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Items relevant to "Phenomenal Pinball Machine, Part 1":
Items relevant to "Human Comfort Indicator":
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Items relevant to "Micropower SSB Transmitter":
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Analog Computers
Part 2: modern-day examples and how they’re used in neural networks
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Contents
Vol.39, No.06
June 2026
12 Analog Computers, Part 2
Analog Computers
Analog computers are making a comeback because of how well-suited they
are for neural network processing. We take a look at some of the modern
analog computers and the features of current-day analog AI workflows.
By Dr David Maddison, VK3DSM
Technology feature
36 Inspection Reports for PCBs
Quality inspection reports are important for ensuring that PCBs will be
made to the required standard from your chosen PCB manufacturer.
Supplied by PCBWay, it includes useful information on manufacturing.
By Steve Mansfield-Devine for PCBWay
PCB fabrication
54 Whole-Home Sound System
Come and see the trials and tribulations brought about by installing a sound
system that covers an entire house. It uses three amplifiers, one preamp,
thirteen speakers and hundreds of metres of wiring!
By Julian Edgar
Home audio
66 Working with e-Paper Displays
The Human Comfort Indicator (listed below) is the first project where we
have incorporated a bare e-paper display into a design. This article goes
into more detail on how e-paper displays work and how we are driving it.
By Tim Blythman
Display modules
26 Phenomenal Pinball Machine
We cover how to design and build every part of your own Pinball Machine.
While we provide a standard layout, you can customise it to your own
tastes, with different artwork, sounds, lighting and more.
Part 1 by Phil Prosser
Gaming project
43 Human Comfort Indicator
Displaying the temperature, humidity and dew point, this handy little device
tells you if an area is comfortable to be in. It’s battery-powered with USB
charging, and stores historical data for the last day, week and month.
By Tim Blythman
Environment measurement project
60 Simple USB Power Monitor
Using under 20 parts, this project can measure voltage, current and power
supplied over USB up to 36V, 3A and 108W. It displays data on a 0.96-inch
OLED screen and supports USB power delivery (PD) 2.0 and 3.0.
By Richard Palmer
Test & measurement project
70 Micropower SSB Transmitters
We wanted to see how small we could make a single-sideband transmitter,
so we came up with three designs, one using just three transistors. Each of
the designs only use through-hole components and no microcontrollers.
By Andrew Woodfield, ZL2PD
Radio communications project
Cover background image: https://unsplash.com/photos/a-close-up-of-a-pinball-machine-18dGkEQ5wSM
Part 2: page 12
Source: www.flickr.com/photos/jitze1942/4304353299/in/
album-72157623284316506
Page 70
Micropower
SSB
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Notes & Errata
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Silicon Chip
Our TV is around 10 years old now. While the picture
still looks fine, its built-in “smart” features are slow and
outdated. So a couple of years ago I bought an Amazon
Firestick 4K, which plugs into an HDMI port and provides
modern smart-TV functionality.
While we use the TV’s internal speakers for everyday viewing, for movies and live concerts I have the
TV’s optical output connected to my CLASSiC DAC (February-May 2013;
siliconchip.au/Series/63), then into an Ultra-LD series amplifier and the Majestic
loudspeakers (June 2014; siliconchip.au/Series/275). This setup provides excellent audio quality.
Recently, I was watching some live concert recordings through VLC on the Firestick (streamed from a computer over WiFi) and noticed that the audio sounded
very muffled. It was like someone had placed a blanket over the speakers, with a
clear loss of high-frequency detail.
This was odd, because I knew the concert recordings used PCM audio (ie, not
digitally compressed), and when I played that same PCM audio directly through
the DAC, it sounded fantastic. So it wasn’t the recording; it was something wrong
with the playback chain.
The audio path in this case is: File Server ▶ WiFi network ▶ Firestick ▶ TV ▶
TOSLINK ▶ DAC ▶ Amplifier ▶ Speakers. I knew the first couple of steps wouldn’t
be a problem, nor anything from the TOSLINK output onward. That narrowed the
problem down to either the Firestick or the TV. I went through the TV’s audio settings but couldn’t find anything suspicious.
On the Firestick, navigating to Settings ▶ Display & Audio ▶ Audio didn’t reveal
many options. However, there was one called “Surround Sound”, which was set to
“Best available”. The other options were “PCM”, “Dolby Digital Plus” and “Dolby
Digital”. I changed this setting to PCM and the problem immediately disappeared.
Playing back the same concert video now produced crisp, clear audio, exactly as
expected.
What surprised me even more is that watching TV shows and movies through
the Firestick now also sounds better than it did previously, particularly in terms of
dialogue intelligibility. This makes me wonder why “Best available” is the default
setting, when it clearly isn’t the best option for systems connected to a proper amplifier and speakers. As far as I can tell, this “best available” mode enables additional
audio processing such as compression and EQ that is optimised for small, tinny
speakers. While that may help on basic TV audio systems, it actively harms sound
quality when used with a decent hi-fi setup.
Even more oddly, the Firestick felt the need to adulterate the audio even when
the source was already in PCM format. I would have expected it to simply pass the
audio through unchanged, but clearly that isn’t what happens.
So if you have a decent sound system connected to your TV, it’s worth checking
the entire signal chain and not assuming the default settings are optimal. I’ve always
found dialogue on this setup a little muffled and simply put up with it, assuming
poor mastering was to blame. Now I know better.
I wish I had realised this a long time ago as it would have made a lot of the media
I’ve viewed a lot more enjoyable. It’s hard enough to understand what’s said in modern movies and TV shows without the audio being artificially muffled!
by Nicholas Vinen
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Installing a car GPS tracker yourself
Cairns has many cars stolen every year. Rather than
install an engine immobiliser that I would find annoying
every time I get in the car, I opted to install a GPS tracker.
I selected a tracker from AliExpress that uses 4G and was
labelled as “global”, using 21 frequency bands. It is called
a “GPSCJ730plus 4g”, and cost $55 delivered (currently
AliExpress 1005007557451623).
It looks just like a standard car relay, complete with a
connector plug containing five wires. Two wires are for
power, with the positive lead having an inline fuse. A third
wire is used for sensing if the accessory power is on, which
indicates that someone has started the vehicle.
The last two wires are heavier gauge and are connected to
a normally closed relay contact inside the device. These can
be used (if desired) to disconnect power to the fuel pump,
effectively disabling the car. The device has an operating
voltage of 9-95V DC, so can be used on a range of vehicles.
The device needs a physical SIM card to function. I purchased a $2 SIM from Amaysim and activated it on my
computer. I selected the “Pay as You Go” plan. This was
a little difficult to find on the Amaysim website, but it is
there. $15 was required to be paid to start this plan, which
lasts for 365 days. The charges are 12¢ per minute for calls,
12¢ per SMS and 5¢ per 1MB of data.
Approximately $4 of the $15 plan is used in setting up
the SIM card, mostly from SMS messages sent to my mobile
acknowledging the setup parameters. In the six months
since then, another $3 has been used up, mostly in data
charges for uploading the GPS position information whenever the car is moving.
All the setup is done by sending SMS messages to the
Amaysim number in the device. The device needs a “Control number” for sending SMS messages under specific
conditions, so I used my mobile phone number for this.
The device also needs the APN of the mobile phone carrier, which for Amaysim is “yesinternet”.
There are numerous other setup options that can be activated, like automatically sending an SMS to the Control
number (my mobile) if a certain speed limit is exceeded.
The process I followed to set it up is:
1. Activate the SIM online
2. Power up the CJ730 and insert the SIM card
3. Wait for the CJ730 to get GPS location and
mobile phone connection (two minutes)
The default user & password for the device
are admin & 123456 (I changed the password after it was all working OK).
Two essential parameters are now
required to be entered into the CJ730:
4
Silicon Chip
4. Set the Amaysim APN by sending an SMS containing
“apn123456 yesinternet” (without the quotation marks).
The response should be “apn ok”.
5. Set the Admin (Control) phone number in CJ730 to my
mobile number. Send an SMS containing “admin123456
0419xxxxxx”. The response should be “admin ok”.
After that, a few SMS commands can be sent from my
mobile, to make sure it is operational:
• “status”, the response includes the battery, GPRS,
GSM, GPS etc levels
• “where”, response = “http://maps.google. ...” with the
GPS coordinates
• “imei”, response = “86209206xxxxxxx”
Once it is all set up, the device uploads its GPS position
data to a website and you pay for this data on the Amaysim
plan. I don’t believe any top-up of the original $15 will be
required in 12 months. It will be necessary to pay another
$15 every 365 days to keep the SIM active, though.
The data uploaded consists of the date, time, latitude,
longitude, speed, direction, accessories on/off and the supply voltage. The device has a motion sensor, so no data is
uploaded when stationary.
By default, data is uploaded about every 20 seconds while
moving to www.gpscj.net, which is in China. This is a free
site that stores your data for 160 days. Below is part of a
screenshot of the web page. I have found this site works
very well. I can access it on my computer or by using an
app called “Yuntrack”. It displays details superimposed
on Google Maps.
You can instead use a free program called “traccar” that
runs on a Raspberry Pi. I plan to go down that path in the
future. You send an SMS to the device containing the URL
and port number to point to the Pi. The device can only
send data to one server at a time.
It has an internal rechargeable battery, allowing it to send
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an SMS if the primary power is disconnected. Disconnection of primary power is considered an urgent situation, so
as well as sending an SMS, the device also rings my mobile
number to get my attention. This was inadvertently tested
when I replaced my vehicle battery.
I can send an SMS of “555” to the device to operate its
internal relay, cutting off the fuel pump if it is wired up that
way. The device has smarts that cause it to intermittently
operate the relay if the car is travelling above a set speed
and fully operate the relay when the speed has reduced.
Another SMS text of “666” will drop out the relay, allowing the motor to be started again.
The GPS receiver in the device works with three satellite
systems: GPS, BeiDou and GLONASS. It reports the number of satellites for each system that it can currently see.
