until
1971. It is similar to an integrated circuit but based on valves, resistors and
capacitors.
It was a high-performance device
designed for building electronic analog computers. Its design eased the
implementation of functions like
addition, subtraction, integration,
Fig.14: the RCA Typhoon, possibly the largest electronic analog computer
ever built. Note the rocket model in the foreground. Source: The Analogue
Alternative, James S. Small, 2001
22
Silicon Chip
Australia's electronics magazine
Fig.12: the first
commercially
available op amp,
the Philbrick K2-W.
Source: https://w.
wiki/HRd3
Fig.13: the first
‘modern’ IC op
amp, the μA741.
Source: https://w.
wiki/3eHA
differentiation, multiplication and
division.
A modular electronic analog computer for solving differential equations
would use a few to dozens of op amps.
Philbrick also made several ‘black box’
K3-series electronic analog computer
components, which can be viewed at
http://philbrickarchive.org/k3_series_
components.htm (see Fig.15).
The K2-W was a significant step in
the miniaturisation, modularisation
and standardisation of electronic analog computers before the development
of transistors.
Central Air Data Computer (1956)
The Bendix Central Air Data Computer was used in US military aircraft
such as the F-101, F-111 and the B-58
Fig.15: a K3 Series component from
GAP/R. This is an adding unit with
four inputs, e1, e2, e3 & e4. Source:
http://philbrickarchive.org/k3_series_
components.htm
siliconchip.com.au
Fig.16: a 1962 model of the Bendix
Central Air Data Computer. Source:
https://w.wiki/HRcy
to compute altitude, airspeed, Mach
number and other values from pressure and temperature inputs. It contains two pressure sensors and an
analog computer built from gears
and servos.
It was a masterpiece of engineering, with 46 synchros (a device to
convert rotation to electrical outputs), 511 gears, 820 ball bearings
and 2781 major parts – see Fig.16 &
siliconchip.au/link/aca2
Perceptron (1958)
The Mark 1 Perceptron was an artificial neural network algorithm originally simulated by Frank Rosenblatt
on an IBM 704 digital computer in
1957 before being built into hardware
as the Mark 1 Perceptron electronic
analog computer. It could distinguish
between simple shapes like squares,
circles, diamonds and the letters X, E
and F with different orientations.
In different experiments, it used
between 500 and 1000 ‘neurons’ and
was trained with up to 10,000 images.
It had three main parts:
1. A set of sensory or S-units comprising a 20×20 array of photocells to
receive optical inputs.
2. A set of 512 association or
A-units, each of which fired based on
inputs from multiple sensory units.
3. A set of 8 response or R-units,
which fired based on inputs from multiple association units.
The S-units were connected to the
A-units via a plugboard (see Fig.17).
The A-units were connected to the
R-units with adjustable weights
encoded in potentiometers, with
weight updates adjusted during learning by electric motors.
You can read an operator’s manual at https://apps.dtic.mil/sti/tr/pdf/
AD0236965.pdf
This was an amazing machine for
the time and the precursor to modern
AI systems.
PACE 231R (1958)
This was Electronic Associates’
flagship computer and became the
world’s most widely used electronic
analog computer, even into the early
1980s – see Fig.18. It was used for simulations for Project Mercury, Project
Gemini, HL-10 lifting bodies (famous
from the Six Million Dollar Man) and
the X-15 rocket plane.
For X-15 simulations, NASA
used three PACE 231R computers
siliconchip.com.au
Fig.17: the Mark I Perceptron showing
the S-unit to A-unit plugboard.
Source: www.researchgate.net/figure/
fig2_345813508
Fig.18: the Pace 231R computer.
Fig.19: the AKAT-1 from Poland. A
very interesting-looking machine!
Source: https://w.wiki/HRcz
containing a total of 380 op amps, 101
function generators, 32 servo amplifiers and five multipliers networked
together. Simulations could be run
between Mach 0.2 and Mach 7.0 at
altitudes up to 321km. Landing simulations were not possible.
AKAT-1 (1959)
From Poland, it was one of the first
differential equation analysers based
on transistors. It was only ever built
as a prototype – see Fig.19.
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May 2026 23
Heathkit EC-1 (1960)
This was an educational electronic
analog computer – see Fig.20. It contained nine op amps.
MUDPAC (1961)
The Melbourne University Dual
Package Analogue Computer was built
by Applied Dynamics in the USA, their
first computer for export. It was used
until 1986. It comprised two consoles,
64 op amps, 80 coefficient potentiometers, 16 multipliers, eight function generators and 20 diode networks. It had
a 1632-hole patch panel – see Fig.21.
Fig.22: the major components of the instrument unit of the Saturn V. Source:
NASA – https://images.nasa.gov/details-0100984
Apollo (1961+)
Analog computers played a critical
role in the 1960s-1970s Apollo program, for ground simulations and in
some on-board systems. Large-scale
analog and hybrid analog-digital computers were used extensively on the
ground for high-fidelity, real-time simulations of Saturn V rocket dynamics
– see Fig.23.
For example, the General Purpose
Simulator (GPS) at NASA’s Marshall
Space Flight Center ran 12-degree-offreedom models of the first stage that
incorporated wind gusts, structural
flexing and fuel sloshing, all in realtime, which was 3000 times faster
than the digital computers of the era
could achieve.
The GPS comprised 50 integrators,
50 summers, 350 coefficient potentiometers, 20 quarter square multipliers and 15 function generators (which
contained an additional 70 op amps).
The Flight Control Computer (FCC)
of the Saturn V instrument unit
(Fig.22) was not purely analog; it was
a hybrid analog/digital system (mostly
analog for the guidance loops, with
some digital logic), translating inertial measurement data into gimbal
commands for the F-1 and J-2 engines.
In contrast, the famous Apollo Guidance Computer (AGC) carried onboard
the Command and Lunar Modules was
entirely digital; it was the first real-time
embedded digital computer flown in
space. It handled navigation guidance
and control of the spacecraft itself.
At the time (in the 1960s), purely
digital computers were too slow and
memory-limited to perform the highspeed, continuous, multi-degree-offreedom simulations required for Saturn V development or the fast innerloop control of engine gimbals, which
is why analog and hybrid solutions
Australia's electronics magazine
siliconchip.com.au
Fig.20: a Heathkit EC-1 educational electronic analog computer. Source:
https://w.wiki/HRc$
Fig.21: the MUDPAC computer used at the University of Melbourne in
1961. Photographer: David Demant, Museums Victoria, https://collections.
museumsvictoria.com.au/items/399902
24
Silicon Chip
remained indispensable on the ground
and in some flight hardware.
EAI PACE (1963)
The EAI PACE/TR-20 transistor tabletop analog computer was
designed for educational use and basic
research, even as digital computing
was growing in prominence.
SR-71 (1964)
The SR-71 Mach 3+ aircraft, first
flown in 1964, used a hydraulic analog computer of cams, levers, pistons
and valves to manage the complex
engine inlet airflows and fuel mixtures. Digital computers of the time
were not fast enough, small enough,
robust enough or heat resistant enough
to handle the task.
Fig.23: a detailed
view of NASA’s
General Purpose
Simulator,
circa 1966.
Source: www.
joostrekveld.
net/?p=1409
Moog synthesiser (1964)
While it was a musical instrument,
many sources call it an analog computer. It shares roots with electronic
analog computers, using the same
building blocks like voltage-controlled
oscillators, filters, amplifiers and envelope generators derived from op amp
circuits. It is arguably a specialised
musical analog computer.
Nebraska-Kansas dispute (~1966)
Early in this dispute concerning the
use of groundwater, which has run for
decades, an analog computer was built
to simulate groundwater flows. Water
was pumped out of test wells to determine the land’s water storage capacity
and resistance to flow. This was simulated with an analog computer made
of a network of 30,400 resistors and
an unspecified number of capacitors
that took a month to build – see Fig.24.
Land with coarse soil, a high storage capacity and low resistance to
flow was represented by a high-value
capacitor and low-value resistors,
while land with fine soil, a low storage capacity and high resistance to
flow was represented by low value-
capacitors and high-value resistors.
The output of the water table profile
was read on an oscilloscope; future
water levels could also be predicted.
Fig.24: simulating
groundwater
flows with a
resistor/capacitor
network (top).
The test well
network is shown
at bottom, with a
high flow well on
the left and low
flow on the right.
Source: Time Life
Science Library
“Water”, 1966
Fig.25: the
Australianmade EAI 180
computer.
Source: https://
artsandculture.
google.com/
asset/eai-180analog-computerelectronicsassociatesincorporated-eai/
IgG4Y3h75wg07g
EAI 180 (1972)
An EAI 180 (Fig.25) was used at the
University of Sydney, Department of
Mechanical Engineering in the 1970s.
It was designed by Electronic Associates Pty Ltd of Sydney and built
by Hawker Siddeley. It was used in
siliconchip.com.au
Australia's electronics magazine
May 2026 25
the 1970s for teaching engineering
students. Prior to this, calculations
were made on mainframe computers (if available) or slide rules.
It was ultimately replaced for
teaching purposes by inexpensive
programmable calculators. The
Powerhouse Museum notes that
this was an Australian version
of the EAI 180 from the US parent company; it sold very well in
Europe, but was not allowed to
be sold in the USA despite being
considered a better machine than
the one made in the USA.
Its reference manual is available at siliconchip.au/link/aca3
Analog Thing (2025)
The Analog Thing by anabrid
(https://the-analog-thing.org) is
an open-source analog computer –
see Fig.26. It has five integrators, four
summers, two comparators, eight coefficient potentiometers, two multipliers, a panel meter and a hybrid port for
analog-digital hybrid programs. Multiple Things can be daisy-chained. It is
available for about A$875 + shipping
(we suspect our readers could build
an equivalent for much less than that).
Mechanical vs electronic
computers
Having looked at some representative mechanical and electronic analog
computers, let’s compare them.
Cost: mechanical computers are
complicated and require expensive
precision machining and extensive
assembly. Electronic circuits also
require high levels of precision,
although that is achieved inexpensively by modern manufacturing
methods. That makes them easier and
cheaper to build, alter and program,
unlike a complex mechanical device.
Speed: mechanical computers rely
on gears, shafts, cams, ball and disc
Fig.27: an op-amp-based integrator
circuit.
26
Silicon Chip
Fig.26: the Analog Thing, an analog
computer available for purchase today.
mechanical integrators etc. They are
limited in speed to a few cycles per
second due to mechanical friction,
inertia, balance etc. Electronic components such as valves or transistors can
easily operate at thousands or millions
of cycles per second.
Ease of programming: reprogramming a mechanical computer can
require complex gear, linkage and
other changes, which could take a very
long time. On an electronic analog
computer, it is just a matter of changing some patch cables, rotating potentiometers, perhaps adding an electronic module with certain functions,
etc. Digital and hybrid computers are
even easier and quicker to reprogram.
• Operational amplifiers (op
amps) can be configured to perform
addition, subtraction, integration,
differentiation and signal amplification.
• Diodes and transistors are
used for signal conditioning,
switching and more complex functions.
• Potentiometers or variable
resistors can be used for scaling
values.
• ICs are used for specialised functions in more modern
machines.
These components can be used
to form basic circuit elements or
modules of an electronic analog
computer, with some examples
as follows.
Circuit elements & functions
The following electronic components are used in an electronic analog computer.
• Resistors and capacitors are used
for scaling voltages (resistors), creating time delays (RC delay circuit) and
forming filters (RC filter).
An electronic analog computer comprises some or all of the following.
• Amplifiers to boost weak signals.
• Filters for processing signals in
real-time, to attenuate high or low
frequencies.
• Function generators and comparators to create waveforms or compare
signal levels. They can be built from
transistors, diodes and capacitors or
specialised ICs or modules.
• Integrators and differentiators, as
mentioned earlier, are usually built
from op amps.
• Circuit blocks to perform mathematical operations like addition,
subtraction, multiplication, squaring,
square rooting, division, exponentiation and logarithms.
A differential equation is one that
relates a function to one or more of its
derivatives (rates of change); solving
it involves finding the original function through the process of integration.
An integrator circuit can be constructed using an op amp, resistor and
capacitor whereby an output voltage
Fig.28. an op-amp-based differentiator
circuit.
Fig.29: an op-amp-based summing
circuit.
Basic electronic components
Australia's electronics magazine
siliconchip.com.au
is produced from the capacitor which
is the integral of a voltage over time,
a fundamental of simulating dynamic
systems (Fig.27).
Similarly, an op amp can be configured for differentiation, in which a
voltage output is produced that is proportional to the input voltage’s rate-ofchange with respect to time (Fig.28).
Another op amp based circuit is a
summing amplifier (for addition) – see
Fig.29. An op amp has multiple voltage
inputs producing a weighted average
of the input voltages.
Other mathematical functions can
be performed. The logarithm of an
input signal can be determined by
exploiting the inherent exponential
relationship between the base-emitter
voltage (Vbe) and collector current (Ic)
of a bipolar junction transistor in the
feedback loop of an op amp, as shown
in Fig.30. The PDF at siliconchip.au/
link/aca4 has more specific details on
this method.
An analog electronic multiplier
takes two analog input signals (usually
voltages) and produces an output signal, typically a voltage or current that
is proportional to the product of the
inputs or, with feedback, their ratio.
Beyond simple multiplication and
division, analog multipliers can also
perform squaring, square rooting,
RMS-to-DC conversion and amplitude
modulation by exploiting their inherent non-linear characteristics.
One implementation of a modern
analog multiplier is built around the
Gilbert cell, invented in 1967, which
is a clever arrangement of transistors
whose currents multiply naturally
because of the exponential relationship between a transistor’s base-emitter
voltage and its collector current.
A modified version of a Gilbert
cell is shown in Fig.31; this is Analog Devices’ implementation, as used
in the classic but now discontinued
Differential equations in computing
A differential equation simply tells us how fast something is changing at any
instant, for example, the rate at which a falling object accelerates due to the force
of gravity acting on it, or the oscillatory acceleration of a mass on a spring due to
spring tension.
Integration is the reverse operation: it turns a rate of change into the total
accumulated quantity, such as the speed of the object as it falls; velocity is the
integral of acceleration, and position is the integral of velocity.
In an electronic analog computer, differentiation and integration are calculated
physically and continuously by the single most important building block, the
integrator circuit. It uses just one operational amplifier, one resistor, and one
capacitor (see Fig.27).
The resistor converts the input voltage (representing the rate of change) into a
current that steadily charges or discharges the capacitor; the voltage across the
capacitor therefore becomes the running total, which is the mathematical integral
of the input, all with virtually zero delay.
As an analogy, think of the capacitor as a bucket collecting water (current) at
a rate set by the input voltage (pressure); the water level at any moment is the
integral, mirrored by the output voltage. Because this happens continuously and in
real time, the falling object differential equation d2y/dt2 = -9.8m/s2 can be solved by
feeding a constant -9.8V into the first integrator. Its output becomes a steadily rising
voltage ramp (velocity), which can then be fed to a second integrator, producing a
downward-opening parabolic voltage vs time curve (position).
An oscilloscope or chart recorder connected to the output can visualise voltage
(y-axis) over time (x-axis) to observe the parabolic trajectory. This is shown in a
YouTube video at https://youtu.be/3tOA8Fo6b7A
Another example is simple harmonic motion, x’’ + ω2x = 0. Two integrators
integrate acceleration (x’’) to velocity (x’) and again to displacement (x) with one
or two inverters to correct the signs.
That is why analog computers were once called differential analysers: they almost
instantly turned differential equations into voltage curves, providing an answer to
many engineering problems. On a digital computer in the 1960s, this would have
required pages of digital code and seconds or minutes of computation even on
the fastest digital machines of the day.
The same humble op amp based integrator principle that powered Apollo
simulations and 1960s control systems is now reappearing with a different
implementation in ultra-low-power-consumption AI chips, proving that for many
continuous, real-world problems, analog integration remains unmatched in speed
and energy efficiency.
Fig.30: in this logarithm converter,
Vy is a constant, while Is is a scaling
parameter of the transistor.
Fig.31: a modified Gilbert cell core, as used in Analog Devices’ AD534. The
inputs are Vx and Vy, while the output is E0. Source: www.analog.com/
media/en/training-seminars/tutorials/MT-079.pdf
siliconchip.com.au
Australia's electronics magazine
May 2026 27
Fig.32: a gyrator
or synthetic
inductor (far
left) and its
equivalent
circuit.
Fig.33: some mechanical and
electrical analogies.
AD534 multiplier chip. It was replaced
by the AD633 and AD734, both still
available. These chips were widely
used in 1970s-1980s analog computing for multiplication, division, powering and root functions.
Explaining how the Gilbert cell circuitry works is beyond the scope of
this article; interested readers can visit
siliconchip.au/link/aca5 and https://w.
wiki/HHbV
For multiplication, the circuit takes
two input voltages Vx and Vy, converts them to currents, multiplies
those currents in the transistor core,
then converts the result back to an
output voltage giving Vout = k × Vx
× Vy (where k is a constant, usually
about 1/10).
By feeding the multiplier’s own output back into one of its inputs (often
through an op amp), you get division (Vout = Vx ÷ Vy). Squaring simply involves connecting both inputs
together. Square-rooting uses the multiplier in a feedback loop that forces
Vout2 = Vin.
The same building block, with a
few extra resistors or capacitors, can
also perform amplitude modulation,
frequency doubling, RMS-to-DC conversion and even logarithmic/exponential functions.
Another simple circuit that can form
part of an electronic analog computer
is the Wheatstone bridge. An unknown
resistance is found by balancing
known resistance values against the
unknown. In essence, multiplication
and division are performed using calibrated resistors to balance the bridge
and find the unknown value.
A modified Wheatstone bridge
can also be used to compute the tangent of an angle or the hypotenuse
Fig.34: the OME P2 is an electronic analog computer made by the Société d’électronique et d’automatisme (SEA) in
1952. It was used for simulations during the development of the Concorde. Source: https://w.wiki/HTe8 (CC-BY-SA 4.0)
28
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Australia's electronics magazine
siliconchip.com.au
of a right-angle triangle. A circuit to
divide and multiply using a Wheatstone bridge was published in the June
1960 edition of Radio-Electronics (see
siliconchip.au/link/aca6).
As inductors are large for use at
low frequencies and have other deficiencies, a gyrator circuit can act as
a ‘synthetic inductor’, comprising an
op amp, resistor and capacitor – see
Fig.32.
Electrical and mechanical
equivalents
One of the main uses of traditional
analog computing was to simulate
mechanical systems. There were two
ways to do this with electronic analog
computers:
1. The impedance analogy (force-
voltage or Maxwell analogy), in which
mechanical force corresponds to voltage and velocity to current.
2. The mobility analogy (force-
current analogy or Firestone), in which
force aligns with current and velocity
with voltage.
Other parameters equating physical
and electrical quantities are shown in
Table 2.
The very name “analog computer”
comes from the ability to generate
analogies. Some examples are shown
in Fig.33. To decide which analogy to
apply, the following are considered:
If a direct mapping of impedance values is desired, so mechanical impedances match electrical impedances
numerically, the impedance analogy
(also called the Maxwell analogy) is
used. Mechanical impedance measures
a system’s resistance to motion, while
electrical impedance measures opposition to alternating current.
This analogy allows direct quantitative correspondence, but has the disadvantage that the topology is inverted,
that is, mechanical series connections
become electrical parallel connections
and vice versa – see Fig.35.
Fig.35: a simple series LCR resonator, mechanical and electrical equivalents.
This is the Maxwell analogy, in which mechanical parallel connections become
series electrical connections. F = force, S = spring stiffness, M = mass and R =
damper resistance.
Fig.36: a simple series LCR resonator with mechanical and electrical
equivalents. This is the Firestone analogy, in which mechanical parallel
connections remain parallel electrical connections.
If, instead, it is desired to preserve
the physical topology of the system so
that the electrical circuit mirrors the
mechanical connections, the mobility analogy (also called the Firestone
analogy) is chosen.
Here, parallel mechanical elements
are represented as parallel electrical
elements, and series elements remain
in series, making this arrangement
more intuitive for complex systems.
However, the impedances are inverted
– see Fig.36.
Figs.35 & 36 are electrically series
or parallel LCR resonator circuits.
Depending on the analogy used, both
can be analogues of the same mechanical system, which could be an automotive suspension or engine mount
system, a tuned mass damper in a tall
building, the suspension of a washing
machine drum or aircraft landing gear.
The equivalent mechanical device
comprises a damper (shock absorber;
R or 1/R), a mass representing inertia
(L or C) and a spring represented by
its stiffness (C or L), all connected in
parallel in both cases.
As mentioned earlier, rather than
using physical inductors for L, impedance inverters (gyrators) are usually used instead. Alternatively, real
inductors could be used, but the circuit could be operated at a higher
frequency than in reality (eg, 10× or
100×).
Next month
That’s all we have space for in this
issue. As we have already discussed
the history of analog computers, the
second and final instalment next
month will concentrate on their presSC
ent and future.
Table 2: mechanical and electrical equivalent quantities in analog computing.
Quantity
Impedance (force-voltage) analogy (Maxwell)
Mobility (force-current) analogy (Firestone)
Force (F)
Voltage (V)
Current (I)
Velocity (v)
Current (I)
Voltage (V)
Mass (m)
Inductance (L)
Capacitance (C)
Damping (b)
Resistance (R)
Conductance (G)
Spring constant (k) Reciprocal of capacitance (1/C)
Reciprocal of inductance (1/L)
Displacement (x)
Magnetic flux linkage (λ) or charge in some contexts Charge (q)
Impedance
Preserved (Ze ∝ Zm)
siliconchip.com.au
Inverted (Ze ∝ 1/Zm)
Australia's electronics magazine
May 2026 29
Power Amplifier
Clipping Indicator
Ensure your loudspeakers are protected from being overdriven and possibly damaged
or destroyed by building this Power Amplifier Clipping Indicator. Not only does it show
when an amplifier clips (however briefly), it can also reduce the signal level applied to the
amplifier to limit subsequent clipping, protecting the speakers.
By John Clarke
A
mplifier clipping occurs when the
output flat-tops because it cannot
increase the output voltage any further
due to power supply limitations. This
means that the amplifier has reached
its limit to deliver power to the loudspeakers. It also means the sound
becomes vastly distorted, leading to
the sound quality suffering. If clipping
is allowed to continue, loudspeakers
can be damaged or destroyed.
With suitable volume levels, the
amplifier reproduces the audio signal faithfully. But if the amplifier is
turned up too much and clipping starts
to occur, you get a compressed signal
30
Silicon Chip
that causes the overall power delivered to the loudspeakers to be greatly
increased, causing them to overheat
and burn out.
Woofers and, to some extent, midrange drivers are less prone to damage
than tweeters. This is because they
utilise more robust and larger diameter wire in their voice coils than their
tweeter counterparts. The tweeter is
more delicate, using a thinner, smaller
and lighter voice coil so it can move
quickly to reproduce higher frequencies.
When loudspeakers are overdriven,
the voice coil windings can burn out
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or the voice coils can soften and permanently distort. Continued excessive
overdrive can result in the loudspeaker
catching fire and/or fusing.
If you want to explore more about
loudspeaker damage due to amplifier
overloading, see www.sound-au.com/
tweeters.htm and www.sound-au.
com/clipping.htm
We have previously published three
Power Amplifier Clipping Indicator
projects, one as a full project and two
Circuit Notebook entries. These all
detect clipping based on whether signal level peaks approach a fixed voltage difference from the amplifier’s
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Features & Specifications
Detects genuine signal clipping and
gross distortion
Doesn’t require opening up the amplifier
Optional automatic signal reduction at
clipping
Separate left and right channel clipping
indicator LEDs
Momentary clipping is shown on LEDs
with a minimum 50ms duration
Suitable for inverting, non-inverting and
bridge-tied amplifiers
Uses commonly available components
Easy to solder
Power supply requirement: 15-24V DC
at 200mA
supply rails. Typically, this was set at
somewhere around 4.7-6.2V less than
the supply rails.
This level is not necessarily the
point of clipping. It depends on the
type of driver devices used in the
amplifier (whether Mosfets or transistors), the driver device’s temperature, and the loudspeaker impedance.
Additionally, to install such a power
amplifier clipping indicator requires
access to the inside of the amplifier to
tap into the power supply rails.
This new Clipping Indicator is
designed to detect when the amplifier
is actually clipping. Only externally
available amplifier connections need
to be accessed: the input sockets and
the speaker outputs.
How it works
The Clipping Detector works by
comparing the signal applied to
the amplifier with the output from
the amplifier. If the amplifier is not
clipping, the two signals should be
identical in shape, only differing in
voltage magnitude. We compare the
signals after reducing the amplifier
output level so it matches that of
the input. That way, any differences
between the two waveform shapes
can be detected.
A summing amplifier compares the
two signals. Typically, the input and
output signals of an amplifier will be
in phase. So when the input goes positive, the output also goes positive.
If we invert the amplifier output
signal and then sum the two signals,
they should cancel out. If there are any
differences, such as phase changes or
clipping, the summing amplifier (or
‘adder’) will produce an output that
becomes a difference or error signal.
We simulated this in LTspice, as
shown in Fig.1. The blue trace is the
amplifier input, the red trace is the
attenuated and inverted amplifier output, while the green trace is the adder
output. We have clipped the positive
output of the amplifier output a little
at the peak of the positive excursion
to show how the adder responds to a
signal difference.
There is a rise in the adder signal
level when the two waveforms differ.
When the two signals are the same
except for being inverted (as shown
for the negative excursion), the adder
output remains close to 0V.
We use the adder output to gauge
the amount of difference between the
two signals. A window comparator
detects when the adder produces a
large enough difference signal to trigger the clipping indication.
To verify this, Scope 1 shows the
amplifier output waveform (yellow
trace) at the point of clipping at 104V
peak-to-peak. The lower cyan trace
shows the output from the summing
amplifier, IC2c. The summing amplifier begins to produce a difference signal at the point of clipping on the output waveform.
Fig.1: a SPICE simulation of a summing amplifier fed with the inverted input
and non-inverted output signals of an amplifier just starting to clip. The output
of this ‘adder’ only varies from zero during clipping.
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Australia's electronics magazine
The clipping is asymmetrical, meaning that the degree of clipping in the
positive portion of the waveform is
greater than in the negative half. This
is due to the differences in the power
amplifier output transistors used for
the positive and negative output drive.
Block diagram
The block diagram, Fig.2, shows the
main sections of the Clipping Indicator. We will describe the sections
briefly since there is more detail in
the circuit description. The diagram
shows the left channel only, and
we’ll explain just that channel; the
right channel designators are shown
in brackets.
The signal input at CON1 is from
a signal source such as a CD player
or preamplifier output. This signal is
buffered by IC1a and goes through a
high-pass filter to remove signals well
below the audible range (sub-20Hz).
Following this is the variable attenuator. This acts to reduce the signal level should extended clipping
occur. It uses a light-dependent resistor (LDR1) and LED2. The LDR forms
a voltage divider with a fixed resistor,
providing more attenuation when the
LED light intensity increases.
Normally, without any light from
the LED, the LDR has a very high
impedance, so there is minimal attenuation. Thus, this section has no effect
on the signal except when the amplifier is driving into clipping. Another
buffer follows (IC1d) before the signal is applied to the power amplifier
input via CON3.
The output from buffer IC1d also
goes to two phase-adjustment filters,
one for the high-frequency end of the
audio spectrum and the other for the
low-frequency end of the audio spectrum. These are adjusted to match the
phase shifts that occur in the power
Scope 1: the amplifier output
waveform (yellow) and output from
the summing amplifier IC2c (cyan).
May 2026 31
amplifier at the lower and upper frequency extremes.
These are inherent to most audio
amplifiers due to capacitors in
the power amplifier causing low-
frequency roll-off where the input and
feedback signals are AC-coupled, and
high-frequency roll-off due to the compensation capacitor used to ensure the
power amplifier’s stability and possibly other RF/noise filters.
We need our clipping detection signal path to have the same phase shift
characteristic as the amplifier so we
can compare the two signals. Otherwise, they will be different even if
there is no clipping, possibly causing
false triggering.
The output from the phase adjustment filters is applied to the summing
amplifier input.
The power amplifier output connects to either the CON5 non-inverting
or inverting amplifier input. Most
power amplifiers are non-inverting,
so the non-inverting input is typically used.
The inverting input is mainly
included so that you can use this
device with a bridge-tied load (BTL)
amplifier, where there are two amplifiers driving the loudspeaker with
one producing an inverted signal
compared to the other. Having the
two input options allows for both
amplifier outputs to be monitored for
BTL amplifiers.
The signal level from CON5 is controlled using trimpot VR4 or VR5, or
both in the case of a BTL amplifier.
The signals are buffered following
the attenuators, and in the case of the
non-inverting amplifier signal, it is
inverted by another op amp, ready for
comparison in the summing amplifier
using IC2c.
IC2c is the summing amplifier
described previously, and the resulting summed signal is monitored by a
window comparator (IC3). Normally,
this signal level will sit close to 0V
when there is no clipping. When the
summing signal reaches a set level
(beyond ±1.25V), the window comparator triggers timer IC4.
IC4 provides a 50ms minimum
output to drive the clipping LED via
transistor driver Q2, ensuring that the
flash is visible even for very brief clipping events. This driver also provides
a fast attack and slow decay voltage
that drives LED2 via transistor Q3.
This reduces the resistance of LDR1,
attenuating the signal that ultimately is
applied to the power amplifier input.
Circuit details
The full circuit is shown in Fig.3. It
comprises four quad op amp ICs and
three single op amp ICs for a total of
Fig.2: the Clipping Indicator is connected between the preamp (CON1/
CON2) and power amplifier (CON3/CON4). A current-controlled attenuator
can reduce the signal going to the amplifier when clipping is detected. After
phase adjustments, the input signal is fed to the adder, along with the amplifier
signal(s). Its output goes to a window comparator that detects clipping, then a
pulse-stretching timer to drive the LEDs.
32
Silicon Chip
Australia's electronics magazine
19 op amps, plus three 555 timers and
two dual comparators, along with two
reed relays and associated diodes, a
regulator, resistors and capacitors.
Three indicator LEDs indicate clipping in each channel and show when
the power is on.
As with the block diagram, only the
left channel is shown, with the right
channel being identical; its alternative designators are shown in brackets. Some op amps provide buffering,
some active filtering, while another
(IC12) provides a low-impedance half
supply.
Looking at the audio signal circuitry
first, through the circuit the signal
common is set at half supply (Vcc/2)
so it can swing symmetrically between
GND and the 15-24V DC supply rail.
This means it can run from a standard
DC plugpack without needing a supply voltage inverter section.
The signal comes in at the CON1
RCA socket and is biased to ground
by a 100kW resistor. This discharges
any AC-coupling capacitor that could
be in the signal source. A 150W series
resistor acts as an RF stopper to prevent radio signals entering the first
buffer op amp.
Following this, the signal is AC-
coupled via a 10μF capacitor to the
non-inverting input of IC1a. This
input is biased to the half supply via
a 100kW resistor.
A 13Hz high-pass filter rolls off very
low frequency components of the signal at 40dB/decade; it is 6dB down at
13Hz. The reason we set this roll-off
at 13Hz is so the signal is only 3dB
down at the lowest audible threshold at 20Hz.
Following the filter is the current-
controlled attenuator. This comprises
a 10kW series resistor in conjunction
with LDR1 and trimpot VR2 shunting some signal to the Vcc/2 reference
point. Normally, the LDR is in complete darkness and its resistance is
around 0.5MW (500kW). In this condition, it produces negligible signal
attenuation until clipping is detected.
IC1d acts as a buffer for the attenuator. At IC1d’s output, the signal
is diverted two ways. One is to the
output to the amplifier. This is AC-
coupled to the relay contact and the
100kW resistor in conjunction with the
10μF capacitor sets the output signal
to swing about ground (0V). In other
words, the 10μF capacitor removes the
Vcc/2 DC bias voltage from the signal.
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Fig.3: the full circuit with only the left channel shown – the right channel components are identical and
their designators are shown in brackets. The sections that are common to both channels are the half-supply rail generator,
power supply (including REG1), on-delay and off-delay sections.
Following the relay contact, the signal is sent to the RCA socket (CON3)
via a 150W resistor. This provides a
small series impedance for the op
amp so it won’t oscillate when there
is a capacitive load connected, such
as screened audio cable.
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The second signal path from IC1d
is to the high-frequency phase adjustment circuit. This is a low-pass filter comprising a series 4.7kW resistor, 100kW trimpot (VR2) and a 22pF
capacitor. It produces an overall
high-frequency roll-off that has an
Australia's electronics magazine
adjustable -3dB point from 4.6kHz to
102kHz. It is used to match the phase
shift within the power amplifier at
higher frequencies.
IC1b buffers the signal from this filter. Following this is the low-frequency
phase adjustment circuit. It comprises
May 2026 33
The board is designed to fit into a UB2 Jiffy
box although it also can be incorporated into
other equipment, such as a power amplifier.
a high-pass filter using a 1μF
capacitor and 100kW trimpot in
series with a 4.7kW resistor. The
range of adjustment for the -3dB point
is from 1.6Hz to 34Hz. This allows it
to match the power amplifier output
phase at low frequencies.
IC5 buffers the output of this filter
and its output is applied to the summing amplifier (IC2c) via a 10kW mixing resistor.
Power amplifier monitoring
The power amplifier’s output(s) is/
are connected via CON5 (as well as
going to the loudspeaker[s]). There are
two inputs. One is the non-inverting
amplifier input, while the other is the
inverting amplifier input. Most amplifiers are non-inverting, so that input is
the most likely the one to use. If you
have an inverting power amplifier,
simply use the inverting input instead.
If your amplifier has a bridge-mode
output, where neither terminal is connected to ground but both are actively
driven in anti-phase, connect both outputs to the two inputs. In this case, a
couple of the summing amplifier resistor mixing values will need changing
– more on that later.
Trimpots VR4 and VR5 are used
to set the signal levels for the non-
inverted amplifier input and inverted
amplifier input, respectively. These
are set to match the signal level that is
applied to the amplifier input. If one of
the inputs is not used, the attenuation
is set to maximum to minimise noise.
The signal for each input is AC-
coupled to buffers IC2a and IC2d. The
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Silicon Chip
inverted amplifier signal is applied to the adder via a
10kW resistor, while the non-inverted
signal is inverted using the IC2b unity-
gain inverter first.
We invert the non-inverting power
amplifier output and don’t invert the
inverting power amplifier output so
that when the power amplifier input
and output signals are summed, the
output will be zero. That’s because
we are adding two waveforms that are
180° out of phase.
The adder sums the signals from
the IC5 output and the IC2b and IC2d
outputs. When these signals sum to
zero, the adder output sits at Vcc/2.
Should any of the signals applied to
the adder cause a difference output,
once that reaches a sufficient level, it
will be detected in the following window comparator.
Window comparator
IC3, a dual LM393 comparator, is
connected as a window comparator
detecting excursions 1.25V above and
1.25V below the Vcc/2 voltage. The
470W resistor and 1MW feedback resistors add hysteresis so the comparator
output does not oscillate when signal
at the inverting input (pin 2) of IC3a is
close to the +1.25V reference.
Resistors of the same values for IC3b
prevent this comparator from oscillating if the input at pin 5 via the 470W
resistor is close to -1.25V.
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IC3a and IC3b
have open-collector outputs, so they
can be connected together. These outputs are pulled high via a 10kW resistor to the 12V supply. They remain
high if the voltage from the adder
remains within ±1.25V of Vcc/2. This
is because the inverting input of IC3a
is lower than Vcc/2 + 1.25V at the non-
inverting input, and the non-inverting
input of IC3b is higher than Vcc/2 –
1.25V at its inverting input.
If the adder output goes above 1.25V,
the IC3a output will go low (near 0V);
if it goes below -1.25V, IC3b’s output
will go low.
In either case, this pulls trigger pin
2 of 555 timer IC4 low, and its pin 3
output goes high. The low voltage at
pin 2 also pulls the base of transistor
Q1 low, preventing the 1μF capacitor
at pin 6 of IC4 from charging via the
47kW resistor.
When the comparator outputs go
high again, Q1 switches off and the
1μF capacitor can charge. When this
voltage reaches 2/3 of the 12V supply
(about 8V), the threshold input at pin
6 detects this, and the pin 3 output
and pin 7 discharge output go low.
The 1μF capacitor is discharged via
the 100W resistor at pin 7.
The output remains low for some
50ms after the pin 2 input is taken
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high, extending the clipping indication by 50ms. This allows very short
time periods from the comparator to be
seen by the user by lighting the LED for
long enough to make it visible.
While the pin 2 input of IC4 is
pulled high via the 10kW resistor to
12V, it does not reach 12V because
transistor Q1’s base-collector junction breaks down like a zener diode
at about -5V. So the maximum voltage
at pin 2 is about 5V. This is more than
sufficient voltage to allow trigger operation at pin 2, since the trigger voltage
needs to go below 1/3 of the 12V supply
(about 4V) to be triggered.
When pin 3 is high, it drives transistor Q2 via a 2.2kW resistor, which
in turn drives the Clipping Indicator
LED (LED1) with its current limited by
an 820W resistor from the 12V supply.
The high level at pin 3 also begins
to charge the 10μF capacitor at Q3’s
base via the 10kW resistor, diode D1
and the 100kW resistor. The emitter of
Q3 follows the base voltage but 0.7V
below the base, and this drives LED2
via an 820W resistor. The longer pin 3
of IC4 is high, the higher the voltage
at the emitter of Q3.
This means LED2 is driven with
a varying current depending on the
charge at the 10μF capacitor. When pin
3 of IC4 goes low, the 10μF capacitor
at Q3’s base discharges via the 100kW
resistor over about one second.
When lit, LED2 lowers the resistance of LDR1 at pin 12 of IC1d, so the
audio signal is reduced via the voltage
divider comprising the 10kW resistor, LDR1 and VR1 to the Vcc/2 reference. VR1 is adjusted for the required
amount of attenuation to reduce signal
clipping but not so that the signal level
drops unnecessarily low.
Power supply
Power is from a DC plugpack ranging from 15V to 24V. There is no
power switch; an inline switch can
be used at the DC plugpack output if
required, instead of controlling power
via the same mains outlet as the power
amplifier. Diode D5 provides reverse-
polarity protection. The supply at its
cathode is labelled as Vcc and is typically about 0.7V below the DC input
supply voltage.