I have the device permanently powered on in my 2005
Mazda 2. Its power consumption is 40mA, or approximately
1Ah per day. That isn’t much higher than the normal parasitic drain, so the battery should last about four weeks
without driving the car.
More commands can be found by searching the web for
“cj730 commands” or “cj720 commands”.
I have yet to experiment with commands that limit the
power consumption when the vehicle is idle. One command
will set the device to only send data when the accessory
power is on. Other commands cause the device to go to sleep
and wake up when its sensor detects vehicle movement.
Sid Lonsdale, Cairns, Qld.
Transistors should be matched on Vbe, not hfe
After reading the article for your new Calliope Amplifier
(April 2026; siliconchip.au/Article/20084), I have doubts
about the value of matching the input transistors for hfe.
Keeping the input transistors matched and minimising the
input offset voltage does provide benefits. Not only is the
output offset voltage minimised, but mismatch in a longtailed pair increases distortion. Whether one deems the
extra effort worthwhile is another matter.
The BC558 and BC556B are from the same family of
devices, with the 556B selected for higher gain. Selecting the 556B alone will reduce the offset voltage without
the added complication of matching by reducing the base
current through the base resistors, so swapping the input
devices between these two devices (556 and 556B) is not
a fair measure of the advantage of matching.
As best as I can tell, matching the hfe of the current mirror transistors will have virtually no effect on the input offset voltage. The current balance in the mirror is primarily
fixed by the requirements of the input stage and the amplifier after global feedback is applied, and the bases are tied
together, so any mismatch will have an insignificant effect
on the balance.
The parameters of most importance to input offset are
the Vbes of the input pair and the mirror resistors, and as
far as I know, there is no significant relationship between
hfe matching and Vbe matching.
The greater impact on input offset from hfe in the input
transistors is simply the combined effects of the transistors’ hfe (and hence base current) and the resistances seen
at their bases. So, to minimise the impact on the offset, the
sensible approach would be to keep those resistances as
low as practical and to maximise the current gain of the
input pair.
6
Silicon Chip
The factors that do significantly impact input offset are
the Vbe matches of the input pair (Q7 & Q8) and the current mirror (Q15 & Q16).
I did some research and circuit analysis. Data from
Philips’ 1977 “Low frequency transistors” data book (SC2
11-77) shows a BC556’s hfe varies from 220 to 480, which
would result in a worst-case offset voltage (cause by mismatched bias currents flowing through input bias resistors)
of approximately 81mV.
The Vbe of a BC556 at 2.5mA varies between 600mV and
750mV, which implies a maximum Vbe mismatch (ie, input
offset voltage) of 150mV. The same figures for the BC549 are
580mV and 700mV, so a maximum Vbe mismatch would
be about 120mV.
An amplifying factor of 1.47 must be applied due to the
emitter resistors in the input pair and the current mirror,
so the maximum offset error caused by a mismatch in the
current mirror Vbe could be over 170mV.
These are the absolute worst-case contributions to
input offset voltage due to mismatched current mirror
and input transistors. These figures are blurred by the fact
that the resolution of the graphs I have had to use is not
great. Another complicating factor that I cannot account
for is the usual distribution of parameters within their
published ranges.
I don’t claim they are particularly accurate, but they do
give a clear indication of the greatest causes of input offsets. Still, the implications are clear: the overall input offset
voltage of the complete amplifier could depend as much
as four times more on Vbe matching than hfe matching.
My advice is to match input transistors for Vbe. Problems caused by mismatched hfe are of minor significance
by comparison, and the bad effects can be overcome by
simply selecting for higher hfe (eg, using BC556Bs instead
of BC558s). Matching only the hfe might appear to provide
benefit, but it is quite likely that it coincidentally produced
a better match in Vbe as well.
Phil Denniss, Darlington, NSW.
Comments: we prefer using higher-gain BJTs where possible since, as you point out, it reduces their base current,
which can bring certain benefits. While difficult to find now
(apparently due to a lack of demand), some Asian fabs still
bin BC556Cs and related devices, which should (in theory)
give even more benefit than the BC556B.
You’re right that Vbe matching is more valuable, and it’s
easy to do with a basic DC power supply, a few resistors,
a breadboard and a multimeter.
All that’s really needed is to apply the same voltage to
the base-emitter junction via the same resistance for both
transistors (say, 5V & 1kW), measure the voltage across the
junction, and select two transistors from a small batch purchased together with almost identical readings.
We strongly recommend using transistors from the same
batch for pairs in amplifiers (input, current mirror etc).
The Vbe variation within a batch is usually on the order
of 10-20mV, not the 100mV+ suggested by the data sheets.
Feedback on the Internet Radio project
After constructing the Internet Radio from the February &
March 2026 issues (siliconchip.au/Series/458), I would like
to share some of the deviations made from the build article.
Initially, I had no audio from the Pi 4. The article suggests using a 3.5mm stereo jack plug, but the Pi 4B has a
Australia's electronics magazine
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the front panel so it’s very easy to learn. There are 4 HDMI video inputs for
ATEM Mini features a “multi-view” that lets you see all cameras, titles and program,
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four-pole 3.5mm audio jack socket, as the audio jack also
has the composite video signal. Swapping the 3.5mm stereo jack plug to a TRRS type fixed the sound.
Since the 3D-printed Internet Radio case has ample room,
I added a cooling fan on the Pi 4, although I am not sure
if it is necessary.
The rest of the construction and software installation
went smoothly. After creating some radio station text files
and saving them to the Pi desktop as per the instructions, I
decided it would be convenient if the Internet Radio automatically opened my favourite radio station on start-up.
The radio station text file on my desktop that I want to run
at startup is named “rock.m3u”.
Raspberry Pi software has multiple different approaches
to do this. After some research, I decided to create a .desktop file and run it in the autostart folder. The first job is to
create a .config/autostart folder. To do this, I opened a Terminal window and typed:
mkdir -p ~/.config/autostart
“~” expands to your home directory, which in my case
is /home/pi. Be sure to add the full stop in front of config.
I then created a VLC autostart file that will be in the .config/autostart folder. In the same Terminal window, I typed:
nano ~/.config/autostart/vlc_start.desktop
This opens the nano text editor. In the text editor, type:
[Desktop Entry]
Type=Application
Exec=vlc /home/pi/Desktop/rock.m3u
Replace “pi” if your username is different and replace
rock.m3u with the radio station text file of your choice.
Press Ctrl+x then y to save the file and then press Enter to
close the text editor.
By default, the Pi File Manager doesn’t show the .config folder (the “.” at the start means ‘hidden’). To view the
folder, go to the “View” menu and click Show Hidden in
the File Manager.
To change which radio station autostarts, use the File
Manager, navigate to .config/autostart and edit the vlc_
start.desktop file by right-clicking on the file and selecting
“Open with text editor”.
With autostart configured, I then tinkered with VLC. The
default VLC window is quite small. To permanently resize
and save it as the default size, you need to close down VLC
via the menu “Media” and “Quit”. Once you’re happy with
VLC window size, you can close VLC with the X or just
shut down the Pi to retain your new default window size.
VLC has some audio visualisations that are accessed via
the Audio → Visualization menu option. Unfortunately,
these are not saved as a preference, so they need to be
selected every time VLC is opened.
To permanently set an audio visualisation, use the Tools
→ Preferences → Audio menu item. Under Effects Visualization, select either 3D OpenGL Spectrum Visualization
or Visualizer Filter. Those are the only two that can be set
as the default.
Mathew Prentis, Port Augusta, SA.
Phil Prosser comments: It is great to see people doing
their thing with the design. I love that Mathew has extended
the installation and I will be updating the radio in the shed
SC
with his advice right away.
8
Silicon Chip
Australia's electronics magazine
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Part 2 by Dr David Maddison, VK3DSM
Analog Computers
A recreation of Charles Babbage’s Difference Engine at the Computer History Museum in Mountain View, California.
Source: Jitze Couperus – www.flickr.com/photos/jitze1942/4304353299/in/album-72157623284316506
Analog computers are making a comeback because they are well-suited to neural
network processing. We’ll cover some of the theory behind that, then look at some
of the new analog computers that are being developed.
T
he extremely high speed of modern
digital computers and the relative
ease of programming compared
to analog computers accelerated the
decline of the latter in the 1970s.
However, analog computing is experiencing a major resurgence, albeit
in a somewhat different form from
traditional analog computers. While
modern analog computers still rely
on analog signals (voltages, currents,
resistances or even light) to perform
calculations, their design bears little
resemblance to the analog computers
of the mid-20th century.
12
Silicon Chip
Instead of racks of discrete op
amps wired via patch panels and
potentiometers, today’s implementations are built on silicon chips using
memristors, floating-gate transistors,
switched-capacitor arrays or photonic
waveguides. They are often digitally
programmable.
They are also far smaller than the
analog computers of yore, and more
precise, being targeted at specific tasks
like AI matrix-vector multiplications
or AI inferencing (using a pre-trained
AI model to produce an output).
That makes it possible to use them in
Australia's electronics magazine
smartphones or embedded devices,
alongside existing digital processors.
The main benefit of modern AI
analog computing is high energy efficiency and high processing speed for
specific AI tasks, like inferencing and
matrix-vector multiplication. These
functions are implemented in AI accelerator chips.
One common feature of AI accelerators (hardware optimised for AI tasks)
is their massively parallel nature. By
using many parallel units operating at
a high speed, they can perform thousands of calculations simultaneously
siliconchip.com.au
and complete billions per second.
They are designed for linear alegbra
and the tensor mathematics used in
AI applications.
Digital AI accelerator chips include
GPUs (graphics processing units,
widely used for training), TPUs (Google’s tensor processing units for neural
networks), NPUs (neural processing
units for on-device AI), ASICs (application-specific integrated circuits for
specific AI functions) or FPGAs (field
programmable gate arrays, reconfigurable chips for various tasks).
On the other hand, modern analog
accelerator AI chips generally fall into
the following categories:
• Resistive/electrical AIMC (analog
in-memory computing).
• Neuromorphic (analog, digital, or
mixed; when analog, they often overlap with AIMC).
• Photonic analog
AIMC is ideal for matrix-vector
multiplications directly in memory
arrays using resistive devices like
PCM (phase change memory), RRAM
(resistive random-access memory) or
flash memory. Examples include IBM’s
PCM-based chips, Mythic’s M1076
(flash analog), EnCharge AI’s capacitors and Peking University’s RRAM
prototype.
These focus on efficient deep
learning inference. We will describe
in-memory computing later.
Neuromorphic chips emphasise
brain-inspired designs, often with
spiking neural networks (SNNs),
event-driven/asynchronous processing and sparsity. These can be analog,
digital or hybrid. Sparse models and
SNNs will be described shortly.
Photonic chips use light-based processing, like Lightmatter and Microsoft’s AI chip. They have the potential
to use even less power than the other
types of analog AI chips.
Features of modern analog AI
Modern analog AI computing has
the following characteristics.
that have been trained using digital AI.
Currently analog AI computers are
mostly used only for energy-efficient
inferencing, not training. However,
research is underway to develop analog AI training models, and it has been
experimentally demonstrated.
Analog computing suits specific AI
workloads
For specific AI workloads, especially inferencing, in-memory matrix
operations and ‘sparse’ models such
as ‘mixture of experts’ (MoE) or spiking networks, analog computing offers
dramatic efficiency gains.
In sparse models, a significant portion (often the majority) of connections
(weights) or activations are intentionally set to zero or left inactive to boost
efficiency in terms of memory, computation and energy without drastically harming performance. Dense
models, by contrast, maintain near-
complete connectivity, which can
capture more complex patterns but at
a higher resource cost.
Sparsity is especially beneficial in
contexts like analog AI, where it aligns
with the nature of the analog hardware.
Analog AI has been suggested as
being highly suitable for MoE models. These are neural network architectures in which a large model is split
into many smaller sub-networks. An
‘expert’ is a small specialised part of
the overall neural network model. A
lightweight routing network dynamically decides, for each input, which
expert (or experts) to activate for a
particular problem.
So, instead of running the entire
massive model for every input, only
a small subset of experts is used. This
makes the system much more efficient
than traditional dense models (where
everything runs every time).
In analog implementations of MoEs,
the unused experts can be completely
powered down, leading to even greater
Analog AI is not a complete
replacement for digital AI
Analog (or analog-inspired neuromorphic/mixed-signal) computing
cannot yet fully replace a digital GPU
cluster like xAI’s Colossus because it
is not a drop-in replacement for general large-scale AI training. Due to
present limitations of analog AI, for
inferencing, analog AI uses models
Fig.37: the model of experts
(MoE) concept.
siliconchip.com.au
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power savings. These analog MoE systems can be fully analog or hybrid (for
example, with digital routing and analog experts).
In reference to Fig.37, a gating network uses weights to adjust each
expert’s contribution to the final
answer. The gating network learns
from experience and decides which
is the most appropriate expert to send
the data to. By sending the data to the
‘best’ expert, the processing is more
effective. This is more effective than
just using a single expert.
Analog MoE models have been
implemented by IBM using phasechange memory (PCM) crossbars for
the expert model weighting; a small
analog router selects 2-4 experts per
input for vision tasks. Mythic’s analog matrix processors use flash memory to carry the expert weighting.
Lightmatter is using optical routing to
switch light paths to different refractive expert layers.
A spiking neural network (SNN), or
spiking network, is a type of neural
network that mimics how biological
brains work more closely than standard artificial neural networks.
With analog AI, the reported possible savings in power consumption
are 10× to 100× (or even as much as
1000× for analog-optimised tasks) for
inference applications compared to
digital AI.
Edge computing
Because analog AI chips consume
so little power, they allow advanced
AI models like large language models
(LLMs) to mimic the human brain’s
efficiency and to run on small ‘edge’
devices like smartphones, autonomous robots, UAVs, wearables etc
without the need for a ‘cloud’ connection.
Energy efficiency
Currently, xAI’s Colossus AI training
supercluster in Memphis, Tennessee is
June 2026 13
recognised as the world’s most powerful AI compute facility with around
200,000 NVIDIA H100/H200 GPU
equivalents. It consumes 280-300MW
peak power.
Meta’s clusters and Microsoft/OpenAI facilities are in the 100-200MW
range. US data centre power consumption today, a large portion of which
is due to AI, is around 40GW and is
projected to reach 78-123GW by 2035.
Even with the low cost of electricity in
the USA compared to Australia, with
such high power consumption, the
running costs are significant.
In a hypothetical 300MW data centre with an inference-heavy workload,
partial analog adoption could reduce
power consumption by 50-90% (eg,
30-150MW). For full training, that
is not as feasible today, but perhaps
a 20-50% reduction is possible with
hybrid computers.
Matrix operations
A fundamental operation in neural
networks is matrix-vector multiplication (often matrix multiplication in
layered neural networks).
Analog circuits can perform this
extremely efficiently and in parallel by
exploiting natural physical laws such
as Ohm’s law (V = IR) and Kirchhoff’s
current law (the total current entering
a junction must equal the total current
leaving), which are intrinsic to electronic circuits.
Inputs are applied as voltages across
a resistive ‘crossbar array’ (typically
memristors, resistive RAM [RRAM] or
resistor grids), and the resulting currents at each column naturally sum
to produce the dot-product outputs,
which represent the matrix multiplication result instantaneously (limited
only by circuit settling time, typically
nanoseconds to microseconds).
A dot product is a simple mathematical operation involving multiplying
two vectors to form a single vector.
A basic 3×3 crossbar array is shown
in Fig.38. The inputs are voltages V1,
V2 & V3 on the rows representing the
input vector (eg, pixel brightness values from an image being analysed).
The matrix weights (obtained via prior
training representing the importance
of an association) are the conductances
(Iij = 1 / Rij) at each crosspoint of the
matrix elements (higher conductance
= more weight).
The outputs are currents I1, I2,
I 3 down the columns, which are
14
Silicon Chip
Fig.38: a 3×3 resistive crossbar array,
the core of many modern analog AI
accelerators (eg, the memristor or
resistor grids in Mythic or IBM chips,
respectively). It performs vectormatrix multiplication instantly via
physics.
automatically the matrix-vector product with no mathematical operations
used; just Ohm’s and Kirchhoff’s laws
doing the work in parallel.
By Ohm’s law, the current through
each crosspoint Iij = Vi × Iij. By Kirchhoff’s current law, the output current
Ik = ∑(Vi × Iij) for j = k. Thus, Ik is the
dot product of the input vector V with
column k of conductance matrix G.
Matrix multiplication is the mathematical powerhouse behind nearly
every modern artificial intelligence
system, especially deep neural networks (the foundation of models like
GPT, BERT, Stable Diffusion and computer vision).
Matrix operations are how neural
networks ‘think’. A neural network
layer takes an input vector, such as
numbers representing pixel values in
an image or words and produces an
output vector. This transformation is
almost always a matrix-vector multiplication: output = weights_matrix ×
input_vector + bias.
The weights matrix contains millions (or billions) of learned parameters that encode what the network
has ‘learned’ during training. Each
layer performs this operation, stacking many layers to create complex
representations (eg, recognising a cat
from pixels).
The bias is an extra adjustable
parameter added to each neuron
(or node) in a layer, alongside the
weighted sum of inputs. It provides a
‘starting point’ for any opinion the AI
might formulate, and this is the basis
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for any political or other bias that AI
engines are deemed to have.
In simplified terms, a neural network layer can be thought of as a team
of experts (neurons). Each expert gives
an opinion weighted by their expertise
(matrix weighting values) on every
piece of input data.
Matrix operations are the bottleneck
for speed and energy use in AI training and inference. Around 90-99% of
computation time and energy in deep
learning is spent on matrix multiplications. That’s why in digital AI, GPUs
(with thousands of cores for parallel maths) and specialised chips (eg,
TPUs, NVIDIA H100s) are designed to
accelerate matrix operations.
Analog AI computing is ideal for
matrix multiplication because it utilises physical laws, as explained
above, allowing it to perform billions of multiplies/adds in parallel
instantly and with little power consumption.
After the matrix operation, the
resulting current (or voltage after conversion) can then be fed to an analog-
to-digital converter (ADC) for further
processing, in the case of a hybrid computer, or it can pass directly to the next
layer of the neural network.
Such analog circuits are ideal for
real-time audio or video processing
since they lack the delays inherent
in digital conversion and processing.
In-memory computing means the
computation occurs directly within
memory cells, using phase-change
memory or RRAM, eliminating the
need to shuffle data out of memory
for processing.
The challenges of analog AI
processing
This is not without its challenges,
which include:
Precision and noise
Analog signals are susceptible to
noise and non-repeatability due to the
variable values within the tolerance of
electronic components. Thus, a calculation won’t necessarily give the same
result every time, although it will be
close enough for some purposes. Digital computers in contrast are precise
and repeatable.
Programmability
Software development tools for
CUDA (NVIDIA’s programming model)
have been in development for decades.
siliconchip.com.au
Whole new software suites have to be
developed for analog computing; companies like IBM have open-sourced
toolkits such as aihwkit (https://github.
com/IBM/aihwkit) to ease the transition.
close to a large source of power, and
the electrical grid doesn’t have to be
extended to accommodate it.
Circuits for modern analog AI
• Optical components in photonic chips; microLED arrays for light
sources to represent the input vector
or neural network activations; spatial light modulators to store neural
network weights and perform multiplication with incoming light; photo-
detector arrays to convert light signals
back into electrical signals for further
processing; and photonic waveguides
as conduits for light that steer and
manipulate it to perform mathematical operations.
• Phase change memory – described
in the IBM entry later.