The Vcc/2 supply is derived using
two 10kW resistors across this rail,
feeding pin 3 of IC12 and bypassed
with a 100μF capacitor to ground. IC12
is connected as a unity gain amplifier to
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Parts List – Power Amplifier Clipping Indicator
1 double-sided, plated-through PCB coded 01104261, 185.5 × 101.5mm
2 white right-angle PCB-mount RCA sockets (CON1, CON3)
[Altronics P0147A]
2 red right-angle PCB-mount RCA sockets (CON2, CON4) [Altronics P0144A]
2 3-way PCB-mount screw terminals, 5.08mm spacing (CON5, CON6)
2 2-way PCB-mount screw terminals, 5.08mm spacing (CON7, CON8)
1 PCB-mount DC socket (CON9) [Altronics P0621A, Jaycar PS0520]
2 12V DC coil PCB-mount reed relays (RLY1, RLY2)
[Altronics S4101/S4101A, Jaycar SY4032]
2 500kW/2-10kW LDRs (LDR1, LDR2) [Altronics Z1621A, Jaycar RD3485]
6 100kW miniature top-adjust trimpots (VR1-VR3, VR6-VR8)
4 5kW miniature top-adjust trimpots (VR4, VR5, VR9, VR10)
4 14-pin DIL IC sockets
8 8-pin DIL IC sockets
1 50mm length of black 6mm heatshrink tubing
1 strip of Blu-tack or similar non-drying putty
Optional case mounting parts
1 197 × 112 × 63mm UB2 box [Altronics H0152/H0202, Jaycar HB6012]
4 25mm M3-tapped standoffs
8 M3 × 6mm machine screws
4 cable glands to suit 3-6mm cable
Semiconductors
4 TL074 quad JFET-input op amps, DIP-14 (IC1, IC2, IC6, IC7)
3 TL071 single JFET-input op amps, DIP-8 (IC5, IC10, IC12)
2 LM393 dual single-supply comparators, DIP-8 (IC3, IC8)
3 555 timers (not CMOS types), DIP-8 (IC4, IC9, IC11)
1 7812 12V 1A linear regulator, TO-220 (REG1)
1 LM336-2.5 2.5V reference, TO-92 (REF1)
5 BC337 45V 0.8A NPN transistors, TO-92 (Q2, Q3, Q5-Q7)
2 BC327 45V 0.8A PNP transistors, TO-92 (Q1, Q4)
4 1N4148 75V 200mA signal diodes, DO-35 (D1-D4)
1 1N4004 400V 1A diode, DO-41 (D5)
5 5mm high-intensity red LEDs (LED1-LED5)
Capacitors (all 16V radial electrolytic unless noted)
1 470μF 25V
5 100μF
SC7649 Kit ($95 + postage)
3 47μF 25V
Includes the PCB and all onboard
1 22μF
parts. The case and power supply
1 10μF 25V
are not included.
10 10μF
2 1μF
2 1μF non-polarised electrolytic
4 220nF 63/100V MKT polyester
13 100nF 63/100V MKT polyester
2 22pF 50V NP0/C0G ceramic
Resistors (all ¼W ±1% axial)
4 1MW
4 22kW
5 820W
1 470kW
18 10kW
4 470W
17 100kW
5 4.7kW
4 150W
4 56kW
2 2.2kW
2 100W
2 47kW
4 1kW
2 10W
4 20kW (only for use with bridge-tied load amplifiers)
Australia's electronics magazine
May 2026 35
buffer this half-supply rail so that loading on that rail doesn’t affect the voltage much. In other words, IC12’s output provides a low impedance source
for the components fed from this rail.
We use REF1, a 2.5V reference, to
provide the Vcc/2 + 1.25V and Vcc/2
– 1.25V reference voltages for the window comparator. So if Vcc/2 is 7.5V,
the resulting reference voltages will
be 8.75V and 6.25V.
REF1 is supplied current via a 1kW
resistor from Vcc to the plus (+) terminal of REF1 and another 1kW resistor
from the negative terminal to ground.
The resulting 2.5V (actually 2.490V)
reference is across the Vcc/2 supply
using two more 1kW resistors to ensure
it’s centred on Vcc/2. There are 100nF
bypass capacitors for the Vcc/2 + 1.25V
and Vcc/2 – 1.25V rails.
The Vcc supply is bypassed with a
470μF capacitor and feeds the input of
a 12V regulator (REG1) that supplies
12V to the 555 timers and relays.
IC11 is a 555 timer that is used to
switch on the audio outputs about 10s
after power is switched on. This prevents large voltage excursions in the
audio signal by waiting to connect the
signal until all the voltage levels have
stabilised.
IC11 is connected as a monostable
timer. At power-on, the discharged
22μF capacitor at pin 2 triggers the
555 so that the pin 3 output goes high
(12V) and so the bottom connection of
each relay coil is at 12V. At the same
time, transistor Q7 is switched on due
to its base being supplied with current
from the Vcc supply.
There is 12V at each end of the relay
coil contacts, so the relays remain off.
This keeps the relay contacts open
and prevents any signal at the audio
outputs.
After about 10s, the 22μF capacitor
charges to about 8V and the threshold
input of IC11 detects this as being over
2/3 of its supply voltage and takes its
pin 3 output low. This energises the
relay coils, closing the relay contacts
and allowing audio signals to pass.
At switch-off, the 4.7kW resistor supplying current to the base of Q7 does
not have voltage, so Q7 switches off
due to the 100kW pulldown resistor.
That removes power from the relay
coils. Diode D4 clamps the back-EMF
produced by the coils, preventing
damage to transistor Q7 from an excessive voltage transient across the collector and emitter.
Construction
The Power Amplifier Clipping Indicator is built using a double-sided,
plated-through PCB coded 01104261.
It measures 185.5 × 101.5mm. You
can install the assembled PCB within
existing equipment, or it can be fitted
into a UB2-size plastic utility box that
measures 197 × 112 × 63mm.
Follow the overlay diagram, Fig.4,
first by installing the resistors and five
diodes. Check the value of each resistor before installation by checking its
colour code and/or measuring with a
multimeter (the latter is less prone to
errors due to similar colours). Make
sure all the diodes are orientated with
their cathode strips as per Fig.4.
There are four 10kW resistors below
IC2 and IC7 that are marked with an
asterisk. These all need to be changed
to 20kW after setup if you are applying signal to both the inverting and
non-inverting amplifier inputs, such
as when connecting to a BTL amplifier. So you may wish to install these
10kW resistors above the PCB surface
to make them easier to remove later.
We recommend using 10kW first
since setting up is easier if each input
is connected independently and
adjusted for level initially. They can
then be changed to 20kW.
Next, install the sockets for the ICs,
taking care to orientate them with
the notches all towards the top of the
PCB as shown. The two relays can be
installed now as well.
Next on the list are the screw terminals (CON5-CON8), RCA sockets
(CON1-CON4) and DC socket (CON9).
Fig.4: fit the components to the PCB as shown here. Watch the orientations of the ICs, diodes, LEDs, transistors & regulator.
36
Silicon Chip
Australia's electronics magazine
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Make sure the screw terminal openings are towards the nearest outside
edge of the PCB.
For the RCA sockets, we used white
for the left channel and black for the
right channel. Red sockets can be used
for the right channel sockets instead,
as this is the standard colour for the
right channel. However, at the time we
purchased these, the red sockets were
out of stock at Altronics and Jaycar
only sells black.
We sell red and white pairs on our
website at siliconchip.au/Shop/7/2615
because they can be hard to obtain at
times. Still, the colour is not absolutely
critical as you can tell which inputs
and outputs correspond.
There are two different values for
the trimpots, which are all standard
vertical adjust single-turn types.
VR1-VR3 and VR6-VR8 are 100kW,
while VR4, VR5, VR9 and VR10 are
5kW. These can be installed now. Be
sure to place the correct value in each
position. The 100kW trimpots may
be labelled with code 104 (10 × 104)
and the 5kW trimpots with code 502
(50 × 102).
The transistors, REF1 and the 12V
regulator (REG1) can be mounted now,
taking care to orientate them correctly
and not get them mixed up. Q1 and
Q4 are BC327s, while the remaining
transistors are BC337s. REF1 is in the
RIGHT IN
Once the assembly is ready, shrink
down the tubing with a hot air gun.
Make sure the LED and LDR leads are
orientated on the same plane. The LED
leads can then be bent over 180° to be
installed into the anode (A) and cathode (K) holes on the PCB, with the LDR
leads inserted into their corresponding holes (the LDR is not polarised).
Now insert the ICs into their sockets, taking care to match up their pin
1 indicators with the socket notched
ends. Also be careful not to mix up the
8-pin ICs as there are TL071, LM393
and 555s in the same package that need
to be placed in their correct positions.
Panel cutouts
If you are planning on installing the
Power Amplifier Clipping Indicator in
a UB2 enclosure, we have provided
a drilling guide diagram (Fig.7). The
height positions assume that the PCB
is on 25mm standoffs. If you prefer to
use a different standoff size, you can
move the holes up or down to suit.
Cable glands can be used to secure the
leads for LED2 & LED4.
Setting up
The Power Amplifier Clipping Indicator needs to be connected to a power
amplifier for setup (one that does not
have any tone controls or preamplifier). If you use a preamplifier, connect
LEFT OUT
RIGHT OUT
15-24V DC
LEFT IN
same type of TO-92 package as the
transistors.
Install the capacitors next. The
electrolytic types (in cans) need to be
orientated with the correct polarity,
and the 25V-rated capacitors must be
placed where indicated. An electrolytic capacitor’s longer lead is positive, so goes into the pad marked +.
The MKT and ceramic types can be
installed either way around.
LED5 can be installed horizontally with its leads bent by 90° so it
can shine through a hole in the side
of the case. The LED is positioned so
the top of the LED dome is 12mm in
front of the PCB edge and the centre
of the lens is located 5mm above the
top face of the PCB. When bending the
leads, make sure the longer anode and
shorter cathode are inserted into the
correct pads on the PCB.
The clipping indicator LEDs (LED1
and LED3) are intended to be wired
to two-way screw terminals, either
mounted onto the side of the enclosure
or remotely using figure-8 wire into a
hole in the amplifier or loudspeaker.
LED2 and LED4 are used in conjunction with LDR1 and LDR2. These are
within lightproof housings made from
20mm lengths of black 6mm diameter
heatshrink tubing with Blu-tack sealing out external light at each end. This
arrangement is shown in Fig.5.
Fig.6: you can download this front panel artwork from siliconchip.com.au/Shop/11/3623
siliconchip.com.au
Australia's electronics magazine
May 2026 37
Fig.5: the LEDs and LDRs are sealed
in heatshrink tubes using Blu-tack at
each end so external light can’t get in.
The photos show this done for LED2
& LED4.
its output to the Power Amplifier Clipping Indicator input, and the audio
signal output from the Clipping Indicator to the power amplifier’s inputs.
Sometimes, the preamplifier and
power amplifier are separate units.
However, if you have an integrated
power amplifier with an input selector, tone controls and preamplifier
included with the power amplifier (eg,
a receiver), the preamplifier output
and power amplifier input will need
to be accessed.
These outputs and inputs are usually available. They are often joined
with a curved loop of 3.5mm diameter plated brass inserted between the
RCA sockets of the preamplifier output
and power amplifier input. Older units
may have a tape monitor (record monitor) loop that provides the same interconnection for the inputs and outputs.
Initially, set trimpots VR1, VR2,
VR4-VR7, VR9 & VR10 fully anti-clockwise. Set VR3 and VR8 fully clockwise.
Connect LED1 and LED3 to CON7 and
CON8 (temporarily if necessary).
You will need a source of 20Hz,
1kHz and 20kHz tones at around 1V
(RMS) AC. These can be obtained from
a computer, smartphone app or signal
generator. There are also CDs that have
audio tones for test purposes. Computer programs such as Audacity can
produce audio tones. The quality of the
output, especially at 20Hz and 20kHz,
will depend on the sound card/DAC
within the phone or computer.
Connect the signal source to the
Clipping Indicator inputs (CON1 &
CON2). Connect one channel, such
as the left, first. CON3 (CON4) goes to
the left (right) channel power amplifier input, while the power amplifier
output goes to CON5 (CON6), using
the non-inverted input for most amplifiers, or the inverted amp input for
amplifiers that invert.
For BTL amplifiers, only connect
one of the outputs at a time, setting up
each output individually first before
changing the 10kW resistors to 20kW.
With everything powered up and a
1kHz signal applied, adjust the power
amplifier so there is a normal listening volume level, ensuring it is not
clipping. The clipping LED will be
lit because the trimpots haven’t been
adjusted yet. Now adjust the relevant
trimpot, VR4 (VR9) or VR5 (VR10),
carefully until the clipping LED extinguishes. Try to find the middle of the
pot range that allows the clipping LED
to remain off.
Now set the audio signal to 20kHz
and adjust VR2 (VR7) so the clipping
LED goes out. Again, find the middle
of the suitable range if you can. In the
unlikely event that you can’t adjust
the trimpot so the LED goes out, the
22pF capacitor for the left (right) channel may need changing. Use a smaller
capacitor if VR2 (VR7) is wound fully
clockwise.
Next, set the audio oscillator to 20Hz
and adjust VR3 (VR8) so the clipping
LED goes out. If you can’t get the clipping LED to go out when VR3 (VR8)
is fully clockwise, the 1μF capacitor
for the left (right) channel will need
to be larger. This is a non-polarised
(NP) capacitor. It’s unlikely that you
will need to change this value, though.
Now repeat all the same adjustments
for the other channel.
Adjusting the automatic attenuator
(using VR1 for the left channel and
VR6 for the right channel) is best done
with the loudspeakers disconnected.
Apply a normal music signal and wind
up the volume until it starts clipping,
as indicated by the LEDs. Adjust VR1
and VR6 so that the signal attenuates
just enough to stop clipping, except
for occasional momentary flashes from
the LEDs.
After that, if you want, you can test
with the loudspeakers connected and
make adjustments for the best clipping
reduction. Take care that you don’t
damage your ears while doing this –
wear ear protection. If you’re using
high-efficiency loudspeakers and a
high-power amplifier, you may need
SC
to skip this step!
Fig.7: the drilling diagram for the sides of the UB2 jiffy box (197 × 112 × 63mm). This diagram is printed at 60% of actual
size and all dimensions are in millimetres.
38
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
AAEON ●
ABP Electronics
Acconeer ●
ADM Instrument Engineering
Advantech ●
AIM Solder Australia
AIM Training
Altium
Altronic Distributors
AMD ●
Ampec Technologies
AppVision
ASRock ●
Asscon ●
Avnet ●
BDTronic ●
Braemac
Chemtools
CNS Precision Assembly
Coiltek Electronics
congatec Australia
Control Devices Australia
Curiosity Technology ●
Deutsch ●
Digilent Inc/Emerson
Dinkle ●
DLC Display
Dyne Industries
Electro Harmonix ●
element 14
Embedded Logic Solutions
Emona Instruments
Entech Electronics
Epson Singapore
ESI Technology Ltd ●
Europlacer
Eurotherm ●
Evident Australia
Fibocom Wireless Inc
Finenet Electronic Circuit Ltd
Fluke ●
FS Bondtec ●
GKG ●
Globalink Electronics
Glyn Limited
GPC Electronics
GW-Instek ●
Hammond Electronics
Harogic Technologies
Hawker Richardson
HIKMICRO ●
Hua Wei Industrial Co Ltd
Humiseal/Chase Corp ●
HW Technologies
IMP Electronics Solutions
Industry Update
Infineon Technologies
Interflux ●
Inventec ●
Japan Unix ●
JBC Soldering ●
Juki inc Cirrus ●
Keysight Technologies
KOH Young ●
Kolb Cleaning Technology ●
Komax Group inc Schlieuniger ●
Leach (SZ) Co Ltd
Lintek
Liquid Instruments
C14
D25
A28
A11
C14
D34
D34
B30
D1
C14
D32
B8
C14
A27
C14
C3
B28
D34
D12
A5
B16
B10
A11
D1
A3
D1
A28
A13
D1
C14
A26
B2
A16
B35
A11
D22
A11
C26
D36
A32
D10
C3
A27
A9
A20
C36
D10
C32
B14
C28
D10
D33
C3
A8
A24
A35
B3
D22
C3
A27
D22
A27
C14
A27
A27
A27
D20
D28
C27
● denotes – Co-Exhibitor Company/Brand
Stand numbers are subject to change
40
Silicon Chip
Electrone
Rosehill Gardens Event Centre
June 3-4
Electronex – The Electronics Design and Assembly Expo
& SMCBA Conference returns to Sydney, to be hosted at
the Rosehill Gardens Event Centre on the 3rd & 4th of
June 2026. Electronex is Australia’s largest exhibition
for companies using electronics in design, assembly,
manufacture and service.
E
lectronex – The Electronics Design
and Assembly Expo returns to
Rosehill Gardens in Sydney on the
3rd & 4th of June 2026. First held in
2010, Electronex is Australia’s major
high-tech exhibition for electronics
design, assembly, manufacture and
service. Over 100 local and international companies will be represented,
with the latest technology and innovations on display.
Electronex features a wide range
of electronic components, surface
mount assembly, rework and inspection equipment, test and measurement
gear, plus other ancillary products and
services. Trade visitors can discuss
their specific requirements with contract manufacturers that can design
and produce what they need.
Noel Gray, Managing Director of
show organiser AEE, stated “We are
delighted with the response, with the
Expo headed for a sellout. Many companies will be launching and demonstrating new products and technology
at the event. Visitors can discover how
AI is revolutionising the industry.”
The event attracts designers, engineers, managers and other enthusiasts
and decision-makers who are involved
in designing or manufacturing electronic products.
Electronex is the only specialised
event for the electronics industry in
Australia. With many Australian manufacturers focusing on niche products
and high-tech applications, the event
provides an important focal point for
Australia's electronics magazine
the industry in Australia and is a valuable networking opportunity.
Free Seminars
A series of free seminars will also
be held on the show floor, with visitors able to attend on the day with no
pre-booking required. These sessions
will provide an overview of some of
the hot topics and key issues for the
industry.
Topics for the seminars include:
» Advancing Physical AI
» Power Integrity Measurement
Fundamentals
siliconchip.com.au
neX 2026
» Affordable Yet Versatile Multifunction 12-in-1 Test & Measurement
Devices
» Transforming Test with AI
» IoT Beyond Cellular Coverage –
3GPP NTN
» Challenges in PCBA Cleaning &
Coatings and Design for Manufacturing Masterclass
» Securing the Australian Electronics Supply Chain
» Precautions for SDR Series Products Manufacturing
» Building Robots in the Age of AI
siliconchip.com.au
Visit the show website for the program and times: www.electronex.
com.au
SMCBA symposium
The SMCBA will also host an industry symposium designed to engage a
broad spectrum of participants with an
interest in electronics. Attendees will
range from engineering professionals
to dedicated hobbyists. Subjects covered include automated high-volume
production as well as those focused on
hand-assembled prototypes.
This dedicated industry event will
bring together regional leaders, innovators and solution providers alongside the wider electronics community.
It will provide a platform to showcase
achievements and capability advancements, explore opportunities for collaboration, and address current challenges.
Ultimately, the symposium aims to
strengthen the industry as a whole,
supporting the development of sovereign capability and contributing to
national economic diversity.
Competitions will also be held on
the show floor, where visitors can test
their skills against their peers. The
SMCBA will be staging the highly
popular Hand Soldering Competition,
where contestants can enter on the day
to battle to become Australia’s champion Hand Soldering expert.
Register to attend the exhibition
now for free at www.electronex.com.
au
Australia's electronics magazine
LPKF Laser & Electronics ●
Macnica Australia
Marque Magnetics Ltd
Mastercut Technologies
MB Tech ●
MEAN WELL ●
Mektronics Australia
Metcase ●
Microchip Technology
Micron ●
Midori ●
Mission 4
Monolothic Power Systems
Multicomp Pro ●
Multispec Trading
Nordic Semiconductor ●
NPA Pty Ltd
NZFH Ltd
Okay Technologies
ONboard Solutions
Ononmondo ●
On-track Technology
Oritech
Oupiin ●
Outerspace
PCBWay
Pendulum ●
Phoenix Contact
Pillarhouse ●
Powertran ●
Precision Electronic Technologies
Radytronic ●
RAK Wireless
Rapid-Tech
Raspberry Pi ●
Rehm Thermal Systems ●
Re-Surface Technologies
Rigol Technologies ●
Rohde & Schwarz (Australia)
ROLEC OKW - ANZ
S C Manufacturing Solutions
Schurter ●
Semitech Semiconductor
Sensiron ●
Shenzhen Cirket Electronics
Shenzhen Sanpin Mould
Silvertone Electronics
SMCBA
Stars Microelectronics PCL
Suba Engineering
Switches Plus Components
Taoglas ●
TDK Lambda ●
TE Connectivity ●
Techal Solutions
Teledyne FLIR ●
Telit Cinterion ●
Thermo Fisher ●
Uni-T Instruments ●
VGL – Allied Connectors
Whats New in Electronics
Vicom Australia
Win-Source Electronics
Viscom ●
Wurth Electronics
Xentronics
Yamaha ●
Yokogawa ●
A26
B32
C9
A15
C3
A11
B4
D14
C21
D1
A11
A28
A28
C14
A6
A28
C4
B22
D34
C3
A28
C23
D22
D1
B25
A10
D10
D18
C3
D1
D26
D1
A28
D10
C14
C3
C28
B2
C8
D14
A2
C14
D6
A28
C13
B1
C26
D21
D3
A27
C4
A28
A28
C14
C22
D10
A28
A11
D10
C10
A33
D13
B33
C3
B20
A14
C28
D10
electronex.com.au
May 2026 41
ABP Electronics Limited
abp.net.cn
stand D25
ABP provides development and
manufacturing services for PCBA
and finished products. For sample
and small batch orders, we can
provide fast quotation, fast
production and fast delivery.
ABP has ISO9001, ISO13485 and
IATF16949 certifications and we
guarantee our customers stable
and qualified products.
Our high-quality PCBs provide reliable electronic
interconnects and mechanical support. We manufacture singlelayer, double-layer and multilayer PCBs (up to 20+ layers) using
FR-4, high-Tg, aluminium-base, Rogers and other substrates.
Capabilities include fine-line and spacing down to 3/3mil, blind
and buried vias, controlled impedance, HDI structures and
heavy copper designs. Surface finishes include ENIG, HASL,
OSP, immersion silver and hard gold.
All boards comply with RoHS and IPC standards, backed by
rigorous quality controls including 100% AOI, flying-probe/
ICT testing and thermal stress verification. ABP’s PCBA service
provides complete, turnkey manufacturing from component
sourcing to final functional testing.
We support SMT, through-hole (THT), mixed-technology and
advanced packaging including BGA, µBGA, 0201/01005 chip
components, fine-pitch QFN/QFP, and press-fit connectors.
With nitrogen reflow, selective soldering, automated optical
inspection (AOI), X-ray (AXI) and in-circuit/functional testing,
we consistently meet IPC-A-610 Class II and III standards.
Additional processes include conformal coating, potting and
box-build integration when required. ABP maintains a robust
supply chain, ESD-safe and cleanroom environments, full
traceability and component authenticity verification.
Altronic Distributors Pty Ltd
altronics.com.au
stand D1
Altronics introduces the S 8741 and S 8742B HD inspection
cameras. Engineered for installers, electricians and plumbers,
these rugged tools provide a high-definition window into the
most inaccessible spaces.
The S 8741 (bottom) is a 1m Wi-Fi enabled camera that
creates its own hotspot, streaming 720p HD video directly to
your smartphone or tablet with a range of
up to 15m. For more intensive tasks, the
S 8742B (top) offers a 5m reach with a
4.3-inch LCD screen, eliminating the need
for external devices. Both models feature
IP67-rated waterproof camera heads (8mm
and 9mm) and integrated adjustable LED
lighting.
Say goodbye to
disposable canned air.
The T 1348 rechargeable
USB jet blower is a
high-power solution
for cleaning sensitive
electronics. Driven by
42
Silicon Chip
a brushless DC motor reaching up to
130,000RPM, it delivers a concentrated blast
of air to remove dust from PCBs, server racks
and intricate machinery. It has four adjustable
speed settings and a removable magnetic nozzle.
A 2500mAh internal battery provides up to two
hours of operation.
The professional-grade T 1576 hydraulic crimping tool delivers a massive 80kN of force, ensuring
cold-welded, gas-tight connections for copper lugs
from 4mm2 to 70mm2. It comes with eight interchangeable
hexagonal dies, all with a high-strength chrome finish to
resist wear and corrosion. Its ergonomic design includes a
rubberised anti-slip handle and a quick-release knob. The
T 1576 ensures that your high-current connections are safe,
secure and compliant.
The T 2181 interchangeable multi-tool features a single
ergonomic high-carbon steel handle with five specialised,
snap-in heads: heavy-duty pliers, a cable cutter, a wire stripper,
crimping pliers and stainless steel scissors. Each is crafted
from premium materials, such as 60CRV and 40CR13 steel, to
ensure durability. Housed in a compact, portable carry case,
the T 2181 is the ultimate space-saving solution for site visits
and rapid repairs.
The X 0437 USB camera magnifier is a versatile tool that
bridges the gap between traditional loupes and desktop
microscopes, featuring a 2.8-inch integrated
circular screen. Offering four magnification
levels (5×, 7×, 9× and 12×), it is equipped
with dual light sources: seven white
LEDs for standard inspection and
four UV LEDs for specialised detection
tasks like counterfeit identification
and fluid leak analysis.
With SD card support for capturing stills and video, plus a
3.5-hour battery life, the X 0437 is the perfect companion for
the modern technician’s workbench or field kit.
The X 0438 handheld magnifier camera is indispensable
for PCB troubleshooting, analysis and quality control. It has a
vibrant screen with 500× magnification in a compact, handheld
form factor. Its internal 900mAh battery allows for 2.5 hours of
field use, while the USB-C connectivity enables seamless PC
and Mac integration. Adjustable LED illumination eliminates
shadows, ensuring that even the smallest solder bridge or
hairline fracture is visible.
The X 4306A HD digital
microscope is designed for
precision electronics work,
biological study and quality
control, with a 7-inch HD LCD
screen (1024 × 600px) that
provides a clear view of the
smallest components. Equipped
with a high-performance 12MP
camera, the X 4306A offers magnification
levels up to 1200×, making it ideal for
identifying hairline fractures in solder joints
or inspecting intricate PCB traces.
The unit features an adjustable metal
stand that can tilt up to 45°, allowing
for ergonomic viewing and better
access for soldering tools under
...continued on page 51
Australia's electronics magazine
siliconchip.com.au
Mega May
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SAVE 20%
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altronics.com.au
Easy USB
recharging!
12V Lithium
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Driver/Drill
Suitable for light to medium
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T 2126
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X 2386 4W 500 Lumen
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LED Solar Sensor Lights
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69 Pc Dual Ratchet Driver Kit
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C 8825
C 8885
Dual Mic Wireless
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C 5060A
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68W Compact
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A 1014
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Simple TV
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Mini Ultrasonic Cleaner
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D 2367
D 2363B
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Plugs into MacBook Pro/Air USB C connections and provides a full suite of peripheral
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13 In 1 USB C Laptop Docking Station
A handy laptop docking station hub for USB C type
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Handy Desktop
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Rugged USB Torch
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Monitor indoor temperature &
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Easy to read backlit screen.
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A handy 40cm
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X 3229
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At less than $20 you can
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Handy Battery Maintainer
6V/12V Battery Chargers & Maintainers
Utilises a microprocessor to ensure your battery is maintained
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battery service life. Suitable for permanent connection for
battery maintenance. Great for caravans & seldom used vehicles.
Weather resistant IP65 casing. Suits lead acid, AGM & LiFePO4.
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D 2326A
M 8882B
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Recharge TEN devices at once.
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Lithium-Ion Vehicle Jump
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279
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M 8195C
Don’t get stuck with a dud battery!
Suits 12V battery vehicles. 24000mAh rated battery provides up to
2400A peak output when cranking. A 90W USB PD output is provided
for your laptop (use it like a giant battery bank!). It also has a 600
lumen LED torch in built.
Easy
DIY install!
Great for
4WDs
99
$
SAVE 10%
35
SAVE 15%
M 8867
M 8863B
25
140W USB Power Delivery Car Charger
45W USB PD Charger
Charge up all your devices from your vehicle! Provides
140W USB C Power Delivery (PD3.0/3.1). Fitted with
convenient 2m cable.
QuickCharge 3.0 port as well as
a USB C port to suit the latest
devices.
SCAN TO FOLLOW US!
Stay up to date on latest releases,
exclusive specials and news on
our socials.
$
$
N 2099A
Monitor your battery from your phone!
Ensure your battery doesn’t go flat with this handy Bluetooth® battery
monitor. Provides live feedback on your vehicle or auxiliary battery,
plus long term stats.
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AV Savers.
BT 5.4 Audio
Receiver
C 9022B
SAVE $30
Compact wireless
audio receiver
to add streaming
to any existing
amplifier. 10m
range with NFC fast
pairing.
Premium
build &
sound!
99
$
NEW!
49.95
$
A 1104A
SAVE $50
D 2321
289
$
16 Channel Mixer With
USB Player & DSP
A 2652
A great small venue audio mixer! Featuring USB playback
with easy to use controls. Plenty of connection options,
all top mounted. MP3 recording capability and Bluetooth
receiver for your smartphone. USB powered.
SAVE 18%
45
$
FutureTour X ANC Headphones
The latest design from HiFuture Featuring
hybrid active noise cancellation (ANC) that
dynamically silences ambient noise. Premium
build and feel with playback time up to a
whopping 35 hours!
Stay charged. Stay on time!
A stylish bedside alarm clock with 15W wireless charging for your phone & FM radio. Display also shows
calendar & temperature.
SAVE 19%
65
$
A 3104
Mini 8K 2 Way HDMI Switcher
Offering 8K <at> 60Hz resolution this HDMI
selector is ready for the latest high res AV
sources. Auto/manual signal switching.
SAVE $25
SAVE $70
129
$
209
$
8K 4 Way HDMI Switcher
A 3105
Professional 8K 2 Way HDMI Splitter
8K <at> 60Hz splitter with EDID management for seamless
HDMI source splitting. Ideal for venues, business signage
and multi screen display requirements.
8K <at> 60Hz switching with IR remote control
for easy source selection from your couch.
Auto/manual signal switching.
SAVE $60
SAVE $100
179
$
299
$
C 5205
A 4201
Powerful &
compact!
H 8126D
SAVE $30
2x50W RMS Bluetooth
Stereo Amplifier
Stream audio directly from your device to
your speakers in the study or entertaining
area. 3.5mm and RCA inputs. Class D
design. Internal headphone amplifier.
Includes power supply, banana speaker
plugs & 3.5mm to RCA cable.
Slides side to side to make
stud wall mounting easy.
150
$
Boomin’ 200W RMS 10” Sub!
Cantilever Arm TV Bracket
Silky smooth cantilever adjustment, stays just where you
want it to. It even has 15° of tilt adjustment. Engineered
for flat screens up to 90” using 800 x 400mm VESA. Max
weight, 60kg.
This stunning active home cinema subwoofer adds
plenty of bass to any home sound system. Features auto
power on, level control, crossover adjustment, and
phase reversal switch. Size: 442 x 246 x 410mm.
NO STRESS 30 DAY RETURNS!
GOT A QUESTION?
Not satisfied or not suitable? No worries! Return it in
original condition within 30 days and get a refund.
Ask us! Email us any time at:
customerservice<at>altronics.com.au
Conditions apply - see website.
A 3106
T 2460A
Tools Galore!
3 preset
channels for
quick temp
selection.
X 4306A
SAVE $120
SAVE 21%
319
55
$
Micron®
Touchscreen Soldering Station
USB Lithium Rotary Tool Set
A sturdy 100W benchtop soldering station featuring
an all aluminium case and 2.8” touchscreen for quick
temperature and preset selection. 100-500°C temp
range with slimline handle featuring burn resistant
cable. ESD safe design. Fast heat up and recovery.
Works with SMD tweezer handle T 2461A ($219).
Drills, cuts, sharpens, cleans, polishes and engraves
most surfaces, this rotary tool is ideal for enthusiasts, hobby makers, or just odd jobs around the
house. 5 speeds from 5000 to 25000RPM. USB C
recharge with 60 mins operation. 42 accessories
included.
T 2125
NEW!
229
$
$
Digital Microscope Camera
Inspect the finest details with this 12MP digital
microscope featuring up to 1200x magnification,
a vibrant 7” HD display, LED lighting, photo/video
recording, and USB PC connectivity.
SAVE $20
79
$
Q 1058
SAVE $30
SAVE $30
99
Great for
cleaning
jewellery &
more!!
109
$
X 0103A
$
Ultimate all in one
electronic screwdriver set.
Folding Auto Ranging Multimeter
Clean & rejuvenate tiny parts
Uses water and detergent, coupled with ultrasonic
waves to clean jewellery, small parts etc, without
damage - no solvents required. 180x87x58mm tank.
Provides in depth functionality for technicians.
Folding design stays put on any surface while
testing, making it great for auto electrical work.
22
$
T 2748A
SAVE 15%
Handy Plier & Cutter Set
T 2758A
A must have for any electronics enthusiast. Includes:
• Side cutters. • Flat long needle nose pliers. • Flat bent
needle nose pliers. • Long nose pliers/cutters.
• Bull nose pliers/cutters
This Jakemy® electronic screwdriver set is great for
device repairs and other maintenance tasks. Driver
offers three-speed torque options with automatic
power save mode. Unique folding case houses all 180
bits and accessories.
T 1526 1-3.2mm2
T 1527 0.5-2mm2
Best
seller!
SAVE 25%
19
$
5” Side Cutters
Tough carbon steel blades, stay
sharp longer. Ideal for cutting solid
core wires. 130mm.
SCAN TO FOLLOW US!
Stay up to date on latest releases,
exclusive specials and news on
our socials.
T 2130
T 2754B
SAVE 15%
15
$
Or buy 2
for $28
Stainless Steel Nippers
High quality stainless steel
spring loaded nippers for
electronics use.
SAVE 24%
23
$
Strip Wires Faster!
The classic easy squeeze spring
loaded quick action wire strippers.
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Stock up & save.
Handy
Breadboard
Our most
popular
size circuit
development
breadboard.
830 holes.
SAVE 22%
P 1021 Pin to Socket
P 1022 Pin to Pin
P 1023 Socket to Socket
4
$ ea
Ribbon Jumper Leads
P 8657 4 Gland
Easy peel apart cables.
SAVE 19%
SAVE 15%
2 for
$
13
$
24
P 1014A 140pc
P 1009A
SAVE 22%
25
$
7
P 1018A 350pc
SAVE 20%
Breadboard Power Supply
3.3/5V output. 6-12V DC input.
15.95
K 9642
LED Assortment Pack
3mm and 5mm LEDs in green, red,
blue, yellow and white. 300pcs.
H 1801
11.95
$
19.95
$
Model
Type
ONLY
P8655
2 Way
P8656
3 Way
P8657
4 Way
P8659
6 Way
$18.50
$19.95
$24.95
$26.95
SAVE 20%
15.95
$
K 9645 90°
K 9646 Straight
K 9643 90°
K 9641 Straight
1.25mm Connection Kit
2.54mm Connection Kit
Single row header connectors.
Includes male & female pin headers,
plus 2.54mm housings.
Boxed 1.25mm PCB connectors and
plugs in 2, 3, 4 and 5 way. Plus crimp
pins. 150pcs total.
Boxed 2.54mm PCB connectors and
plugs in 2, 3, 4 and 5 way. Plus crimp
pins. 150pcs total.
High Temperature
Polyimide Tape
Great for 3D printing
and other electronics
applications. Leaves no
residue!
Model
Width
NOW
T 2971A
8mm
T 2972A
12mm
T 2973A
16mm
T-Tap Crimp Connectors
T 2974A
19mm
Designed to tap into a wire mid-span
without the need to cut, strip, or solder.
A perfect time-saving solution for vehicle
wiring. 120pcs from 22-10AWG
T 2975A
24mm
T 2976A
36mm
T 2978A
70mm
$9.75
$14.50
$13.50
$13.75
$14
$25
$40
SAVE 10%
22
$
171pcs,
75mm/45mm
lengths in
3.2-12.7mm.
2:1 shrink ratio.
T 1090 0.5mm
T 1100 0.8mm
T 1110 1mm
SAVE 15%
26
$
Quality Leaded Solder
60/40 leaded resin core.
200 gram rolls.
T 1075 0.5mm
T 1078 0.8mm
T 1080 1mm
18
$
57
$
Tin 99.3%, Copper 0.7%.
250gram rolls.
Easy way to
make quick wire
joins. Includes 10
white, 20 red,
15 blue and 5
yellow splices.
SAVE 20%
SAVE 16%
Premium
Lead Free Solder
Solder
Splice 50
Pack
Multi
Colour Heat
Shrink Pack
W 0887
W 0884A
NO STRESS 30 DAY RETURNS!
GOT A QUESTION?
Not satisfied or not suitable? No worries! Return it in
original condition within 30 days and get a refund.
Ask us! Email us any time at:
customerservice<at>altronics.com.au
Conditions apply - see website.
15.95
$
310pc Jumper Header Kit
15%
OFF
NEW!
P 8659 6 Gland
SAVE 20%
SAVE 20%
$
210 pieces of
45mm and
75mm long
heat shrink.
Size 2.5- 20mm.
2:1 shrink ratio.
Great build quality
with IP68 rated
sealing and screw
terminal block.
Z 6355
Pre cut and trimmed solid
core wire for breadboarding.
Red/Black Heat
Shrink Pack
Waterproof
Junction Boxes
$ ea
Prototyping Wire
Z 0003
Wiring problem solver!
SAVE 15%
SAVE 22%
28
$
W 0816
Maker Bits.
SAVE 10%
Z 6240A
UNO R4
27
$
SAVE $20
Top
seller!
99
$
Z 6315A
SAVE 24%
25
$
Includes
UNO R3
165 Piece Arduino Parts Pack
Includes a huge selection of sensor boards, LEDs, pots,
jumper wires, a breadboard, LCD screen and much
more! Plus a UNO R3 compatible board to get you
designing fast. A handy storage case keeps it neat when
you’re finished.
SAVE 15%
Z 6385A
ZW6240A
UNO R4 WiFi
ESP32 Wi-Fi &
Bluetooth Board
42
$
UNO R4 Compatible Boards
A development board integrating
802.11b/g/n WiFi, Bluetooth 4.2 and
BLE. Fully Arduino compatible and perfect for wireless projects.
Get designing on the UNO R4 compatible
development boards - same form factor as earlier
Arduinos for maximum shield compatibility, but with
expanded memory and faster clock speed.