• Resistive RAM (RRAM) – the
practical implementation of a technology that uses memristors to store
information.
• Switched-capacitor arrays –
described in the EnCharge entry later.
We will now look at some modern
experimental or commercial chips
analog computing chips and systems.
Key electronic components in modern analog AI chips are:
Hybrid necessity
• Analog-to-digital converters
AI systems involve two main
(ADCs) and digital-to-analog convertphases: training and inferencing.
ers (DACs) to interface between the
Training is the computationally digital and analog worlds.
expensive phase where a model (gen• Calibration circuits, to mitigate
erative or discriminative) learns pat- the natural variability in analog comterns from massive data, often requir- ponents, noise and thermal drift.
ing hyperscale data centres. Infer• Field programmable analog arrays
encing is the computationally lighter (FPAAs) – more on these later.
phase, where the trained model is used
• Ferroelectric devices (emerging) –
on new inputs to produce outputs, these use ferroelectric materials where
eg, answering questions, generating the polarisation state can be switched
images, or classifying objects.
to modulate conductance or capacThe two major model categories are itance, enabling non-volatile analog
generative models, which create new weight storage.
content, and discriminative models,
• Floating-gate transistors – stanwhich make decisions or classifica- dard transistors with a ‘floating’ gate
tions.
that traps a variable amount of charge,
While analog computing excels at storing information. This charge modACCEL
siliconchip.au/link/aca7
edge AI inferencing (eg, on smart- ulates the transistor’s conductance,
The All-analog Chip Combinphones or IoT devices) and lower- allowing precise analog storage of neu- ing Electronic and Light computpower tasks, it is not yet suitable for ral network weights. They are used in ing (ACCEL) is an experimental
hyperscale training.
flash memory, such as by Mythic.
photonic-
electronic chip from ChiA full switch to 100% analog is
• Gain cells (emerging) – a type of na’s Tsinghua University, announced
speculative; a hybrid digital/analog memory with two or three transistors in 2023. It is claimed to classify highapproach is a possible short-term path. and possibly a capacitor that can store resolution images over 3000 times
In a hybrid system, a digital processor a variable amount of charge represent- faster and with up to four million times
handles logic and control, while ana- ing the stored information.
less energy than state-of-the-art GPUs
log accelerators do the maths.
• Memristors – resistors with a like NVIDIA’s A100.
memory. Their resistance depends on
An input image is processed in the
The AI scaling crisis
the amount of charge that has flowed optical domain for feature extraction;
This is the realisation that simply through them in the past, so the resis- the resulting light field strikes a phoadding more data, computing power tance can be adjusted to the desired todiode array, converting it to phoand electrical energy to AI models value.
tocurrents that feed directly into an
will hit physical, economic and practical limits. AI-driven data centres use
Ternary computing
so much electricity that the availabilTraditional digital computers use ‘binary’, with memory cells and logic lines
ity of electricity in specific regions
(‘bits’) being in one of two states (0 or 1). In contrast, analog computers operis the limiting factor, not chips. As
ate with a continuum of values.
a result, companies like Amazon are
An intermediate concept is ternary logic, which uses three possible states
purchasing nuclear-powered data
for
a bit or ‘trit’, typically -1, 0, +1. They could be encoded electrically as (for
centres.
example)
0V, half supply and full supply, or even active low, high-impedance
There is also the problem of ‘plaand active high.
teauing intelligence’. Simply increasOne of the earliest examples was Thomas Fowler’s mechanical ternary caling the AI model size does not result
culator
in 1840. The first electronic ternary computer, Setun, was built in the
in much increase in reasoning ability.
Soviet
Union
in 1958 by Nikolay Brusentsov. Fifty units were produced until
Also, the AI industry is running out of
1965. It was a remarkably balanced and efficient design that unfortunately
high-quality data to train models on.
lost out to the mass production of binary systems.
Analog AI computing offers a possible
Interest in ternary computing largely faded in the West due to the domisolution to these problems.
nance
of binary hardware, but like analog computing, it is attracting renewed
We’ve already discussed how
research interest today for much the same reasons as analog, primarily for
analog AI techniques overcome the
its theoretical energy efficiency (fewer state transitions per information unit)
power consumption problem. Another
and potential advantages in certain algorithms.
advantage of this is that decentralisaHowever, practical AI applications remain experimental and far less develtion becomes possible; it will no lonoped than analog or neuromorphic approaches.
ger necessary for data centres to be
siliconchip.com.au
Australia's electronics magazine
June 2026 15
Fig.39: an example of emulating convolutional neural network (CNN) layers
in the optical domain using diffractive layers. Original source: www.mdpi.
com/1424-8220/23/12/5749
electronic analog computing unit for
final classification, all without the
need for an ADC.
The front-end uses diffractive optical analog computing. An input optical
image shines through a series of engineered diffractive layers. Each layer
causes light waves to interfere and diffract in a way that naturally performs
linear transformations (dot products &
convolutions). The final light pattern
at the output plane encodes the result,
with no active electronics involved.
It is completely passive (like a lens),
ultra-fast (limited only by the speed
of light), and consumes almost zero
energy in the optical part. The resulting light field hits a photodiode array,
converting it to analog electrical currents that feed into the electronic analog computing unit for final classification, keeping the entire pipeline analog end-to-end.
Its main advantage is that the diffractive part handles the bulk of the
matrix multiplications passively at
light speed.
The ACCEL chip mimics convolutional neural network (CNN) operations of a digital or modern analog
computer in its optical front-end. This
diffractive optical neural network
(DONN) performs feature extraction
equivalent to convolutional layers in
a CNN, while the electronic analog
backend handles non-linear classification – see Fig.39.
ACCEL is currently specialised for
vision tasks (static images), but could
be scaled to other linear operations.
Anabrid
https://anabrid.com
Anabrid has several analog computing projects. In 2024, it produced their
16
Silicon Chip
ABRGPX1 Anabrid General Purpose
Experimental Test Chip analog multiplier (see Fig.40). It is a test chip for
the upcoming commercial offerings, a
hybrid digital/analog chip that allows
analog capabilities to be integrated
with digital systems.
Anabrid are also the makers of The
Analog Thing, the open source analog computer mentioned last month.
lucidac is a reconfigurable analog/
digital hybrid computer intended for
early adopters and educational purposes. It has suggested uses in robotics,
speech recognition and automotive
electronics – see Figs.41 & 42.
redac (Fig.43) is said to be the world’s
first reconfigurable analog supercomputer. It has six modular clusters with
432 multipliers, 864 integrators, 1728
summation lanes, 124,416 switching
elements and 3456 scaling elements.
It has digital interfaces for programming and control, using the Python
and Jupyter languages.
Its purpose is to solve complex ordinary and partial differential equations,
solve optimisation problems and act
as a testbed for unconventional computing. It is claimed to be significantly
faster than conventional computers
for certain problems and can provide
real-time solutions that are difficult to
achieve with conventional computers.
Uses proposed for anabrid products are real-time flight wing adjustments, motion control in automation
and energy-efficient supercomputers.
Aspinity
www.aspinity.com
Aspinity produces ultra-low-power
analog machine learning (analogML)
chips for always-on edge AI applications. It claims to have produced the
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Fig.40: the Anabrid ABRGPX1 chip
‘floorplan’. Source: https://anabrid.
dev/about/news/2024-09-19-tc01press-release
world’s first fully analog machine
learning chip, the AML100, from
2022.
Its technology processes raw analog sensor data in the analog domain,
detecting relevant events with nearly
no power consumption, waking digital processors only when needed, thus
achieving a 10-20× battery life extension. The chip’s current draw is only
about 20-100µA.
Applications include security monitoring of a parked vehicle using up
to four sensors; monitoring of smart
homes for events such as glass breaking, smoke, carbon monoxide, leaks,
intruders, a baby crying etc; or waking
IoT devices for voice/keyword, vibration, or other movements; all with low
power consumption.
Fig.44 compares conventional
Fig.43: the redac analog
supercomputer, which is used to solve
differential equations.
siliconchip.com.au
Fig.41: the lucidac software editor.
Source: https://anabrid.com/lucidac
Fig.42: the lucidac analog/digital
hybrid computer. Source: https://
anabrid.com/lucidac
monitoring vs monitoring with the
AML100 analog processor. analog AI
inference is used to identify only relevant data to pass on to the digital processor. The avoidance of unnecessary
analog-to-digital conversion saves a
lot of power.
Aspirare Semi
www.aspirare.io
This Canadian company has developed a range of hybrid neuromorphic
AI accelerators using analog compute
cores and digital components. Their
Gen 1, Gen2 and Edge models and are
commercially available.
Blumind
https://blumind.ai
Another Canadian company that
has developed all-analog neuromorphic processors such as the BM110 for
low-power edge tasks like always-on
voice (eg, keyword detection) and sensor processing. The BM110 is in volume production, while the BM210,
intended for video image classification, is scheduled for volume production.
BrainScaleS-2
siliconchip.au/link/aca8
BrainScaleS-2 from Heidelberg
University is part of the EU Human
Brain Project. It is a mixed-signal/
analog-emulated accelerated neuromorphic system using analog circuits
to emulate neuron/synapse dynamics up to 10,000× faster than biology,
with digital connectivity. It is ideal
for large-scale spiking neural network
simulations.
DYNAP-SE2
siliconchip.au/link/aca9
DYNAP-SE2, developed by the
Fig.44: a comparison of the AML100 senses (bottom) with conventional methods
(top). With the AML100, unnecessary analog-to-digital conversion is avoided.
Source: www.aspinity.com/aml100
siliconchip.com.au
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Institute of Neuroinformatics (INI)
at the University of Zurich and ETH
Zurich, is an experimental mixed-
signal neuromorphic chip designed
for real-time, low-power spiking neural network processing. It features
1024 analog neurons, each with up to
64 programmable synapses, combined
with digital event routing for flexible
connectivity.