Z 6497
Z 6317
SAVE 24%
SAVE 19%
15
$
Temperature & Humidity Controller
A 2 channel board which activates a connected load
at preset temperature (-20 to 60°C) or humidity
(0-100%). Runs off 12V DC with 10A relay outputs.
Z 6319
SAVE 19%
24
8
$
Digital Temperature Controller
The STC-1000 controller is a 12V DC heating/
cooling controller allowing you to activate or
deactivate loads up to 10A. Includes 1m sensor.
$
Precision Temperature Controller
12V input with single 10A relay for on/off control.
Waterproof sensor with -30 to +110°C range and 0.1°C
accuracy. In-built 3 digit display.
SAVE 22%
14
$
Z 6316
Z 6494
SAVE 28%
SAVE 24%
20
$
Z 6489
15
$
Bluetooth Relay Board
60W Digital Power Amp
Dual 12V 10A relay and control
board with the ability to switch
on and off loads using eWeLink
app on your phone.
A high-performance audio amplifier
designed for applications requiring
compact size, low resistance, and high
power output. TPA3118 chip.
Z 6427
Wi-Fi ESP8266
Relay Module
A handy Wi-Fi activated
3A relay module for
wireless switching applications. 3.3V input.
Z 6334
SAVE 19%
SAVE 24%
8
$ ea
6
$
Turn a USB charger
into a power supply.
Allows you to connect to a USB
PD power supply and output 5,
9, 12, 15 or 20 Volts.
DC-DC Buck
Module
Generate a lower voltage
output from a higher
supply. 3-40V DC in,
1.5-35V DC out. 3A max.
Sale Ends May 31st 2025
Shop in-store at one of our 11 locations around Australia:
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© Altronics 2026. E&OE. Prices stated herein are only valid until date shown or until stocks run out. Prices include GST and exclude freight and insurance. See latest catalogue for freight rates.
B 0005
the lens. It has onboard microSD recording for photos and
video, plus USB connectivity for PC-based analysis.
congatec Australia Pty Ltd
congatec.com
stand B16
congatec has unveiled the industry’s most comprehensive
lineup of Computer-on-Modules (COMs) powered by Intel Core
Ultra Series 3 processors, delivering exceptional on-module AI
performance and eliminating the need for discrete accelerator
cards in many embedded applications. There are five new COMs
across four form factors, from COM-HPC Mini and COM-HPC
Client to COM Express Mini and COM Express Compact variants.
With up to 16 CPU cores, an integrated NPU5 delivering up
to 50TOPS for low-power AI inferencing, and up to 12 Xe3 GPU
cores supporting ~120TOPS, developers can run local NLP, LLM
execution, image classification, sensor fusion and advanced
SLAM without added hardware. With high-speed I/O such as
PCIe Gen5 and USB4, these COMs enable high-bandwidth
connectivity and performance density in size, weight and power
(SWaP)-optimised designs.
The broad OS support—including Windows, Linux and realtime systems—plus application-ready aReady.COM options
accelerate development, reduce system complexity and cut
time-to-market for embedded AI solutions.
The conga-HPC/mIQ-X COM-HPC Mini Computer-onModule, powered by Qualcomm Dragonwing IQ-X processors,
has up to 12 Oryon CPU
cores and a dedicated
Qualcomm Hexagon NPU
capable of up to 45TOPS
AI performance. The
credit-card-sized module
(95 × 70mm) integrates
up to 64GB of soldered
LPDDR5X memory and
supports an extended
temperature range of
-40°C to +85°C. Connectivity includes 2× 2.5GB Ethernet, up
to 16 PCIe Gen3/4 lanes, USB4, USB 3.2 and multiple camera
interfaces.
The module has exceptional AI and graphics processing with
an integrated Adreno GPU supporting up to 8K resolution and
three displays, enabling advanced vision and analytics without
external accelerators. With support for UEFI firmware and
Windows on Arm, development cycles are simplified, reducing
time to market. It is also available as application-ready aReady.
COM, with pre-validated OS and software building blocks to
jump-start deployments and lower design effort and cost.
congatec is expanding its railway certification program for
the COM Express module family. In accordance with IEC 60068
environmental standards and IEC 61373 railway shock and
vibration requirements, congatec’s COM Express Compact Type
6 modules are proven for longterm operation under extreme
mechanical and climatic stress.
congatec’s new congaTCRP1 COM Express 3.1 Type
6 compact computer-onmodules integrates the latest
AMD Ryzen AI Embedded P100
Series processors to accelerate
embedded AI applications
with a balanced mix of CPU,
siliconchip.com.au
GPU and dedicated AI performance. These modules run in
environments from -40°C to +85°C, making them suitable for
sectors such as transportation, smart infrastructure, medical
technology, robotics, retail/POS and industrial automation.
Combining AMD Zen5 performance and energy-efficient
Zen5c CPU cores, an RDNA 3.5 GPU and an XDNA 2 NPU
delivering up to 50TOPS, it achieves up to 59TOPS of combined
AI inferencing performance. The TDP is configurable from 15W
to 54W with up to 96GB of DDR5-5600 RAM and optional ECC.
Connectivity includes PCIe Gen4, 2.5GbE, USB3.2 and SATA/
NVMe. It is available in application-ready aReady.COM variants.
Control Devices Australia Pty Ltd
controldevices.com.au
stand B10
The Micra-M Max digital
panel meter sets the
b e n ch ma r k fo r h i g h performance industrial
monitoring. Engineered for
maximum versatility, this
digital panel meter bridges
the gap between hardware
reliability and modern IoT connectivity. It is
a multi-input powerhouse, supporting process signals (mA,
V), temperature sensors (Pt100, thermocouples J/K/T/N), and
load cells.
Its tri-colour programmable display allows operators to
assign green, amber or red to specific alarm states for instant
visual diagnostics. The latest firmware supports an extended
display range of up to 99,999 points.
• Integrated Bluetooth enables seamless setup via the Ditel
Connect Mobile App, while a built-in webserver allows real-time
data viewing from any browser
• Native MQTT compatibility ensures automatic data
transmission to the cloud, facilitating remote monitoring and
asset management
• A REST API allows developers to integrate live data into
third-party software or automation platforms
The PK CAN-bus keypad series redefines user interaction
by integrating programmable OLED displays directly into the
keypad’s keys. This allows a single device to manage complex
functions without cluttering the control panel. Each key acts as
a functional window, capable of showing icons, scrolling text,
or real-time status updates.
• Users can toggle through sub-menus where key labels
change instantly based on the current operation
• Immediate confirmation of commands through colour
changes or animated icons
• Consolidates multiple bulky switches into one compact,
intelligent array
Despite its high-tech display integration, the PKD Series
does not compromise on APEM’s signature
durability. Its robust construction is designed
for long-cycle reliability. The keys provide a
positive tactile snap.
The APEM PKI Series stands out as an
advanced solution for complex industrial
control. The PKI Series integrates CANbus technology, transforming a standard
keypad into an intelligent node within
a networked system. Using J1939 or
CAN-open protocols, these keypads
significantly reduce wiring complexity,
Australia's electronics magazine
May 2026 51
requiring only a four-wire connection to manage multiple
functions. This simplifies installation and enhances system
diagnostics and reliability.
It is built for the extremes and designed for rugged
environments—from agricultural machinery to heavy
construction equipment. The PKI Series boasts:
• High-intensity RGB LED backlighting ensures visibility in
low-light conditions, with programmable status indicators for
real-time feedback
• Engineered with high-travel silicone keys that provide
distinct tactile feedback, even when operated with heavy
gloves
• Rated at IP67 and IP69K, these units are impervious to
high-pressure wash-downs, dust and salt spray
Digilent Inc
digilent.com
stand A3
Our customisable solutions accelerate development for even
the most experienced professionals, while maintaining a low
barrier to entry for advancing engineers.
The new USB 3.0 Analog Discovery Pro 2440 (shown below)
and Analog Discovery Pro 2450 portable high-resolution MSOs
deliver serious measurements for engineers. They have:
• Four analog inputs at either 12-bit, 600MS/s, 100+MHz
bandwidth (ADP2440) or 8-bit, 1GS/s, 200+MHz bandwidth
(ADP2450)
• Dual mode and low latency memory segmentation
• Arbitrary waveform generator with 15MHz bandwidth
• Freely allocatable deep buffer memory
• 16 digital inputs/outputs supporting a variety of
communication protocols
• Bode plot, dedicated FFT, impedance analyser, bus
analyser, data logger and more
• Extensive and powerful software support with WaveForms
and WaveForms SDK
element14 Australia
au.element14.com
stand C14
The UP Xtreme PTL Edge is a slim computer with an Intel
Core Ultra Series 3 CPU:
• DDR5 7200 Dual Channel SODIMM × 2, up to 128GB
• HDMI × 2, DP × 2 via USB4.0 Type-C
• USB 3.2 Gen 2 (Type-A) × 2, USB 4.0 (Type-C) × 2, 2.5GbE
LAN × 2
52
Silicon Chip
• M.2 2230 E-Key × 1, M.2 2280 M-Key × 2
• Onboard TPM 2.0
• 19V~36V DC input
Advantech AMD Ryzen AI Embedded P100 series platforms,
based on the latest Zen 5 architecture, deliver up to 12
cores and 24 threads with AVX-512 support, including VNNI
and BFLOAT16 for high compute density and accelerated AI
performance. Integrated RDNA graphics provides up to 30TOPS
via the AMD ROCm ecosystem, supporting up to four 4K/120Hz
displays, including a hardware codec accelerator.
The XDNA 2 NPU adds up to 50TOPS at lower power, enabling
up to 80TOPS total AI performance (approximately 160TOPS
dense) within a heterogeneous architecture designed for
low latency and power efficiency across Windows and Linux
environments. The platform supports DDR5-5600 memory up
to 128GB, PCIe Gen 4 ×8, NVMe, HDMI 2.1, DisplayPort 2.1,
and USB4, with TDP options from 15W to 54W, operating from
-40°C to 105°C.
The AMD Ryzen AI Embedded P100 Series boards are
validated for Windows 11 LTSC and Ubuntu LTSC. The EdgeAI
SDK enables efficient cross-platform AI deployment using
AMD Ryzen AI capabilities, while DeviceOn provides remote
monitoring, predictive maintenance and centralised device
management.
Advantech provides a full portfolio of Ryzen AI Embedded
P100 Series platforms for diverse EIoT applications:
The MIO-5380 is a 3.5-inch single board computer with:
• MCIO flexible PCIe extension for GPU cards
• EdgeBMC for out-of-band remote management and
recovery
• USB 4.0 for external MXM GPU and USB Type-C for 100W
Power Delivery (PD)
The AIMB-2210 Mini-ITX motherboard has:
• USB Type-C Alt Mode with optional 100W PD, supporting
four independent 4K displays
• 5 × USB 3.2, 2 × USB 2.0, 1 × USB-C, 2 × 2.5GBE, 4 × COM
ports (optional TTL and CCtalk)
• Multiple expansions: PCIe Gen4 × 16, M.2 M-key, and E-key
The SOM-6874 is a COM Express Compact Type 6 with:
• DDR5-5600 dual-channel SODIMM memory up to 96GB
• 4 independent 4K displays with LVDS/eDP and HDMI/
Display Ports
• Up to 18 PCIe lanes for high-speed connectivity
• Multiple I/O expansion: up to 18 PCIe lanes, 2.5GBE LAN,
USB 3.2, USB 2.0
The EDGE+ VPR-7P132 Mini-ITX embedded motherboard is
a powerful combination of AMD’s Ryzen AI Embedded V4526iX
processor (Zen 5 CPU, RDNA 3.5 GPU, 50+ TOPS XDNA2 NPU)
with AMD’s Versal AI Edge Gen2 VE3558 adaptive SoC (world
class programmable logic, ARM CPUs and AI engines). It
supports dual 4K displays, 10GbE, M.2 WIFI, SSD storage, and
USB interfaces to offload the Versal adaptive SoC of non-time
critical functions.
Schurter’s (schurter.com/en) EKO series
of fuses is engineered for demanding highvoltage environments, offering protection up to
1000V DC (and 1250V AC for selected models)
and current ratings from 50A to 1100A. With
a breaking capacity of up to 50kA DC,
these square-body fuses deliver safety and
reliability.
Schurter’s new Pyrofuse-APO series sets a
new benchmark for safety. Unlike conventional
Australia's electronics magazine
siliconchip.com.au
fuses, the APO Fuse operates actively. In the
event of a short circuit or accident, the
control unit sends a trigger signal to an
integrated micro gas generator. Within
milliseconds, the generator produces a high
pressure that drives a piston to mechanically
sever the solid copper busbar. The resulting
arc is safely suppressed in a dedicated extinguishing chamber.
The outcome is complete galvanic isolation in less than two
milliseconds (as fast as 0.9ms).
The new ARO fuses from Schurter provide robust protection
for HV applications, integrating seamlessly into
charging cables and connectors. Rated voltage:
250V AC; rated currents: 16A, 32A and 63A;
breaking capacity: 50kA.
The innovative surface-mount USE 2410 fuse from Schurter
is a quick-acting F fuse in the 2410 footprint, designed for 125250V AC and 86-125V DC. With a temperature range from
-55°C to 125°C, it is suitable for demanding conditions.
It has a breaking capacity up to 200A and precise
tripping. The compact form factor saves space.
The new Schurter USL 0603 low-current fuse has an
extended creepage distance of 1.1mm (pad-to-pad), meeting
the requirements of IEC 60079-11 for 60V DC applications. It
is one of the few fuses in the 0603 format that can be used in
ATEX applications, such as in the oil and gas industry, chemical
processing or mining.
The Schurter MSM II mechanical switch family is growing,
with a variant that uses a common anode to control the RGB LED
illumination. This combines the familiar, robust mechanics with
visualisation technology for clear feedback, easy integration,
and maximum reliability in control and operating solutions.
The Schurter EDC (Electronic Direct Current) switch was
specifically engineered for the reliable switching of direct
current in compact systems. It combines the mechanical
precision of a microswitch with integrated power electronics,
making it completely arc-free. When the
contact is opened, the integrated
electronics detect the disconnection
process at an early stage and interrupt
the current in a controlled manner before
an arc can occur.
The MSS-IO is based on the successful
Schurter MSS electronic switch, which has
been expanded to include an IO-Link module.
Instead of capacitive technology, a precise
change in electrical resistance is used for switch
detection; sensitive enough to detect the smallest changes in
pressure, robust enough for industrial series processes.
Emona Instruments Pty Ltd
emona.com.au
stand B2
Established in 1979, with a head office in Sydney and branch
offices in Melbourne, Brisbane, Adelaide and Perth, Emona
Instruments Pty Ltd is a high-tech engineering company
specialising in electronics, electrical, education and additive
manufacturing equipment. Rigol Technologies, represented in
Australia by Emona Instruments for over 20 years, are launching
three new series of high-performance test instruments at
Emona’s display at Electronex 2026.
Rigol’s new DNA5000/6000 series vector network analysers
(VNA) bring network analysis to every engineer’s test bench.
They provide a frequency range from 5kHz to 26.5GHz,
siliconchip.com.au
Rigol's new
DNA5262 and
DNA6264
vector
network
analysers
support two or four test ports and deliver high-performance
RF component characterisation with powerful S-parameter
measurement capability.
Rigol’s new RSA6000 series real-time spectrum analysers
offer bandwidths up to 26.5GHz. Featuring up to 200MHz
real-time bandwidth, low phase noise and advanced analysis
modes, they capture transient signals and complex interference
efficiently for R&D, wireless, EMI and compliance testing
applications.
Rigol’s MHO900 series high-resolution digital oscilloscopes
combine portability with powerful mixed-signal performance.
Offering up to 800MHz (1GHz special edition) bandwidth,
4GSa/s sampling, 12-bit resolution and deep memory, they
deliver precise signal visibility, fast waveform capture and
advanced analysis.
Emona’s Electronex 2026 display will cover oscilloscopes,
generators, power supplies and EMC test equipment through to
our range of 3D printers and additive manufacturing solutions.
The latter range from prototyping in composites through to
production-scale printing in thermoplastics and metal.
Fibocom Wireless Inc
fibocom.com/en/
stand D36
Fibocom’s LE271-GL is a global LTE Cat.1 bis module offering
single-SKU worldwide connectivity for IoT devices. Its compact
17.7 × 15.8mm design is pin-compatible with Fibocom’s MC661,
LE270 and LE37X series. Supporting both FDD-LTE and TDD-LTE
bands, LE271-GL ensures global frequency coverage.
The module is built on an OpenCPU architecture and
Australia's electronics magazine
May 2026 53
ISO13485:2016 certifications and exports to Southeast Asia,
Australia, Europe and the USA.
Globalink Electronics (S) Pte Ltd
https://globalink-e.com
achieves registration in under 3.5 seconds. With ultra-low
power consumption, its microamp-level sleep current makes
it ideal for asset tracking, IP cameras, new energy systems
and consumer electronics. It has rich features such as eSIM,
dual-SIM, LBS + Wi-Fi positioning, and multiple IoT protocols.
The Fibocom LE270-EU delivers exceptional power efficiency
and stability for IoT applications across Europe. It achieves as
low as 2.5µA in PSM mode and under 100µA in the IDLE state.
Even in TCP keep-alive scenarios with a one-minute heartbeat,
the average power consumption remains below 2mA.
Fibocom’s SC126-EAU module:
• Comes with a built-in 64-bit Arm Cortex-A53 quad-core
processor at up to 2.0GHz
• Supports dual Image Signal Processors and multi-channel
camera input
• Support up to a 1080p <at> 30FPS display and 1080p <at>
30FPS video recording
• Is equipped with the latest Android operating system,
allowing long-term lifecycle usage
• Planned multiple regional versions for global AloT
applications
Fibocom’s AI Lawn Mower Terminal features:
• Autonomous navigation: AI-powered path planning and
obstacle detection for precise and safe mowing
• Real-time monitoring: track mower status, location and
battery levels remotely via mobile or cloud platforms
• Smart scheduling & control: set mowing schedules, adjust
cutting modes, and receive notifications anywhere
• Energy Efficiency: optimised operations for longer battery
life and reduced energy consumption
• Seamless integration: connects easily with smart home
ecosystems and IoT platforms
Finenet Electronic Circuit Ltd
www.finenetpcb.com.cn/?lg=en
stand A32
Founded in 2000, Finenet Electronic Circuit Ltd is one of the
largest integrated solution providers in the high-tech PCB
manufacturing industry, with a monthly production capacity
of 50,000m2.
The company integrates production, sales, and service,
with its main products including single-sided, doublesided, multi-layer, HDI, impedance-controlled, metal base
(aluminium substrate),
press-fit and flexible
PCBs. Surface finishes
include lead-free HASL,
ENIG, chemical tin and
OSP, serving industrial,
automotive, consumer
electronics, lighting and
power applications.
T h e co m p a n y has
recognition as a Guangdong–
Hong Kong Clean Production Partner. Finenet has achieved
UL, IATF16949:2016, ISO9001:2015, ISO14001:2015, and
54
Silicon Chip
stand A9
Globalink Electronics is an established EMS service
provider with fully integrated manufacturing
facilities in China. Its services include design
verification, sourcing, procurement and
final assembly, including the production
of buzzers, transducers and switches.
Glyn Pty Ltd
glyn.com.au
stand A20
Onomondo provides IoT connectivity infrastructure that
eliminates the cost and complexity of traditional telecom
systems. Our software-defined core network integrates directly
with 680+ carriers in 180+ countries, giving programmable
control over connectivity settings and the ability to deploy
globally without multiple regional contracts. At Electronex, we
will demonstrate our SIM management platform, packet-level
troubleshooting, and live SoftSIM-enabled devices.
TDK’s compact GUS series of single-output AC-DC industrial
power supplies are available
with 12V, 24V, 36V and 48V
outputs in an economic,
compact footprint and can
deliver up to 350W, 600W
or 1000W. GUS350 is
convection-cooled, while
GUS600 and GUS1000 have
an integral cooling fan. Remote on/off is an option
for all models. Efficiency of up to 95.5% (model dependent) is
possible.
Compact HWS3000G AC-DC power supplies can deliver
1500W with a low-line input voltage of 85-132V AC and 3000W
at high-line 170-265V AC. The HWS3000GT is rated at 3000W
with a three-phase input voltage of 170-265V AC. With nominal
output voltages of 24V, 48V, 60V and 130V, the output voltages
and currents are fully programmable (CV/CC) from zero up to
their maximum rating using a serial RS485 interface (MODBus
protocol), 1-5V or 4-20mA signals. Up to three units can be
connected in series and/or ten units in parallel.
The DUSH 960W uninterruptible
power supply for DIN rail applications
has wide input and output voltage
ranges of 10-60V DC in and 10-58V DC
out. It can be deployed in a multitude
of applications such as industry
automation, plant engineering,
building control systems, test &
measurement, or information &
communication technology.
The D1SE series is a cost-effective
and reliable power supply, with
outputs of 120W, 240W and 480W and
AC or DC operation. They are equipped with push-in terminals
and, for applications in challenging environments, models with
coated PCBs are available.
The DDSM series of DC-DC converters offer 120W and 240W
output powers in a compact, lightweight design with wide input
and output ranges. The series is fully digitally controlled; the
7-segment display shows precise system values, status and
Australia's electronics magazine
siliconchip.com.au
alarm codes. It can be operated directly via three push buttons.
The DDSM can be operated with the PowerCMC software tool
using the Modbus over USB connection.
Suitable for 19-inch rack mounting, GENESYSAC (GAC)
programmable power sources have a very high-power density.
The series offers power levels
of 2kVA and 3kVA
(1U) or 6kVA
a n d 9 k VA
(3U), with the
possibility of
paralleling
units to increase the output
power. Its auto-ranging power output can be single-phase or
three-phase, with an adjustable voltage from 0V to 350V AC
and ±500V DC (GAC-PRO models). The frequency range is 16Hz
to 1.2kHz (up to 5kHz for the GAC-PRO).
Remote programming methods include built-in LAN, USB,
RS232 and RS485. The GAC-PRO models include the realtime analog control functionality necessary for complex test
scenarios. The series has a full-colour, multi-language LCD
touch panel display and a software GUI interface. Optional
avionics and IEC test libraries are available.
Hawker Richardson
https://hawkerrichardson.com.au
stand C28
Our complete turnkey SMT solutions bring together world-class
equipment, intelligent automation and software-driven process
control into a fully integrated production environment. From
equipment supply to commissioning and ongoing support,
each SMT line is engineered to deliver consistent quality, high
throughput and repeatable manufacturing:
• High-performance pick and place systems for speed,
accuracy, and flexible component handling
• Inline quality control, incorporating SPI, AOI and X-ray
inspection to detect defects early
• Advanced reflow systems delivering stable thermal
profiles and consistent soldering results
• Precision rework stations for BGA, QFN, CSP and finepitch components
At the heart of every turnkey SMT line is YSUP intelligent
SMT software. YSUP connects all machines into a single,
coordinated workflow through machine-to-machine (M2M)
communication with:
• Closed-loop feedback that automatically feeds inspection
results back upstream to prevent defects from progressing
down the line
• A visual data editor to simplify programming, reduce setup
time, and minimise operator error
• Real-time dashboards providing live visibility of
performance, defects, and line efficiency
• Intelligent algorithms that automatically detect and
correct issues such as component polarity
Ya ma ha ’ s n e w Y R M
placement machine is
designed for odd-form and
specialised components
that standard SMT heads
struggle with. Odd-form
components (such as large
connectors, transformers,
and sockets) historically
required manual assembly.
siliconchip.com.au
High-capacity heads like the LM head can handle them
automatically, improving yield and reducing labour costs.
Modern EVs rely on heavy-duty, high-current connectors and
power modules that standard SMT heads cannot lift or place.
The rapid expansion of generative AI has increased demand for
large, high-pin-count components such as BGAs and FPGAs,
which require the precise force control and handling capability
of LM-class heads. The LM head’s ability to mount parts up to
500g, 90 × 139mm in size and 40mm in height, along with other
heads for smaller parts, allow for this extreme range.
The LM Head has 100N placement-force management for
press-fit parts, and vision software recognising up to 20,000
BGA balls.
Now exclusively represented in Australia and New Zealand by
Hawker Richardson, PDR brings world-leading rework capability
to local electronics manufacturers and repair specialists.
Designed for today’s increasingly complex PCBs, PDR Focused
IR systems deliver precise, repeatable rework without thermal
shock or unnecessary stress to surrounding components:
• Focused infrared heating targets only the component
being reworked, ensuring controlled, stress-free removal and
replacement of BGAs, QFNs, CSPs, LEDs and leadless devices
• PC-based closed-loop thermal management precisely
controls both component and board temperatures, delivering
repeatable results and protecting sensitive assemblies
• Tool-free, gas-free operation with instant thermal response
simplifies setup, reduces operating costs and creates a cleaner,
more efficient rework environment
• From entry-level systems like the IR-E1 to advanced semiautomated platforms, the modular design allows systems to
scale as rework complexity and production demands increase
Hua Wei Industrial Co Ltd
www.hwlok.com
stand D33
The new range of TEFZEL (ETFE) cable ties is engineered for
applications requiring exceptional chemical resistance, thermal
stability and long-term durability. Made from high-performance
fluoropolymer material, the product delivers outstanding
resistance to extreme temperatures, UV exposure, chemicals
and ageing.
TEFZEL cable ties maintain mechanical strength and
dimensional stability across a wide operating temperature
Australia's electronics magazine
May 2026 55
range, ensuring reliable fastening performance where
conventional nylon ties may fail. The material’s flame
resistance and low-smoke characteristics further enhance
safety in critical installations. A precision-moulded locking
mechanism provides secure fastening while allowing efficient,
tool-free installation.
These cable ties are particularly well-suited for aerospace,
automotive, electronics, chemical processing, and industrial
equipment applications, as well as environments exposed to
fuels, solvents, or corrosive substances.
PA66 nylon cable ties are heat stabilised up to 120°C (248°F).
They are UL and CE certified for industrial and professional use:
• Internal serrations ensure a secure and positive grip on
cables and pipes
• Optimised head design delivers high tensile strength
while maintaining low insertion force
• Available in a wide range of sizes to suit almost any
application
• Flammability rating: UL94 V-2
• Colours available: black, red
IMP Electronics Solutions
imppc.com.au
stand A24
The new DT035CTFT series of 3.5-inch colour IPS
LCD modules features a high-resolution 320 ×
480 pixel display. With a super-high-brightness
backlight and a wide IPS viewing angle, these
displays ensure excellent readability and
consistent colour performance in indoor and
outdoor environments. Available with an
optional capacitive touch panel, this 3.5inch IPS TFT is an ideal LCD for industrial,
consumer and medical devices.
The DT050CTFT series of 5.0-inch
colour IPS LCD modules has an 800 ×
480 resolution, offering crisp visuals,
wide viewing angles and consistent
colour reproduction. Its super-highbrightness LED backlight ensures
excellent readability in any lighting
condition, including direct sunlight. An optional
capacitive touch panel provides responsive,
intuitive input for interactive applications.
The EEMB high-capacity lithium polymer
battery is designed for greater energy density, safer, wide
temperature range and high power delivery in ultra-thin,
flexible form factors. By optimising electrode structure and
materials, the high-capacity batteries achieve higher energy
density without increasing size.
EEMB ultra-low-temperature battery technology delivers
reliable performance in extreme cold environments. From
emergency rescue equipment in polar regions and high-end
outdoor gear to drone logistics and monitoring systems, EEMB
low-temperature batteries provide critical power support and
operate reliably in the most demanding conditions.
ONBoard Solutions Pty Ltd
onboardsolutions.com.au
stand C3
HumiSeal 1B59 SEC is a synthetic rubber-based conformal
coating designed to enhance sharp edge coverage while
providing superior moisture and environmental protection.
This latest formulation optimises edge retention, ensuring
uniform thickness across complex geometries. It is fast-drying
56
Silicon Chip
The HumiSeal 1B59 SEC coating shown wet (left) and dry (right).
and easy to apply, suitable for spraying, dipping and selective
coating processes.
Its superior moisture and chemical resistance provide
robust environmental protection against harsh conditions.
The UV tracer allows for easy inspection under UV light.
Ideal applications for HumiSeal 1B59 SEC are high-reliability
electronics, automotive and aerospace PCBs, and industrial
and consumer electronics requiring moisture resistance.
PROMOSOLV DR3 from Inventec Performance Chemicals
is a non-flammable, low-GWP solvent designed as a highperformance replacement for 3M Novec 7030 in light-duty
cleaning and rinsing applications.
It delivers exceptional cleaning performance with very low
surface tension (13.6 dynes/cm), enabling deep penetration
into tight geometries and complex assemblies. It is thermally
and chemically stable in use, offering short cleaning, rinsing
and drying times in both mono-solvent vapour phase and
co-solvent processes.
With no flashpoint, PROMOSOLV DR3 supports safer
workplace operation while aligning with evolving environmental
regulations. The product is compatible with all metals and
alloys, including sensitive substrates, and demonstrates
strong material compatibility across a wide range of
applications.
Photonics’ laser depaneling systems deliver highprecision, non-contact separation of PCBs, enabling
manufacturers to achieve clean, burr-free edges
without mechanical stress. Traditional mechanical
depaneling methods can risk board damage,
delamination, or component stress. Photonics’
laser-based approach uses a controlled, high-energy
beam that precisely cuts the substrate according to
programmed patterns.
The system utilises advanced laser optics and motion control
to produce repeatable results with a range of materials, from
standard FR-4 to high-performance laminates and flexible
substrates. Non-mechanical depaneling eliminates tool wear,
reduces particle generation and minimises post-process
cleaning. With integrated vision systems
and programmable cut paths, the
modular architecture enables
seamless integration into SMT
and box-build lines.
The MBtech NC25 precision
cleaning system is designed
to address a wide range
of contaminants, including
flux residues, particulates,
oils and process soils. Built
around a robust wash-rinsedry architecture, it uses
carefully controlled spray
dynamics and chemical
management to achieve
Australia's electronics magazine
thorough cleaning across complex assemblies, fine geometries
and mixed-technology boards.
The system’s modular design allows flexible configuration
to match customer process requirements, including ultrasonic
enhancement and rinse stage optimisation.
PCBWay
pcbway.com
stand A10
PCBWay’s transparent PCB
is manufactured using a
halogen-free transparent
resin substrate. Unlike
traditional glass-based
substrates, it delivers
high optical clarity while
maintaining excellent mechanical and thermal performance.
The material is lightweight, heat-resistant, and impactresistant, making it suitable for advanced applications where
both transparency and reliability are required.
Depending on board thickness, transparent PCBs can
be combined with flexible displays and are well suited for
innovative products such as transparent displays, transparent
televisions and smart devices. The material is fully compatible
with standard FR-4 processing, allowing direct integration
into existing production lines without additional investment,
ensuring high manufacturability and process adaptability.
Transparent PCBs have outstanding resistance to yellowing,
chemicals, heat and CAF (Conductive Anodic Filament),
meeting demanding design requirements for high reliability
and superior optical performance.
They have low moisture absorption and are suitable for leadfree reflow soldering, with high impact resistance, superior
CAF resistance and reliable through-hole performance and
solderability.
Transparent PCB specifications:
• Flammability rating: 94V-HB
• Maximum operating temperature: 130°C
• Layer count: 1-6 layers
• Base material: transparent FR-4
• Solder mask: transparent
• Board thickness: 0.002in (0.05mm) to 0.080in (2.0mm),
suitable for both small and large formats
• Copper weight: 1/3oz to 5oz, available for multi-layer and
double-sided boards
• Film format: roll material or small panel formats
• Glass cloth (prepreg): 106, 1080, 2116, 7628 or customised
upon request
• Minimum trace/spacing: 4mil
• Surface finish: immersion gold, ENEPIG or OSP
• Silkscreen: custom colours available
Rohde & Schwarz (Australia)
www.rohde-schwarz.com/au
stand C8
Rohde & Schwarz will be back at Electronex in 2026 with a
wide range of test and measurement products to demonstrate,
including the new generation R&S MXO 3 Oscilloscope series:
Fast. Precise. Compact. Key facts:
• Unmatched performance with bandwidths from 100MHz
to 1GHz
• World’s fastest oscilloscopes with 4.5 million waveforms/s
and up to 99% real-time capture
• Industry-leading architecture with 12-bit ADC and 18-bit
HD mode
siliconchip.com.au
• The most compact eight-channel oscilloscope with MSO,
generator and large 11.6-inch display
• Up to 50,000 FFTs/s with independent time and frequency
settings
The MXO 3 Series put big capabilities in a small package.
Enjoy unmatched performance to quickly and easily gain expert
understanding of your device under test. Powered by next-
generation MXO technology, the oscilloscope delivers fast and
precise measurements in a small package.
Instantly see more signal detail with the world’s highest
acquisition rate of up to 4.5 million waveforms per second
and real-time signal capture of up to 99%. Capture every detail
with clarity and confidence thanks to 12-bit ADC resolution at
all sample rates, enhanced 18-bit HD mode, advanced digital
triggering and 125Mpoints of standard memory.
Save space without sacrificing usability: enjoy the brilliant
11.6-inch full HD display and seamless integration into any
setup with just a 5U rack height across all models.
The MXO 3 Oscilloscope has unmatched performance in both
time and frequency domain debugging and testing.
Semitech Semiconductor
semitechsemi.com
stand D6
Semitech Semiconductor, a proudly Australian semiconductor
company, sells its flagship SM2400 power
line communications chip
for smart grids, stadium
lighting, airport runway
lighting, semi-trailers,
smart building systems and
mining drill rigs. Semitech’s
market-leading chips are
designed in Australia with
wafers manufactured by TSMC.
Semitech has teamed up
with Texas Instruments to offer
the latest G3 Hybrid network
architecture to the global smart grid market. Smart Grid
networks modernise traditional electricity grids by integrating
two-way digital communication. They support applications
such as advanced metering infrastructure (AMI), demand
response, distributed energy resources (DERs), fault detection
and distribution automation.
Power line communication (PLC) is uniquely positioned
in smart grids by using the existing medium-voltage (MV)
and low-voltage (LV) electricity distribution networks as the
communication channel, eliminating the need for new cabling,
while overcoming the shortcomings of wireless communication.
Utilising modern signal processing and mesh networking
techniques, G3 Alliance developed the G3 PLC and G3 Hybrid
standards to provide a ubiquitous and reliable network
architecture with unprecedented reach without requiring new
infrastructure investment. G3 PLC networks have been deployed
in over 60 countries, with over 1 million devices connected, and
are rapidly expanding.
Semitech offers a best-in-class G3 PLC solution built on
the versatile SM2400A PLC modem, designed for advanced
narrowband PLC protocols:
• Advanced dual-core architecture for low-cost and power
efficiency
• Multi-protocol support, including G3 PLC and G3 Hybrid
• Superior noise resilience with advanced preamble
detection and <20dBµV sensitivity
Australia's electronics magazine
May 2026 57
• Certified G3 stack supporting full OFDM-based PHY, MAC,
and 6LoWPAN ASL
• Built-in security with an integrated AES-256 security
engine
• High-Speed PLC with data rates above 600kbps
• AC and DC power line compatible
• Global frequency band compatibility, including CENELEC
(Europe), FCC (North America) and ARIB (Japan)
• Future-proof software-defined performance with remote
firmware updates
• Flexible integration options, including external flash or
host-loaded modes and a wide range of compatible line drivers
• Easy to develop, troubleshoot and prototype, with
complete developer-friendly tools and evaluation kits
Hybrid networks seamlessly integrate PLC with RF mesh into
a single, unified infrastructure. This dual-medium approach
improves the network’s robustness and capacity, making the
network more resilient even in hard-to-reach locations. In
partnership with Texas Instruments, Semitech delivers a G3
Hybrid platform that seamlessly combines PLC and sub-GHz
wireless for maximum reach and reliability:
• Full integration of TI’s CC1312R wireless MCU and
Semitech’s dual-core SM2400 PLC
• High-performance sub-GHz wireless MCU for robust,
reliable long-range RF communication
• Dynamic mesh routing, automatically sensing and
selecting RF or PLC communications for ideal connectivity
• RF-only mode for battery-powered edge devices; +14dBm
RF output power with temperature compensation
• Dual media reliability with automated PLC or RF path
selection
• Seamless networking with full mesh routing across both
PLC and RF
• Long-range wireless utilising TI’s high-performance MCU
for 802.15.4
Shenzhen Cirket Electronics
szckt.cn
stand C13
The HackRF Pro is an advanced software-defined radio (SDR) for
testing and developing modern radio technologies. It operates
as a half-duplex transceiver, supporting frequencies from
100kHz to 6GHz, with tuneable ranges up to 7.1GHz and sampling
rates up to 20Msps (40Msps in oversampling mode). It features
a high-speed USB 2.0 interface with a Type-C connector, SMA
antenna connectors
and a built-in TCXO
crystal oscillator.
Compared to its
p r e d e ce s s o r, t h e
HackRF Pro has a
wider frequency
range, better RF
performance with
a flatter frequency
The HackRF Pro. Source: r e s p o n s e a n d a
www.youtube.com/watch?v=C0W-pYcgHeA power-efficient FPGA
replacing the old CPLD. It also offers extended-precision mode
with 16-bit samples for low sample rates and half-precision
mode with 4-bit samples at high rates.
The HackRF Pro enables applications like signal analysis,
protocol development and wireless security testing. Its opensource nature, portable design, and backward compatibility
make it a versatile and cost-effective solution for exploring
58
Silicon Chip
radio communication systems. Shenzhen Cirket company is
the biggest HackRF One manufacturer over the past decade.
LED PCBAs longer than 1.5m are used in building wall,
bridge, shopping mall, road tunnel and some other lighting
construction projects. Shenzhen Cirket Electronics Co Ltd
has three SMT lines for long PCB assembly. Our solder paste
printer can print PCBs up to 1.8m long. We have added
additional tracks on both sides of a Yamaha pick and place
machine, with a 500mm PCB conveyor between two mounting
machines. Each machine can mount components on half of
the long PCB.
As the board is long, the pad position tolerance is larger
than for smaller PCBs. Thus, the PCB factory needs to provide
high-precision boards. The stencils must use good-quality steel
sheet to remain stiff enough. A strong and stable solder paste
printer ensures all solder paste is in the correct locations. Our
factory has extensive experience in this process.
Our factory, Shenzhen Cirket, has mastered complex PCBA
processes. One recent production involves a 10-layer PCB
with Isola 370HR material, specifically processed to maintain
structural integrity at a high Tg of 180°C. A key challenge we
managed is the copper weight distribution, ranging from 0.5oz
to 1.5oz across different layers, ensuring consistent plating
quality and thermal performance.
For interconnect reliability, we utilised advanced copperfilled thru-via technology. These vias are plated over to create
a perfectly flat surface, critical for high-density contactor areas.
An ENEPIG surface finish provides a superior, flat interface that
is exceptionally friendly to fine-pitch BGA soldering, eliminating
the risks of ‘black pads’ and enhancing joint strength.
The BGA ball spacing for this board is 0.25mm. We use
high-reliability Alpha tin with 3% silver as the solder paste.
Too active solder paste can cause short circuits very easily
with close BGA ball spacing. Thus, a proper oven temperature
chart is very critical.
Silvertone Electronics
silvertone.com.au
stand C26
The VSG200 20GHz vector signal generator features a low phase
noise, agile local oscillator with a 200µs switching time, enabling
frequency-hopping spread-spectrum testing. A dual 14-bit DAC
runs at 2× or 3× the I/Q symbol rate, using digital oversampling
to provide a flat, clean baseband. A digitally adjustable
internal VCTCXO ensures
frequency errors are
kept to a minimum
over temperature,
o r a n e x t e r na l
10MHz input may
be used for 0ppm
frequency error.
Australia's electronics magazine
siliconchip.com.au
R&S®ESSENTIALS
SMALL IN SIZE, BIG IN IMPACT.
The new MXO 3 oscilloscope. Fast. Precise. Compact.
With a combination of features that rival much higher-class oscilloscopes,
in a deceptively small package, the MXO 3 ensures you catch rare signal
anomalies, debug complex issues, can take it wherever your work demands
and still have plenty of time to high-five your entire team.
Explore more
• Available modulation types: LTE, 802.11a/n/ac/ax,
Bluetooth LE, custom OFDM, 16/64/256/1024-QAM, 2/4/8/16PSK, 2/4/8/16-FSK, ASK, GMSK, AWGN channels, ramp/chirp,
stepped sweep, multi-tone, pulse, FM, AM, CW, arbitrary/
custom
• Digital modulation impairments/effects: custom channel
response, AWGN, sampling rate error, frequency and level
offset, I/Q offset, spectrum inversion
The PCR4200 four-channel phase-coherent receiver is a
high-performance, 100kHz to 20GHz, four-channel phase
coherent receiver, streaming I/Q data over a VITA 49 interface.
Each channel on the PCR4200 may be configured as a phasecoherent channel using the high-performance shared local
oscillator (LO), or independently tuned using that channel’s
dedicated LO. Any single channel may be configured to provide
swept spectrum data at up to 200GHz/s.
• Streams 40MHz bandwidth per channel over 10GBE SFP+
• Built-in sub-octave preselectors from 45MHz to 20GHz
• Noise figure: 10dB typical at 2GHz
• Calibrated I/Q data
• Ultra-low phase noise: -136dBc/Hz 10kHz offset from 1GHz
centre frequency
• Internal GPS
• 110dB dynamic range
• Independent channel configuration
• Up to 16 phase-coherent channels
Applications include simultaneous multi-band spectrum
monitoring, emitter detection and geolocation, multi-channel
transmitter testing, SIGINT/COMINT/ELINT, drone detection and
MIMO channel testing.
Stars Microelectronics
starsmicro.com
stand D3
Stars Microelectronics is the only Thailand-based company that
delivers world-class EMS, SMT, OSAT, advanced IC packaging
and advanced photonics solutions, serving industries including
microelectronics, telecom, industrial automation, professional
audio/video, automotive RF & power electronics, medical
devices and clean energy.
Our commitment to world-class standards, certified facilities
and strict quality assurance means that every product we
deliver is crafted to exceed customer expectations every time.
Leveraging Free Trade Zone advantages and supported by
global offices, we provide seamless, reliable and cost-effective
solutions that strengthen your competitive edge in the global
market.
Suba Engineering Pty Ltd
suba.com.au
stand A27
The new SubaScope Ultimate has a CMOS camera that includes
multiple output modes (HDMI, WiFi, USB 3.0 and network). The
camera uses an ultra-high-performance CMOS sensor. It can be
directly connected to an HDMI display or to a computer via WiFi
or USB and images and videos can be saved directly for on-site
analysis and subsequent research. The user can directly control
the camera hardware with the software ToupView or ToupLite.
60
Silicon Chip
SubaScope Ultimate is enhanced with an embedded ARM
core. The camera has a built-in auto focus system, which can
realise the best auto focus specification areas of the sample.
Some key features are:
• 16MP Sony CMOS sensor
• 4K / 1080p auto-switching according to monitor resolution
• USB flash drive for captured image and video storage,
supporting local preview and playback
• Autofocus supporting Canon EF-mount lenses – the
SubaScope is the only digital microscope on which you can
change from far distance to close distance by changing the
Canon camera lens
• Embedded XCamView for control of the camera and
image processing, supporting automatic edge finding and
measurement functions
• ToupView and ToupLite software for PC
• iOS and Android applications for smartphones or tablets
Switches Plus Components
switchesplus.com.au
stand C4
Compact HMI controls can have a large impact
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Australia's electronics magazine
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May 2026 61
SC7657 Kit ($45 + postage): includes everything in the parts list
a compact and simple
¬C Meter
by Andrew Woodfield
This little LC meter uses just 20 parts and delivers accurate results across a wide
measurement range. Importantly, no costly or hard-to-find precision parts are needed.
Compact, lightweight, inexpensive and easy to build
Inductance range: <10nH to about 100mH
Customer 3D-printed case
M
62
Silicon Chip
Capacitance range: <10pF to about 1μF
Typical accuracy: ±2%
any years ago, I built my
first LC meter using the Atmel
89C8051 microprocessor. It
worked very well, but it drained batteries fast. This was not really a problem because I rarely used it for more
than a few minutes at a time.
When I moved to another country
several years later, I designed my own
LC meter using one of the Microchip
ATtiny microcontrollers and a twoline I2C alphanumeric LCD screen. It
was powered by a standard 9V battery via an LP2951 low-dropout voltage regulator. While it drew very little current, unfortunately, just when I
most wanted to use it, the 9V battery
would require replacement.
Returning home, I modified it to
use a single 1.5V AA alkaline cell and
a tiny boost converter. The AA battery version had a surprisingly good
life. One reason was the complete
absence of relays in the design. Some
LC meters use anywhere from one to
four (!) relays.
This new version quickly became
my ‘go-to’ LC meter. It was also borrowed periodically by friends because
of its accuracy and ease of use. I was
asked if I could design a smaller,
cheaper, easier-to-make version.
While I had expected the change to
a single AA cell to bring about a reduction in the overall size of the LC meter,
it was still constrained by the size
and shape of the alphanumeric LCD
Measures capacitor and inductor values
Power supply: single AA cell
screen and the added boost converter.
That LCD was also a relatively costly
device. These factors, along with the
perceived need for 1% tolerance parts
for calibration, were all seen as barriers by potential builders.
The wide availability of smaller,
inexpensive 0.91-inch OLED screens
was the catalyst for a further redesign.
It offered the opportunity to further
reduce the size, cost and parts count.
The product of this latest redesign is
the LC meter described here.
By finally doing away with any
regulator and using any convenient
USB-C 5V power supply, the LC meter
has now been reduced to the volume
roughly of a pair of AA batteries.
Note that the 2-pin USB-C connector
used is not standards-compliant and
may not work with all USB-C/USB-C
cables and power supplies. It should
work with all USB-C/USB-A cables.
A little LC meter theory
Almost all LC meter designs use an
LC resonant circuit in a simple oscillator. These typically operate around
500kHz (the ‘reference frequency’)
when no actual inductors or capacitors
are being measured. A 100μH inductor and a 1nF capacitor are the typical
resonant circuit values used.
When an unknown capacitor or
inductor is added to this resonant circuit, the oscillator frequency drops. By
Fig.1: an LM311 comparator is commonly used in the LC measurement
oscillator
in electronics
most LC meters,
but it requires a relatively high number
of parts.
Australia's
magazine
siliconchip.com.au
measuring this reduction, the value of
the unknown part can be determined.
One variation of this approach uses
two capacitors in the basic tuned circuit. The additional frequency measurements were claimed to give more
accurate results. However, this additional capacitor proved unnecessary.
Even the value of the reference inductor can be ignored when calculating
the value of the capacitor or inductor
being measured.
For those interested in the details,
refer to the panel titled “Only one
capacitor is required”.
Only one capacitor is required
A simple LC resonant circuit, shown in Fig.a, lies at the heart of the LC meter.
It sets the output frequency of the meter’s 74HC04 inverter-based oscillator.
This LC circuit resonates at a frequency determined by the values of L and C:
f1 = 1 ÷ (2π√LC).
If another capacitor, Cx, is added in parallel with this circuit (Fig.b), the oscillator frequency falls to a lower frequency, f2 = 1 ÷ (2π√LC + LCx).
If the value of capacitor C is known, we can calculate the value of the unknown
capacitor, Cx, from the original frequency f1 and the new, lower, oscillator frequency f2 using this formula:
The LC meter backstory
Most current LC meter designs are
derived from the original AADE design
published by Neil Heckt in Electronics Now magazine, June 1996, or variations based on a later design and software by Phil Rice, VK3BHR.
However, the approach used in these
LC meters is actually much older.
For example, the Tektronix model
130 LC meter first released in 1959
(June-August 2020; siliconchip.au/
Series/346) used the same method,
although using an analog display.
Some thirty years later, Bill Carver,
K6OLG, used a FET-based oscillator and some Pascal software in a
design described in Communications Quarterly magazine in Winter
1993 to achieve a similar result. But
it took until 1998 for these ideas to be
integrated into Neil Heckt’s compact
design, complete with a digital display.
Fig.a: a simple
parallel resonant
LC network.
This means that the unknown capacitor
value may be calculated directly using the
value of the reference capacitor (C) and the
two oscillator frequencies (f1 and f2).
It is also possible to measure an unknown
inductor with the LC circuit. In this case, the
unknown inductor (Lx) is added in series with
the existing inductor L, as shown in Fig.c. The
frequency again falls from f1 to f2.
Fig.c: adding inductance
in series with the original
L also lowers the resonant
frequency.
Design optimisation
The oscillator at the heart of many
of these designs uses a fast comparator
such as the LM311 (see Fig.1). While it
can work very well, it uses a relatively
high number of parts. Also, at times,
I’d found the LM311 hard to find and/
or relatively expensive. We’ve also
heard from some people who’ve built
these circuits and they fail to oscillate.
Swapping the LM311 usually fixes it.
Few details were typically given
about the best parts to use for the
main oscillator components (L1 and
C1 in Fig.1). A few builders suggested
that this oscillator required low-ESR
coupling capacitors. Several internet
forums mentioned problems with specific types of inductors. Details based
on measurements and testing, however, were scarce.
Since I wanted to identify the best
parts to use for L1/C1, I also used this
siliconchip.com.au
Fig.b: adding more
parallel capacitance
(externally) lowers the
resonant frequency.
Once again, this equation calculates the value of the unknown inductor Lx
based only on the value of the two resonant frequencies, the first (f1) with only
L and C in circuit and the second (f2) with the addition of the unknown inductor. The only other parameter needed is the value of the reference capacitor, C.
Therefore, the value of unknown capacitors and inductors can be measured
by knowing the value of just the reference capacitor, C.
opportunity to look at a simpler and
less costly alternative oscillator. Based
on some previous work with 74HC04
CMOS hex inverters in oscillators, this
device looked like a good candidate.
This choice might address another
problem. The LC meter’s accuracy
relies on a very accurate clock source.
Australia's electronics magazine
Most LC meters use the chosen microcontroller’s internal oscillator and an
external crystal. Unfortunately, by opting for a small 8-pin ATtiny processor
in my LC meter, only one pin remained
free for an external clock. That meant
I had to use a separate external crystal oscillator.
May 2026 63
Initially, I used a discrete single-
transistor oscillator based on a Jim
Williams design (in Linear Technology
Application Note 12, October 1985)
which also offered temperature compensation, but this took more parts as
well as PCB real estate. The availability
of several spare gates in the 74HC04
allowed me to build a suitable crystal
oscillator with just a crystal and three
extra passives.
Fig.2: the value of
MKT capacitors
can change
significantly
with frequency,
making them
a poor choice
for an LC
meter reference
capacitor. Source:
Ostrava MKT
datasheet.
Resonant circuit components
Since the reference frequency is
determined almost entirely by the
value of the inductor and capacitor
used, it is important that their values
are stable during any measurement(s).
In practice, as with any analog oscillator, the reference frequency changes
slightly with changes in temperature.
It’s a sensitive circuit. Simply
switching on the LC meter and passing
the tiny current through the LC circuit
as it starts oscillating results in a slight
change in temperature.
One measurement method can
largely negate the impact of this drift.
By measuring the reference frequency
prior to connecting the unknown part,
then quickly measuring the oscillator’s
frequency once the part is connected,
the impact of drift can be mitigated.
The best solution, however, is to
select stable components. The reference
inductor and capacitor should ideally
be perfectly stable with temperature.
An inductor wound on a high-Q ferrite
toroid might appear ideal. However,
the typical temperature coefficient
(TC) for this type of inductor is up to
10,000ppm/°C (!), making it unsuitable.
Similarly, a silver mica capacitor
would appear the ideal choice for the
reference capacitor. These have excellent temperature stability and, while
relatively expensive, ±1% tolerance
parts can be obtained.
My tests showed that the optimal
solution is to balance the TCs of the reference capacitor and inductor. This is a
similar approach to that used in legacy
analog RF variable frequency oscillators (‘VFOs’). After testing a variety of
inductors, this design uses a cheap and
widely available axial choke inductor
and a polystyrene capacitor.
The axial choke has a positive TC of
about 300-500ppm/°C, while the polystyrene capacitor has a TC of around
-150ppm/°C.
While it’s tempting to suggest substituting a polyester (-200ppm/°C to
600ppm/°C) or Mylar (-300ppm/°C)
capacitor, they can suffer from changes
in capacitance with frequency, especially the MKT types that come in
rectangular packages. Some polyester/Mylar capacitors may be suitable,
but it’s hard to know which without
checking the data sheets.
For example, one manufacturer’s
specifications for an MKT capacitor
(Fig.2) shows a variation in capacitance
of around 4% from 1kHz to 1MHz.
Circuit details
The resulting circuit is shown in
Fig.3. It is built around two inexpensive devices: the 8-pin ATtiny85
microcontroller and a 74HC04 CMOS
hex inverter. Three inverters in the
74HC04 provide the measurement
oscillator and buffer. It uses less current and requires fewer parts than the
more familiar LM311-based oscillator.
This is configured as a Franklin
oscillator using two of the gates of
Fig.3: an inexpensive CMOS hex inverter (74HC04) is used in the two oscillators required in this LC Meter, while a
Microchip (Atmel) 8-pin ATtiny85 calculates the value of the unknown inductors or capacitors and drives the OLED display.
64
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
the 74HC04 (IC1f & IC1e). The third
gate (IC1d) buffers the oscillator and
connects the output to the ATtiny85
microcontroller (IC2).
Relay switching is avoided through
the use of a simple two-pole changeover slide switch, S1. Contacts on this
switch also tell the processor whether
the user wants to measure inductance
or capacitance. It’s simple, inexpensive
and reliable. It also has the considerable advantage of drawing no current.
The Microchip ATtiny85 8-pin
microcontroller with its 8kiB of internal flash program memory is the brains
of the meter. It measures the frequency
of the LC reference oscillator, monitors
the user LC mode selection and calibration switch inputs, and drives the
OLED display.
The software is written in Bascom-
AVR, and it consumes 99% of the
8kiB memory, although a few hundred
bytes are consumed for the arguably
cosmetic ‘splash screen’ image that’s
shown when power is applied.
There are three further inverters
available in the 74HC04 used for the
crystal oscillator circuit. HCxx inverters are not usually considered suitable for crystal oscillators. However,
by configuring these gates again as a
Franklin oscillator with minimal feedback coupling, the resulting crystal
oscillator delivered a reliable solution
while further reducing the parts count,
current drain and cost.
Incidentally, this circuit was tested
with a variety of 1-30MHz crystals
from several sources and it proved
quite reliable. Using this circuit with
other crystal frequencies for other
designs will require a change to the
value of the coupling capacitors to
ensure reliable operation.
Each line in an I2C interface (SDA &
SCL) usually requires a pull-up resistor to the supply rail. Usefully, these
are already on the OLED module, saving another two parts.
This LC meter draws about 25mA
during operation. The OLED screen
is responsible for about 70% of that.
The earlier I2C LCD version drew less
than 15mA, but those LCDs are also
more expensive and harder to find
than OLED displays now.
The ±1% reference capacitor
Practically every DIY LC meter
or capacitor meter design seems to
demand one (or more!) ±1% tolerance
capacitors, at least for the capacitor
siliconchip.com.au
Measuring capacitance accurately
This simple method can measure capacitor values within about ±1.5%. It requires a lowcost function generator with a low impedance output (eg, 50W), an oscilloscope and a
digital multimeter. A frequency counter may be required if your function generator does
not have a digital display (and you don’t have one built into your oscilloscope). The measurement setup is shown below.
The oscilloscope is used to measure the magnitudes of Vin and Vout. A digital AC millivoltmeter is a better choice if you have one (we’ve published several suitable designs).
If the output voltage Vout is exactly half that of the input voltage Vin then C = √3 ÷ 2πfR.
Let’s assume the function generator (used as the signal generator) is set to generate
a sinewave at about 10kHz. Ideally, the frequency used should allow the resistor value
(R) to be accurately measured with at least 3½ digit accuracy using the multimeter, eg,
123.4W or 1234W.
Let’s say the capacitor to be measured is labelled “10nF” (although we don’t yet know
its precise value), and f = 10kHz. In that case, R = √3 ÷ (2π × 10kHz × 10nF) = 2757W.
The nearest standard value is 2.7kW. Reach into your parts bin and take out a 2.7kW
resistor, then measure its actual value with the digital multimeter. My old Fluke Model
75 multimeter has a stated accuracy of ±0.7% when measuring resistors, although the
typical Model 75 actually had an accuracy closer to ±0.3% ex-factory.
The “2700W” resistor I selected measured 2762W. Use that resistor as “R” in the circuit below. The “unknown” capacitor C is the 10nF value to be accurately measured.
Set the function generator initially to 10kHz. Measure the frequency with a frequency
counter if the function generator’s display is not sufficiently accurate. You should be
able to set the function generator frequency with an accuracy better than ±50Hz (±0.5%
<at> 10kHz). Most function generators will display the frequency much more accurately
than this without the need to use a frequency counter.
Connect your oscilloscope to measure Vin and Vout. Many modern oscilloscopes
have a digital measurement function that will report these values to three-digit accuracy.
Adjust the frequency of the function generator so that the output voltage (Vout) is
exactly half that of Vin as measured on the oscilloscope. Some adjustment of the generator’s output level may be required to measure both voltages accurately to achieve
the best result. Measuring this 2:1 ratio accurately is the source of the greatest measurement error in this process, so care is required.
I found the generator had to be set to 9611Hz, so C = √3 ÷ 2πfR = √3 ÷ (2π × 9611Hz
× 2762W) = 10.385nF.
The scope probe’s tip capacitance
is in parallel with the Vout measurement. This capacitance is typically
stated on the probe; mine was specified as 15pF. Deducting this from
the calculated capacitance gives
10.37nF.
This is the exact value of the
How to accurately measure a capacitor’s
capacitor. With the test equipment
value using a function generator,
and procedure described, the result
frequency meter and multimeter (for
can be shown to be accurate to
measuring the R value).
±1.5%.
in the main resonant circuit. Some
require another for calibration. These
parts can be difficult to find, and they
can be expensive to buy.
One solution used in the past by the
home builder was to measure several
±5% or ±10% tolerance capacitors,
selecting one that is as close as possible to the desired value. This worked
at a time when many parts were not
sorted by tolerance bands, so selecting
one from many parts yielded a value
close to the desired value.
Australia's electronics magazine
This approach also required a very
accurate capacitance meter. The lack
of such a meter is often the reason for
building an LC meter in the first place!
While a few constructors may have
access to a suitable meter through work
or a friend, this problem can be a significant barrier for potential builders.
One solution to this ‘chicken and
egg’ capacitor problem was described
by retired Hewlett Packard engineer
Jim McLucas in an article entitled
“Circuit measures capacitance or
May 2026 65
Photo 1: the prototype PCB without the OLED fitted. The socket for IC2 differs
slightly from the approach described in the text. The USB-C connector is
mounted at upper-right.
Photo 2: a side-view of the
prototype shows how the
OLED sits just above or on
the ATtiny85. This construction
method reduces the overall
height of the meter.
Photo 3: the PCB sits in the lower half of the 3D-printed case.
The pressed-in nuts can be seen at upper left and lower right.
Photo 4: the Simple LC Meter
measuring a 47μH test inductor.
Photo 5: this simple jig makes
it easier to measure the
value of small SMD
components.
Fig.4: only a few parts are mounted on the board; this PCB overlay shows
clearly their locations and the orientations of IC1 and IC2.
66
Silicon Chip
Australia's electronics magazine
inductance” from Electronic Design
magazine, October 21, 2010 (see the
panel on “Measuring capacitance
accurately” above).
Careful measurements using several methods and meters showed this
technique was as accurate as claimed.
The procedure is also relatively easy,
especially when measuring a single
capacitor value such as 1nF (1000pF).
In this LC meter, the capacitor in
question needs only to be approximately 1000pF. Using one of these
methods, it is possible to accurately
establish the value of the chosen reference capacitor. Write the value down,
because this value will be programmed
into the ATtiny85 later.
It actually doesn’t matter if your
capacitor is actually 5% or more away
from the preferred or ideal value. For
example, one version of this meter
used an 820pF polystyrene capacitor
to accurately measure inductors and
capacitors for years!
In short, in this design, provided
the value of your chosen capacitor is
accurately measured and saved in the
LC meter’s EEPROM memory, the LC
meter software takes care of the rest.
Construction
The LC Meter is built on a double-
sided PCB coded 04103261 that measures 67 × 20mm. Start by fitting the
resistors and capacitors, then the
74HC04 IC, using the overlay diagram (Fig.4) as a guide. Proceed to fit
the USB-C connector and the 8MHz
crystal. You’re almost 50% of the way
through construction already (by parts
count, anyway)!
Next, mount the IC socket for the
ATtiny85 to the PCB. It is drilled to
allow the socket to fit down into the
PCB to reduce the overall height of the
assembly. The excess pin length can
be trimmed from the IC socket after it
is soldered into place.
Fit the four-way female pin strip
for the OLED display on the PCB.
OLED screens often come with standard square pin headers (sometimes
soldered, sometimes separate) but
the LC meter’s size can again be usefully reduced if machined IC socket
pin strips are used. So, if your screen
has a header soldered to it, remove
it and re-fit the round-pin machined
header. Photos 1 & 2 show the general
arrangement.
The OLED display should be fitted
with a matching connector, in this case
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a four-way machined IC male-male pin
strip. As Photo 2 shows, when the display is attached to the PCB, it will rest
on or very slightly above the top surface of the ATtiny85 (IC2).
Solder the DPDT slide and pushbutton switches in place, then proceed to mount the reference capacitor,
followed by the inductor. Space both
about 1mm above the PCB to allow
them to be more easily bent over at a
slight angle. This is to allow the PCB to
be mounted in the compact 3D-printed
enclosure.
Do not fit the crocodile clips yet.
This will be done as part of the
3D-printed enclosure assembly.
Before final assembly, you’ll need to
program the ATtiny85 unless you purchased a pre-programmed chip. The
instructions for this are in the text box
“Programming the ATtiny85”.
Once programmed, carefully fit the
ATtiny85 into the IC socket, making sure the chip is correctly orientated. Pin 1 of the ATtiny85 is usually
marked with a tiny circle. The orientation can also be checked against the
component overlay on the PCB (Fig.4).
Now plug the OLED screen into place.
Final assembly
the soldering iron doesn’t go anywhere
near the 3D-printed parts!
Slide the LC meter PCB into the base
and arrange it so it is flat and the USB
socket aligns with the matching hole in
the base. Check that your USB-C cable
can connect with the PCB-mounted
connector. Leave it in place briefly
while adding a couple of drops of hot
glue to the edges of the PCB to keep it
firmly in place, if necessary.
Finally, secure the cover in place
with the two M2 machine screws.
Inductor & capacitor testing
A wide variety of methods have
been tried for connecting the components being tested. The LC test
inputs on the PCB allow for various
builder preferences. The approach
shown here uses a pair of small alligator (crocodile?) clips on short lengths
of stranded hookup wire. I find this
the easiest, most practical and robust
approach.
SMD parts may prove troublesome
to clip onto, though. For the occasional
test, the clips are fine, if a little clumsy
at times. One alternative for testing
SMD parts I tested is shown in Photo 5.
I cut a very thin slot into the copper side of a scrap of single-sided PCB
substrate. A further blank PCB scrap
was milled to match the dimensions
of the most commonly used SMD
parts: M2012/0805 (2.0 × 1.2mm),
M3216/1206 (3.2 × 1.6mm) etc. This
was glued on top of the first PCB so
Parts List – Simple LC Meter
1 double-sided PCB coded 04103261, 67 × 20mm
1 3D-printed enclosure [STL files: Silicon Chip SC3581]
1 3D-printed pushbutton extender [STL file: SC3581]
1 74HC04 SMD hex inverter IC, SOIC-14 (IC1)
1 ATtiny85-20PU microcontroller programmed with 0410326A.HEX/EEP
(IC2) [Altronics Z5105 or Jaycar ZZ8721 (both unprogrammed)]
1 128×32-pixel 0.91-inch I2C OLED display module
[AliExpress 1005003743893780, Silicon Chip SC7484]
1 pair of small red & black crocodile/alligator clips (CON1a/CON1b)
[Jaycar HM3020]
1 female machined 4-pin strip (CON2)
[cut from Altronics P5400A or Jaycar PI6470]
1 4-pin machined male-to-male header strip (for the OLED)
[AliExpress 1005007564228387]
1 USB-C Type C-05 PCB-mount 2-pin socket (CON3)
[AliExpress 1005005371954812]
1 100μH axial RF choke (L1) [Jaycar LF1534]
1 SS22H02-G5 5mm miniature PCB-mounting vertical DPDT slide switch
(S1) [AliExpress 1005009907089109]
1 4-pin PCB-mounting tactile pushbutton switch with 6mm-long actuator
(S2) [Altronics S1124, Jaycar SP0603]
1 8MHz crystal, HC-49U (X1) [Altronics V1249A or Jaycar RQ5287]
1 8-pin DIL machine pin IC socket (for IC2)
2 M2 × 5mm countersunk head machine screws and hex nuts
2 short (~100mm) lengths of medium-duty hookup wire
Capacitors (all SMD M2012/0805-size 50V X7R unless noted)
1 1μF
1 100nF
1 1nF 50V polystyrene [AliExpress 1005006112435371]
2 4.7pF NP0/C0G
Resistors (all SMD 0805-size ±1%)
1 1MW
1 22kW
1 100kW
1 5.6kW
These next steps assume the use
of the 3D-printed enclosure designed
for this meter, although the PCB can
be mounted into almost any suitable
enclosure. The 3D-printed case usefully avoids the need for precision
drilling and cutting of the various
holes required.
There is also a little pushbutton
shaft extender, also 3D-printed. This
is suitable for 6-10mm shaft length
miniature pushbuttons. This is placed
over the top of the pushbutton shaft
just prior to screwing on the top cover.
Begin final assembly by inserting
the two M2 nuts into the base using a
soldering iron. Locate them in place
and press them into the base with a
light and very brief press of the soldering iron tip. They should lie just at
or slightly below the mating surface of
the base and cover.
Attach the red and black miniature
crocodile clips to two 55mm lengths
of stranded hookup wire. Strip 4mm
of insulation from the free ends and
tin the stranded wire with solder. Pass
these ends through the hole located
on the left-hand side of the lower half
of the enclosure and carefully solder
them to the LC test pin inputs. Ensure
Figs.5-7: the enclosure and
pushbutton cap may all be
3D-printed with PLA filament. The
prototype was printed with grey PLA
for the case, while the pushbutton
cap was printed in a contrasting blue.
siliconchip.com.au
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May 2026 67
Programming the ATtiny85
Download the HEX and EEP files for the LC meter from siliconchip.au/Shop/6/3580
The EEP (EEPROM) file provided contains a nominal value of 1000pF for the reference
capacitor.
If you have an in-circuit programmer like the USBasp, you will also need a way to connect the correct lines to the pins on the chip. This is most easily done using an adaptor
board. It saves adding a 6-pin programming socket to each PCB.
My 8-pin adaptor was published in the September 2020 issue (page 47; siliconchip.
au/Article/14563) and the PCB is still available (siliconchip.au/Shop/8/5642)
Once you have the chip plugged into an adaptor, connect the programmer to your
computer. Download and open a programming application (such as Extreme Burner)
and load the HEX and EEP files into this program.
It is almost certain you will need to modify the contents of the EEP file with the precise
value of your reference capacitor. The value is saved in picofarads, eg, 1.015nF is saved
as 1015 (pF). EEPROM values are usually edited as two-digit hexadecimal bytes (in this
case, two bytes, making up a four-digit hex value). You can use the following website to
convert the value to hex: www.rapidtables.com/convert/number/decimal-to-hex.html
One of my LC meters used a 995pF capacitor; 995 is 03E3 in hexadecimal. This value
was entered into cells 02 and 03 in the first line of the EEPROM tab in Extreme Burner
(see Screen 1). Just click your mouse on the cell to be changed and enter the new value.
Note that the least significant byte (E3 in this case) comes first, in cell 02, and the most
significant byte (03) goes in cell 03.
Now program your ATtiny85 with the HEX file, then the EEP file. Click on the “Write”
tab in Extreme and select the file you are sending to the ATtiny85. Next, program the
hardware configuration fuses in the ATtiny85. Table 1 shows the required fuse settings.
You need to set these after loading the HEX and EEP files before the LC Meter will work.
To set the fuses, click on the Fuse Bits/Setting tab (Screen 2), enter the values shown,
and click on the Write selection boxes for the Low and High fuses (the others may safely
be ignored). When you have done this, write the fuse settings to the ATtiny85 by clicking
on the Write button at the lower right of this tab. That’s it!
If you need more information about the programming procedure, there are some helpful tutorials on this topic that can be found on the Adafruit and Instructables websites.
Table 1 – ATtiny85 fuse settings
Fuse
Hex value
Comment
Lock byte
FF
Flash not locked
Extended byte
FF
Self-programming disabled
High Byte
5F
Defaults except RSTDISBL=0
Low byte
E0
Defaults except CKDIV8=0 & CKSEL1=0
Silicon Chip
Operation
A simple sign-on message is displayed when the meter is powered up.
Once the measurement mode (inductance or capacitance) has been selected
with the LC switch, the meter must
then be calibrated.
Press CAL and wait a moment. You
will see a display prompting you to
short the test leads together (for inductance measurements) or leave them
open (for capacitance measurements).
Once calibrated, the component
can be connected, and the meter will
then display its value. The meter also
reports the oscillator frequency during
the measurement. This allows invalid
results to be easily detected; for example, if a faulty component is tested or
one with a value outside the range of
the meter.
The prototype will measure values
from less than 10nH to about 100mH
and from less than 10pF to about 1μF.
If the reference capacitor has been
carefully measured, the results can be
expected to be within ±2%.
Final remarks
Screen 2:
another tab in
Extreme allows
the fuse bits to
be set and then
written. Do this
after you have
written the HEX
and the EEP files
to the ATtiny85.
This meter, in one form or another
and with minor variations in the software, has been in continuous use on
my bench for well over a decade. The
latest version described here has been
in use for over 18 months. It is, by far,
the most compact and convenient to
use. The only problem has been that it
is also small enough to become buried
under other stuff on my workbench!
It is quick, simple & inexpensive to
build, and so convenient to use that I
find myself taking its convenience and
accuracy for granted. I have long since
forgotten just how time-consuming the
alternative methods were prior to the
arrival of such LC meters.
Even if you already have an LC
meter, I encourage you to take the
time to build this one. Once built,
you’ll find yourself reaching for it all
SC
the time, too.
Australia's electronics magazine
siliconchip.com.au
Screen 1: the
value of the
reference
capacitor
entered into the
EEPROM tab in
the application.
68
that the slot sat midway in this gap
(see Photo 5).
The SMD part can easily be placed
into this assembly for testing and measurement. The arrangement can then
be connected to the LC meter using
the alligator clips. Another version
used miniature pin connectors, which
allowed the assembly to be plugged
into a different version of the LC meter
when required.
O
ver 20 years ago, my mother was
becoming infirm and had a tendency to fall and couldn’t get up.
I lived too far away to visit every day,
but near enough that I could attend
in an emergency. What was needed
was a way to alert me to any potential problem.
These were the days before the
internet was common in the home,
so I devised a plan to connect the PIR
(passive infra-red) movement sensors
in the burglar alarm to a cheap landline telephone handset from the local
discount store. All that was needed
was an interface between the alarm
panel and the ‘phone.
The system potentially saved my
mother’s life on three occasions, when
she had fallen and couldn’t get up. On
a fourth occasion, she had been taken
into hospital but had not bothered to
tell family, friends or the local community services, causing a major panic.
I got the alert just as I landed in
Amsterdam for a well-earned weekend
break. However, at least I was able to
inform family members of a potential
problem.
The original solution
The original circuit is shown overleaf for interest (Fig.1). The burglar
alarm’s communicator outputs and
three PIR sensors on separate zones
were connected to a PIC16F84 microprocessor (IC1) via NPN transistors
Q1-Q5. This allowed the PIC processor
to detect activity in the three PIR zones,
monitor for alarm conditions and also
determine whether the burglar alarm
was set (armed) on unset (clear).
I removed the keypad, microphone and ‘off hook’ switches from
the ‘phone. The keypad was replaced
Image source: https://unsplash.com/photos/a-black-and-white-alarm-clock-on-a-white-background-CfuOZPNSr6E
WiFi Alarm
Monitor
If someone lives by themselves,
especially if they are elderly,
they can end up in situations
where they need help but
can’t get it. This alarm system
provides a way to alert others
when there is a problem.
A project to help the elderly by Kenneth Horton
by two quad opto-isolators (IC3 &
IC4) driven by a 74LS139 dual 1-of-4
decoder, IC6. The ‘off hook’ switch
was replaced by relay RLY1; both were
activated by the PIC16F84.
I replaced the microphone with a
1:1 ratio isolating transformer. The
first version sent an alert in Morse
code, but this was later replaced by
an ISD1110 voice encoder chip (IC5)
to give spoken alerts.
If the burglar alarm was activated,
or no movement was detected for a
set period, the PIC processor would
dial my mobile number and the voice
chip would inform me that there was
a problem. Monitoring whether the
panel was set (armed) or unset (clear)
allowed different time intervals to
be set.
The top and bottom of the PCB used to prototype the WiFi Alarm Monitor. It’s
very simple compared to the older landline-based circuit shown in Fig.1
siliconchip.com.au
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My mother set the panel at night
upon going to bed, and in this case,
there was a much longer time delay
without movement before an alert was
generated than during the daytime
when the panel was unset.
Bringing it up to date
I am not yet at the stage where I am
infirm, but I know that the time may
come when my family are as concerned about me as I was about my
mother. I decided that I should update
the design, making use of the now
widely available internet and WiFi,
and install it while I have my faculties.
The system performs two functions:
first, it will alert me or my family in
case of an alarm condition, such as the
burglar alarm being set off. Second, it
will monitor my daily activity. If none
is detected, it will alert the family of a
potential problem.
In my case, the alarm system consists of both door switches and PIR
detectors, but the solution can be tailored to individual requirements.
Monitoring alarm conditions is
straightforward. However, monitoring
daily activity is more in-depth. There
are three different modes:
• Daytime, when the occupant is
at home and the alarm panel is unset.
• Nighttime, when the occupant is
in bed and the panel is set (armed).
• When the occupant has left the
premises and presumably armed the
alarm.
May 2026 69
Fig.1: the circuit of my original alarm dialler, which interfaced with the (now
largely obsolete) public telephone network by connecting to an old handset
via CON2, CON3 & CON4. That allowed it to dial me after a
delay if it sensed a lack of activity.
The WiFi Alarm monitor uses
a single Raspberry Pi Pico W
(shown enlarged).
Fig.2: the new Alarm Monitor is
simpler and more modern, using a
Raspberry Pi Pico W to send emails
and/or SMSs if the activity coming
from the alarm via level-shifters IC2
and IC3 looks suspiciously quiet.
▶
During the daytime, the system
needs to check on activity by monitoring door switches and PIRs. At night,
when the panel is set, the system needs
to check that the panel is unset the following morning.
If the occupant has gone out, the
activity monitor needs to be disabled
because the user may simply have
popped to the shops, or they may have
gone on a three-month world cruise!
In this case, inactivity alerts would be
annoying, to say the least!
The use of the exit door within minutes of the panel being set (armed) differentiates between the panel being set
70
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siliconchip.com.au
give a degree of separation between the
alarm panel and the interface.
These 12 inputs, together with an
optional test button (S1) are connected
to a Raspberry Pi Pico W, which provides all the intelligence and a connection to the internet. The Raspberry
Pi Pico W is the version with built-in
WiFi.
The only other components are a
simple linear power supply with an
axial fuse to convert the 12V from the
panel to five volts for the Raspberry
Pi Pico W. This is fed to the Raspberry Pi via a schottky diode so that
it can safely work in parallel with a
USB supply.
Software description
while the user is in the premises and
when he or she has gone out.
The system can send emails to four
different groups of people, depending
on what has triggered the alert, and can
also send SMSs to up to four different
telephone numbers. To send SMS text
messages, you will need a free Twilio
account.
Setting one up is easy; visit www.
twilio.com for more details. Twilio
works in the UK, Australia, NZ, EU,
USA and many other countries too.
Circuit description
As with many modern circuits, the
siliconchip.com.au
hardware is relatively simple, and all
the intelligence is within the software.
The updated circuit is shown in Fig.2.
Up to 12 inputs from the alarm
panel, both individual zones and communicator outputs, can be monitored
via CON1 & CON2. Communicator
outputs are typically: panel armed,
alarm condition, fire, panic and abort,
together with a 12V supply.
The 12 inputs are connected via
10kW resistors to two 74HC4050
high-voltage input non-inverting buffers, which allow the (typically) up to
12V signals from the alarm panel to be
safely converted to 3.3V. The resistors
Australia's electronics magazine
The software for the Raspberry Pi
Pico W is written in MicroPython.
There are three files: main.py, umail.
py and parameters.py. The first two
files should be installed as supplied.