The chip is reconfigurable, supports
adaptive and learning behaviours (eg,
spike-timing-dependent plasticity)
and operates at extremely low power,
typically below 1mW for many workloads. SynSense markets and sells
related development kits or boards
featuring the DYNAP-SE2.
EnCharge
www.enchargeai.com
EnCharge announced the EN100
commercial accelerator chip in 2025.
It uses analog in-memory computing for high-performance AI applications. In the EN100, neural network
weights are stored in digital SRAM,
while computation is performed by
charging capacitors to various levels
and then connecting them together to
redistribute the charge.
This mechanism avoids the noise
problems of other analog AI designs.
The M.2 laptop chips can deliver >200
TOPS (trillions of operations per second) using just 8.25W of power. There
is a PCIe card version of the processor
for AI workstations that delivers >7.4
PetaOPS of capacity (1000 trillion
operations per second).
Compared to other forms of in-
memory computing (see Fig.45 overleaf), EnCharge claims a superior
signal-
to-noise ratio, compatibility
with standard CMOS 4nm technology
June 2026 17
nodes, broad support for existing AI
models and scalable technology.
IBM
siliconchip.au/link/acaa
IBM is using phase-change memory (PCM) devices for analog in-
memory computing (AIMC). These
are nanoscale resistive elements that
store neural network weights as varying resistance states and perform
matrix-vector operations in-place.
Prototypes include multi-core chips
with tens of millions of PCM cells,
achieving high accuracy on tasks like
speech recognition and image classification while using far less power than
digital equivalents.
In PCM, an electrical pulse is
applied to a material, which causes
heating and changes its conductance
by switching the material between its
amorphous (glass-like) and crystalline phases.
A small pulse results in there being
more crystalline material and lower
resistance. A large pulse results in
The resistance value corresponds to
a neural network weight. The PCMs
are arranged in a crossbar configuration – see Fig.46. This enables analog matrix-vector multiplication in a
single-step as explained before.
Fig.46: IBM’s PCM crossbar
configuration that allows matrixvector multiplication in one step.
Source: https://research.ibm.com/
blog/the-hardware-behind-analog-ai
more amporphous material and more
resistance.
Between pure crystalline and pure
amorphous phases, there is a mixture
of both, representing a continuum of
resistance values between 0 and 1.
Imec
www.imec-int.com/en
They produced the experimental
AnIA (Analog Inference Accelerator) chip in 2020, which uses analog
in-memory compute (AiMC) architecture. The AnIA has reached a high
efficiency of 2900 TOPS per watt for
vector matrix multiplications. The
technology is intended for pattern recognition with tiny sensors and other
edge devices.
Lightmatter
https://lightmatter.co
Lightmatter makes the Envise photonic analog AI accelerator chip,
which is in a late prototype stage. It is
a photonic chip like ACCEL, but while
ACCEL relies on diffractive optics,
Envise relies on ‘Mach-Zehnder inter-
Fig.45: EnCharge’s comparison of traditional AI accelerators, other in-memory computing (IMC) and their own IMC
model. NVM is non-volatile memory, MAC is memory and compute and SNR is signal-to-noise ratio. Source: www.
enchargeai.com/technology
18
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
ferometers’ to perform light manipulation. Also, ACCEL is intended
for research and is not a commercial
product.
Envise has a hybrid design, with
photonic circuits handling the heavy
analog computation and digital silicon
parts managing control, memory (eg,
SRAM) and digital tasks. Lightmatter
has announced a multi-chip package
with six dies, 50 billion transistors,
and one million photonic components
using 3D stacking.
This chip achieves 65.5 trillion
operations per second using just 78W
electrical and 1.6W of optical power.
Microsoft
siliconchip.au/link/acab
Microsoft produced an experimental Analog Optical Computer (AOC)
in 2025. Like the products from
ACCEL and Lightmatter, it is photonic,
although it is not a chip but built with
discrete components. It aims for a 100×
improvement in energy efficiency for
large language models (LLMs).
The AOC combines 3D optics
(lenses, micro-LED arrays) with analog electronics (eg, CMOS sensors
from smartphone cameras) to perform
computations directly with continuous light intensities, bypassing binary
digital conversions and the von Neumann bottleneck.
It excels at massively parallel vector-
matrix multiplications (core to neural
networks) and iterative operations,
using physical properties of light for
addition/multiplication via interference and detection. Nonlinearities are
handled electronically, making it a
hybrid analog-optical design that runs
at room temperature with consumer-
grade parts.
Fig.47 shows a simplified view of
the vector-matrix multiplication unit
in the foreground. This consists of a
linear array of micro-LEDs, a 2D modulator array (using display projectors),
and a linear array of silicon sensors.
Fig.48 shows the actual computer. For
more information, see the video at
https://youtu.be/cswAkdU_6yk
Fig.47: a simplified diagram of Microsoft’s AOC setup. Source: www.microsoft.
com/en-us/research/project/aoc
Fig.48: Microsoft’s AOC computer. Source: https://news.microsoft.com/source/
features/innovation/microsoft-analog-optical-computer-cracks-two-practicalproblems-shows-ai-promise/
An analog computer kit from 1961
An article from Popular Electronics describes two simple analog computer kits,
one from Edmund Scientific (Figs.49 & 50) and one from General Electric, both
available in 1961. You can read it at siliconchip.au/link/acah
The Edmund Scientific computer, based on a voltage divider circuit using
three potentiometers, is described in more detail at siliconchip.au/link/acai
That page describes how to build your own, with modern components;
there is even a file
to download for
the front panel
and potentiometer discs.
Mythic
https://mythic.ai
Mythic produces the M1076 Analog Matrix Processor (Fig.51), a single-
package analog AI accelerator. It is
designed primarily for edge AI inference (running trained neural networks
efficiently on devices like cameras,
drones, robots or servers with low
power consumption).
Figs.49 & 50: an original
Edmund Scientific analog
computer kit and matching
circuit from the 1960s.
Source: www.servomagazine.
com/magazine/article/
alternative-computingmodels-part-3-electronicanalog-computing
siliconchip.com.au
Australia's electronics magazine
June 2026 19
Fig.51: the Mythic M1076 on an M.2 card, the same format used for many
modern plug-in solid-state storage drives. Source: https://mythic.ai/products/
mm1076-m-2-m-key-card
Fig.52: the operation of a Mythic AI processor. X and Y are row and column
addresses. Original source: https://mythic.ai/technology/analog-computing
It delivers up to 25 TOPS while typically consuming only 3-4W (a comparable GPU might use hundreds of
watts). The chip can store about 80
million weight parameters onboard
and performs computations without
external memory.
The M1076 contains 76 tiles (small
chips inside the main package) each
comprising one Analog Compute
Engine (ACE). Each ACE has an analog flash memory array that stores neural network weights as varying resistances, and it performs matrix multiplications in-memory, using physical
currents with low power consumption
and at high speed. ADCs read out the
results precisely.
Each ACE has a small digital subsystem for support: a 32-bit RISC-V
processor (for control/tasks), a SIMD
(single-instruction, multiple-data) vector engine (for non-matrix ops), 64kiB
of SRAM (local scratchpad) and a network-on-chip (NoC) router (to connect
tiles efficiently).
The flash memory cells are used as
tuneable resistors to store the weights
of a neural network. This can be
achieved by controlling the charge
stored in each cell. Input data is represented by voltages across the memory cells (in rows).
These voltages across a known resistance produce a current determined by
Ohm’s law, the product of the input
voltage (the data) and the neural network weight.
By summing all currents in a column, a vector-matrix multiplication
can be performed. The result of the
matrix multiplication is then read with
the ADC (see Fig.52).
Neurogrid
siliconchip.au/link/acac
Neurogrid from Stanford University is a mixed-signal experimental
20
Silicon Chip
multichip neuromorphic system capable of simulating one million neurons
and billions of synaptic connections in
real time with very low power (about
3-5W).
It is primarily used for large-scale
brain simulations and employs analog computation to emulate synaptic connections and neuron dynamics. It is a landmark example of early
mixed-signal neuromorphic hardware
from around 2014.
NeuRRAM
siliconchip.au/link/acad
NeuRRAM from UC San Diego/
MIT is an experimental neuromorphic mixed signal analog computein-memory chip using resistive RAM
(RRAM) for energy-efficient AI inference on edge devices.
It runs a wide variety of AI tasks
(eg, image classification, speech recognition and reconstruction) directly
in memory with far less power than
traditional methods.
Okika
https://okikadevices.com
Okika acquired Anadigm and now
produce field-programmable analog
array (FPAA) chips (see Fig.53).
These are not specifically designed
for analog computing but can be used
for such. FPAA chips contain configurable analog blocks like op amps,
differential amps and programmable
capacitor arrays that can
be programmed as
capacitors or resistors.
Fig.53: an
FPAA from Okika
Devices mounted on
a PCB. Source: https://
okikadevices.com
Australia's electronics magazine
A capacitor can emulate a resistor
by switching it at high speed with two
transistors or some other technique.
This technique is called switched-
capacitor resistor emulation.
These chips can be used for sensor
interfacing, audio processing, industrial control and low-power analog
computing. They are the analog equivalent of a field programmable gate
array (FPGA). There are a large number of analog components available
for programming from the FlexAnalog FPAA Design Library – see Fig.54.
Peking Uni
siliconchip.au/link/acae
Peking University announced a prototype analog AI chip using resistive
random-access memory (RRAM). It
achieved high accuracy with 24-bit
precision (comparable to 32-bit
floating-
point digital systems) and
claims 1000× faster speed and 100×
less energy consumption than digital
AI computing.
Sagence AI
www.sagence-ai.com
This Silicon Valley company has
developed analog in-memory computing chips, particularly for large generative AI models like Llama2-70B. The
chips are currently in the customer
evaluation phase.
SynSense
www.synsense.ai
A leading manufacturer of ultralow-power mixed-signal neuromorphic chips and sensors, targeting edge
applications such as audio processing and keyword detection, gesture and scene
recognition, wearables,
bio-signal analysis (eg,
ECG, EMG, breath, and
gait), behavioural monitoring, smart toys, home automation, security systems, industrial
siliconchip.com.au
Fig.54: the many different design elements that can be programmed into Okika FPAA, from the FlexAnalog FPAA Design
Library. These include filters, op amps, differential amps, sample-and-hold circuits, differentiators, integrators and more.
Source: https://okikadevices.com/collections/an231e04-reconfigurable-flexanalog-fpaa-chip-with-4-cabs
testing, robotics, drones and more.
AI research in Australia
UWS Deep South (siliconchip.au/
link/acaf) is a neuromorphic computer
to simulate the human brain, but is
entirely digital and uses FPGAs.
Conclusion
We have traced the development of
analog computing from its mechanical origins through the electronic era,
siliconchip.com.au
followed by a long period of dormancy
as digital computing came to dominate.
Today, we are witnessing a modern
revival driven by the need to overcome
digital computing’s limitations, particularly its high power consumption for
AI workloads.
The dramatically lower power
requirements of analog and analog-
inspired AI systems open the door to
intelligent local ‘edge’ devices, such
as smartphones and sensors. If these
Australia's electronics magazine
technologies fulfil their potential, they
could usher in a new golden age of efficient, brain-like computing.
For anyone interested in learning
more about analog computers, we recommend checking out the two links
below:
• An analog computing book collection: siliconchip.au/link/acaj
• Introduction to Analog Computer
Programming by Dale I. Rummer:
SC
siliconchip.au/link/acak
June 2026 21
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Part 1: introduction and overview
T
Machine
Have you ever wanted to build your own pinball machine
with a custom layout, artwork, sounds and lighting? It
might seem like a daunting project, combining electronics,
mechanics and software. In this series, we show how to
design and build every part at home, from scratch!
his major project, presented
over the next few issues, will provide you with all the pieces to make
your own pinball machine. You can
pick and choose all aspects of it and
‘roll your own’ by 3D printing. Not
only does that make it incredibly customisable, it avoids the expense of
buying commercial pinball machine
parts. They can add up fast!
It seems like just a few months
ago that I was talking with our most
esteemed editor and asked what he
thought a fun project would be. His
answer was somewhat unexpected:
a pinball machine. My immediate
response was, “Sure, why not. I always
wanted to build one of those as a kid.”
I should have reflected on the reasons why I never went ahead with that
before. In retrospect, that was a bit of
a “... hold my beer” moment!
The technology in a pinball machine
is not advanced, but it is definitely in
the complex electromechanical world.
There are some very substantial forces
involved in many of the mechanisms
on a pinball deck, and controlling
them reliably is not easy. There is a lot
of electrical sensing and control, and
therefore (in old-school machines, at
least), a lot of wiring.
Make no mistake, if you decide to
follow my lead, you will be embarking
on a major project, and there will be a
lot of work. However, nothing about it
is really difficult, especially since we
have already done much of the hard
work. We will be presenting triedand-tested electronic and mechanical designs.
Critically, you will be able to download some files and start printing tested
and verified 3D parts immediately.
While the PCB and wiring are superficially impressive, the majority of the
effort in this project has gone into realising a DIY-friendly approach to making the critical kickers, flippers, targets
and bumpers.
Of course, it is possible to buy parts
to make a pinball machine; however,
they are excruciatingly expensive.
Also, many of the parts on the market
are second-hand, which introduces
reliability concerns.
So what we did was draw on some
experience and skills in 3D printing
to bring more of a DIY approach to
this project. That keeps costs down,
as does using a Raspberry Pi Pico 2
microcontroller module as the ‘brains’
of the system.
Australia's electronics magazine
siliconchip.com.au
Phil Prosser’s Phenomenal
Pinball
26
Silicon Chip
This also means that should anything break in the future, it will be
easy to repair. Simply print a replacement part, swap it in, and away you
go! We could even see Silicon Chip
readers making and sharing their own
elements to enhance this new ‘pinball
ecosystem’.
Don’t get the impression that following my instructions will completely
remove the need for mechanical skills.
Still, you will be making parts that
we (and you) know will work when
assembled and wired correctly.
We spent a lot of time simplifying
the wiring, with ribbon cables for most
of the lights and sensors, and a control
board that is ‘plug and play’. This was
an attempt to keep the inevitable spaghetti wiring manageable!
We will present all the component
parts required for a decent pinball
machine, including:
Flippers
Bumpers (that kick radially)
Kickers (that kick outwards)
Targets
Rollovers (which detect the ball
passing over)
Loader and ball release
A range of lighting parts
A scoreboard
A control system and a power
supply
You will be able to use some or all of
the parts we used. You may decide to
make more or fewer of some of them,
or make your machine larger or smaller
than ours.
Before deciding if you’re going to
build your own pinball machine, you
will probably want to see what ours
looks like and how it is to play. To
that end, in addition to the photos in
this and the following articles, we also
have several gameplay videos you can
view at the following link: siliconchip.
com.au/Video/Pinball1
The controller includes more
self-testing functions than we would
normally include, allowing you to use
a computer to monitor the state of the
machine and test every component.
So, we have some pretty solid built-in
help for debugging. In a complex system like this, you want to be confident
that you can track down any problems
that arise.
In addition to electronic and electromechanical parts, we will also provide
several 3D-printable deck sections,
especially around the reloader and
ball release, which we think is pretty
📍
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siliconchip.com.au
cool. You don’t have to use these if
you don’t want to; you may prefer to
do some woodworking instead, or flex
some of your other skills. The controller won’t care.
So, you can make a deck that suits
your needs; you don’t need to copy
ours (but you certainly can if you want
to!). We have included all the Fusion
360 CAD files in our download section,
so if you want to modify these parts,
you can do so. This software is free for
non-commercial (hobbyist) use.
The defining aspects of a pinball
machine include a spring-launch
mechanism and a playfield with obstacles and targets. Hitting the targets
increases your score. The game ends
when the ball goes into the ‘gutter’ a
few times (usually three).
Variants of the pinball game with
these features have been
around since the 1700s. In
the 1900s, more complexity was added, including
flippers and a coin operation mechanism, allowing
pinball to become a commercial game.
Post-WWII (the early
1950s) saw the widespread
introduction of electrification and automated flippers, with the familiar
placement of flippers near
the bottom of the deck,
allowing longer play and better control of the ball.
Through to the mid1970s, all pinball
machines remained
electromechanical devices utilising relays for
control and
capturing
scoring.
In the
mid-1970s, microprocessors were
introduced, which enabled much more
complex lights, sounds, scores and
other functions.
My rash promise to the editor was
to bring the essence of this very long
history of the game together into a
project that you can make yourself. As
implied above, you will be able to ‘mix
and match’ and even customise our
part designs into your own creation.
As a final comment, this collection
of the controller, electromechanical
parts, example deck and software
will do a lot of your heavy lifting.
Even so, building a machine is a substantial undertaking. Keeping an oldschool pinball machine operational
is a very technical job, and building
one from scratch inevitably has some
tricky parts.
Photo 1: the
general layout
of the Pinball
Machine.
It’s highly
configurable;
you don’t need to
do everything the
same as us. You
could have more
or fewer bumpers,
kickers, LEDs and so
on. It’s designed to be
flexible, to suit your
idea of how a pinball
game should work.
June 2026 27
Fig.1: the system block diagram.
Inputs are shown with red lines
and outputs with blue. All inputs
are active-low inputs, some from
open-collector inductive sensors
and some from pushbutton
switches and microswitches.
The outputs are direct drive for
the 7-segment displays, opencollector outputs for the LEDs
and open-drain Mosfet outputs
for the high-power devices.
For those of you with an artistic bent
(or who know people with such skills),
this will be an opportunity to let your
creativity loose. We have made basic
decorations for our machine, but we
are sure that you, the reader, will come
up with something even more unique!
For those with a software background, we are also providing the full
Visual Studio code, so you can hack
into it and change the logic, tunes,
sound effects, light sequences and
whatever else you want. The world is
your oyster.
Let’s start with the system block diagram, shown in Fig.1.
The central Control Board is a
hefty 246.5 × 240.5mm, loaded full of
through-hole parts. None of these are
remotely fancy; the Raspberry Pi Pico
2 is the only high-tech part.
This board has inputs for all buttons
and sensors, LED drivers for the displays (a mix of 7-segment displays and
individual LEDs), 12 Mosfet outputs
that can drive very heavy loads, and
interfaces for inductive proximity sensors. For the LEDs, the 7-segment displays are driven directly by 74HC595
serial-to-parallel registers, while individual LEDs have bipolar transistor
buffers to handle higher currents.
28
Silicon Chip
All the inputs and LED connections are via 10-way ribbon cables,
which run to small breakout boards
local to where the LEDs and inputs
are (see Photo 2). This simplifies the
wiring considerably, as you can crimp
a 10-way IDC ribbon connector in seconds using a vise or (ideally) a dedicated crimping tool.
All power outputs are via pluggable headers using figure-8 cables. We
used cheap speaker cable. This all
operates at 24V DC and up to 6A, so
we can’t use lightweight connectors.
We recommend pluggable screw terminals, which again are quick and
easy to assemble. If you are tempted to
solder these wires to the board, have
a bit of a think about servicing this
machine later.
Australia's electronics magazine
We found the best arrangement
was to have the power supply and
controller behind the main display,
with ribbon cables and high-current
cables running from there to breakout
boards at your sensors and effectors –
see Photo 2.
The Control Board is busy, as you
can see from Photo b1 overleaf.
Top deck
We 3D printed the entirety of the
top deck. We did this because we
could dream up a rather complex layout, print it, try it, then tweak it so the
game played better. The flippers can
drive the ball in a range of angles, for
example we wanted to have interesting things happen fairly often, so we
moved the bridge entry to the left of
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3D-printed Electromechanical Parts
Here’s an overview of the critical
parts of the pinball machine that
can be 3D-printed using files you
can download from our website. In
addition to the printed parts, some
standard hardware is used (screws,
nuts, washers etc) plus, depending
on the part, pre-made switches,
solenoids and other bits and pieces.