The parameters.py file needs to be
edited to tailor the system to your individual requirements.
The parameters.py file contains
numerous constants and arrays. The
program has been designed to be as
flexible as possible, to allow for many
different scenarios. The file parameters.py can be edited in a text editor,
or with Thonny, as described later.
Note that MicroPython’s code is
strictly case sensitive, so great care is
needed while editing to avoid unintentional errors!
The first section of parameters.py
contains constants that should not
be altered. The user-defined parameters are from around line number 47
through to the end of the file. Looking
at each section in turn:
The first section of comments on
lines 47 to 77 is not essential, but
I found it useful in clarifying my
requirements. I suggest that you review
and change these comments to define
your own requirements. Don’t forget
to include a hash mark (#) at the start
of each comment line.
Editor's note: the line numbers do
not match up to the Listings shown in
this article (taken from “parameters.
py”, as we have removed the comments and line breaks due to space
restrictions. The downloaded file
match the referenced lines.
The next section (lines 78-101, Listing 1) sets timings for various functions in seconds, minutes or hours as
appropriate.
May 2026 71
83.
84.
85.
86.
87.
88.
89.
90.
91.
92.
93.
Watchdog = const(True)
Set_timeout = const(11 * Hours)
Primary_timeout = const(8 * Hours)
Secondary_timeout = const(5 * Hours)
Exit_timeout = const(3 * Minutes)
First_delay = const(30 * Seconds)
Second_delay = const(5 * Minutes)
WiFi_timeout = const(15)
WiFi_retry = const(10 * Minutes)
Maximum_retries = const(3)
Periodic_checking = const(7 * Days)
Listing 1: this section of the code defines various delays and settings. We have
removed comments and new lines for brevity. The line numbering isn’t an exact
match to the actual file, it’s just there to make it easier to follow.
107.
108.
109.
110.
111.
112.
113.
114.
115.
116.
117.
118.
119.
120.
121.
122.
123.
124.
125.
WiFi_username = "Your SSID"
WiFi_password = "Your password"
smtp_address = "smtp.aaa.com"
smtp_port = 25
smtp_username = "Your login"
smtp_password = "Your password"
Email_from = "from<at>aaa.com"
Email_subject = "Alarm status report"
Email_to_1 = "Contact1<at>aaa.com"
Email_to_2 = "Contact2<at>aaa.com"
Email_to_3 = "Contact3<at>aaa.com"
Email_to_4 = "Contact4<at>aaa.com"
Twilio_Account = "Twilio account number"
Twilio_Auth = "Twilio authorisation"
Twilio_phone_no = "Twilio phone no"
SMS_to_1 = "00000000001"
SMS_to_2 = "00000000002"
SMS_to_3 = "00000000003"
SMS_to_4 = "00000000004"
Listing 2: the WiFi, email, and SMS settings.
136. Zone_name = {
137.
0: ["Front door", Primary_zone | Exit_zone],
138.
1: ["Lounge PIR", Secondary_zone],
139.
2: ["Dining door", Primary_zone],
140.
3: ["Back door",
Primary_zone],
141.
4: ["Hall PIR",
Secondary_zone],
142.
5: ["Kitchen PIR", Secondary_zone],
143.
6: ["Abort",
Abort_status],
144.
7: ["Panic",
Communicator],
145.
8: ["Spare",
Spare_zone],
146.
9: ["Spare",
Spare_zone],
147.
10:["Panel",
Panel_status],
148.
11:["Alarm",
Alarm_status],
149.
12:["Test",
Test_button]
150.
}
Listing 3: the zone definitions.
Watchdog should be set to “True”.
Only set it to “False” while testing.
Set_timeout is the amount of time
before an alert is sent when the panel
is set.
Normally, this will be at nighttime
when the alarm panel is set and the
user is in bed. As noted previously,
this timeout is disabled if the exit zone
has been triggered, indicating that the
user has left the premises.
The values Primary_timeout and
Secondary_timeout similarly set the
amount of time before an alert when
the panel is unset; usually, this will
be during the day, when the user is
its home.
Primary zones are where there is
a definite action by the person being
monitored, such as opening or closing
a door that has a door switch.
Secondary zones are typically PIR
movement sensors, and these may
be triggered accidentally by a person
who has fallen trying to get up unsuccessfully, or a pet wandering through.
As such, they are less reliable as an
indication of activity compared with
the primary zone. When relying on
PIRs, you need to monitor more than
one zone!
Exit_timeout defines the amount
of time between the panel being set
(armed) and the exit door being triggered; it will usually be two or three
minutes. It must be set for a longer time
than that set in the alarm panel itself.
Otherwise, the exit condition will not
be recognised.
First_delay is the amount of time
between an alarm condition and the
first alert being sent, and is typically
set to one or two minutes so that false
alarms can be cancelled.
Second_delay is the amount of time
between the alert being sent to the first
contact and the subsequent contacts.
WiFi_timeout is the length of time
the system tries to connect to the router
before timing out.
180. Alarm_types = {
181.
"Alarm":
["Alarm", Delay1 | Email_Contact1 | Delay2 | SMS_Contact2],
182.
"Communicator":
["Communicator", Email_Contact1],
183.
"No_Activity_Clear": ["No activity panel NOT set", Email_Contact1 | Delay2 |
Email_Contact2 | SMS_Contact3],
184.
"No_Activity_Set":
["No activity panel set", Email_Contact1 | Delay2 |
Email_Contact2 | SMS_Contact3],
185.
"Test":
["Test message", Terminal | Email_Contact1],
186.
"Check_in":
["Periodic check-in", Email_Contact1],
187.
"Restart":
["Alarm monitor restart", Email_Contact1]
188. }
Listing 4: the actions to be performed for each alert condition.
72
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WiFi_retry is the amount of time
between attempts to connect to the
WiFi network, assuming that it has
been unsuccessful.
Maximum_retries sets the maximum number of attempts to connect
to WiFi or send an SMS text message.
This is to prevent the monitor from
entering an endless loop due to a WiFi
or SMS problem, and allows it to move
on to subsequent actions.
Periodic_checking enables the monitor to send a periodic email or text
message to confirm that it is up and
running. A value of 0 disables it.
The next section (lines 103 to
125, Listing 2) sets your WiFi username and password, and your email
login details, followed by the email
addresses and SMS phone numbers
of your contacts. I have found different email providers to be a little fickle
about the format of parameters, so
some tailoring may be required. You
should be able to set more than one
email address, possibly separated by
a semicolon (;).
Caution and careful testing are
needed when setting the email login
parameters. Incorrect values can cause
the program to crash and thus not send
the alert messages. As previously mentioned, you will need a free Twilio
account to send SMS text messages.
The following section (lines 127 to
150, Listing 3) defines the function of
each of the 13 input channels to the
system. For each input channel, there
are two parameters: a text description,
followed by its functions. More than
one function can be defined with the
‘inclusive or’ symbol (|), so “Primary_
zone | Exit_zone” defines the input as
both a primary zone and an exit zone.
• Panel_status defines whether the
alarm panel is set (armed) or unset
(clear).
• Alarm_status is set when the burglar alarm is activated (an alarm condition) by an intruder.
201. Activity_conditions = [
202.
[2,0],
203.
[1,2],
204.
[0,3],
205.
[-1,-1]
206.
]
Listing 5: this section of the code sets
the number of primary/secondary
zones that need to be triggered to
indicate activity.
siliconchip.com.au
Parts List – WiFi Alarm Monitor
1 single-sided PCB coded 01304261, 57 × 57mm
1 suitable plastic enclosure (eg, 3D printed)
1 Raspberry Pi Pico W microcontroller module (MOD1)
2 20-pin headers, 2.54mm pitch (for MOD1)
2 20-pin female header sockets, 2.54mm pitch (for MOD1)
1 250mA miniature axial fuse (F1)
2 74HC4050 level-shifter ICs, SOIC-16 (IC2, IC3)
1 AMS1117-5 5V LDO linear voltage regulator, SOT-223 (REG4)
1 1N5819 40V 1A axial schottky diode (D1)
12 10kW ±5% or better axial resistors (4.7kW to 22kW resistors would likely work too)
2 100nF 50V X7R SMD ceramic capacitors, M2012/0805 or M3216/1206 size
1 10μF 50V X7R SMD ceramic capacitor, M3216/1206 or M3226/1210 size
4 3-way miniature (0.15in/3.81mm) screw terminal blocks (CON1, CON2)
OR
3 4-way miniature (0.15in/3.81mm) screw terminal blocks (CON1, CON2)
1 2-way polarised header and matching plug, 2.54mm pitch
(CON3; optional; for S1)
1 2-way miniature (0.15in/3.81mm) screw terminal block (CON4)
1 momentary pushbutton switch (S1; optional)
• Communicator is typically the
‘panic’ or ‘fire’ communicator outputs,
if required.
• Abort_status indicates that an
alarm condition has been cancelled.
• Spare_zone defines any unused
inputs; these should also be connected
to ground electrically.
• Test_button monitors the 13th
input (S1) and will send a test message.
The next section (lines 152 to 188,
Listing 4) defines which actions are
to be performed for each of the alert
conditions:
• alarm
• communicator output
• no activity while the panel is not
set (clear)
• no activity while the panel is set
(armed)
• test message
• periodic ‘health’ check-in
• start-up/reset
These are fixed conditions in the
software and should not be altered.
For each of the alert conditions,
there is a text description followed
by a list of actions. These consist of
delays, emails and SMS messages to
various contacts.
• Delay1 is typically a short delay
to allow time for a false alarm to be
cancelled.
• Email_contactx sends an email
to that contact or group of contacts.
• SMS_contactx sends an SMS
message to a single contact.
• Delay2 sets a delay between contacting contact 1 and the other contacts.
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• Terminal is for testing only and
sends output via the USB interface.
All the actions occur in a fixed
sequence, defined in the subroutine
Poll_alerts() in main.py. The sequence
is: Delay1, Terminal, Email_contact1,
SMS_contact1, Delay2, Email_contact2, SMS_contact2, Email_contact3,
SMS_contact3, Email_contact4, SMS_
contact4.
If no action is required for a certain condition, it can be set to 0. For
example:
“Restart”: [“Alarm
monitor restart”, 0]
If a WiFi connection cannot be
made, the interface keeps trying at
WiFi_retry intervals until Maximum_
retries has occurred and will not move
on to the next action until a successful
connection is made or the retry limit
is exceeded.
Maximum_retries also applies to
attempts to send emails. No check is
made that emails or SMS messages
have been completed successfully;
the interface will simply move on to
the next action. If an email or SMS is
unsuccessful, it is likely to be a hard
fault due to a parameter error, and the
interface would be tied up indefinitely!
The final section (lines 190 to 206,
Listing 5) sets the number of primary
and or secondary zones that need to be
triggered to indicate activity. As previously mentioned, primary zones give
a clear indication of activity, while
secondary zones may be triggered by
a person in distress or a pet.
May 2026 73
So, for accurate monitoring, a minimum of two secondary zones are
needed unless a primary zone has
been triggered. As a result, various
combinations of primary and secondary zones can be set, for example [two
primary zones] or [one primary zone
and two secondary zones] or [three
secondary zones].
Obviously, you cannot define more
primary or secondary zones than those
that are being monitored. Each line has
the number of primary zones followed
by the number of secondary zones.
Each additional line provides an
‘inclusive or’ function, so 2,0 followed
by 1,2 means [two primary zones and
no secondary zones] or [one primary
zone and two secondary zones].
Software libraries
My software makes use of a thirdparty library, uMail (MicroMail) for
MicroPython (https://github.com/
shawwwn/uMail). Also, for the SMS
interface, I used code from Mahmood
Mustafa Shilleh at siliconchip.au/
link/acat
Construction
The prototype was built on a single-
sided printed circuit board with a RPi
mounted on headers and sockets so it
can be easily removed (and because
there’s a diode mounted underneath
it). The 74HC4050 ICs, linear voltage
regulator and associated capacitors are
all surface-mount devices.
Axial resistors were used on the
inputs of the 74HC4050s, as the layout of the gates on these chips is not
particularly user-friendly and resistors
are a convenient way of bridging to the
input connectors.
The prototype used Molex KK-style
connectors for compatibility with previous wiring, but the PCB has been
re-designed to use miniature screw terminal blocks with 0.15-inch (3.81mm)
pin spacing (not the more typical
0.2-inch/5.08mm spacing).
Looking at Fig.3, I recommend fitting the surface-
mount components
first, followed by the resistors and then
the other components.
If you only require a maximum of
six inputs, the second 74HC4050 can
be omitted; the weak internal pullups on the Raspberry Pi Pico module
will automatically disable the remaining inputs.
The finished board can be mounted
in any convenient plastic project box,
or if there is room, within the alarm
panel itself. The author made a custom 3D-printed enclosure, but that is
not necessary. If you do want to print
that, the STL files are included in the
software package at siliconchip.au/
Shop/6/3613
Software installation
The software is installed on the
Raspberry Pi using the free Thonny
integrated development environment
(IDE). The first step is to install the IDE
from https://thonny.org
Installation is quite straightforward
and you will find a lot of useful information on the Thonny website and
also at https://github.com/thonny/
thonny/wiki
Once Thonny is installed, connect
the Raspberry Pi to your computer
using a USB lead while holding down
the white button (BOOTSEL) on the
Raspberry Pi, then start Thonny. You
should see a window similar to that
in Screen 1. Click on the bottom right
corner where it says <no backend>
and then select Install MicroPython
(Screen 2).
You should then see Screen 3. Target
volume sets the location of the Raspberry Pi and should be filled in automatically. If it is blank, you need to
disconnect the Raspberry Pi and connect it again while pressing the white
button. Set:
• MicroPython family to ‘RP2’
• Variant to ‘Raspberry Pi • Pico W
/ Pico WH’
• Version should be set automatically to the latest.
Check that the parameters are correct and then click Install.
When the installation is complete
(which should only take a few seconds), click on the stop button (white
square inside the red circle) and you
should see Screen 4. If it does not
appear, close Thonny, disconnect
and reconnect the USB without pressing the white button, and then restart
Thonny.
The next step is to copy the source
files onto the Raspberry Pi. As previously mentioned, MicroPython is
strictly case sensitive, and this applies
to file names as well as the source program. In the next step, the source files
from your computer will be copied
onto the Raspberry Pi.
Editing files either on your computer or on the Raspberry Pi, does
not update the other copy. You need
to explicitly make a copy. Note that
it may not be obvious whether files
you are editing in the Thonny editing
window are located on the computer
or Raspberry Pi.
The files main.py, parameters.py
Fig.3: the board can be easily etched as it is single-sided, with all the through-hole parts on the top and a few SMDs on
the underside. Take care with the polarity of the SMD ICs (their pin 1 indicators go towards the Pico) and note how D1 is
mounted underneath the Pico W module. Because of that, and to make maintenance easier, it’s best to socket the Pico W.
74
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siliconchip.com.au
Screen 1: the initial
state of Thonny (a
Python IDE) when
you run it after
installation.
and umail.py need to be copied from
your computer onto the Raspberry Pi.
This is the time to edit the parameters.
py file if you haven’t already done it
(use your favourite text editor). Don’t
forget to save a copy both to your computer and to the Raspberry Pi.
In Thonny, click File → Open... and
then select “This computer”. Open
umail.py from your computer, then
click File → Save copy... and this time
select “Raspberry Pi Pico”. Type the
filename “umail.py” and click OK.
Repeat the above for the files main.
py and parameters.py after making
your edits.
Now close Thonny, disconnect and
reconnect the USB lead. The green
light on the Raspberry Pi should flash
at one-second intervals.
Connecting the interface to
the alarm panel
Different alarm panels will vary
slightly, but all should have multiple
zones and a set of communicator outputs. The communicator outputs are
fairly standard, as they are designed
to interface with a range of devices.
Each zone usually has two connections, ignoring tamper circuits. One
connection will be at a fixed voltage
(or ground), while the other is used
to detect the input from the switch or
sensor. It is necessary to connect the
interface to this active signal. A quick
test with a multimeter should identify the correct input to use. Failing
that, try one and, if it does not work,
try the other.
On my Honeywell alarm panel, the
active inputs are on the left.
Don’t forget to ground any unused
inputs. If they are left floating, they
can overwhelm the Raspberry Pi with
unwanted interrupts.
If you want to send SMS messages, don’t forget to get a free Twilio
account!
The author’s monitor has been
running without failure for over 18
months, so the Raspberry Pi and
MicroPython software appear to be
extremely stable.
If possible, once the unit is installed,
there should be easy access to the USB
connector so that parameter updates
can be easily installed.
The Raspberry Pi will need to connect to a reliable WiFi network, so this
needs to be taken into account. In particular, metal enclosures are unlikely
SC
to be suitable.
siliconchip.com.au
Screen 2: this menu
lets you install
MicroPython on the
Pico W.
Screen 3: set the
options in this dialog
as per the instructions
in the text to install
MicroPython.
Screen 4: the Thonny IDE with MicroPython on the Pico W up and running.
Australia's electronics magazine
May 2026 75
By Andrew Levido
Power
Electronics
Part 7: Resonant Converters & Soft Switching
Higher switching frequencies can make input and output filters simpler, with smaller
magnetics. They also allow a faster response to changes in the load current. Switching
losses become a major problem at higher frequencies, but there is a solution.
W
e saw last month that switching
losses in power electronic converters can become dominant
as switching frequencies increase.
However, higher frequencies are
desirable as they allow the designer
to increase the bandwidth of the control system, so it can respond to load
changes more quickly.
We will start with a quick review of
how a Mosfet switches on and off. The
upper-left part of Fig.1 shows a typical boost converter. We will assume
this is operating in periodic steadystate and that the inductor current is
more-or-less constant at the timescale
of the switch-on and switch-off of the
Mosfet, typically in the 10ns range.
We will also assume that the Mosfet
is off and the full load current is flowing through the diode at the instant of
switch-off.
I have also drawn the gate equivalent
circuit of the Mosfet below the boost
converter circuit. When the device is
off, the gate voltage is zero, the gatesource capacitance (Cgs) is fully discharged and the gate-drain capacitance
(Cgd) is charged to the drain voltage,
vd. The gate-drain capacitance is much
smaller than the gate-source capacitance, but it plays a big part in switching losses, as we shall see.
The resistance Rg is the combination
Fig.1: in inductive circuits such as
this, a Mosfet’s drain voltage cannot
begin to change until the current
fully commutates to or from it. This
results in significant switch-on and
switch-off losses. The diode reverse
recovery current makes this worse.
76
Silicon Chip
Australia's electronics magazine
of the internal gate resistance and
the source impedance of the Mosfet
driver. The voltage vg(int) represents
the voltage at the gate metallisation
on the Mosfet die that modulates the
conductivity of the channel.
The plot labelled “Mosfet switch-on”
shows what happens when we switch
the Mosfet on. When the gate voltage
is applied at time t0, nothing happens
immediately because the internal gate
voltage (black trace) has yet to charge
to the switch-on threshold.
Once the threshold voltage is reached
at time t1, the drain current (red trace)
begins to rise. Because the load is
inductive, the drain current must rise
to its full extent before the drain-source
voltage can begin to fall, at time t2.
You can understand why this is the
case with reference to the boost converter schematic. When the Mosfet
starts to conduct, the current shifts
(commutates) from the diode to the
Mosfet. Until the Mosfet takes over
100% of the inductor current, the
balance continues to flow through
the diode, keeping the Mosfet’s drain
voltage fixed at the converter’s output voltage.
This same phenomenon occurs in
many converter types, including buck
converters, but it’s easiest to visualise with the boost converter since the
Mosfet is grounded.
The rate at which the drain voltage
can fall is determined by how fast Cgd
can be discharged. The only thing discharging Cgd is the current i Cgd provided by the gate drive. While vds is
falling, all the gate current is diverted
into Cgd due to the Miller effect, so the
internal gate voltage remains essentially constant until the drain-source
voltage reaches (almost) zero at time t3.
This ‘flat spot’ on the internal gate
voltage is known as the Miller plateau.
After t4, the two gate capacitances
are effectively in parallel, and the
siliconchip.com.au
siliconchip.com.au
20V
18V
16V
V(vg)
14V
12V
10V
8V
6V
4V
2V
0V
8kW
V(vd)* - I(R1)
6kW
4kW
2kW
-2kW
500V
30A
400V
24A
300V
18A
200V
12A
100V
6A
0V
380.96μs
380.97μs
380.98μs
380.99μs
381.00μs
381.01μs
381.02μs
381.03μs
381.04μs
381.05μs
-I(R1)
0kW
V(vd)
gate voltage continues to rise to its
final value at t4, where the channel is
fully enhanced and the Mosfet’s on-
resistance is minimised. Switch-off is
basically the reverse of this process.
The importance of all this is that
there is a period, from t1 to t3, where
there is significant voltage across and
current flowing through the device at
the same time, and therefore considerable power dissipated during the
relatively short switch-on and switchoff periods. In fact, things are worse
than I just described if we take into
account the ‘switch-off’ characteristics of the diode.
When a diode switches from the
conduction state to the blocking state,
it does not switch off instantaneously.
A large reverse current flows for a
short period while the diode recovers
its blocking capability – shown in the
“Diode switch-off” plot.
This ‘reverse recovery’ current
occurs because the majority carriers
stored in the PN junction have to be
extracted when the diode is reverse-
biased. The amount of this charge
(Qrr in the data sheets) is small, but
because it moves very quickly, the
peak current can be high. This does
not have a huge impact on the diode
losses, but can contribute significantly
to Mosfet losses.
When the Mosfet switches on at
time t2 and the inductor current commutates from the diode, the Mosfet
sees an additional current spike due
to the diode’s reverse recovery (bottom
chart). This occurs while the drainsource voltage is still high, so it adds
to the Mosfet switch-on losses.
While it is often convenient to think
of power Mosfets as voltage-driven
devices, the description above demonstrates the importance of gate current
in the switching process. The rate of
change of drain-source voltage (dv/dt)
during switching depends on the gatedrain capacitance and the gate current
that charges and discharges it.
You generally need to drive the gate
hard if you want to increase the dv/
dt and minimise switching loss. However, a higher dv/dt produces in significantly more conducted and radiated EMI, so finding a compromise is
usually necessary.
How significant are these switching losses? I made a simulation of
the boost converter circuit using the
SiHA120N60E Mosfet. This is a 650V,
25A-rated device in a TO-220 package.
0A
381.06μs
Fig.2: this simulation of the circuit in Fig.1 uses the SiHA120N60E Mosfet
switching 400V at 20A. The switch-on losses peak at 7.5kW, although only
for a few nanoseconds.
Fig.3: a resonant circuit like this can be described by two quantities: the
natural frequency and the damping factor. We often use the ‘quality factor’
or Q to describe the relationship between the two.
I set the boost converter input voltage
to 200V, the output voltage to 400V and
the load current to a slightly unrealistic 20A. I drove the gate to 15V via a
10W gate resistor.
The simulated switching waveforms
are shown in Fig.2. You can clearly see
that the drain current (red) rises fully
before the drain-source voltage (blue)
can begin to fall. You can also see
the Miller plateau in the gate voltage
(green). The purple trace is the instantaneous power dissipation in the Mosfet. It peaks at about 7.5kW, although
the whole spike is only about eight
nanoseconds long.
The total energy dissipated at
switch-on is about 30µJ. If we assume
the same for switch off, the total will
be 60µJ per cycle. At 10kHz, this corresponds to a modest 600mW in losses,
Australia's electronics magazine
but if we want to switch at 1MHz, we
are looking at switching losses of 60W
– a much less attractive proposition!
Resonant circuits
Since switching losses are the
product of voltage across and current
through the switch, one way to reduce
or eliminate switching losses would
be to ensure that one or both of these
quantities is zero at the time of switching. This type of switching is sometimes called zero-voltage switching
(ZVS), zero-current switching (ZCS)
or just described by the generic term
‘soft switching’.
The usual way to ensure that voltage or current is zero when we switch
is to exploit resonance. For a quick
refresher on resonance, take a look
at Fig.3, which shows a simple RLC
May 2026 77
filter with a DC source and a switch
that closes at time zero.
When the switch initially closes, a
current will build up in the inductor,
charging the capacitor through the
resistor. The voltage on the capacitor
will continue to rise past Vsrc to the
point where the current in the inductor
reverses and it begins to fall. When the
capacitor voltage falls low enough that
the inductor current reverses again, it
starts to rise.
This oscillation continues, but is
damped by the resistance. Eventually,
the capacitor voltage settles at Vsrc
and the inductor current goes to zero.
This is a damped oscillation. If the
resistance were zero, the oscillations
would continue indefinitely (in theory). If the resistor had a very high
value, the circuit would behave like a
standard RC filter, with the capacitor
voltage rising smoothly (and exponentially) to Vsrc.
We can therefore describe these
resonant circuits with two quantities:
the natural frequency and the damping factor. The natural frequency,
designated ω0, is the frequency at
which the undamped LC network
would oscillate. This is given by ω0
= 1 ÷ √LC.
The damping factor, designated by
the Greek letter α, is equal to R ÷ 2L.
The damped circuit will oscillate at a
frequency lower than the natural frequency. This frequency, ωd, called the
natural frequency, is equal to √ω02 –
α2. These frequencies are expressed in
radians per second, where 2π radians
per second equals 1Hz.
We don’t generally use the damping factor directly in our design process. Instead, we use a related quantity, the ‘quality factor’ or Q of the
circuit. Q relates the damping factor to the natural frequency by the
expression Q = ω0 ÷ 2α. A resonant
circuit with high Q has low damping,
and vice versa.
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Fig.4: if we switch this resonant DC-AC converter at its natural frequency,
the inductive and capacitive reactances cancel, and maximum power is
transferred to the resistive load. By shifting the frequency above or below
the natural frequency, we can control the power to the load.
of the square wave. This gain is called
the ‘tank gain’.
If the switching frequency is a little
higher or lower than the natural frequency, the circuit looks a bit inductive or capacitive, respectively. The
tank gain falls off either way, and the
amount of power transferred to the
load reduces. We can therefore control the load power by frequency-
modulating the drive signal.
We can choose to use either ‘above
resonance’ or ‘below resonance’ control strategies. We will see how this
works in practice later.
The graph in Fig.4 suggests that
switching occurs at the current
zero-crossing, but this is a bit misleading. It is true that the current is
near-zero at the time of switching if
the switching frequency is precisely
aligned with the resonant frequency,
but we have already discussed that we
will operate at a higher or lower frequency to control the output power.
However, it is easy enough to modify this circuit to achieve zero-voltage
switching. It just requires the addition of a small capacitor across each
switch and a short ‘dead time’ during
which both switches are off. This is
shown in Fig.5. Here, we are using
over-resonance control, so the LC filter looks inductive and the current lags
the voltage by the angle θ.
The charts to the right of the figure show the load current (blue) and
the voltage across the lower switch,
S2 (red). During period A, the upper
switch S1 is conducting, so C1 is discharged and C2 is charged to Vsrc.
At the beginning of period B, S1
opens while the load current is still
positive. Capacitors C1 and C2 take
over providing the load current, and
the voltage across S2 falls while C1
charges and C2 discharges.
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Silicon Chip
You can play around with substituting these expressions into each other
and get two other useful definitions:
Q = ω0L ÷ R and Q = 1 ÷ ω0CR.
We can use this information to
build a resonant DC-AC converter, as
shown in Fig.4. A DC source feeds a
half-bridge switch followed by an LC
series filter and a resistive load. The
end of the load is held at ½Vsrc by the
two bypass capacitors. These have a
value large enough that their midpoint
voltage remains more-or-less constant
at the switching frequency.
The voltage across the filter and
load is therefore a square wave with
amplitude ½Vsrc, as shown in the red
trace. If we switch the converter at a
frequency equal to the damped natural frequency of the filter and load,
the load current and voltage will be
a relatively pure sinusoid at that frequency.
With the switching frequency equal
to the natural (resonant) frequency, the
inductive and capacitive reactances
cancel out, so the load looks resistive
and the maximum possible energy is
transferred to it. We say that the voltage gain of the resonant tank is unity
under these conditions.
By this, we mean that the AC voltage
across the resistive load (blue) is equal
to the amplitude of the fundamental
If the capacitor values are chosen such that the period B is large
with respect to the (~10 nanosecond)
switching time, the voltage across S1
at the time it opens will be effectively
zero – C1 will hold the voltage across
S1 to zero while it opens.
At the start of period C, C1 is fully
charged to Vsrc and C2 is fully discharged. The still-positive load current now commutates to the freewheeling diode, D2. At this time, S2 can be
closed while the voltage across it is
zero. When the load current reverses
at the start of period D, S2 is closed,
ready to take the load current for the
bulk of its negative excursion.
At the start of period E, S2 is
opened, while C2 holds the voltage
across it to zero. The capacitors support the load current until the start
of period F, when the freewheeling
diode, D1, takes over. This is when
S1 is closed, while its drain-source
voltage is zero.
The upshot of all this is that both
switches only ever open or close with
zero voltage across them, resulting in
very low switching loss. The caveats
to this are that the device switch-off
time is small compared to the charge/
discharge times of C1 and C2, and that
there is enough phase lag that the freewheel diodes are conducting when the
switches are on.
The former is not such a challenge,
since the switching time is short, but
the latter means that we cannot operate
too close to natural frequency so the
filter inductance remains high enough.
Resonant DC-AC converters like this
are pretty common – for example, most
induction cooktops work this way.
A typical large domestic induction
cooktop contains resonant converters
capable of a power output up to 7kW
at frequencies in the 20-100kHz range.
This would not be practical without
zero-voltage switching.
Fig.5: with the addition of capacitors across the switches and a short deadtime when both switches are off, we can achieve almost lossless switching. The
switching frequency must always be a little above the natural frequency for this
to work.
Resonant DC-DC converters
You could also imagine rectifying
and filtering the output of a resonant
DC-AC converter, perhaps after passing it through a transformer, to produce
a DC output, as in Fig.6. Frequency
modulation could be used to control
the resulting DC output voltage.
We can think of this converter as
a series of four blocks, each with its
own voltage gain. The product of these
gains is the voltage transfer function of
the converter: Vl ÷ Vsrc = Gi Gt Gx Gr.
siliconchip.com.au
Fig.6: a resonant DC-DC converter can be thought of as four distinct blocks, each
with its own gain. This simplifies the analysis enormously.
Australia's electronics magazine
May 2026 79
Calculating some of these gains is
easy. The inverter puts out a square
wave with a peak-to-peak amplitude
of Vsrc, so an amplitude of ½Vsrc. The
current is sinusoidal, so only the fundamental component of this voltage
can transfer real power.
We have seen many times before that
the amplitude of the fundamental frequency of a square wave is 4 ÷ π times
its amplitude. Since the amplitude is
½Vsrc, the gain through the inverter
must be Gi = 2 ÷ π.
The gain of the tank is much more
complex. I won’t go through the derivation (life is too short as it is), but it
can be shown to be the ugly expression under the resonant tank block
in Fig.6. The important thing to note
is that the tank gain depends on the
ratio of the damped-to-undamped natural frequencies and the Q of the tank.
We’ll look into this more when we get
to an example.
The transformer’s voltage gain is
trivial to calculate – it is just the turns
ratio, as you would expect. Calculating
the rectifier’s gain is a bit harder, but
not much. Fig.7 shows how.
The resonant tank current driving
the transformer primary will be sinusoidal, so we can model the transformer’s secondary current as a sinusoidal
current source, is, with some amplitude I, which will depend on the primary current and the turns ratio. The
waveforms associated with this simplified circuit are shown on its right.
If we assume the filter capacitor is
large enough to make the voltage ripple
negligible and the diodes are ideal, the
transformer secondary voltage vs will
be a square wave with amplitude Vl.
Because is is sinusoidal, only the fundamental component of vs can contribute real power to the load.
Again using the relationship for the
fundamental of a square wave, the gain
of the circuit Vl/vs(1) is π ÷ 4.
We also need to work out the equivalent AC resistance of the rectifier
and load. This is important because
it is this resistance, seen through the
transformer, that loads the resonant
Fig.7: this diagram shows how we
calculate the equivalent AC resistance
of the rectifier filter so we can
understand the damping seen by the
resonant tank.
Fig.8: the curves show the tank gain vs normalised frequency for various
values of Q. The example in the text operates in the region bounded by the
dotted lines and the Q=1 and Q=4 curves.
80
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Australia's electronics magazine
tank and determines its damped natural frequency and Q, both of which
will affect the tank gain.
Dividing vs(1) by the secondary current gives an equivalent AC resistance
of the rectifier and filter of R(ac) = (4
÷ π) × (Vl ÷ I). Expressed in terms of
the converter’s power output, R(ac) =
(8 ÷ π2) × (Vl2 ÷ P). Noting that the
last bracketed term is equal to the load
resistance, R(ac) = (8 ÷ π2) × Rl.
A practical example
We now have all the equations we
need to look at a practical design example. There is not enough space here
for a comprehensive design exercise,
but I want to show how one would
approach such a design.
Let’s imagine we are building an
isolated resonant DC-DC converter
to operate from rectified mains and
deliver 10V DC at 20A (so 200W) into
a resistive load. The input voltage
range should be 300-400V to accommodate a range of mains voltages (let’s
not worry about supporting 110-120V
AC mains just yet).
Because we are using the frequency
to control the output power, we need
to specify a minimum load so the frequency range is bounded at both ends.
We will use a minimum load of 5A
(50W) for this exercise. We will use
above-resonance control with a target switching frequency in the range
of 500kHz to 1.5MHz, or thereabouts.
I will break the design up into steps.
1. We can start by calculating the
maximum and minimum load resistances corresponding to the minimum and maximum output currents:
Rl(min) = 0.5W and Rl(max) = 2W. We can
also choose an undamped natural frequency at the low end of our desired
range, say 600kHz or 3.77 × 106 radians per second.
2. We have to design the transformer turns ratio so we can achieve
the desired output voltage when the
source voltage is at its minimum. The
minimum DC voltage times the inverter
gain Gi gives us a minimum input voltage of 191.0Vrms. On the other side of
the transformer, the 10V output voltage
divided by the rectifier gain Gr tells us
that the fundamental of the secondary
voltage must be 12.7Vrms.
The ratio of these values gives us
a transformer gain Gx (secondary to
primary turns ratio) of 0.067. We actually need a bit more gain than this
because I have neglected the rectifier
siliconchip.com.au
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11V
V(vl)
10V
9V
8V
7V
6V
12V
10V
8V
6V
4V
2V
0V
-2V
-4V
-6V
-8V
-10V
-12V
250μs
V(vs1)-V(vs2)
diode drops and any other losses. I
will therefore use a nice round turns
ratio of 0.1 (ten primary turns for every
secondary turn).
3. Now we can calculate the required
tank gain. This is easy because we
know the inverter gain, the transformer
gain, the rectifier gain and the required
end-to-end voltage gain (Vl/Vsrc).
Because we have a range of input voltages, we will also have a range of tank
gains. It turns out that the tank gain
Gt has to range between 0.5 and 0.67.
4. The last thing we have to do before
we can calculate the component values
is to work out what the load resistance
looks like from the primary side of the
transformer. This is the resistance that
will load the resonant circuit.
We saw from the analysis of the
rectifier that the secondary-side AC
resistance of the load is (8 ÷ π2) × Rl.
This transforms our 0.5W and 2W minimum and maximum load resistances
to 0.405W and 1.62W respectively.
We then have to reflect these resistances through the transformer ratio
by multiplying them by (N1 ÷ N2)2,
which just means multiplying them
by 100 in our case. The effective resistance loading the tank is therefore in
the range of 40.5W to 162W.
5. We calculate the resonant tank
component values based on the Q.
The minimum Q occurs when damping is highest and the resistance is at
its maximum, corresponding to light
loading on the converter. We can just
choose the minimum Q to be 1 and
calculate the resonant inductor from
Q = (ω0L) ÷ R.
Rearranging to make L the subject
and plugging in the other values (ω0 =
3.77 × 106 radians per second and R =
162W) gives an inductance of 43.0µH.
We can then calculate C from the relationship ω0 = 1 ÷ √LC to give 1.63nF.
6. Finally, we can calculate the maximum Q, which occurs when the load
is heaviest and the resistance load on
the tank is lowest. We can use the same
Q = (ω0L) ÷ R formula, this time plugging in the inductance we just calculated and the 40.5W minimum resistance. This gives us a maximum Q of
4, which is not unreasonably high.
7. You could use the ugly formula
for tank gain in Fig.6 to calculate
what this means for the damped natural frequency, but it is probably easier to follow if you look at the graph
in Fig.8. This plots the tank gain vs
the normalised frequency (the ratio of
251μs 252μs
253μs
254μs
255μs
256μs
257μs
258μs
259μs
260μs
261μs
262μs
263μs
264μs
265μs
266μs
267μs
268μs
269μs 270μs
Fig.9: this simulation of the example resonant DC-DC converter agrees with
the calculations. The upper green trace is the output voltage and the lower
mauve one is the transformer secondary voltage.
damped natural frequency to the natural frequency) for various values of Q.
Our converter will operate in the
region bounded by the two horizontal
dotted lines (tank gain of 0.5 to 0.67)
and the curves corresponding to Q=4
(purple) and Q=1 (blue/cyan). The
tank gains correspond to the range of
input voltage and the Q values correspond to the load resistance range.
We can then read off the minimum
and maximum normalised frequencies
from the horizontal axis. I have marked
these points with large dots. In this
example, we expect the resonant frequency to range from 1.15ω0 to 2.1ω0.
This corresponds to a frequency range
of 690kHz to 1.24MHz.
Results
I find this type of graph very intuitive. The lowest switching frequency
corresponds to a heavy load, low input
voltage scenario. The highest switching frequency corresponds to the
lightest load and highest input voltage scenario. You can see now why
we have to set a minimum load – the
switching frequency will go through
the stratosphere if the load resistance
gets too high.
I could not resist simulating this circuit, as shown in Fig.9. The inverter
block on the left just contains a
behavioural voltage source that produces a 50% duty cycle square wave
with the frequency and amplitude
specified on the front. The resonant
Australia's electronics magazine
tank and transformer are obvious,
and the rectifier block consists of a
full-bridge of ideal diodes and a 10µF
capacitor.
The simulation run below the schematic was at the highest load, lowest
input voltage operating point. The
results are a bit unspectacular, with
the DC output voltage in green and
the transformer secondary voltage in
purple. However, it does confirm that
this switching frequency is roughly
correct to achieve the output voltage
we desire.
There is obviously a lot more to
designing a resonant converter, especially one at this power level. In fact,
this article has just given a small introduction to resonant and soft switching
converters; there are countless variations out there, including some quite
novel and interesting circuits.