1. Flippers (Photo a1) – these are
the way the user interfaces with the
ball. They’re positioned near the
bottom of the machine and pivot
upwards when the user presses a
button. If timed correctly, they will
fling the ball up as it passes near
them into the location desired by
the user. If timed incorrectly, the
ball may go somewhere you don’t
want it – including in the gutter at
the bottom, ending your turn. They
use two solenoids to give enough
speed and power to kick the ball
properly.
Photo a1: one flipper; a pair of these are
what the player uses to move the balls
around the deck and (hopefully) score
points while avoiding the ball falling
down the bottom, ending their turn.
Note that this flipper is missing its
rubber band.
2. Bumpers (Photo a2) – these
are circular objects on the deck that
detect when the ball hits them and
push it away rapidly (driven by a solenoid). They make noise, flash lights
and cause the ball to ping around rapidly, making the game much more
exciting.
3. Kickers (Photo a3) – these are
positioned touching a flexible band. If
the ball hits the band, that is detected
by a switch and the kicker then
pushes the band out, causing the ball
to fly away. They’re a bit like bumpers
except they operate semi-linearly,
rather than radially.
4. Targets (Photo a4) – these are
basically labelled switches that
detect when they are hit by the ball,
usually increasing the player’s score.
They’re typically placed against the
side of the machine, where the player
can fling the ball (if they have sufficient skill).
siliconchip.com.au
5. Rollovers (Photo a5) – these
are designs drawn on the deck with
a corresponding inductive sensor
underneath. The machine detects
when the ball rolls over the image,
increasing the score or having
some other effect.
Photo a2: bumpers like this
are scattered (or clustered)
around the deck, giving the
ball a little boost while
flashing lights and
making noises (and
possibly adding to the
score).
Photo a3: kicker(s) work
somewhat similarly to
bumpers but in a more linear
fashion. They’re usually
attached to taut bands that
push the ball away when the
kicker moves them.
where it started and moved the targets
up the deck.
Making a ball game with a bridge is
the one thing I wanted to do as a kid.
You will probably form your own
opinions on the layout; there is nothing stopping you from moving stuff
around. Mind you, by the time we
were satisfied with our layout, the
sales staff in our local electronics shop
were convinced we were 3D printing
a battleship!
While we used Fusion 360 to design
all our parts, for those at the start of a
3D modelling journey, there are much
simpler tools like Tinker-Cad that you
could start with. Our experience is that
you need to be willing to try different
versions of the overall layout until you
find one that plays well.
Photo a5:
inductive
sensors
mounted under
the deck form
‘rollovers’,
which can add
to the score or
trigger other
actions. The
zones are
indicated on
the deck with
decorations
like circles or
starbursts.
Photo
a4: aim the
ball perfectly
at these targets for
bonus points! They’re
illuminated and trigger
microswitches when hit.
Photo 2: the machine’s wiring is greatly simplified by using 10-way ribbon cable
for most runs. Breakout boards at the far end make it easy to connect to LEDs,
inputs and so on.
Australia's electronics magazine
June 2026 29
Electronic Parts
The Pinball Machine uses more
than a dozen boards, most of them
breaking out ribbon cable connections to simplify the wiring.
1. Control Board (Photo b1) – this
hosts the Raspberry Pi Pico 2 and a
lot of I/O. It senses all the switches
and other inputs, then makes decisions to take action, triggering various outputs like LEDs and solenoids. It also keeps score, keeps
track of the current player, and controls the flippers and ball launching
mechanisms.
2. Power Supply (Photo b2) – the
whole machine is run from a 24V
DC 5A ‘brick’. This board derives +5.5V
and +3.3V rails from the incoming
24V DC, then distributes all three rails
to the Control Board.
3. Player & Score Displays (Photo
b3) – these are mounted on the backboard and show the current player
number and their score. They connect
to the Control Board with one 10-way
ribbon cable per digit and are driven
from 74HC595 IC outputs with current-limiting series resistors.
4. Cascade & Bumper LED Boards
(Photo b4) – these simplify the construction of groups of LEDs that shine
through small windows on the deck.
They connect back to the Control
Board via one or two 10-way ribbon
cables for each assembly.
5. Bumper & Kicker Interface
Board (Photo b5) – this connects
up to three bumpers and two kickers to the Control Board. Placing it
near those devices simplifies the
wiring. It connects the switches
back to Control Board inputs via
a 10-way ribbon cable, with additional figure-8 cables for each solenoid.
6. Power Distribution Board
(Photo b6) – this makes it easy to
connect multiple solenoids or other
Photo b1: the Control Board. It’s a bit of a monster, but all the parts are
cheap, commonly available and easy to solder. In a sense, it’s just a
Raspberry Pi Pico 2 with a lot of I/O.
Photo a1: one flipper; a pair of these are
what the player uses to move the balls
around the deck and (hopefully) score
points while avoiding the ball falling
down the bottom, ending their turn.
They’re driven by two solenoids each to
give good ball acceleration!
Photo b2: the power supply
simply derives 3.3V and
5V DC rails to power the
Pico 2, LEDs and so on
from the 24V supply. It
also passes the 24V
supply through to
power the solenoids
and audio amplifier.
The final version moves the
output connectors to align with
those on the Control Board.
Photo b3: the current player and score
displays are simple
7-segment LED digits
mounted on a PCB.
The current-limiting
LEDs are on the
Control Board.
If your woodworking skills are
strong, you could start by making
much of the deck out of timber, such
as plywood. That may make it easier
to experiment. You can either paint
it to get a good finished product, or
replace pieces with 3D-printed plastic parts once you have finalised the
configuration.
Bite-sized chunks
There are quite a few parts to this
project, which we will describe in sections. This article presents the overview and how it all comes together,
the architecture and top-level software
description.
Over the next couple of months,
we will describe the electronic modules and provide parts lists along
30
Silicon Chip
with assembly and testing instructions. That will include the controller and I/O board, plus several other
related parts
If you’re planning to build the Pinball Machine, that will give you time
to gather the components and start getting the electronics up and running,
which will help with testing the electromechanical parts later.
Once all the electronic parts have
been described, we will provide the
3D printing files and describe how
to put those parts together. That will
include the electromechanical parts
such as the kickers, flippers and suchlike. You can make these ‘standalone’,
purchase commercial versions, or even
design your own.
When all the parts have been fully
Australia's electronics magazine
explained, we’ll give more details on
our example layout for the machine
we built. This allows us to present
how to bring this lot together; we hope
inspires you to develop your own deck
layout, artwork and gameplay.
That means the construction details
for this new Pinball Machine will be
spread out over the next few issues,
finishing before the end of the year.
Pico 2 software
The processing is all done by the
Raspberry Pi Pico 2. We gravitated to
this as it is so easy to use, powerful
enough for the job, and inexpensive
too. The design does need to grapple
with somewhat limited I/O, but by
normal standards, the Raspberry Pi
has plenty.
siliconchip.com.au
higher-power devices to a single
output on the Control Board.
7. Rollover Interface Board
(Photo b7) – this simplifies the
wiring to inductive rollover sensors, allowing up to eight to be connected to the Control Board via a
single 10-way ribbon cable.
8. Input & LED Breakout Boards
(Photo b8) – these simplify wiring
to switches and LEDs, allowing up
to eight of each to be wired back
to the Control Board via a single
10-way ribbon cable. The three-pin
headers are for inductive sensors,
like with the rollovers.
Photo b7 (above): this board makes it easy
to connect up to eight inductive sensors
to the Control Board via a single ribbon
cable. Use more than one if you want
more than eight rollovers!
Photo b5 (lower left): this board provides a local
connection point for the wiring of up to three bumpers
and two kickers. All the inputs go to the Control
Board via a single ribbon cable, while the
solenoid drive comes from the Control Board via
one figure-8 wire per bumper/kicker.
Photo b6 (lower right): this allows you to
connect several high-current devices to
simplify the wiring. These are straightthrough connections with added flyback
diodes.
Photo b4 (above): these
boards arrange 15 and
8 LEDs, respectively,
and connect them back
to 10-way header(s)
for connection to the
Control Board. Much
easier than wiring them
by hand!
The software is essentially a state
machine. There are two main modes:
normal operation and Self-Test. If you
hold the TEST button while it is booting, the machine goes into the Self-Test
mode; otherwise, the system boots into
normal operation. The software structure is shown in Fig.2.
After normal initialisation, the system goes into the Idle state, monitoring
the coin, player add and start inputs.
The coin input can be a simple push
button, but if you want to be a little
bit fancy, you could create a coin slot.
All it needs to do is pull the coin input
low each time a coin is sensed.
Once “Start” is pressed in the idle
state, and assuming you have sufficient credit, the machine moves to
the RunGame state. The system runs
siliconchip.com.au
Photo b8: these three input and LED
output breakout boards simply break
out the eight connections on the
10-wire ribbon cable to eight separate
polarised headers for easy wiring and
maintenance.
Photos 4 & 5: the adjacent photo
gives an idea of what the wiring
is like on the underside of the
Pinball Machine.
The photo below and right is an
expanded view of the Control
Board wiring that is shown in
Photo 2.
Fig.2: the software has two main
modes: test mode and normal
gameplay. The code is written in
Visual Studio C, and does nothing
tricky, so most software-conversant
people should be able to modify it.
a loop that looks at all the inputs and,
depending on changes to any inputs,
triggers the required action:
For the flipper, kicker, bumper
and reload mechanism sensor inputs,
this action is to trigger the associated
solenoid for the required time, then to
return to an idle state. Scores are incremented for some of these. The flippers
are a little different; if the player holds
these, the system continues to generate a solenoid output but with a lower
duty cycle using pulse-width modulation (PWM) – there will be more on
why that’s necessary later.