Conclusion
This article concludes our series
on power electronics. We have covered a lot of ground, including DC-DC,
AC-DC and DC-AC converters. We
have touched on control systems, magnetics and EMI filtering, and with this
article, resonant converters.
As I stated at the outset, this series
was not meant to be a university-style
course on power electronics. Rather,
I hope I have provided some insights
and a few tools and techniques that
may be useful in exploring this endSC
lessly fascinating topic.
May 2026 81
Installing a Hidden
CB Radio
in your Car
by Julian Edgar
You can improve your safety and convenience when driving on country
roads with a near-invisible radio. Shown here is a GME all-in-one CB
radio. Using this type of design means you only need space on the
dash or centre console for the handheld microphone. The rest of the
electronics is housed in the small box that is easily tucked away.
M
any people don’t realise that having a CB radio in a car can be
very beneficial, especially in rural
Australia. Such a radio can be nearly
invisible, both in terms of occupying
dashboard space and the presence of
the antenna.
Safety and convenience
Nearly every truck in Australia is
fitted with a UHF CB radio. They’re
used by the driver when the truck is
entering a building site (that’s why you
see signs like “UHF 21” on entrance
gates to such sites). More relevant to
us, on country roads, they’re set permanently to Channel 40.
Unlike in old movies (“Breaker,
breaker, got a copy Big Bear”), truck
drivers mostly talk about road hazards, warning other trucks of the problems they’re about to encounter. This
makes listening on a CB radio incredibly useful for anyone who drives on
rural roads.
I have used CB radios in nearly
all my cars of the last 40 years and,
over that time, I have been warned
82
Silicon Chip
of thousands of road hazards. That
includes car and truck accidents,
floods, vulnerable touring cyclists,
vehicles broken down but not sufficiently pulled off the road, road works,
wide loads, trucks with dangerously
loose tie-down straps and chains – the
list goes on and on.
I have also used the radio to tell
trucks their rear lights aren’t working,
to warn them of hazards I have seen
that await them, and on one memorable occasion, to request a pickup from
my broken-down car, at night and over
100km from the nearest town (yes, a
truck stopped!).
Unlike amateur radio, no license is
needed for CB radio operation. You
simply buy it, fit it and use it!
To anyone used to operating a radio
in a formal situation, truckies on CB
might sound like anarchy in action –
but it isn’t. In fact, the communication
is strongly codified by tradition. It’s
in cities where (unfortunately) every
idiot is on the radio screaming meaningless rubbish.
Over time, you get used to listening
Australia's electronics magazine
for the tone of communications, the
radio just burbling away in the background. A driver saying hello to a
friend who he (they’re nearly always
male) has seen travelling the other
way has one tone; the escort vehicle
of a wide load warning other trucks
that the load is coming through has
a quite different tone; and a warning about an accident has a different
tone again.
As an example of the radio in action,
the other day I drove from my home
north of Canberra down the Barton
Highway towards the city. When I
turned onto the highway, I immediately knew that something was up; I
heard a snatch of conversation where
a driver was asking if traffic was being
allowed through. That gave me an indication that there had been an accident
and the road may be closed.
So it proved. As I got closer, the
radio chat increased until, by the time
I reached the stopped traffic, I knew
the type of vehicles that had been in
the accident, the length of the traffic jam and the likely duration of the
siliconchip.com.au
A UHF CB radio installed on the dash of my MG4 electric car. Glass-mount CB radio antennas are unobtrusive and can
be installed in minutes. The antenna cable connection is via a small box that sticks to the inside of the glass – no holes are
needed!
delay. Coincidentally, as I got to Canberra, there was a further delay; this
time I asked what the problem was and
was immediately told there had been
another car crash.
A stealth CB installation
Most people don’t want a gigantic
antenna on their car – there’s also the
hassle of fitting it, trying to get a cable
into the cabin and also finding space
on the dash for the radio. Luckily, you
don’t need any of that.
There are two approaches that make
fitting a largely invisible CB radio quite
easy. The first is to use a glass-mount
antenna.
As its name suggests, a glass-mount
antenna sticks to the front or rear glass
of the car. Normally, you place it on
the windscreen, high up near the roof.
The antenna comprises just a very
short whip (typically 200mm long)
with a small mounting square at its
base that sticks to the glass with strong
double-sided tape.
Attaching this takes, oh, about 30
seconds! Clean the glass, peel off the
backing tape, stick it into place.
So, how does the cable connect to
the antenna? Don’t you have to drill
a hole through the windscreen? No;
instead, the connection through the
glass is made by RF, with a little rectangular box stuck inside the windscreen
at the antenna’s location.
To run the small-diameter antenna
cable to the box, you simply tuck the
cable behind the roof headlining and
then down behind the A-pillar moulding. Typically, the provided cable
siliconchip.com.au
doesn’t need to be cut – any surplus
length is just coiled out of sight.
Editor’s note – this cable route is
also suitable for the power cable on
many dash cams.
The second approach is regarding
the radio itself. The trick is to use a
5W radio where the microphone is an
‘all-in-one’ control. That is, the microphone is also the speaker and has all
the radio’s controls and displays on it.
Radios of this design have a separate
box that houses the main electronics, small enough that it can be easily
tucked behind the dashboard or centre console – yes, even in current cars.
All you then need to do is to find a
source of power (invariably I access
this at the back of the cigarette lighter/
accessory power socket) and find a
place to mount the compact microphone on the dash or centre console.
The radio will have an inline fuse in
its power feed, so you don’t even need
to add a fuse.
Don’t cut the wires at the cigarette
lighter socket; just bare a short length
of the positive and negative leads and
solder the power and ground leads
of the radio appropriately. Having
said that, you should pull the cigarette lighter fuse first and thoroughly
insulate all connections with tape
before restoring it.
Compared to installing a traditional
CB radio and antenna, especially in
modern cars, the process is quick
and easy.
In the past, the bane of a CB radio
was engine ignition noise, which can
be very annoying and is often quite
hard to get rid of. However, in my
experience, modern cars are much
less likely to generate such noise. My
current car, an EV, generates no audible RF noise at all (not even from the
inverter) – something I was not sure
about before fitting the radio.
Conclusion
A glass-mount antenna and all-inone CB radio will cost more than a traditional CB antenna and radio. It also
won’t have the reception or transmitting range of a large antenna mounted
on a bull bar, but it will be absolutely
fine for monitoring road conditions
and talking to nearby vehicles.
If you drive on country roads, a CB
is a must-have for safety and convenience. Using an all-in-one radio and
glass-mount antenna means that only
the closest of observers will even realSC
ise you have a radio on board.
Squelch and transmission range
All CB radios have an adjustable squelch control that quietens the radio unless
a signal is received (ie, someone is talking). This means that for much of the
time, the radio is silent – it’s not a continual distraction or annoyance. Also,
because of the limited range (less than 5km for the set-up described here),
when someone does talk, it’s often relevant.
Australia's electronics magazine
May 2026 83
By Tim Blythman
Remote Controller
DCC Booster
Stepper Motor Driver
μDCC Decoder
microDCC Decoder
μDCC
The DCC Decoder design in the December 2025 issue is very small, but sometimes not small
enough. The μDCC Decoder is designed to be a bare minimum decoder to take up less space, but
we’ve still managed to squeeze in a couple of handy features that make it very useful beyond just
Image source: https://unsplash.com/photos/black-model-train-moving-through-a-garden-hc9xarcmpM8
being smaller than its predecessor.
W
e designed the DCC Decoder, from the
December 2025 issue, as a simple,
inexpensive but complete unit
that can add DCC capabilities to small
model railway locomotives in the HO
and N scales.
As I started adding them to my
fleet of models, I realised that I could
make a couple of changes that would
improve their usefulness. I’m not saying that this design is better or worse
than the original Decoder, but it is
smaller, and I have added some features that I think might be of interest.
I recently made the jump to N scale
after previously working with HO scale.
With the help of a 3D printer, I started
scratch-building some model trams,
which are even smaller than trains!
I thought that the original Decoder
would be a good size for what I wanted
to model, but those who have done
any work at this scale will know that
anything that can save space will
Features & Specifications
be helpful. So I looked at the earlier
design to see what I could take out to
make it even smaller.
First, I didn’t think that I really
needed four function outputs, so I
discarded two of them. This removes
four resistors and two transistors from
the board. Next, I removed the circuitry to sense the incoming supply
voltage; two more resistors removed.
This means that the μDCC Decoder has
only two function outputs and does
not have the ability to compensate for
supply voltage changes.
I also figured I could do without
the 100nF capacitor on the microcontroller since the micro would be close
enough to the existing 10μF regulator
output filter capacitor.
Hardware-wise, these are pretty
much the only differences between
the original Decoder and the μDCC
Decoder. The newer board is only 12
× 18mm, down from 13 × 28mm; only
In model railways, smaller
is generally better. The μDCC
Decoder is only 12mm ×
18mm with two function
outputs and even has a
basic sound function.
🛤 Size: 18 × 12 × 4mm
🛤 Two 100mA function outputs
🛤 Sound output
🛤 Standard DCC features like the December 2025 DCC Decoder
84
Silicon Chip
Australia's electronics magazine
60% of the area! Fig.1 shows the circuit diagram, and you can see that it
really is just a cut-down version of the
earlier design.
It looks like there are some unused
pins that are wasted, but I have redeployed I/O pin 11 to supply the 3.3V
reference that came directly from the
3.3V regulator in the earlier design; the
firmware simply holds this at a high
level (3.3V) at all times. This avoids
an awkward trace that would otherwise have had to cut across the board.
Having a few unused pins made
the PCB trace routing easier and more
compact, so it actually ended up being
a good compromise. I have made some
extra signals available on the RA0/PGD
and RA1/PGC pins; they have been
chosen mainly because they already
have external connections available
at the ICSP (in-circuit serial programming) header.
Just like in the earlier design, track
power is rectified by diode bridge
BR1. REG1 provides 3.3V to power
the microcontroller. The DCC signal
polarity is sensed via the two 100kW
resistors, and the micro drives the
outputs on pins 2, 3, 5 and 6 to control transistors Q1 and Q2 and motor
driver IC2. These would be connected
siliconchip.com.au
Fig.1: the μDCC Decoder circuit is very similar to the December 2025 DCC Decoder, with a few components removed. The
3.3V reference for the motor driver IC comes from a pin on IC1 to simplify the PCB routing.
to accessories (such as lights) and the
locomotive motor, respectively.
The 100W resistor and series diode
D1 allow a capacitor to be fitted to provide ‘keep-alive’ power that can help
compensate for intermittent contact
due to dirty track. In other respects,
operation is the same as the earlier
design.
Bonus features
The PIC16F181xx family of chips
has an 8-bit DAC (digital-to-analog
converter) that has reasonable drive
strength. It isn’t specified what current it can deliver, but tests indicated
that it would be possible to source and
sink up to 20mA.
After removing excess features
from the earlier Decoder firmware,
the PIC16F18126 has around 12kB
of unused flash memory, which is
enough to hold a fraction of a second of
8-bit sampled audio data. So I investigated driving a small piezo transducer
with the DAC to reproduce audio.
The DAC output is directed to pin
13, since this is broken out amongst the
ICSP pins. It has a ground pin next to
it on the ICSP header, so it’s fairly easy
to make the necessary connections to
the transducer. An electromagnetic
siliconchip.com.au
speaker will likely have an impedance
that is too low to work; you must use
a high-impedance device like a piezo
transducer.
The piezo I tested measures 9mm
square and 2mm thick. Its model
code is in the parts list; I’ve managed
to squeeze this device into several
N-scale models. The piezo transducer
has a peak response around 4kHz,
which is quite high, and I quickly
found that high-pitched sounds were
reproduced much better than lower-
pitched sounds.
This means that a high sampling rate
is needed; fortunately, the DCC firmware already includes a 22μs timer
interrupt, which (at 45.4kHz) is fairly
close to the 44.1kHz sample rate used
in audio from sources like CDs. This
made it easy to experiment with existing samples.
So, onboard audio production is
possible, but the result is not hifi! Still,
I was able to recreate some recognisable sounds for a model railway. The
best sound I could recreate was a tram
bell. This could also pass for the level
crossing bell used on some diesel locomotives. The μDCC Decoder would
also work well as a stationary decoder
for a level crossing’s lights & bells.
I figured that a steam locomotive
whistle might also be sufficiently highpitched to work, so I’ve synthesised
a sample that emulates this. We’ve
made a recording of these sounds being
played by the μDCC Decoder, so that
you can hear for yourself. It’s an MP3
audio recording from siliconchip.au/
Shop/6/3587
The 8-bit microcontroller has modest processing power and would struggle to mix the two sounds, so we have
DCC PROJECT KITS
DCC Base Station, January 2026 (SC7539, $90)
DCC Remote Controller, February 2026 (SC7552, $35)
DCC Booster, March 2026 (SC7579, $45)
DCC Stepper Motor Driver & Decoder, April 2026 (SC7601, $30)
microDCC (μDCC) Decoder, May 2026 (SC7617, $25)
includes all the parts and the optional piezo (wire not included). Specify if
May 2026 85
Australia's
electronics
magazine
you
want a bell
or whistle
sound programmed into the microcontroller.
Pay close attention to the resistor
values and component polarities.
Fortunately, the two capacitors are
of the same value. The regulator
and transistors are all in SOT-23
packages, so be sure not to mix them
up.
Screen 1: It’s incredible what is
possible with model trains; tiny LCD
modules like these add another element
of realism. The CV48 serial data feature
is intended to control features that don’t map well to traditional DCC
function outputs. Source: https://youtu.be/tC_t22RfQ0c
created two firmware files: one for
the bell sounds and one for the whistle sound. If combined, the samples
would also have to be shorter.
Sound is controlled by a function
output. The bell sound will repeat as
long as the function is active, and a
cheery “ding-ding” will be heard if
the function is held for about half a
second. The whistle sound will ramp
up and keep playing until the function
is switched off, after which it quickly
decays to silence.
We’ve also added another output to
the μDCC Decoder. It is intended to
allow communication with another
microcontroller that could implement
other features.
One application that came to mind
is a form of headboard or destination
display, such as a second microcontroller driving a small OLED module or
LCD. When it receives a byte over the
serial link, it can update the display.
This would only happen occasionally,
so would be easy to control with the
Base Station’s CV programming page.
The YouTuber diorama111 has
implemented this type of display in
HO scale models, although it is controlled through an infrared remote control. Screen 1 shows a still from the
video at https://youtu.be/tC_t22RfQ0c
The output is a UART (serial data)
signal that is available on RA1/PGC,
the other I/O pin that is free on the
ICSP header. It operates at 3.3V, 9600
baud with eight data bits. This protocol
EEPROM location
Stepper Driver
μDCC Decoder
Extra output
Decimal Hex
86
DCC Decoder
CV Default
Hex
CV Default Hex
CV Default Hex
0 0x00
29 2
0x02
29 2
0x02
29 2
0x02
1 0x01
1 3
0x03
1 3
0x03
1 3
0x03
2 0x02
19 0
0x00
19 0
0x00
19 0
0x00
3 0x03
18 0
0x00
18 0
0x00
18 0
0x00
4 0x04
17 192
0xC0
17 192
0xC0
17 192
0xC0
5 0x05
2 0
0x00
3 0
0x00
2 0
0x00
6 0x06
3 0
0x00
4 0
0x00
3 0
0x00
7 0x07
4 0
0x00
5 64
0x40
4 0
0x00
8 0x08
5 0
0x00
33 1
0x01
5 0
0x00
9 0x09
6 0
0x00
34 2
0x02
6 0
0x00
10 0x0A
33 1
0x01
35 0
0x00
33 1
0x01
11 0x0B
34 2
0x02
36 0
0x00
34 2
0x02
12 0x0C
35 4
0x04
37 0
0x00
35 4
0x04
13 0x0D
36 8
0x08
49 255
0xFF
36 0
0x00
14 0x0E
37 0
0x00
50 255
0xFF
37 0
0x00
15 0x0F
49 255
0xFF
11 0
0x00
49 255
0xFF
16 0x10
50 255
0xFF
50 255
0xFF
17 0x11
51 255
0xFF
11 0
0x00
18 0x12
52 255
0xFF
19 0x13
11 0
0x00
20
0x14 Chip47 0
Silicon
0x00
TableAustralia's
1: CV toelectronics
EEPROMmagazine
mapping
is simple and common enough that
any microcontroller should be able
to receive it and provide some custom functions.
It is controlled through a virtual configuration variable (CV), CV48. Operations mode programming allows this
CV to be programmed ‘on the mainline’. Any time the μDCC Decoder
receives a write command to program
CV48, it sends the corresponding data
byte over the serial output. That’s all
there is to it.
These pins are shown on the overlay/wiring diagrams later in the article. If you don’t want or need these
two features, you can just leave these
pins disconnected.
Construction
Like the earlier Decoders, this is a
small design using surface-mounting
parts, so you’ll need the gear and
expertise to handle that. Many of the
comments from the DCC Decoder also
apply here. For example, you can
increase the value of the 0.68W resistor to reduce the motor current limit,
although you should not decrease it
below 0.68W.
The μDCC Decoder is built on a
double-
sided PCB coded 09111247
that measures 12 × 18mm and is
0.8mm thick. Work through the overlay diagrams, Figs.2 & 3. Start with the
side that has IC2 and BR1. Solder these
first, noting their polarity. Follow with
D1, making sure its cathode stripe is
nearest the pads marked T.
Also on this side is one of the 10μF
capacitors, right next to the bridge rectifier outputs. The two 100kW resistors,
the 100W resistor and the 0.68W resistor are also on this side of the PCB.
Flip the board over and fit REG1 (near
IC1) and Q1 and Q2 (near the edge of
the board).
Solder IC1 in place with its pin 1
marker nearest to REG1. The resistors on this side are the 10kW and 10W
siliconchip.com.au
Programming a DCC Decoder without a DCC Programmer
We’ve presented a thorough series of DCC
system components over recent issues,
including the Base Station hardware, which
has comprehensive DCC programming capabilities. But it occurred to us that many of
our readers will probably have hardware at
their disposal that will allow programming
our Decoders (from this series) without a
dedicated DCC programmer.
Our Decoders are all based on PIC microcontrollers, which are easily programmed
with devices like the various PICkit programmers or even the Snap programmer (which we
now carry in the Silicon Chip Online Shop at
siliconchip.au/Shop/7/7588).
The configuration variables (CVs) that are
involved in Decoder programming are simply
locations in EEPROM and thus they can be
changed with the appropriate PIC programming hardware. So this guide explains how
to program the CVs in our Decoders using a
PIC programmer.
Table 1 shows which CVs correspond to
which EEPROM address on each Decoder.
Below we explain how to modify the EEPROM
values for programming. We’ll assume you’ve
used a programmer like this before, and know
how to make the necessary wiring connections to program a PIC microcontroller. It’s
also assumed that you understand the CVs
that you want to program.
Read-only locations like CV7 and CV8 are
not implemented in EEPROM, so cannot be
modified. Of course, we have provided the
source code for all three projects, so you
can modify the source code and recompile
the project (using MPLAB X IDE) to make
those or any changes you like. The default
values for all the CVs are set near the start
of the dcc.h file.
If you are simply looking to adjust some
of the CVs, we recommend just using the
MPLAB IPE (integrated programming environment) software. Screen 2 shows the IPE
with the PIC16F18126 selected; as you would
need for any of the Decoder projects.
Select the appropriate HEX file by using
the Browse button and then open the
EEPROM view from Window → Target Memory Views → EE Data Memory. From here,
you can edit the EEPROM values directly.
The hexadecimal values in Screen 2 correspond to the original DCC Decoder from
December 2025.
Editing the EE Data Memory window will
not directly change the HEX file, but you can
export the edited file from the File menu as
a new HEX file. The exported HEX file can
be reloaded later using the Browse button
noted above.
When you have made the necessary edits,
hook up your programmer to the Decoder,
press Connect and then press Program
to change the values stored on the chip.
Remember that you should not have anything else connected to the ICSP pins during
programming.
You can also download the contents of the
PIC’s non-volatile memory (including flash
memory, configuration bits and EEPROM)
with the Read button. You can then edit the
EEPROM values and program the new values
back into the chip.
While this is a slightly convoluted
method of CV programming, you can also
use it to save and restore program memory images and CV settings of the decoders
for safekeeping. We had a detailed guide
to CV programming in the Getting Started
with DCC guide in the January 2026 issue
(siliconchip.au/Article/19560).
◀ Screen 2: The MPLAB IPE can be
downloaded as part of the MPLAB
X IDE and provides an interface for
programming PIC microcontrollers (and
other Microchip parts). The EEPROM
entries at the bottom match the DCC
Decoder, with other locations left blank
(0xFF).
parts, so take care not to mix them up.
Don’t forget the other 10μF capacitor.
Clean the board of any excess flux,
inspect the board and allow it to dry.
If necessary, you can program the
chip at this point. Note that you cannot
use a PIC16F18124 or PIC16F18125 for
this project, since the larger flash memory of the PIC16F18126 is needed to
store the audio samples. You shouldn’t
need to program the chip if you have
purchased it from the Silicon Chip
Online Shop.
Also be sure not to connect the piezo
transducer or any other circuitry to
the ICSP pins (except a programmer)
siliconchip.com.au
during programming, since this will
interfere with the programming process. The remaining steps for testing
and wiring the μDCC Decoder to a
locomotive are much the same as the
DCC Decoder.
Operation
The μDCC Decoder operates in
much the same fashion as the DCC
Decoder from December; the implemented CVs all work the same. We’ve
given the μDCC Decoder a model
ID (CV7) of 0x5E (94 in decimal) to
differentiate it from the other two
Decoders.
Australia's electronics magazine
The other main differences (compared to the DCC Decoder) are that it
lacks CV47, CV51 and CV52. CV47 is
for voltage compensation, which the
μDCC Decoder can’t do. CV51 and
CV52 are not needed, since the corresponding function outputs have been
deleted.
The EEPROM Mapping panel in the
December issue has more information
about the CVs, see the panel on programming with a PIC programmer.
The audio output is equivalent to
the green wire function output (F1)
in other decoders. There are no effects
that can be applied, but it’s possible to
May 2026 87
Figs.2 & 3: the external connections
to the μDCC Decoder are via bare
solder pads as shown here. We
have been able to keep the main
DCC connections on the same side
of the PCB, with the audio output
using some of the ICSP pads on the
reverse.
Parts List – microDCC (μDCC) Decoder
1 double-sided 12 × 18mm PCB coded 09111247, 0.8mm thick
1 PIC16F18126-I/SL 8-bit microcontroller programmed with 0911124G.HEX
(bell sound) or 0911124W.HEX (whistle sound), SOIC-14 (IC1)
1 DRV8231DDAR motor driver IC, SOIC-8 (IC2)
1 MCP1703A-3302 3.3V LDO linear regulator, SOT-23 (REG1)
2 2N7002 N-channel Mosfets, SOT-23 (Q1, Q2)
1 MBS4 or CD-MMBL110S 1A SMD bridge rectifier (BR1)
1 1N5819WS 40V 1A schottky diode, SOD-323 (D1)
1 2cm length of 20mm diameter heatshrink tubing (to insulate Decoder)
2 10μF 25V X5R SMD M2012/0805 size MLCC capacitors
1 Same Sky CPT-9019A-SMT-TR piezo transducer (optional)
various lengths of wire as needed
Resistors (all SMD ±1%, M2012/0805 size, ⅛W unless noted)
2 100kW
3 10kW
1 100W
2 10W
1 0.68W ¼W
reduce the volume by adding a resistor
in series with the transducer.
The default setting maps the audio
to the F1 function output, so you can
use the F1 control on the Base Station to test the sound. The mapping
is due to the value of 4 appearing in
CV35. You can use other function outputs to control the audio by ORing
88
Silicon Chip
CV33-CV37 with a value of 4. For
example, to use F2 to control it, program CV36 with the value 4.
CV48 is not mapped into EEPROM,
so it can’t be read back. It will respond
to writes in all programming modes,
but we expect it will be most useful in operations mode on the main
track. Base Stations will typically send
Australia's electronics magazine
repeated programming packets, so the
μDCC Decoder may deliver multiple
serial bytes in response to this.
Custom sounds
It’s possible to change sounds, but
you will need to recompile the project files to do this. The audio samples
and config are in audio.c and audio.h.
The maximum sample size is around
13kB, which corresponds to around
300ms at 44.1kHz. Be sure to select
compiler optimisation level 2, which
is available even with a free license.
The samples are effectively 8-bit
unsigned values, but they should start
and end with a zero value (by ramping
up from zero and down to zero) so that
the DAC idles at 0V when not playing.
This will prevent power supply noise
from being produced at these times.
There are options to play the audio
either as a one-shot or as a loop. Note
that the one-shot will repeat if the
function stays on.
Use the bell sound as a template
for one-shot sounds and the whistle
as your guide for looping sounds. For
looping, you’ll need to set the AUDIO_
LOOP_START and AUDIO_LOOP_
END points. During playback of a looping sound, the sound will play up to
the loop end point and jump back to
the loop start to maintain a continuous sound.
Our process to generate the samples
is to use Audacity (free software) to
create an 8-bit, 44.1kHz mono WAV
file. We then use the HxD hex editor
program to strip out the 44-byte WAV
header and export the file contents as
a C byte array that can be pasted into
the assignment for the audioData variable in audio.c.
The code can automatically work
out the data size to stop playback
when the end of the data is reached.
The available sample space will be
slightly smaller for looping sounds,
since there is extra code needed to
handle the looping that will use up
some of the flash memory allocation.
Summary
While I had intended this design
to allow me to add DCC to some of
my smaller models, I’m quite proud
of being able to cram some simple
sound effects and other features into
a tiny 8-bit microcontroller. I’ve built
a few of these μDCC Decoders and
now all my N scale models are soundSC
equipped!
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Review by Tim Blythman
BrisbaneSilicon
ELM11 Microcontroller Board
The inexpensive ELM11 development board from BrisbaneSilicon uses the Lua
programming and scripting language and is fairly inexpensive. It’s great to see this
type of thing being designed in Australia, so we were curious to try it out.
T
he folks from BrisbaneSilicon
(https://brisbanesilicon.com.au)
work in FPGA (field programmable
gate array) and embedded systems
engineering. They contacted us to see
if we were interested in trying out their
ELM11 microcontroller board.
ELM stands for Embedded Lua
Machine and, as you might expect, it
can be programmed using the Lua language. BrisbaneSilicon sent us a couple of ELM11 boards to experiment
with; here is what we found.
Lua
Lua is an interpreted scripting language that was originally developed
to streamline data entry at a Brazilian
petrochemical company.
It has developed into a simple yet
powerful language that is used in
many places where a scripting language is needed. That includes games
and embedded (microcontroller) environments.
Scripting languages are generally
easier to use and develop for, especially for particular applications, with
the trade-off being that they are usually slower and more memory intensive than compiled languages like C
or C++.
Lua is the Portuguese word for
moon; one of Lua’s predecessors was
named SOL, or sun. Lua’s interpreter
is written in the C programming language, so is easy to port to platforms
that have a C compiler. It is also
designed to easily interface with C
code, so it can be used to add scripting to projects written in C. You can
read more at https://lua.org/about.html
We’ve written a separate panel about
the Lua language for those who want
to know more. The ELM11 presents a
REPL interface, where REPL stands for
The ELM11 is a compact and tidy development board that provides an
embedded interpreter for the Lua programming language. There isn’t much on
the underside of the board apart from pin markings. All the components are on
the top of the board, including two tactile pushbuttons and numerous LEDs. The
ELM11 includes a Gowin GW1NR FPGA and a separate microcontroller that
provides a virtual USB-serial port and can also reprogram the FPGA chip.
90
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Australia's electronics magazine
read, evaluate, print and loop. You can
also write and then run complete programs for more complex tasks.
In this regard, it is similar to devices
like the PicoMite running MMBasic.
MicroPython is similar; it can run on
many microcontroller boards, including the Raspberry Pi Pico. All these
devices and languages allow you to
enter simple commands or write and
run complex programs.
The ELM11
The ELM11 measures 60 × 26mm
and has two rows of 18 pins on a 0.1inch (2.54mm) pitch with 0.9 inches
(22.86mm) between the rows. This is
a fairly standard layout for modern
development boards, allowing them
to be easily used with breadboards or
prototyping PCBs. The pin headers are
provided loose and need to be soldered
to the module.
The ELM11 is shown in the photos.
It has a USB-C socket, which is good,
since they are much more robust than
the micro-B USB sockets that are sometimes seen on boards like this.
Interestingly, the large chip that
you might expect to be the microcontroller is in fact a Gowin Semiconductor GW1NR FPGA. An FPGA
is made of many logic elements that
can have the connections between
them rerouted after production. It can
be compared to how you might program a microcontroller to customise
its operation.
Microcontrollers are also made of
logic elements, so an FPGA can be
programmed to behave as a microcontroller, among many other things.
The GW1NR comes in a QFN-88
siliconchip.com.au
package (quad-flat no-leads with 88
pins) and incorporates 8640 LUTs
(lookup tables) with 8MiB (64Mib)
of RAM. It also has a smaller amount
of BRAM (block RAM) and includes
flash memory to store the configuration bit stream.
There is a separate Puya P25Q32SH
4MiB (32Mib) flash memory chip in a
SOIC-8 package, which is available as
non-volatile storage for the Lua interpreter. The smallest QFN chip is a
TMI7003 three-channel power management IC that incorporates a buck
regulator controller. It provides the
multiple supply rails needed by the
FPGA chip.
The remaining QFN chip is a BL702
RISC-V microcontroller that is used
to provide a USB interface to implement a virtual serial port interface for
communicating with the Lua interpreter. It also provides a JTAG programmer that can be used to reprogram the FPGA.
There are 36 pins available on
the two headers, four of which are
for power: 3.3V, 5V and two ground
pins. The remaining pins are numbered from one to 32. Sixteen (1-16)
of these pins are for general purpose
I/O, while the remainder are labelled
as an I/O bus. The I/O pins operate
at 3.3V levels.
Fig.1 shows the pin mapping of
the ELM11, including the peripherals that can be mapped to each pin.
The mapping is set by the FPGA configuration, and it appears that different ‘hardware overlays’ are possible.
This can change which peripherals
are available on which pins, amongst
other features.
There are also several LEDs on the
board with different functions. Three
are configured to reflect the status of
I/O pins 1, 2 and 3, making it straightforward to start blinking the LEDs with
Lua, without connecting any external
hardware. There are two small tactile
switches. One can be used to reset
the ELM11, while the other can be
detected on I/O pin 1.
This combination of a GW1NR
FPGA and a BL702 microcontroller
can also be found on the Tang Nano
9K development board. More information on the Nano 9K can be found
at siliconchip.au/link/ac9z
Using the ELM11
The ELM11 presents a virtual
serial port to communicate
with the Lua REPL
interface. It operates at 115,200 baud, 8
bits, no parity and one stop bit. Screen
1 shows the prompt after booting, plus
a few commands and their responses.
We used the Tera Term terminal program under Windows.
We found it easy to enter Lua statements at the terminal prompt; the
results are printed back to the terminal. The import statement is needed
to load the functions used to access
features like the GPIO pins. A simple
import(“all”) can be used to quickly
load all extra functions, although you
can also import individual functions
to reduce memory usage.
BrisbaneSilicon has provided some
simple code examples that can be
used in the REPL. They are set up to
be copied and pasted directly into a
terminal program and can be found at
https://brisbanesilicon.scrollhelp.site/
emblua/example-usage
We found that we had to set a 100ms
per line delay in TeraTerm to allow
the processor to complete the import
command for multi-line examples;
this appeared to be more than sufficient for other commands. This setting
can be found in TeraTerm’s menu
under Setup → Serial
port… → Transmit
SPI
UART
PWM
Function
Pin
Pin
Function
TX
TX
PWM
GPIO
1
19
I/O BUS
CS, CLK, TX
RX
PWM
GPIO
2
20
I/O BUS
CS, CLK, TX
TX
PWM
GPIO
3
21
I/O BUS
CS, CLK, TX
RX
PWM
GPIO
4
22
I/O BUS
CS, CLK
TX
PWM
GPIO
5
23
I/O BUS
CS, CLK
RX
PWM
GPIO
6
24
I/O BUS
CS, CLK, RX
TX
PWM
GPIO
7
25
I/O BUS
CS, CLK, RX
RX
PWM
GPIO
8
26
I/O BUS
CS, CLK, RX
TX
PWM
GPIO
9
27
I/O BUS
CS, CLK, RX
RX
PWM
GPIO
10
28
I/O BUS
CS, CLK
TX
PWM
GPIO
11
29
I/O BUS
CS, CLK
RX
PWM
GPIO
12
30
I/O BUS
TX
PWM
GPIO
13
31
I/O BUS
RX
PWM
GPIO
14
32
I/O BUS
TX
PWM
GPIO
15
33
I/O BUS
RX
PWM
GPIO
16
34
I/O BUS
GND
17
Fig.1: The data sheet includes this I/O pin
5V
18
map that also shows the layout of the main
features of the board. The button at upper left is RST and the other
one to its right is BTN1. Note that the pin numbering shown here is
different to that printed on the PCB silkscreen.
35
GND
36
3.3V
siliconchip.com.au
May 2026 91
Australia's electronics magazine
delay. The GPIO and PWM examples
are designed to use the onboard LEDs.
Even without having much knowledge of the Lua language, it was simple
to copy and paste example code from
the BrisbaneSilicon website and see
the results on the LEDs and console
immediately. The library functions
are detailed at https://brisbanesilicon.
scrollhelp.site/emblua/api
There is also a so-called Command
Mode, which is used to access system
and configuration settings. You can
also use it to do things like upload
programs.
A Python program is required on the
host computer to upload the program
over the serial port. Programs can also
be run from Command Mode.
We tested the program upload utility and found it worked well enough,
although it is necessary to disconnect
the terminal program to allow it to
access the serial port.
Complete programs can be found at:
https://brisbanesilicon.scrollhelp.site/
emblua/example-programs
The reset button can be easily used
to reset the processor to get back to a
known state. A running command or
program can be interrupted by pressing the ‘q’ key.
The ELM11 data sheet has more
detail on the interface; see https://
brisbanesilicon.com.au/docs/ELM11_
Datasheet.pdf
ESR Test Tweezers
Complete Kit
SC6952: $50
June 2024
siliconchip.au/Article/16289
This kit includes everything needed to build the ESR Test Tweezers. The three resistors and single
capacitor needed for calibration are also included. But this kit does not include the CR2032 (or
CR2025) coin cell or optional 5-pin header CON1.
The board we received is a beta
(pre-production) release of the ELM11,
and the data sheet notes that some
of the SPI and I2C functions are not
implemented yet. We were able to
bit-bang I2C data using GPIO pins to
(slowly) drive a small OLED module.
Other I/O features such as PWM
(pulse-width modulation) and UART
(asynchronous serial) worked as
expected. There is also a help statement that prints out a user guide on
the serial terminal.
The ELM11 platform
The ELM11’s architecture has been
optimised for working with Lua. BrisbaneSilicon refers to this as ‘hardware
acceleration’. The advantage of using
an FPGA is that the processor core can
be tweaked to improve performance
for the intended use; in this case, as a
Lua interpreter.
The ELM11 data sheet notes that
different so-called hardware overlays are available. These appear to
include options like different I/O features and processor characteristics.
It also appears that it may be possible to configure it with a multi-core
processor.
Using an FPGA also enables the
ability to add other so-called IP
cores. These are modular features
that can be added to the FPGA fabric and could include things like display and communication drivers or
other processors. Some examples are
listed at https://brisbanesilicon.com.
au/ipcores
With its similarity to the Tang Nano
9K, it may also be possible to use the
ELM11 as a general-purpose FPGA
development board, although we have
not investigated this in detail.
Conclusion
Screen 1: the interactive Lua prompt can be used to enter commands and see
responses. The last three commands are all that are needed to light one of the
LEDs on the board.
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Australia's electronics magazine
The ELM11 combines several interesting features. Lua is simple yet
powerful, making the Embedded Lua
Machine easy to use and versatile. The
FPGA platform offers a lot of flexibility in that it can be configured with
different capabilities using hardware
overlays.
Even though we rarely use the Lua
language, we found the ELM11 easy
to use, with many examples that can
be run on just the bare board or with
some components on a breadboard.
It’s an inexpensive way to learn Lua
in general and to provide an embedded environment.
The ELM11 is available online from
BrisbaneSilicon for US$14.95 (about
AU$21) before shipping – see https://
SC
brisbanesilicon.com.au/elm11
siliconchip.com.au
The Lua Language
This is not the first time we have
encountered Lua; the Mini Wireless Webserver (using the OpenWRT firmware) in the November &
December 2012 issues (siliconchip.
au/Series/20) was configured and
programmed using Lua.
Its utility as a scripting language is well-established, and the
open-source OpenWRT router firmware uses Lua extensively. OpenWRT’s web configuration interface is called LuCI (Lua Control
Interface) and, as we saw from the
Mini Wireless Webserver, Lua can
even be used to generate custom
web pages.
Lua has been used for scripting and automation in computer
games since at least 1997, when
it was used by LucasArts in the
framework of their Grim Fandango
adventure game. It is estimated
that about half of all Lua users are
involved with game development.
The NodeMCU project for Espressif microcontrollers (such as the
ESP8266 and ESP32) allows boards
based on these chips to be programmed using the Lua language.
See https://github.com/nodemcu/
nodemcu-firmware
In these applications, Lua is used
similarly to the likes of Micromite
BASIC, PicoMite MMBasic or even
MicroPython. If you have seen
some Lua code, you might think
it doesn’t look very different from
these languages. It does have subtle differences, but it is fairly forgiving and easy to learn. Some background is provided at www.lua.org/
history.html
The designers have aimed for
simplicity of the language, so it
is not surprising that it looks like
other languages. The webpage
above indicates that the optional
use of semicolons (as statement
separators) in Lua came about to
appease users of both C and FORTRAN! A minimal Hello world program looks like this:
print(“Hello World”)
Lua implements well-understood
control structures like if/then/else/
end and while and for loops. The for
loop uses the keywords for, do and
end; each control structure has a
siliconchip.com.au
corresponding end statement, so the
scope is clear.
Interestingly, variables do not
have a type, but values do. The types
include number, string, function and
table. There is also a nil type, which is
understood to be the default value of
an uninitialised variable. Functions
can be defined and can return one or
more values; a function can even be
assigned to a variable. Lua supports
multiple variable assignments in the
same statement.
Tables are associative arrays; this
means that the index does not have
to be a number. Tables can be used
to implement ordinary arrays, sets,
lists, dictionaries, trees and queues.
There is a variant of the for loop that
can be used to iterate over the items
in a table. One thing to watch is that
numeric array indexes are 1-based,
unlike many other languages (eg C/
C++ are 0-based).
So-called meta-tables can be
used to override the behaviour of
mathematical operators when non-
numeric arguments are provided.
Thus, they can be used to emulate
object-oriented methods. The developers of Lua call these features meta-
mechanisms. The intent is to keep the
underlying language quite simple, but
provide a means for a programmer
to create complex behaviours when
required.
These advanced language features
might sound intimidating, but if you
are looking to use Lua for straightforward scripting, you don’t need
to use them. If you are comfortable
with the likes of MMBasic, you’ll
probably need to do little more than
learn a few different keywords and
some minor syntax differences.
If you have worked with BASIC,
C or Python, aspects of Lua like
expressions and mathematical
operators will appear familiar.
Numerical values are typically
stored as floating point, but some
implementations (including the
ELM11) use 32-bit signed integers.
It’s worth remembering that Lua
code is case-sensitive.
Like Python, the language can
be extended with the import keyword. For example, the interface
for the I/O features of the ELM11 is
simply a set of functions that can
be imported to make them available
to the interpreter. Lua’s simplicity
also means that is also renowned
amongst interpreted languages for
its speed.
Summary
Lua is an interesting language,
and we found it easy to learn
the basics. Despite this, it can be
extended in multiple ways to provide advanced programming features. Here is a relatively simple
sample program:
#!/usr/bin/lua
print(“Content-type: text/html\n”)
print(“<HTML><HEAD><TITLE>Relay control</TITLE>“)
print(“</HEAD><BODY>“)
local f = io.open(“/dev/ttyACM0”, “r+”)
f:write(“quiet\n”)
if os.getenv(“QUERY_STRING”):upper() == “ON” then
f:write(“D0=1\n”)
print(“Relay is now on.”)
elseif os.getenv(“QUERY_STRING”):upper() == “OFF” then
f:write(“D0=0\n”)
print(“Relay is now off.”)
else
print(“Error.”)
end
f:close()
print(“</BODY></HTML>\n”)
This snippet of Lua code was presented in the series on a Mini Wireless
Webserver to generate a web page and send data over a serial port to
control a relay. Even if you haven’t used Lua before, it’s fairly clear how
the program works.
Australia's electronics magazine
May 2026 93
CIRCUIT NOTEBOOK
Interesting circuit ideas which we have checked but not built and tested. Contributions will be paid for at
standard rates. All submissions should include full name, address & phone number.
SOT-223 adaptor for amplifier VAS transistors
As explained in the Calliope amplifier article (April 2026; siliconchip.au/
Article/20084), it is becoming increasingly difficult to find suitable throughhole transistors for an amplifier’s voltage amplification stage (VAS).
That’s because these transistors
need a combination of characteristics
(moderate current and power handling, wide bandwidth, low capacitance etc) that used to overlap with
CRT horizontal output stages. With
CRTs no longer being manufactured in
any real quantity, such transistors have
also met the fate of the dodo.
There are still some decent VAS
transistors available as SMDs, mostly
in the medium-power SOT-223 package. But those won’t easily fit onto
existing amplifier PCBs designed for
TO-126 or TO-220 through-hole transistors.
You can buy SMD-to-through-hole
adaptor boards, but they usually aren’t
designed to handle devices with any
significant dissipation, leading to overheating.
This adaptor board design is shown
here at 400% scale. It connects the
three main pins of the SOT-223 device
to three pads that accept a standard 2.54mm/0.1-inch pitch header
(straight or right-angled). It also connects the tab of the device to a fairly
substantial area of copper, with vias
through to the other side of the PCB,
where there’s an even larger copper
area.
This means the transistor can safely
dissipate at least 1W, perhaps a little more, which is typical of what’s
expected for a VAS transistor. That
brings it roughly on par with its
TO-126 equivalents, which can handle
up to about a watt before they need a
small heatsink.
The pinout of SOT-223 NPN transistors is almost universally B-C-E.
Through-hole transistors are not standardised and can vary, but luckily,
most common VAS transistors (including the BF469 and KSC3503 that we’ve
used previously) have the E-C-B pinout, which is a mirrored version of
this adaptor.
To ensure it’s the right way around,
mount the adaptor PCB vertically
using a right-angle pin header with
the SOT-223 device on the side of the
adaptor PCB that is where the TO-126
device tab would have previously
gone. That should ensure the base,
collector and emitter are all connected
as expected.
You can
purchase this
PCB from
siliconchip.
com.au/
Shop/8/7570
You could also use this board
for your own devices, as a general-
purpose SOT-223 adaptor, provided
you have the space. That will give you
more thermal headroom when working with such devices than standard
adaptors.
Phil Prosser,
Prospect, SA. ($60)
Automatic Level Crossing Controller for model railway
This controller uses an Arduino
Nano module and passive reflective
infrared (IR) sensor modules placed an
appropriate distance on each side of
the crossing to monitor for approaching trains and automatically activate
the crossing booms, lights and bells. It
operates for trains travelling in either
direction.
The sensor modules are types
commonly available via eBay or Ali
Express, consisting of an IR LED, an
IR phototransistor and an LM339 comparator, with a threshold (sensitivity)
that is set via a trimpot.
The Arduino “VarSpeedServo”
library is used to slow the movement
94
Silicon Chip
of the boom servos for a more realistic
effect. A separate flasher module using
a 4093 quad schmitt-trigger NAND IC
was used to simplify Arduino programming, avoiding the use of interrupts
or timing loops in the sketch. It alternately drives the common-anode LED
crossing lights at approximately 1Hz.
The use of opto-isolators at the sensor input pins of the Arduino is a convenient way to overcome any false
triggering due to noise pickup in the
sensor connecting wiring. At startup,
both sensors are checked. They must
remain continuously inactive for a
period to make sure the crossing is
clear before continuing.
Australia's electronics magazine
When a train is detected by either
of the sensors, the crossing is closed.
Bell sounds and flashing lights are activated, and there’s a short pause before
the crossing booms are lowered. To
allow for trains of different lengths,
the passage of the train through the
crossing section is fully monitored.
A timeout with reset will occur if the
train, having triggered the ‘approach’
sensor, does not activate the ‘depart’
sensor within a set time. The timeout
is adjustable via a trimpot, which is
read via an analog port, digitised and
remapped to within a range set by maximum and minimum limits defined
within the sketch.
siliconchip.com.au
Once the train has reached and activated the ‘depart’ sensor, that sensor
must then remain continuously inactive for a minimum time before the
train is considered to have departed
and the crossing is then clear. This
minimum inactive time requirement
allows for breaks in sensor triggering
due to the gaps between items of rolling stock and to make sure the train
has fully cleared the crossing.
The crossing is only then re-opened
– the crossing booms are slowly
raised, there’s a short pause, then the
bell sounds and flashing lights are
switched off.
There is monitoring for any further, close-following train during the
crossing opening sequence, in which
case the crossing returns to the closed
condition.
Crossing bell sounds are achieved
using a DFRobot DFPlayer Mini audio
module to play a crossing bells audio
file from a microSD card. The bell
audio file is played using the player’s
loop mode, so it repeats continuously
until the Player is commanded to stop.
In this playback mode, the audio file
must be the first file loaded from the
microSD card.
siliconchip.com.au
There are numerous crossing
bell-ringing audio files free to download from the Internet. The DFPlayer
module’s volume is also adjustable
via a trimpot, which is read via an
analog port, digitised and remapped
to within a range set by maximum
and minimum limits defined within
the sketch. For more information on
the DFPlayer Mini, see the December
2018 issue, pp74-77 (siliconchip.au/
Article/11341).
The trimpot adjustments for both
timeout and DFPlayer volume control
are not dynamic. They are read only
once at startup to set their respective
parameters. Changing a trimpot setting while the controller is running
will have no effect until the power
is cycled or microcontroller is reset.
However, an extra routine to dynamically set the DFPlayer volume is
Australia's electronics magazine
included in the sketch startup process. It is invoked if pin D7 is found
to be pulled low (switch S1 closed)
at startup.
This extra routine commands the
DFPlayer to play the bell audio file in
a loop while continuously reading the
volume trimpot setting and using that
to adjust the volume.
This continues until pin D7 goes
high by opening the switch for the
resumption of normal operation. If
pin D7 is found to be high at startup
(switch open), the volume setting routine is skipped. If this feature is not
required, pin D7 may simply be left
with no connection.
You can download the Arduino
sketch for this circuit from siliconchip.
au/Shop/6/3333
Bob Martindale,
Mill Park, Vic. ($120)
May 2026 95
Simple battery charging using relay & lamp
I built several batteries from rescued
good cells from discarded lithium-ion
tool batteries and developed this simple charger for them.
All relay coils have a voltage potential where the magnetic attraction will
no longer hold the contacts closed.
This is the dropout (or release) voltage and is fairly constant for a particular relay.
A typical Li-ion cell is fully charged
when it reaches 4.2V per cell. A 5V
relay could drop out at, say, 2.8V
(determined by experimentation). A
Li-ion battery full-charge voltage is
4.2V multiplied by the number of cells,
eg, 25.2V (6 × 4.2V). Add the 2.8V
relay drop-out voltage to get 28V; this
is the value to adjust the boost module output to.
When the battery voltage reaches
25.2V, there is no longer enough voltage to hold the relay in, so it drops out
and charging stops. The photos below
show a unit I made on a piece of protoboard, with pins that clamp to the
boost module output terminals.
The adjustable boost module I used
was Jaycar Cat XC4609. It is available
at a lower price from online suppliers,
but once you consider the postage cost,
that saves little. Since the module can
only provide an output voltage that’s
higher than the input, or a little lower,
use a phone charger or 5V USB as the
power source to enable low enough
output voltage settings to charge 1-3
cell Li-ion batteries.
To set it up, measure the current
battery voltage and adjust the boost
module output to 5V higher. Connect
the battery, press the start switch and
the relay should pull in. The current
through the battery is the relay current plus the globe current. Slowly
decrease the boost module’s output
voltage, and when the relay drops out,
note the voltage.
The relay drop-out voltage is this
voltage minus the battery voltage.
For example, if the relay drops out
when you reduce the boost module
output to 18.8V, and the battery measures 16V, the relay drop-out is 2.8V
(18.8V – 16V).
Increase the module’s output voltage
to 1-2V higher and repeat the process a
few times to establish an average dropout voltage for your relay. Now you
can set the module voltage to the fully
charged battery voltage plus the relay
drop-out voltage and start charging.
Various globes in parallel with the
relay coil can be used to set the charge
current. I found that a Dolphin torch
globe (not the LED type) gave 0.3A, a
12V 5W car wedge lamp gave about
0.5A and an old radio panel globe gave
about 0.1A. Select a globe to suit by
experimenting.
The resistance temperature coefficient of your globe will give a charge
current that only varies a small amount
and will have just a small effect on
your relay drop-out voltage.
Don’t forget to record your relay
dropout voltage for future use.
Victor Duffey,
Rosanna, Vic. ($75)
I built my prototype on a small piece
of protoboard, with some pins that
attach it to the boost module.
96
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
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PRE-PROGRAMMED MICROS
For a complete list, go to siliconchip.com.au/Shop/9
$10 MICROS
$15 MICROS
ATmega328P
ATtiny45-20PU
ATtiny85-20PU
PIC12F617-I/P
110dB RF Attenuator (Jul22), Basic RF Signal Generator (Jun23)
2m VHF CW/FM Test Generator (Oct23)
Graphing Thermometer (Mar26), Simple LC Meter (May26)
Active Mains Soft Starter (Feb23), Model Railway Uncoupler (Jul23)
Battery-Powered Model Railway Transmitter (Jan25)
PIC16F1455-I/P
Battery-Powered Model Railway TH Receiver (Jan25)
Dual Train Controller (Transmitter / TH Receiver, Oct25)
PIC16F1455-I/SL Battery Multi Logger (Feb21), USB-C Serial Adaptor (Jun24)
Battery-Powered Model Railway SMD Receiver (Jan25)
USB Programmable Frequency Divider (Feb25)
Dual Train Controller (SMD Receiver, Oct25)
PIC16LF1455-I/P New GPS-Synchronised Analog Clock (Sep22)
PIC16F1459-I/P
K-Type Thermostat (Nov23), Secure Remote Switch (RX, Dec23)
Mains Power-Up Sequencer (Feb24 | repurposed firmware Jul24)
8CH Learning IR Remote (Oct24), Heat Transfer Controller (Aug25)
Vacuum Controller (Oct25)
PIC16F15214-I/SN Silicon Chirp Cricket (Apr23), Mic The Mouse (Aug25)
PIC16F15214-I/P Filament Dryer (Oct24), Tool Safety Timer (May25)
PIC16F15224-I/SL Multi-Channel Volume Control (OLED Module; Dec23)
NFC IR Keyfob Transmitter (Feb25), Rotating Light (Apr25)
PIC16F18126-I/SL RGB LED Star (Dec25), DCC/DC Stepper Motor Driver (Apr26)
μDCC Decoder (May26; bell [G] or whistle [W])
PIC16F18146-I/SO Versatile Battery Checker (May25), RGB LED ‘Analog’ Clock (May25)
USB-C Power Monitor (Aug25), DCC Remote Controller (Feb26)
DCC Booster & Reverse Loop Controller (Mar26)
PIC16LF15323-I/SL Remote Mains Switch (TX, Jul22), Secure Remote Switch (TX, Dec23)
STM32G030K6T6 Variable Speed Drive Mk2 (Nov24)
PIC16F1847-I/P
PIC16F18877-I/PT
Digital Capacitance Meter (Jan25)
Dual-Channel Breadboard PSU Display Adaptor (Dec22)
Wideband Fuel Mixture Display (WFMD; Apr23)
PIC16F88-I/P
Battery Charge Controller (Jun22), Railway Semaphore (Apr22)
PIC24FJ256GA702-I/SS
Ohmmeter (Aug22), Advanced SMD Test Tweezers (Feb23)
ESR Test Tweezers (Jun24)
PIC32MX170F256D-501P/T 44-pin Micromite Mk2 (Aug14), 4DoF Simulation Seat (Sep19)
PIC32MX170F256B-50I/SP Micromite LCD BackPack V1-V3 (Feb16 / May17 / Aug19)
Advanced GPS Computer (Jun21), Touchscreen Digital Preamp (Sep21)
PIC32MX170F256B-I/SO
Battery Multi Logger (Feb21), Battery Manager BackPack (Aug21)
PIC32MX270F256B-50I/SP ASCII Video Terminal (Jul14), USB M&K Adaptor (Feb19)
STM32L031F6P6
SmartProbe (Jul25)
$20 MICROS
ATmega32U4
ATmega644PA-AU
PIC32MK0128MCA048
PIC32MX270F256D-50I/PT
Wii Nunchuk RGB Light Driver (Mar24)
AM-FM DDS Signal Generator (May22)
Power LCR Meter (Mar25)
Digital Preamplifier (Oct25)
$25 MICROS
PIC32MX170F256B-50I/SO + PIC16F1455-I/SL
Micromite Explore-40 (SC5157, Oct24)
PIC32MX470F512H-120/PT Micromite Explore 64 (Aug 16), Micromite Plus (Nov16)
PIC32MX470F512L-120/PT Micromite Explore 100 (Sep16)
$30 MICROS
PIC32MX695F512H-80I/PT Touchscreen Audio Recorder (Jun14)
PIC32MZ2048EFH064-I/PT DSP Crossover/Equaliser (May19), Low-Distortion DDS (Feb20)
DIY Reflow Oven Controller (Apr20), Dual Hybrid Supply (Feb22)
KITS, SPECIALISED COMPONENTS ETC
VARIOUS MODULES & PARTS
- 0.96in 128x64 OLED screen with SSD1306 (PicoSDR, Apr26; SC6176)
- 3.5in LCD module with ILI9488 controller (PicoSDR, Apr26; SC5062)
- 0.91in 128x32 I2C OLED module (Simple LC Meter, May26; SC7484)
μDCC DECODER KIT (SC7617)
$10.00
$10.00
$7.50
(MAY 26)
Includes all the parts and the optional piezo (wire not included). Specify if
you want a bell or whistle sound for the microcontroller (see p88, May26)
SIMPLE LC METER COMPLETE KIT (SC7657)
(MAY 26)
POWER AMPLIFIER CLIPPING INDICATOR (SC7649)
(MAY 26)
Includes all the parts and the 3D-printed enclosure (see p67, May26)
$25.00
$45.00
siliconchip.com.au/Shop/
DCC DECODER KIT (SC7524)
(DEC 25)
EARTH RADIO KIT (SC7582)
(DEC 25)
RP2350B COMPUTER
(NOV 25)
Includes everything in the parts list (see p73, Dec25)
Includes everything to build the radio itself except the case and battery,
plus the plug for the antenna (see p65, Dec25)
$55.00
Assembled Board: a fully-assembled PCB with all non-optional components,
front and rear panels are sold separately below (SC7531; see p28, Nov25)
- front & rear panels (SC7532)
- 8MiB APS6404L-3SQR-SN PSRAM SOIC-8 IC (SC7530)
Short-form kit: includes the PCB and all onboard parts, the case and power supply
are not included (see p35, May26)
$95.00
- pair of red & white PCB-mounting RCA sockets (SC2615)
$4.00
PICKIT BASIC POWER BREAKOUT KIT (SC7512)
(SEP 25)
STEPPER MOTOR DRIVER KIT (SC7601)
(APR 26)
RP2350B DEVELOPMENT BOARD
(AUG 25)
$35.00
CALLIOPE AMPLIFIER PARTS (SC6021)
(APR 26)
Assembled Board: a pre-assembled PCB with all mandatory parts fitted,
optional components are sold separately below (SC7514; see p49, Aug25)
- 40-pin header (two are required, SC3189)
$15.00
MIC THE MOUSE KIT (SC7508)
(AUG 25)
DCC BOOSTER / REVERSE LOOP CONTROLLER KIT (SC7579)
(MAR 26)
USB-C POWER MONITOR KIT (SC7489)
(AUG 25)
433MHz RECEIVER KIT (SC7447)
(JUN 25)
VERSATILE BATTERY CHECKER KIT (SC7465)
(MAY 25)
Includes all required parts for DCC or DC mode (see p55, Apr26)
Includes some of the harder-to-get transistors, resistors and a capacitor
Includes all required parts, except for the Jiffy box, OLED screen (see below),
power supply and front panel (see p58, Mar26)
- 0.91-inch OLED screen (SC7484)
DCC REMOTE CONTROLLER KIT (SC7552)
$45.00
$7.50
(FEB 26)
Includes all required parts, except for the case and wire/cable (see p63, Feb26) $35.00
Includes all parts except the jumper wire and glue (see p39, Sep25)
Includes all parts except a CR2032 cell (see p64, Aug25)
Includes all non-optional parts except the case, cell & glue (see p39, Aug25)
Includes the PCB and all onboard parts (see p66, Jun25)
MAINS HUM NOTCH FILTER (SC7598)
(FEB 26)
DCC BASE STATION KIT (SC7539)
(JAN 26)
RGB LED ‘ANALOG’ CLOCK KIT (SC7416)
(MAY 25)
RGB LED STAR KIT (SC7535)
(DEC 25)
USB POWER ADAPTOR COMPLETE KIT (SC7433)
(MAY 25)
Includes everything except for the case and power supply (see p53, Feb26)
$50.00
Includes everything but the plastic case, power supply and some optional parts.
The Pico 2 is supplied but not programmed (see p39, Jan26)
$90.00
Includes the mostly-assembled board and all non-optional components
except the power supply (see p43, Dec25)
$80.00
$25.00
Includes everything in the parts list (including the case), except the optional
components, batteries and glue (see p30, May25)
$90.00
$7.50
$5.00
$20.00
$30.00
$1.00ea
$37.50
$60.00
$20.00
$65.00
Includes all the parts except the power supply. When buying the kit select either a BZ-121
GPS module or Pico W (unprogrammed) for the time source (see p66, May25)
$65.00
Includes everything in the parts list and a choice of one USB socket: USB-C power only;
USB-C power+data; Type-B mini; or Type-B micro (see p80, May25)
$10.00
*Prices valid for month of magazine issue only. All prices in Australian dollars and include GST where applicable. # Overseas? Place an order on our website for a quote.
SERVICEMAN’S LOG
Turning a pile of junk into computers
Bruce Pierson of Dundathu, Queensland,
repairs many laptop/notebook
computers. He often gets them
inexpensively (or even for free) because
they’re broken, then uses parts from
one to fix another. Here are several
stories of computers he’s fixed lately...
I have a few old laptops that I have installed various
versions of Linux on to try out. Among these is a Compaq
CQ60 that was my younger daughter’s first laptop. The last
time I looked at it, it had a stuck key, causing it to beep
continuously while on. Fixing that would require replacing the keyboard.
I got it out recently and looked through my box of keyboards that I had salvaged from old laptops over time. I still
did not have a keyboard that would suit this laptop and
was reluctant to spend $25 to buy a new one for a device
I’m not using.
I then noticed that one corner of the keyboard surround
near the screen was sticking up. I checked under the laptop
and the screw was in place, so something must have broken inside. I removed the screws on the bottom that held
the keyboard surround on and found that the brass nut had
broken out of the post in the corner that was sticking up.
I considered how I could repair this part. I decided to
get out my 40W soldering iron to heat the brass nut and
press it into the now shorter post. That worked, and I put
the screw in to make sure it sat vertically. A bit more heat
allowed me to true it up. Now I would need a longer screw
for this corner.
I looked through my laptop screws but I had nothing longer than the original screw. Then I remembered that several years ago, someone had given me a small
parts cabinet with around 30 small drawers
98
Silicon Chip
in it. I looked through the drawers; most of the parts were
for PCs, but I found some laptop screws. They were mainly
short, but in another drawer, I found one that was exactly
the right length.
I refitted the keyboard surround, but when I went to use
the replacement screw, I discovered that the head was a
larger diameter and it would not fit in the hole. So I put the
screw in my small electric drill and, with the drill running,
I used a file to reduce the diameter of the head, checking it
periodically against the original screw to get the diameter
approximately the same.
With the screw modified, I was able to install it and now
the keyboard surround is fitting correctly. Now I just need
a good keyboard to get it back in working order.
Toshiba C50D-A screen replacement
Recently, a friend asked me if I could have a look at his
Toshiba laptop. It had a round ‘black hole’ in the screen
that was becoming increasingly annoying. The laptop was
fine apart from this. I have seen some weird things with
faulty screens in the past, but this is the first time I’ve seen
one with a black hole.
The cost of a new screen was over $90, so he wondered if
I might have a good screen from an old laptop that would fit
his. As it happened, I had recently disassembled a Toshiba
L650 laptop that no longer worked, and I still had the shell
and screen sitting on a shelf. I did some online research
and found that both laptops use exactly the same screen.
I started by removing the battery, then the RAM and
HDD cover, and I took out the hard drive and RAM. Then
I removed the optical drive plus the 15 screws securing the
back shell, allowing me to remove the back shell.
Australia's electronics magazine
siliconchip.com.au
Items Covered This Month
• A tale of four computers
• Repairing a Hisense 65U8G power board
• A faulty IR sensor in a carport
Dave Thompson runs PC Anytime in Christchurch, NZ.
Website: www.pcanytime.co.nz
Email: dave<at>pcanytime.co.nz
Cartoonist – Louis Decrevel
Website: loueee.com
This laptop is very unusual in that the bottom shell comes
off, leaving the motherboard in the top panel, whereas with
most laptops, the top panel comes off, leaving the motherboard in the bottom shell.
I could see that I would need to remove the motherboard to detach the cable going to the screen. This meant
removing the keyboard. That turned out to be a nightmare
with the way the keyboard is fitted into the top panel, but
I finally got it out and unplugged the cable.
Next, I removed the CPU fan and I was surprised by the
amount of junk that was almost entirely blocking the fins
on the heatsink. It’s a wonder the laptop had not been overheating; it was one of the worst I’ve seen.
I unplugged all the plugs in various locations around
the motherboard, then removed the single screw from the
motherboard and lifted it up to unplug the video cable.
After removing the motherboard, I cleared the rubbish
off the heatsink and cleaned the small amount of dust off
the fan.
After removing the last two screws from each of the
hinges, I had the lid with the screen free. Removing the two
screws in the bottom front corners of the screen allowed
me to prise the inner surround free from the lid.
Then I noticed a problem. On one lower corner of the
lid, the two small brass nuts had come out due to the old
plastic becoming brittle over time and breaking.
There was no easy way to remedy this situation. There
would be no way to secure the hinge on that side to the lid
without coming up with a solution. I did not have a spare
lid for this laptop.
My friend asked me what I could do to get the repair
completed, as this laptop was very useful to him. I said
I could put two screws through the lid from the back to
secure the hinge, but that he would see the screws in the
back of the lid. He said that he wasn’t concerned how the
lid looked from the back.
So I got the screen from the L650, unplugged the cable
from it and removed the hinges. Then I did the same with
the original screen and I fitted the original hinges and original cable to the replacement screen.
With the screen re-fitted to the lid, I lined things up,
drilled the two holes through the lid and then lightly countersunk them on the outside of the lid. I had to find two
small screws and nuts that were long enough to do the job.
This is not easy, as laptop screws do not commonly come
that long. But with some searching through my containers
of laptop screws, I found two suitable ones.
I used the two small brass nuts that had come loose from
the lid to fit the screws in the lid. This ensured that the
hinges were in the correct place. I eventually found two tiny
nuts to finish the repair. I fitted one to the screw through
the hinge, then I replaced the surround and screwed the
last nut onto the screw in the corner of the screen.
The very dirty Toshiba
C50D.
siliconchip.com.au
Australia's electronics magazine
May 2026 99
I could now reassemble the laptop. I fitted the two screws
to each hinge to hold the lid onto the laptop, then I connected the screen cable to the motherboard and sat the
motherboard back in place. I screwed in the single screw
that holds it to the top panel.
I connected the rest of the cables to the motherboard,
then put the CPU fan in place and installed the two screws
that hold it to the motherboard, and plugged in its cable. I
sat the back shell in place so I could turn the laptop over
and connect the keyboard.
I plugged in the keyboard cable, then I had a lot of trouble getting the keyboard back in place. I have never had
this much trouble removing and refitting a keyboard on
any other laptop previously. But I got it correctly fitted
in the end.
I closed the lid, turned the laptop back over and screwed
the back shell on. Then I fitted the hard drive, RAM and
optical drive. I replaced the cover for the hard drive and
RAM, and installed the battery.
I tested the laptop and everything was good with it now.
I gave the keyboard a quick clean. My friend was really
happy to see his laptop nice and clean, no longer with a
hole in the screen.
While it may not have been a cosmetically perfect repair,
at least it saved the laptop from being scrapped.
HP 15 Notebook RAM upgrade
I wanted to try Windows 11 so, using a Windows 10 laptop, I downloaded the Windows 11 25H2 ISO file and used
Rufus to copy it to a 16GB flash drive.
I had an unused HP laptop but it won’t boot from a flash
drive, like many later PCs will, so I had to run the setup
from inside Windows 10. This laptop had no personal
information on it, so I just wiped everything and started
fresh with Windows 11.
The installation went smoothly until I got to connecting
to the internet. I knew that if I connected to the internet,
that I would have to log in with a Microsoft account, which
I did not want to do, as it would be a massive inconvenience to need internet access every time I wanted to log
into Windows.
I got to a command prompt by holding Shift and pressing F10, and I entered the command “oobe\bypassnro”.
This initiated a reboot, and it then showed “I don’t have
internet”, so I could log in with a local account, just like
in Windows 10.
At the Windows 11 desktop, the first thing I noticed
was that the start button was in the middle of the taskbar,
which was impractical. I found the setting and changed it
back to where it should be. Then I found that many of the
usual features were missing from the taskbar.
I did some searching online and I found a way to fix this.
I found Explorer Patcher and tried to download it using
Microsoft Edge, but it would not complete the download,
stopping before it was completed. So I downloaded and
installed Google Chrome and then I was able to download
Explorer Patcher and run it. That fixed the taskbar and I
was then able to put Quick Launch back on it.
This HP laptop only had 4GB of RAM, which is very low
for Windows 11. I wanted to upgrade the RAM to 8GB. This
HP laptop is one of those laptops that must be completely
dismantled to replace the RAM or change the hard drive,
which makes upgrading or changing anything difficult.
With the top panel removed, I had to remove the motherboard to find the RAM. At this point, I was becoming
concerned that the RAM might be soldered to the motherboard and not be upgradeable, as I’ve found this on some
laptops previously. But after removing the motherboard, I
found that there was a single 4GB RAM module in a slot,
so it could be upgraded, unlike the soldered CPU.
Now I needed an 8GB RAM module. I still had several
old, non-working laptops, so I started by checking all the
The HP 15 motherboard; the RAM is next to the CMOS cell.
100
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
HP laptops, but I did not find any 8GB RAM modules. Then
I also checked other brands of non-working laptops and I
removed several hard drives and RAM modules, but I still
had no 8GB RAM module.
Then I found an Asus F553M laptop that was another
one of these laptops that needs to be completely dismantled to access anything. I dismantled it and it had one 8GB
RAM module.
I got my Dell laptop that has Linux on it and I removed
the two 4GB RAM modules and installed the single 8GB
RAM module. Running MemTest86+, it went through the
entire test with no errors, so I knew that I had a good 8GB
RAM module.
I then installed the 8GB RAM module in the HP laptop.
Next, I decided to check the CR2032 cell to see what condition it was in. I first tested it with my multimeter and it
read 2.97V, a sure indication that it had reached the end
of its life. I got out my dedicated cell and battery tester
and checked the cell and it read 1V, 0%, so it needed to
be replaced.
The new cell measured 3.2V and 100%, so I fitted it
to the laptop motherboard. It’s always a good idea to test
replacement cells to make sure they are still good, as some
cells may be getting old and losing their voltage, which
happens over time, even when a cell is not being used.
Some laptops have the CMOS battery (cell) located in a
convenient location under one of the covers, usually the
RAM cover. But a lot of laptops have it in a location that
is not visible, and it’s necessary to dismantle the laptop in
order to replace the cell.
Some laptops even have the cell soldered to the motherboard, but these are mostly rechargeable cells and they
don’t normally need replacing for the life of the laptop.
With the laptop reassembled, I could see that the battery had started charging after sitting on 0% for some time
while I had been using it. Laptop batteries that have been
sitting around for a long time will usually go flat. Often
they will not charge up again, but in some cases they will
come good if left on charge for a long time.
I ran msinfo32, which brought up the specifications for
the laptop. This is a very handy command for finding out
just what’s inside a laptop, as it shows the CPU, hard drive,
RAM and many other details.
Compaq CQ42 CPU upgrade
I was setting up a Compaq CQ42 to run Linux when I
found that the CMOS battery (cell) was flat. It would be a
big job to change the cell, as the laptop would need to be
completely dismantled and the motherboard removed to
access the cell.
Unfortunately, this is another of that frustrating class of
portable computers that has the CMOS cell mounted in an
inaccessible place. So once again, I’d have to totally dismantle it to complete the swap.
Seeing that I would have to go a lot of trouble just to
replace the cell, I thought I would upgrade the CPU while
I had it apart. It had a Celeron T3100 at 1.90GHz; I had
some spare CPUs that I’d salvaged from dead and defective laptops.
I started by searching through the CPUs that had the
same socket (PGA478). I set aside any processor that was
faster than 2GHz – I had four. Next, I checked which CPUs
were compatible with the CQ42 motherboard. I found the
siliconchip.com.au
Australia's electronics magazine
May 2026 101
I figured that while replacing the CR2032 cell in this Compaq CQ42 laptop, I could also replace the CPU,
best option to be a Pentium dual-core P4500 at 2.3GHz, as
it was listed as the most common CPU in the CQ42. I had
a faster 2.4GHz CPU but it was not compatible.
The first step was to remove the battery and the cover
for the hard drive, then the cover for the RAM. Next, I
removed the optical drive. I first opened it with an optical
drive eject tool so that I could pull on the tray and not the
front panel. Then I removed the WiFi card after removing
the mounting screw and unplugging the two wires.
Next, I removed the three screws holding in the hard
drive and unplugged the connector. Most hard drives are
not held in with screws like this one.
Many laptop keyboards are held in with small clips at
the top or bottom of the keyboard, or occasionally screws
at the top of the keyboard that are accessible after removing
a panel. The CQ42 is quite different in that the keyboard
is held in by six screws from the underside.
I removed the six screws and then used the optical drive
eject tool to push up on the keyboard through one of the
screw holes.
This allowed me to lift up the keyboard, disconnect
the cable and lift the keyboard clear. I then removed the
remaining screws on the bottom of the laptop and the one
screw under the keyboard, unplugged the four cables and
prised the top panel off.
Servicing Stories Wanted
Do you have any good servicing stories that you would like
to share in The Serviceman column in SILICON CHIP? If so,
why not send those stories in to us? It doesn’t matter what
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102
Silicon Chip
After removing one screw holding in the CPU cooling fan
and two holding in the motherboard, I unplugged all the
cables and lifted out the motherboard. I could then unscrew
the six screws holding the heatsink and fan to it and remove
the heatsink with the fan still attached to it. Then I cleaned
the old heatsink compound off the CPU heatsink.
I fired up the compressor and blew compressed air
through the fins of the heatsink. Quite a lot of junk
came out, so it was definitely in need of cleaning. I also
cleaned the fan’s fins with a damp, squashed cotton bud
so that the assembly would be ready to refit after changing the CPU.
I changed the CPU, applied new heatsink compound
and reinstalled the heatsink. Then I changed the CMOS
battery (cell), which was the main reason for completely
dismantling the laptop. With that done, it was time to
reassemble it.
I put the motherboard back in the bottom shell and
installed the two screws to hold it in and the one screw
to hold in the CPU cooling fan. Next, I reconnected all
the cables, put the top panel back in place and connected
the four cables that were in the top shell. I installed the
one screw in the top shell and all the screws in the bottom shell.
I then plugged in the keyboard cable, put the keyboard in
place and reinstalled the six screws from the bottom. After
reinstalling the WiFi card and connecting its two wires, I
refitted the optical drive and installed the screw that holds
it in place. Then I plugged in the hard drive connector,
sat the hard drive in place and drove in the three screws.
I put the hard drive cover on, installed one 2GB RAM
module and put the battery back in.
The battery was not charged, so I connected a charger
and pressed the power button. I tapped the Esc key and
then I pressed the F10 key to access the BIOS setup. I set
the time and date, then checked the other settings before
exiting setup and saving the new settings.
Now that I was ready to install the operating system, I
switched it off, inserted the other 2GB RAM module and
Australia's electronics magazine
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put the RAM cover back on. I considered upgrading the
RAM to 8GB, but I decided not to, as Linux is pretty light
on RAM usage and I would only be using it for web surfing and research.
I had already set the laptop to boot from the optical drive
as the first choice, so I booted from the PearOS Monterey
installation DVD. Installing Linux on these old laptops
gives them a new lease on life. It can fit on a 40GB hard
drive, but I usually use 120GB or larger.
Hisense 65U8G power board repair
This LCD TV has a dimmable LED backlight, using more
power than a normal LCD TV with a simple backlight. The
advantage is higher contrast (stronger blacks). An LCD panel
does not fully block the backlight, so the blacks appear dark
grey. By selectively switching off the backlight elements,
the blacks are more black.
In the future, RGB panels, with a matrix of red, blue, and
green LEDs, promise to provide a high-contrast screen better than OLED TVs.
The power board in this TV has a power factor correction (PFC) stage using an IPD2308 IC that makes its current draw more sinusoidal, in phase with the mains voltage waveform.
The normal capacitor input supplies used in LCD TVs
take large spikes of current at the peak of the mains voltage
and are not popular with supply companies.
This PFC circuit is unusual in that it uses two transformers, each driven by a separate input Mosfet, although both
Mosfets are driven by the same IDP2308 chip. I think this
is done because it’s easier to fit two smaller transformers
than one large one. The outputs of the two transformers are
connected so that only one Mosfet half-bridge is required
on the output side.
The power fuse to the board was blown, and both the
input Mosfets were shorted. The input Mosfets share the
same 0.05W current-sensing resistor (3 × 0.15W in parallel). These were blown open. The circuits driving the input
Mosfets were damaged as the Mosfets shorted, and the
IPD2308 was also destroyed.
Each Mosfet had a PNP emitter-follower transistor to
speed up its switch-off. Surprisingly, the PNP transistors
survived, but two resistors in each driving circuit were
open-circuit.
So quite a few components to replace. As the IC and
resistors are surface mount, you need a hot air gun for
the IC and hot tweezers for the resistors. So you have to
decide whether to repair or buy a second-hand board on
eBay or similar.
Roger Sanderson, Sinnamon Park, Qld.
IR motion sensor repair
We have a sensor in our carport looking at the driveway to
detect visitors as they enter the property. This is necessary
as the driveway is not easily seen from inside the house.
The sensor is a simple infrared motion detector (transmitter) with a separate light/beeper box (receiver) to provide
an indication of activity in the driveway.
The units are connected wirelessly and run off batteries that seem to last forever. I bought the unit from Altronics, and it has proved reliable and just the right solution
for the job.
After many years of flawless service, the unit developed
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an intermittent fault. The lights in the receiver would flash
when triggered, but the audible alarm would not sound.
As the beeper unit normally sits on the hall table where it
can’t be readily seen, this was a problem.
I assumed the transmitter unit was working correctly.
I duly inspected the receiver unit, replaced the batteries,
and the beeper came back to life. Good! The unit was put
back into service and continued its duties until the beeper
failed again several months later.
This time, I took the back off the receiver and gave it a
thorough inspection. It was a fairly simple construction, a
main printed circuit board with a small wireless receiver
board soldered to its side. Nothing was obviously amiss.
I touched up a few possibly cold solder joints, but still no
sound.
Checking the loudspeaker, I found it was fine, measuring 95W and producing a healthy click each time the meter
probes were attached. I removed a transistor that seemed
to switch the input to the audio circuits and tested it, but
it was reported as working correctly, so I returned it to
the circuit.
Various other components were checked in-circuit with
nothing obvious showing up. Fortunately, most of the components were marked with their values, and that allowed
easy checking.
As I worked through these components, it came to the
point where a small IC on the board was the only untested
component in the beeper circuit. I could not figure out what
it actually did; it had an obscure part number that failed
to show up in web searches.
At that point, I decided it was time to give up and look
for a replacement driveway detector. After much looking
around at various modern equivalents that had up to 50
tones, pushbuttons galore, connecting to my phone and
everything else I did not want, I found Altronics were still
selling the original unit and duly ordered a new one.
While waiting for the new unit, I could not leave the
thought alone that it was a simple unit, the fault had to be
in the beeper circuitry, and I could not allow myself to be
defeated! So instead of tidying up my bench and sweeping
the faulty unit into the bin, I had another look.
Having eliminated all the likely components around the
beeper circuit, I realised that the beeper had two sound
levels that were controlled by a two-pole, three-position
slide switch located on the other side of the board. The
switch doubled as the on/off switch and was connected to
the beeper circuit by two tracks that meandered across the
board, avoiding other tracks and components.
Testing the switch contacts, I quickly found that
they were either open-circuit or had a high resistance.
I bridged out the switch, and the beeper came to life! I
decided that as we only ever used the unit on low volume, it was easier to leave the switch bridged than find
a replacement. The on/off side of the switch seemed to
be working fine.
With 20/20 hindsight, I realised that in circuits such
as these where there is little loading of parts, and barring
a random component failure, the most likely component
to fail is the one subject to mechanical wear. So I probably should have looked at the switch first. The unit was
returned to service, and I now have a brand new unit sitting on my shelf as a backup!
SC
Nigel Dudley, Ocean Beach, WA.
Australia's electronics magazine
May 2026 103
Vintage Radio
Airzone 6552A Concert Star
from 1947
This Australian post-war
set is based on a design
from 1941. The circuit is a
conventional superhet design;
its appeal lies mainly in the
flamboyant cabinet styling,
reminiscent of a concert hall.
By Assoc. Prof. Graham Parslow
T
he almost-identical Airzone
6651A was first offered for sale in
1941 but the government stopped all
domestic radio production when components were reserved for war manufacture. A contemporary advert read:
Airzone have presented another
star to join their constellation. It is
a new brighter and better star in the
mantel world – the sparkling Concert
Star. Buy the best mantel in Australia
for £17/10/-.
The model 6552A was almost the
same radio when it was released in
1946, although the retail price had
increased to £20/12/6. The styling
was comparable to other late-1930s
Bakelite radios and it used heritage
circuitry.
The speaker in this radio is stamped
September 1947; it is unclear whether
this electromagnet field coil speaker
would have been made in 1947 or
pulled from shelves that had been
storing components during the war.
In 1947, Rola were making excellent
permanent-magnet speakers that were
a better choice unless old stock needed
to be used.
A friend acquired this radio and
passed it onto me for checking and restoration. A quick glance was enough to
104
Silicon Chip
confirm that it was not a quick plugin-and-return task.
It never ceases to amaze what debris
ends up inside old radios. In this case
it was chicken bones!
The dirtier the chassis at the start
of a restoration, the greater the satisfaction with seeing a resplendent end
product. This one was certainly dirty.
My standard procedure is to remove
all the valves first. For very dirty radios
like this one, the next step is a blow-off
with compressed air. Turpentine and
a brush can then remove or loosen a
lot of the surface accumulations. Then
comes a final compressed air blow-off.
The Airzone factory that used
to be on Paramatta road.
Australia's electronics magazine
Extensive light surface rust on this
chassis was covered with chrome
paint. The transformer and valve
shields were repainted. This was
adequate to satisfy me that the result
would be gratefully appreciated when
it was returned.
Ian Batty (another Vintage Radio
author in Silicon Chip) informed me
that perfection is the enemy of the
good. In other words, a lot of time can
be wasted in seeking perfection when
something is adequate.
A bit of Airzone history
At age 30 in 1925, engineer Claude
Plowman established a business fabricating components for crystal sets.
This was two years after the introduction of public radio transmissions. He
had judged the market well and learnt
that delivering quality products was
best done by manufacturing in-house.
Plowman registered the trademark
Airzone in 1926. The coils wound by
Airzone stood out for excellence. There
was continuous growth in the output
from Airzone through the 1930s.
Airzone produced some of the most
collectable Australian radios from the
1930s, due to their beautiful designs
and the quality of their timber and
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Bakelite cabinets. The growth of Airzone was helped by wartime manufacture of instruments for radar testing,
various communications items and
making ASDIC (sonar) echo-location
equipment.
This led to opening a large factory at
Paramatta Road in Sydney in 1944 (see
the drawing opposite). Post-war, Airzone returned to domestic radio production and badge-engineered radios
to be sold as Malvern Star, Mullard
and Peal. Their success led to a company take-over by the large EMAIL
(Electricity Meter & Allied Industries
Ltd) group, although Claude Plowman
remained as manager.
The changes brought about from the
takeover resulted in the termination of
Airzone radio production in 1955. The
Airzone legacy to collectable Australian radios is substantial.
Circuit details
The circuit has been scanned from
page 25 of the Official Australian
Radio Service Manual (OARSM) Volume 5, 1946.
The valve lineup (6A8G, 6U7G,
6B6G, 6F6G and 5Y3) is a classic prewar superheterodyne arrangement,
widely used in Australian mantel
radios of the late 1930s and early
1940s. By the time this set reached
the market post-war, the design was
already conservative but well proven,
offering reliable performance rather
than innovation.
R1 (10kW) is connected in parallel
with the primary antenna coil. Per
Roger Johnson (Electronics Australia,
November 1998, p62), this broadens
the tuning of the antenna circuit by
lowering the secondary Q by damping the primary winding. Without the
detuning lower frequency stations are
emphasised over higher frequency
stations.
After this, the switching between
MW and SW is relatively simple.
The tuning is accomplished by conventional ganged variable capacitors.
There is a switch linked to the band
change mechanism, between two sets
of dial lamps, that could be used to
switch the lamps. However, on this
radio, the four dial lamps remain on
regardless of band selection.
The representation of the 6A8
mixer valve uses an old convention
of drawing crinkled electrodes much
like a resistor. All of the electrodes are
drawn stacked between the cathode
siliconchip.com.au
The top two photos show the rear of the cabinet and the chassis in their
unrestored and very dusty condition. The bottom photo of the chassis is what it
looked like after a good clean.
Australia's electronics magazine
May 2026 105
This is what the underside of the chassis looked like before any work was done.
and anode, rather than set apart as a
pentode and triode.
The 6A8 was released in 1935 and is
relatively common in pre-war radios.
Two separate local oscillator coils pass
a mixing frequency to the 6A8 via
capacitor C2. The result is an intermediate frequency (IF) output at 456kHz.
The 6U7 IF amplifier is a pentode,
although it is drawn as a tetrode. The
omitted electrode is connected internally to the cathode.
AGC is applied to both the 6A8 and
6U7 via 1MW resistor R7, which connects to the detector diodes in the 6B6.
A second IF transformer passes the signal to the detector diodes. Audio from
the diodes passes to the volume control potentiometer, R12; the slider is
connected directly to the top-cap grid
of the 6B6. The negative voltage from
the diodes is prevented from reaching
the 6B6 grid by 10nF capacitor C11.
The 6F6 output pentode is another
venerable valve from 1935. It is drawn
here as if it were only a tetrode. This
valve needs a relatively high grid bias
voltage to minimise distortion. A grid
bias of -13V is specified in the circuit
diagram. The 460W wirewound cathode resistor, R16, delivers that bias
(measured as -10.7V in this radio).
The 6F6 grid is held at Earth potential by resistor R15 (5MW), a resistor
that is more commonly encountered as
500kW. C13, the 10nF audio coupling
capacitor, needs to be leakage-free to
prevent voltage from the 6B6 anode
from driving the 6F6G grid positive.
The use of a 5Y3 full-wave rectifier
is another link to heritage parts. The
5Y3 is the old type 80 valve with four
pins, repackaged into an octal base. It
is an excellent rectifier, but has two
drawbacks.
First, the cathode is directly heated,
so almost immediately from switch-on,
the 5Y3 is generating a
The recabled speaker and restored chassis are
shown here. Note the replaced mains lead.
106
Silicon Chip
higher voltage than the eventual voltage under load when the other valves
have warmed up. This can stress components in the HT line, causing failure.
The other downside is the need for a
separate 5V AC transformer winding,
increasing the cost of the transformer.
At the time, a range of indirectly
heated rectifier valves such as the 6V4
were available.
1947 was close to the end of the
period when octal-base valves were
used in radios, because new miniature
7-pin and 9-pin valves were becoming available. Due to large inventories
and war surplus, octal valves continued to appear in radios well into the
mid-1950s.
Radio service people often had
substantial numbers of spare valves.
Such new-old-stock and salvaged
valves have generated a valve bank
of approximately 70,000 held for the
use of members of the Historical Radio
Society of Australia (see hrsa.org.au).
Electrical restoration
The two-core mains lead was
replaced with a newly-manufactured
cloth-covered three-core cable. That
original old two-core cable was commonly also used for light fittings. The
expense of using specially-made new
cable is readily justified by keeping
the external appearance of the radio
true to period.
More importantly, adding an Earth
wire can both improve performance
and enhance safety. Additionally, the
dial cord was replaced and new dial
lamps installed.
The speaker cable was unserviceable and was rewired with coloured
wire reclaimed from old switch-mode
computer power supplies. The old
computer wire is handy for medium-
current applications and colour tracking separate lines.
Under the chassis
The first power-up was with without
valves and the four globes illuminated
with a stable power draw of 15W. 8W
of this was just the globes. Sometimes
all capacitors remain serviceable, and
I had a good feeling about this radio.
Accordingly, without the mains connected, I connected a bench HT supply ramped it up to 250V DC, allowing
the electrolytics to re-form.
In the end, it only drew 2mA at
250V. This tested all the paper capacitors subjected to high voltage with one
important exception: C13, the audio
coupling capacitor, which I replaced
before a full power-up. With the valves
installed and power applied, only two
strong stations were received very
faintly.
A signal tracer showed good signal
input from multiple stations was delivered to the volume pot. The wiper on
the pot was broken and made no connection. After replacing the pot, the
radio worked properly again, drawing
52W from the mains.
At raised volume, the speaker was
poling and distorting. Luckily, this
was easily fixed by re-gluing the cone
to the rim where it had separated.
Restoring the cabinet
The chief detraction from the cabinet was the soiled grille cloth. The
cloth was folded into the theatre-
curtain pattern that was in vogue in
the late 1940s (recall that this radio is
called the Concert Star).
I took a gamble that worked in this
case. I sprayed automotive degreaser
onto the cloth and brushed it in.
Copious water cleansing followed, to
remove the degreaser, and the result
was an impressively clean grille cloth
unharmed by the harsh treatment.
The case suffered from the kitchen
ceiling disease, which is contracted
when a ceiling is roller-painted without
adequate protection to what is below.
It has a light covering on the face, but a
much heavier spatter was over the top.
The globs of white paint were
removed by careful rubbing with grade
zero steel wool soaked with carnauba
wax (car polish). This had the twin
benefit of cleaning and polishing the
SC
cabinet.
Fig.1: the circuit for the Airzone
6552A radio with the components
labelled for convenience.
siliconchip.com.au
Australia's electronics magazine
May 2026 107
PRINTED CIRCUIT BOARDS & CASE PIECES
PRINTED CIRCUIT BOARD TO SUIT PROJECT
SALAD BOWL SPEAKER CROSSOVER
PIC PROGRAMMING ADAPTOR
2M VHF CW/FM TEST GENERATOR
TQFP-32 PROGRAMMING ADAPTOR
↳ TQFP-44
↳ TQFP-48
↳ TQFP-64
K-TYPE THERMOMETER / THERMOSTAT (SET; RED)
MODEM / ROUTER WATCHDOG (BLUE)
DISCRETE MICROAMP LED FLASHER
MAGNETIC LEVITATION DEMONSTRATION
MULTI-CHANNEL VOLUME CONTROL: VOLUME PCB
↳ CONTROL PCB
↳ OLED PCB
SECURE REMOTE SWITCH RECEIVER
↳ TRANSMITTER (MODULE VERSION)
↳ TRANSMITTER (DISCRETE VERSION
COIN CELL EMULATOR (BLACK)
IDEAL BRIDGE RECTIFIER, 28mm SQUARE SPADE
↳ 21mm SQUARE PIN
↳ 5mm PITCH SIL
↳ MINI SOT-23
↳ STANDALONE D2PAK SMD
↳ STANDALONE TO-220 (70μm COPPER)
RASPBERRY PI CLOCK RADIO MAIN PCB
↳ DISPLAY PCB
KEYBOARD ADAPTOR (VGA PICOMITE)
↳ PS2X2PICO VERSION
MICROPHONE PREAMPLIFIER
↳ EMBEDDED VERSION
RAILWAY POINTS CONTROLLER TRANSMITTER
↳ RECEIVER
LASER COMMUNICATOR TRANSMITTER
↳ RECEIVER
PICO DIGITAL VIDEO TERMINAL
↳ FRONT PANEL FOR ALTRONICS H0190 (BLACK)
↳ FRONT PANEL FOR ALTRONICS H0191 (BLACK)
ARDUINO FOR ARDUINIANS (PACK OF SIX PCBS)
↳ PROJECT 27 PCB
WII NUNCHUK RGB LIGHT DRIVER (BLACK)
SKILL TESTER 9000
PICO GAMER
ESP32-CAM BACKPACK
WIFI DDS FUNCTION GENERATOR
10MHz to 1MHz / 1Hz FREQUENCY DIVIDER (BLUE)
FAN SPEED CONTROLLER MK2
ESR TEST TWEEZERS (SET OF FOUR, WHITE)
DC SUPPLY PROTECTOR (ADJUSTABLE SMD)
↳ ADJUSTABLE THROUGH-HOLE
↳ FIXED THROUGH-HOLE
USB-C SERIAL ADAPTOR (BLACK)
AUTOMATIC LQ METER MAIN
AUTOMATIC LQ METER FRONT PANEL (BLACK)
180-230V DC MOTOR SPEED CONTROLLER
STYLOCLONE (CASE VERSION)
↳ STANDALONE VERSION
DUAL MINI LED DICE (THROUGH-HOLE LEDs)
↳ SMD LEDs
GUITAR PICKGUARD (FENDER JAZZ BASS)
↳ J&D T-STYLE BASS
↳ MUSIC MAN STINGRAY BASS
↳ FENDER TELECASTER
COMPACT OLED CLOCK & TIMER
USB MIXED-SIGNAL LOGIC ANALYSER (PicoMSA)
DISCRETE IDEAL BRIDGE RECTIFIER (TH)
↳ SMD VERSION
MICROMITE EXPLORE-40 (BLUE)
PICO BACKPACK AUDIO BREAKOUT (with conns.)
8-CHANNEL LEARNING IR REMOTE (BLUE)
3D PRINTER FILAMENT DRYER
DUAL-RAIL LOAD PROTECTOR
VARIABLE SPEED DRIVE Mk2 (BLACK)
FLEXIDICE (RED, PAIR OF PCBs)
DATE
SEP23
SEP23
OCT23
OCT23
OCT23
OCT23
OCT23
NOV23
NOV23
NOV23
NOV23
DEC23
DEC23
DEC23
DEC23
DEC23
DEC23
DEC23
DEC23
DEC23
DEC23
DEC23
DEC23
DEC23
JAN24
JAN24
JAN24
JAN24
FEB24
FEB24
FEB24
FEB24
MAR24
MAR24
MAR24
MAR24
MAR24
MAR24
MAR24
MAR24
APR24
APR24
APR24
MAY24
MAY24
MAY24
JUN24
JUN24
JUN24
JUN24
JUN24
JUL24
JUL24
JUL24
AUG24
AUG24
AUG24
AUG24
SEP24
SEP24
SEP24
SEP24
SEP24
SEP24
SEP24
SEP24
OCT24
OCT24
OCT24
OCT24
OCT24
NOV24
NOV24
PCB CODE
01109231
24105231
06107231
24108231
24108232
24108233
24108234
04108231/2
10111231
SC6868
SC6866
01111221
01111222
01111223
10109231
10109232
10109233
18101231
18101241
18101242
18101243
18101244
18101245
18101246
19101241
19101242
07111231
07111232
01110231
01110232
09101241
09101242
16102241
16102242
07112231
07112232
07112233
SC6903
SC6904
16103241
08101241
08104241
07102241
04104241
04112231
10104241
SC6963
08106241
08106242
08106243
24106241
CSE240203A
CSE240204A
11104241
23106241
23106242
08103241
08103242
23109241
23109242
23109243
23109244
19101231
04109241
18108241
18108242
07106241
07101222
15108241
28110241
18109241
11111241
08107241/2
Price
$10.00
$5.00
$5.00
$5.00
$5.00
$5.00
$5.00
$10.00
$2.50
$2.50
$5.00
$5.00
$5.00
$3.00
$5.00
$2.50
$2.50
$5.00
$2.00
$2.00
$2.00
$1.00
$3.00
$5.00
$12.50
$7.50
$2.50
$2.50
$7.50
$7.50
$5.00
$2.50
$5.00
$2.50
$5.00
$2.50
$2.50
$20.00
$7.50
$20.00
$15.00
$10.00
$5.00
$10.00
$2.50
$5.00
$10.00
$2.50
$2.50
$2.50
$2.50
$5.00
$5.00
$15.00
$10.00
$12.50
$2.50
$2.50
$10.00
$10.00
$10.00
$5.00
$5.00
$7.50
$5.00
$2.50
$2.50
$2.50
$7.50
$7.50
$5.00
$15.00
$5.00
For a complete list, go to siliconchip.com.au/Shop/8
PRINTED CIRCUIT BOARD TO SUIT PROJECT
SURF SOUND SIMULATOR (BLUE)
COMPACT HIFI HEADPHONE AMP (BLUE)
CAPACITOR DISCHARGER
PICO COMPUTER
↳ FRONT PANEL (BLACK)
↳ PWM AUDIO MODULE
DIGITAL CAPACITANCE METER
5MHZ 40A CURRENT PROBE (BLACK)
BATTERY MODEL RAILWAY TRANSMITTER
↳ THROUGH-HOLE (TH) RECEIVER
↳ SMD RECEIVER
↳ CHARGER
USB PROGRAMMABLE FREQUENCY DIVIDER
HIGH-BANDWIDTH DIFFERENTIAL PROBE
NFC IR KEYFOB TRANSMITTER
POWER LCR METER
WAVEFORM GENERATOR
PICO 2 AUDIO ANALYSER (BLACK)
PICO/2/COMPUTER
↳ FRONT & REAR PANELS (BLACK)
ROTATING LIGHT (BLACK)
433MHZ TRANSMITTER
VERSATILE BATTERY CHECKER
↳ FRONT PANEL (BLACK, 0.8mm)
TOOL SAFETY TIMER
RGB LED ANALOG CLOCK (BLACK)
USB POWER ADAPTOR (BLACK, 1mm)
HWS SOLAR DIVERTER PCB & INSULATING PANELS
SSB SHORTWAVE RECEIVER PCB SET
↳ FRONT PANEL (BLACK)
433MHz RECEIVER
SMARTPROBE
↳ SWD PROGRAMMING ADAPTOR
DUCTED HEAT TRANSFER CONTROLLER
↳ TEMPERATURE SENSOR ADAPTOR
↳ CONTROL PANEL
MIC THE MOUSE (PCB SET, WHITE)
USB-C POWER MONITOR (PCB SET, INCLUDES FFC)
HOME AUTOMATION SATELLITE
PICKIT BASIC POWER BREAKOUT
DUAL TRAIN CONTROLLER TRANSMITTER
DIGITAL PREAMPLIFIER MAIN PCB (4 LAYERS)
↳ FRONT PANEL CONTROL
↳ POWER SUPPLY
VACUUM CONTROLLER MAIN PCB
↳ BLAST GATE ADAPTOR
POWER RAIL PROBE
RGB LED STAR
EARTH RADIO
DCC DECODER
DCC BASE STATION MAIN PCB
↳ FRONT PANEL
REMOTE SPEAKER SWITCH
↳ CONTROL PANEL
DCC REMOTE CONTROLLER
MAINS HUM NOTCH FILTER
MAINS LED INDICATOR
DCC BOOSTER / REVERSE LOOP CONTROLLER
↳ FRONT PANEL
SOLAR PANEL PROTECTOR (WHITE)
GRAPHING THERMOMETER
PICOSDR CONTROL PCB
↳ RF PCB
↳ FRONT PANEL (BLACK)
DCC/DC STEPPER MOTOR DRIVER
CALLIOPE AMPLIFIER
MICROMITE AUDIO PLAYER ADD-ON
↳ ALL-IN-ONE
DATE
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PCB CODE
Price
01111241
$10.00
01103241
$7.50
9047-01
$5.00
07112234
$5.00
07112235
$2.50
07112238
$2.50
04111241
$5.00
9049-01
$5.00
09110241
$2.50
09110242
$2.50
09110243
$2.50
09110244
$2.50
04108241
$5.00
9015-D
$5.00
15109231
$2.50
04103251
$10.00
04104251
$5.00
04107231
$5.00
07104251
$5.00
07104252/3 $10.00
09101251
$2.50
15103251
$2.50
11104251
$5.00
11104252
$7.50
10104251
$5.00
19101251
$15.00
18101251
$2.50
18110241
$20.00
CSE250202-3 $15.00
CSE250204 $7.50
15103252
$2.50
P9054-04
$5.00
P9045-A
$2.50
17101251
$10.00
17101252
$2.50
17101253
$2.50
SC7528
$7.50
SC7527
$7.50
15104251
$3.50
18106251
$2.00
09110245
$3.00
01107251
$30.00
01107252
$2.50
01107253
$7.50
10109251
$10.00
10109252
$2.50
P9058-1-C
$5.00
16112251
$12.50
06110251
$5.00
09111241
$2.50
09111243
$5.00
09111244
$5.00
01106251
$5.00
01106252
$2.50
09111245
$5.00
01003261
$7.50
10111251
$2.50
09111248
$5.00
09111249
$5.00
17112251
$7.50
04102261
$3.00
CSE251101 $5.00
CSE251102 $5.00
CSE251103 $7.50
09111242
$2.00
01111212
$5.00
01110251
$2.50
01110252
$5.00
μDCC DECODER
SIMPLE LC METER
WIFI ALARM MONITOR
POWER AMPLIFIER CLIPPING INDICATOR
MAY26
MAY26
MAY26
MAY26
09111247
04103261
01304261
01104261
NEW PCBs
$1.50
$2.50
$2.50
$15.00
We also sell the Silicon Chip PDFs on USB, RTV&H USB, Vintage Radio USB and more at siliconchip.com.au/Shop/3
ASK SILICON CHIP
Got a technical problem? Can’t understand a piece of jargon or some technical principle? Drop us a line
and we’ll answer your question. Send your email to silicon<at>siliconchip.com.au
Help building the
Internet Radio
The headline/article grabbed my
attention (February & March 2026;
siliconchip.au/Series/458), but on
reading the article, reality struck.
I don’t know anything about Raspberry Pis or 3D printing. Can you direct
me to articles that can provide some
background on the Raspberry Pi so I
can consider building the radio? 3D
printing might be another issue. Are
there files that I might be able to persuade a mate to print for me? (R. P.,
Kingsvale, NSW)
● The designer, Phil Prosser,
responds: the files to print the radio
can be downloaded from siliconchip.
au/Shop/6/3593
If you don’t have a 3D printer (they
are available from Jaycar and Altronics), it would be a good idea to ask a
friend for help. I suggest you talk to
them and see if they are OK with running a long print job for you. I would
also buy the filament for them as you
really want to start with a couple of
rolls of your chosen type and colour.
We used PLA filament, which is cheap
and easy to print with.
On setting up the Raspberry Pi, I suggest you follow the instructions in the
article to get the Pi booted and running
with a normal computer monitor, keyboard and mouse. At that point, I think
you will be surprised at how familiar
it is. If you have a question, Google is
your friend.
Raspbian (and Linux in general) has
a massive support base, so typing a
straightforward question into Google
leads to very clear advice. I am a very
infrequent Linux user, so I did exactly
that myself.
As a result of the strong support for
Linux, which is what the Raspbian
environment really is, there is a stunning range of free applications and
tools ready to download. These are
not dinky copies of what you might
seek; you can get properly supported
mainstream tools for pretty well anything you choose to do.
siliconchip.com.au
So, short of giving you a list of sites,
I suggest you get a Pi 4 or 5 (they are
about the same price but if you want
to try Linux, the Pi 5 is better – note
the absence of onboard audio, though)
and get it running, I expect you will
quickly realise the support for this is
broad and accessible.
Correct component
placement is important!
I purchased the USB-C Power Monitor short-form kit (SC7489; August
& September 2025; siliconchip.au/
Series/445). After completing the
assembly, I was unable to get the display to function. Initially, I thought
that I had made some error in construction and examined all soldering
joints, component placement, connections etc.
After a detailed investigation, I
found that the I2C and power signals
for the PCB differed from the circuit
diagram and source code for the board.
The board and PCB artwork that I
downloaded have the display VCC
from pin 6, SCL from pin 5 and SDA
from pin 4. The magazine circuit and
the source code show VCC supplied
from pin 16, SCL from pin 15 and SDA
from pin 14.
Monitoring the CPU pins, the firmware on the chip follows the circuit
diagram, not the PCB layout. I’m not
sure how many of these boards have
been sold, but the CPU firmware I was
supplied is not the correct version for
the PCB.
I have no facility to reprogram the
microcontroller and there is a risk of
melting the plastic cases of switches,
the potentiometer and switches using
Difficulty getting Ultrasonic Cleaner to resonance
I built the High-Power Ultrasonic Cleaner from the September & October 2020
issues (siliconchip.au/Series/350). The unit works fine in troubleshooting mode,
but it will not operate properly in ‘normal mode’.
If I start normally by pressing START, the red LED goes off and the second
green LED lights. Then LEDs 2 & 3 light, but it falls back to the second green light.
It alternates between these two states.
After a while, just the second green LED was lit steadily, and the red LED came on
and stayed on. At that stage, TP1 = 1.46V, with a frequency of about 3MHz. If I then
go to troubleshooting mode, all seems well, ie, all five green LEDs light, TP1 = 1.27V.
By varying the pot, I can see the TP1 voltage vary and frequency vary, around
about 40kHz, as expected. Adjusting the pot for a peak voltage, max TP1 = 2.10V
at 39.0kHz.
I know the TP1 voltage seems low compared to the expected 4V or so, but I
already put 10 more turns on the transformer with only a small increase in the
voltage at TP1.
I am thinking of rewinding a new transformer, removing the cover and glued
transducer from the tank to make sure the transducer is hard up against the tank,
and maybe positioning it under the tank.
● Sorry you are experiencing trouble with the Ultrasonic cleaner. Regarding the
operating frequency, it seems that the transducer resonance can’t be found. The
cleaner won’t operate correctly in that case. This could be because the number of
windings on the transformer is not right for the transducer.
We note that you added 10 turns to the transformer. This is probably too large a
step, and you may have missed the resonance point with the change being so large.
Perhaps unwind nine turns, then add one winding at a time, retesting each time.
Use the diagnostic mode to find resonance, then try normal operation. Obtaining
4.2V at TP1 is important.
If you are still unsure, please re-read the final section in the October 2020 article
titled “Troubleshooting”.
Australia's electronics magazine
May 2026 109
Avoiding 5G interference with satellite TV
The 5G network is causing a lot of interference with my satellite TV reception. Is
it better to get an LNC on the feedhorn, or should I use a PLL LNB converter with
a 5G filter built in? (J. E., via telephone)
● We asked Garry Cratt of Av-Comm Space & Defence and he responded: the
5G frequency allocation overlaps part of the internationally recognised C band
(3.4-4.2GHz) in many parts of Australia.
The typical satellite signal falling on Earth is in the fractions of a microvolt, and
a 5G base station must transmit a few watts. The effect of such a strong signal
in close physical proximity to a C-band satellite dish is to overload the LNB (LowNoise Block converter).
The only solution to remedy this without physically moving the satellite dish out
of the line-of-sight of the signal source is to filter out the 5G frequency before it is
amplified by the LNB.
Fortunately, in recent years, we have been able to manufacture LNBs with
sufficient filtering to exclude the interference. Unfortunately, the cost of this kind of
LNB means that is only being used by commercial operators (radio and TV stations
etc). For private satellite enthusiasts, the only realistic solutions are relocating the
dish or finding another source of the desired programming.
hot air to rework the board. It shouldn’t
be necessary to reverse engineer the
PCB and modify the source code to
get this project working. How can this
situation be rectified? (H. K., Mount
Evelyn, Vic)
● For VCC, SCL and SDA to be
present on pins 6, 5 and 4 of IC1, it
would have to be rotated 180° relative to the orientation shown in the
Fig.6 PCB overlay diagram on page 80
of the September 2025 issue. Note the
dot and ‘1’ marker showing that pin
1 is at bottom right. We are confident
that if you carefully desolder IC1 and
rotate it by 180°, then resolder it, the
kit will work.
An ideal bridge rectifier
for power amplifiers
I am inquiring whether the “Ideal
Bridge Rectifier kit” is suitable for
the SC200 Amplifier. If it is suitable,
which version of the Ideal Bridge
Rectifier kit should I be buying? (W.
L., Singapore)
● We have two different sets of Ideal
Bridge Rectifier kits, some based on
the December 2023 Ideal Bridge Rectifier (siliconchip.au/Article/16043) and
some on the September 2024 Discrete
Ideal Bridge Rectifier (siliconchip.au/
Article/16580).
You would need two of the December 2023 kits, as one can’t provide the
split rails the amplifier requires. The
SC6850, SC6851 and SC6852 kits can
all operate up to 72V/10A. That should
be sufficient in theory. Still, it would
be better to use two of the SC6854 kits,
rated at 72V/20A, to ensure it’s robust
enough to handle the switch-on inrush
current and such.
They’re only slightly more expensive. You can see the information or
purchase them at this link: siliconchip.
au/Shop/20/6854
That kit uses large SMD transistors
in D2PAK/TO-263 packages, which
are not difficult to solder (although
they require a fair bit of heat). They’re
heatsinked by the board. We have a
similar kit using through-hole TO-220
transistors, which is also rated at 20A,
although it’s currently out of stock
(code SC6855). We will be restocking
it, but only in small quantities.
Note that you also need a transformer with two separate secondaries,
not one centre-tapped secondary, but
that is how most high-power transformers are configured anyway.
The September 2024 design is limited to ±40V, so it would be a good
choice for a lower-power amplifier
like the Hummingbird but would need
modifications to work with the SC200.
We’re considering whether it can be
upgraded in future to handle at least
±60V, making it more suitable for use
with high-power hifi audio amplifiers.
isoundBar speaker
driver alternatives
I am interested in making a sound
bar, but I have some problems with the
August 2022 isoundBar (siliconchip.
au/Article/15426).
Two of the Vifa-Peerless drivers used
are not available from Wagner Electronics, the original supplier. Can you
suggest alternatives or another Australian source?
Also, the width of the overall unit is
too wide to fit between the feet of my
TV, so I’d like to change the box dimensions to 1m wide from the original
1240mm. I will need to recalculate the
size of each speaker section to retain
the original volume, either sealed or
vented. I won’t go to this trouble if no
drivers are available/suitable.
I have a spare 24V AC transformer,
so I’d make a power supply for the
WARNING!
Silicon Chip magazine regularly describes projects which employ a mains power supply or produce high voltage. All such projects
should be considered dangerous or even lethal if not used safely. Readers are warned that high voltage wiring should be carried
out according to the instructions in the articles.
When working on these projects use extreme care to ensure that you do not accidentally come into contact with mains AC
voltages or high voltage DC. If you are not confident about working with projects employing mains voltages or other high voltages,
you are advised not to attempt work on them. Silicon Chip Publications Pty Ltd disclaims any liability for damages should anyone
be killed or injured while working on a project or circuit described in any issue of Silicon Chip magazine.
Devices or circuits described in Silicon Chip may be covered by patents. Silicon Chip disclaims any liability for the infringement of such patents by the manufacturing or selling of any such equipment. Silicon Chip also disclaims any liability for projects
which are used in such a way as to infringe relevant government regulations and by-laws.
Advertisers are warned that they are responsible for the content of all advertisements and that they must conform to the Competition & Consumer Act 2010 or as subsequently amended and to any governmental regulations which are applicable.
110
Silicon Chip
Australia's electronics magazine
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amplifier, but can I locate this inside
the vacant area next to the amplifier
board? (I. S., Glenhaven, NSW)
● Alternative drivers are available
from Wagner Electronics but you will
need to change a few dimensions to
fit them.
The critical TC6FD00-04s can be
replaced with 2.5-inch Daichi midrange/woofers, Wagner Cat HFS6415-8. These are rated at 8W rather than
4W, meaning a higher supply voltage
may be desirable, and they will need
a larger diameter hole (55mm). They
are slightly taller, needing a 70mm
tall baffle (your proposed changes will
accommodate this).
For the tweeters, you could use Daytona 6W 20FA-6 3/4-inch Neodymium types, Cat ND20FA. The slightly
higher impedance should not cause
any problems.
An alternative to the Vifa TG9FD1004 woofer is the Dayton PC83-4 3-inch
siliconchip.com.au
full-range 4W driver, also available
from Wagner.
This is slightly taller at 46.5mm and
has a smaller diameter (78.5mm) so
you will need to change the cut-out
dimensions to fit it up.
While these substitute drivers are
similar, they will probably require
different relative drive levels to the
original set, but that’s easily accommodated by the suggested amplifier,
which lets you adjust the levels individually by ear.
Changing the isoundBar width to
1m is fine. As you’re reducing the
width by 19.4%, increasing the internal height by 19.4%, from 64mm to
80mm, should keep the internal volumes similar. That will help you fit
the slightly larger drivers too. You
should also adjust the baffle positions proportionally, reducing the
width of each internal chamber by
roughly 20%.
Australia's electronics magazine
It’s OK to install the power supply
in the box, but ensure adequate cooling and shielding, and make sure any
mains wiring is properly insulated
and the wire colours are correct. We
purposefully avoided any mains voltages in the project to make it beginner-
friendly. We hope this advice helps
you.
Connector pin order
isn’t obvious
Hi, I recently purchased the Pico
BackPack Kit and during assembly, I
determined that the PCB (07101221
RevC) differs from the circuit diagram in March 2022 (siliconchip.au/
Article/15236). The circuit diagram
that I have shows jumper JP2 connected to pin 9 of CON4 and pin 13
of CON4/GP16.
When I was about to install JP2, I
noted a track to pin 2 of CON4, which
May 2026 111
is GND. I have confirmed continuity
between the two pads. Has there been
a circuit diagram change? I wonder if
someone there would be able to comment on what looks like an error. (M.
F., Gulfview Heights, SA)
● It isn’t marked as such on the PCB,
but pin 1 is at the other end of CON4.
The clue is that pin 1 has a square pad,
while the others are rounded. So that
pin of CON4 you are referring to is
actually pin 13 (second from the end),
which connects to JP2 as expected.
The trace to pin 9 is on the underside
of the PCB.
This probably isn’t helped by the
fact that pins 15-18 don’t exist on
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Next Issue: the June 2026 issue
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112
Silicon Chip
CON4 (on the PCB); they correspond
to the four pins at the other end of
the LCD module for its (unused) SD
card slot.
Bench supply upgrade
query
Can you advise me if Silicon Chip
has published a design for a variable-
voltage, variable-current linear power
supply, delivering (say) 0-30V at 0-5A
(or so), using something like 2N3055
series pass output transistors?
I have recently acquired a WONI
bench power supply that appears to
be working, but the design is rather
woeful, mainly in regard to the voltage control potentiometer. The design
of the supply has the pot wired as an
adjustable resistor (just two wires from
the pot to the PCB) and the voltage
variation is far from linear.
Rather than playing around with
the existing design, I think I would be
happier to build and retrofit a Silicon
Chip design, which I know would perform properly. (P. W., Pukekohe, New
Zealand)
● We have a few designs that may
suit you. In October 2019, we published a 45V, 8A linear bench supply (siliconchip.au/Article/12014).
It would have plenty of headroom to
operate at 5A but, being a linear supply, it is on the bulky side.
Alternatively, you could consider
the 40V Switchmode/Linear Bench
Power Supply (April-June 2014 issues;
siliconchip.au/Series/241).
It uses a fast-acting final linear stage
for output regulation and current limiting, with a tracking switch-mode regulator before it for better efficiency.
As such, it doesn’t require a large
heatsink.
Using a Pico 2 W for
the WiFi Time Source
I have several clocks I wish to adapt
to using the New GPS-Synchronised
Analog Clock from September 2022
(siliconchip.au/Article/15466). I was
intending to use the WiFi Time Source
for GPS Clocks project with it (June
2023; siliconchip.au/Article/15823).
Is there any advantage to using a Pico
2 W over the Pico W in this project?
If I use the Pico 2 W, what changes
would I have to make to the WiFi Time
Source project, if any? (P. N., Engadine, NSW)
Australia's electronics magazine
● The Pico 2 W uses a different
processor from the Pico W (RP2350A
rather than RP2040) so you can’t load
a UF2 file compiled for the Pico W on
a Pico 2 W. It will just ignore it.
In theory, the existing source code
should compile if the target is changed
to the Pico 2 W, but we have not tried
that, or tested the result. So we recommend you stick with the Pico W since
we know it works and have a compiled
UF2 file ready to use. Also, there’s no
real advantage to using a Pico 2 W in
this scenario, and it costs more.
While it’s possible that simply
recompiling the code for the Pico 2
W target will be sufficient, there may
be breaking changes in the C SDK and
its API that mean that more work is
needed. The Pico W’s capabilities are
more than sufficient for the task, so we
don’t see any need to port the code at
this stage.
The Raspberry Pi Foundation says
that the Pico W will remain in production until at least January 2036.
Case advice for
Roadie’s Test Oscillator
Can I use a plastic enclosure for the
Roadie’s Test Oscillator project (June
2020; siliconchip.au/Article/14466)? I
don’t need it to be drop-proof or rugged. (R. M., Melville, WA)
● Yes, a plastic enclosure is suitable. Note that you must use a type
where the lid is attached to the base
using screws to comply with safety
standards restricting access to the coin
cell that powers the oscillator. The cell
can be a severe health hazard to young
children if they can access it.
RF Probe wanted
I was just looking at a video from
Carlson’s Lab where Carlson troubleshoots electronic circuits with a device
he created himself that he calls the
Carlson Ultra Probe.
It is a very high-gain and sensitive
amplifier that uses a coaxial cable
as a probe. It can be used as an RF
or AF detector and amplifier. I was
wondering whether Silicon Chip has
created such a project. (P. J., Lenah
Valley, Tas)
● We published a similar Audio
Signal Injector and Tracer with a
matching AM Demodulator Probe in
the June 2015 issue (siliconchip.au/
SC
Article/8603).
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