For targets and rollovers, this
action can be to light up LEDs and to
increment scores.
Sounds are triggered by these
inputs or time passing.
Because the majority of the pinball
machine is fairly one-to-one causal
input-to-output, you don’t need to use
all the inputs or outputs. You have
great flexibility in how you build your
machine.
We provide the source code as part
of the download, so if this is your
thing, you can modify the software to
make it your own. Indeed, we encourage this. If you make something cool,
please let us know and share it!
Once the player loses and the ball
📍
📍
📍
32
Silicon Chip
is sensed in the reloader mechanism,
the system preloads the ball using
a solenoid, and the player number
increments. The system indicates the
player whose turn it is on the main display and provides their score. Players
have a total of three balls (programmable) and they take turns for each
of their three balls in round-robin
fashion.
In the GameOver state, the system
presents the score for each player in
turn. Once this cycle completes, the
system returns to the Idle state.
We will describe the significant selftest capabilities of the software later,
after we’ve built some of the hardware.
During construction, this is probably
the most important part of the code.
Software development
The Raspberry Pi Pico add-on for
Visual Studio is a joy to use. Coming
from a hardware engineer who turns
the air blue every time software has to
be written, this is high praise. While
this author has generated many lines of
code for this and other projects, every
time I write code, it is an exercise in
learning (and patience!).
The Pi development add-on to
Visual Studio with AI assistance is
truly a generational step forward, and
Australia's electronics magazine
we encourage you to look inside the
code and give it a crack. The best outcome is your own awesome machine,
and the worst is you revert to the baseline code.
Control Board
The Control Board carries a lot of
parts but is not that complex. Its heart
is the Raspberry Pi Pico 2, mounted
via a pair of headers. There is a small
power interface and an audio section.
The remainder is all buffered inputs
and outputs (I/Os). This is required for
the sensors and outputs such as LEDs
and solenoids.
The Control Board has six main
functional areas, as per Fig.3. These
sections are also delineated by silkscreen ink on the actual board; we will
describe in general how the Control
Board works below.
Sensor inputs: the Controller monitors all inputs, including user controls
like the flipper buttons, coin slot, start
button and such. At the same time, it
also watches gameplay inputs such
as target sensors, rollover sensors and
mechanism sensors on kickers and
bumpers.
State changes on these inputs trigger actions. This includes changes
in the state of the game, the score
siliconchip.com.au
Pinball Machine Kits
Note that we are supplying partial
kits for this project, primarily
for the Control Board and Power
Supply - see the Online Shop on
page 86 for details.
and controlling outputs. The outputs
affected might drive lights, bells, LEDs,
or more active outputs like flippers and
kickers. This would be really easy were
it not for the sheer number of inputs
and outputs.
Low-power outputs: there are 40 of
these, for driving the 7-segment LED
displays that show the current player
and score. They can source or sink
about 8mA each.
Medium-power outputs: there are
64 of these to drive LEDs for effects
spread around the playing area. 16 of
these sink around 30mA for driving
white LEDs, while the other 48 sink
around 20mA for red LEDs. You could
change the current limit mix to suit
your machine.
High-power outputs: these are for
driving solenoids and such, supplied
from 24V, at up to an amp or more
(although the 5A power supply limits
the total current and thus the power
of all loads).
Control and audio section: this
includes the Pico 2, a ‘heartbeat’
LED and the audio amplifier, which
is driven from a PWM output on the
Pico 2.
Power supply interface: the separate Power Supply Board does all
the heavy lifting here. The six-way
siliconchip.com.au
power connector on the Control Board
matches that on the Power Supply
Board.
How will it all come together?
The Control Board has a six-way
pluggable connection to the power
supply. There are seventeen 10-way
IDC-style box headers for the inputs
and LED outputs, and twelve high-
current outputs to the solenoids and
high-power devices via two-way pluggable terminals.
The Control Board normally lives
in the backboard cabinet on a pinball
machine. The I/O wiring runs from
this to distributed local boards, either
for direct presentation of LEDs or local
wiring to the sensors.
By using lots of 10-way ribbon cables
with IDC connectors at each end, we
keep the wiring much simpler and
neater than if single-wire spaghetti ran
everywhere. That means your job will
be much easier in building it. An initial prototype we built without using
this system, instead using crimp connectors on individual wires, turned out
to be quite annoying to build.
Next month
In the next issue, we will start by
building the electronics, starting with
the Control Board, then the Power Supply and the other electronics. After
that, we will walk readers through
the construction and testing of the
bumpers, kickers, flippers and other
3D-printed parts. Then we’ll get to the
fun bit – putting it all together into a
cohesive game!
Finally, overleaf you will find the
part lists for all the electronics. If you’re
keen to build the Pinball Machine, start
gathering them and we’ll have the conSC
struction details next month.
Fig.3: the six main functional blocks of the Control Board, which you will find
outlined on the board itself.
Australia's electronics magazine
June 2026 33
Parts List – Pinball Machine Electronics Modules
Control Board (one required)
1 double-sided PCB coded 08107261, 246.5 × 240.5mm
17 2×5-pin boxed IDC headers (CON1-CON9, CON11-CON18)
4 2-pin polarised vertical headers, 2.54mm pitch
(CON10, CON35-CON37)
1 4-pin polarised vertical header, 2.54mm pitch
(CON20; optional, for future expansion)
12 2-way vertical pluggable terminal blocks, 5.08mm pitch
(CON21-CON28, CON31-CON34)
1 6-way vertical pluggable terminal block, 5.08mm pitch
(CON38-CON40)
2 20-pin header strips (for MOD1)
2 20-pin female headers (for MOD1)
1 SPST momentary PCB-mount tactile key switch (S1)
1 10kW logarithmic taper 16mm single-gang potentiometer (VR1)
Semiconductors
1 Raspberry Pi Pico 2 microcontroller module (MOD1)
4 74HC165 8-bit parallel-to-serial shift registers, DIP-16 (IC1-IC4)
15 74HC595 8-bit serial-to-parallel shift registers, DIP-16
(IC5-IC9, IC11-IC18, IC22-IC23)
1 LM384N 5W power amplifier IC, DIP-14 (IC10)
12 IRLZ44NPBF N-channel Mosfets, TO-220 (Q21-Q28, Q31-Q34)
64 BC338 or similar 100-800mA NPN transistors, TO-92 ▲
(Q111-Q188 ■)
1 3mm or 5mm LED (LED1)
13 1N4004 400V 1A diodes (D1, D21-D28, D31-D34)
64 1N4148 or 1N914 75V 200mA signal diodes ▲ (D111-D428 ■)
■ not all numbers in the range are used
▲ it may be cheaper to buy 100
Capacitors
2 2200μF 35V electrolytic, 7.5mm pitch
4 470μF 25V low-ESR electrolytic, 5mm pitch
1 47μF 16V electrolytic, 2.5mm pitch
1 4.7μF 50V electrolytic, 2.5mm pitch
33 100nF 50V radial ceramic, 5mm pitch
Resistors (all axial ¼W ±5% or better)
1 2.2kW
41 220W
3 100W
1 2.7W
145 1kW
48 150W
16 82W
Power Supply (one required)
1 double-sided PCB coded 08107262, 106.5 × 83mm
1 miniature 5/5.08mm-pitch 2-way terminal block (CON41)
1 PCB-mount DC barrel socket (CON42) [Altronics P0620]
1 6-way vertical pluggable terminal block, 5.08mm pitch
(CON43-CON45)
2 LM2576T-ADJ 3A adjustable buck regulators, TO-220-5
(REG1, REG2) [Altronics Z0589]
2 1N5822 30V 3A schottky diodes (D2, D3)
6 M205 fuse clips (F1-F3)
1 M205 5A fast-blow fuse (F1)
2 M205 2A fast-blow fuses (F2, F3)
2 100μH 3-5A toroidal inductors (L1, L2) [Altronics L6622]
3 2200μF 35V electrolytic capacitors, 7.5mm pitch
2 470μF 35V electrolytic capacitors, 5mm pitch
2 100μF 35V electrolytic capacitors, 5mm pitch
4 100nF 50V ceramic or film capacitors, 5mm pitch
1 3kW ±1% ¼W axial resistor
1 1.6kW ±1% ¼W axial resistor
2 1kW ±1% ¼W axial resistors
Player LED display board (one required)
1 double-sided PCB coded 08107263, 37 × 52mm
1 red common-anode 12.7mm (0.5-inch) 7-segment single-digit
LED display (DISP7) [Altronics Z0191, Mouser HDSP-511E]
1 2×5-pin boxed IDC header (CON107)
Score LED display board (one required)
1 double-sided PCB coded 08107264, 142 × 51.5mm
6 red common-anode 12.7mm (0.5in) 7-segment single-digit LED
displays (DISP1-DISP6) [Altronics Z0191, Mouser HDSP-511E]
4 2×5-pin boxed IDC headers (CON101-CON104)
2 BC338 or similar 100-800mA NPN transistors, TO-92 (Q1, Q2)
2 1kW ¼W axial resistors
12 220W ¼W axial resistors
LED output board (one or more required)
1 double-sided PCB coded 08107265, 49 × 38.5mm
1 2×5-pin boxed IDC header (CON50)
8 2-pin polarised vertical headers, 2.54mm pitch (CON51-CON58)
Bumper LED board (several required)
1 double-sided PCB coded 08107266, 84.5 × 84.5mm
1 2×5-pin boxed IDC header (CON48)
8 5mm ultra-bright clear-lens 20mA red LEDs (LED17-LED24)
[Mouser 941-C503BRCNCW0Z0AA1]
Cascade LED board (one required)
1 double-sided PCB coded 08107267, 89.5 × 99mm
2 2×5-pin boxed IDC headers (CON46, CON47)
15 5mm ultra-bright clear-lens 30mA white LEDs (LED1-LED15)
[Mouser 941-C503DWANCCBEB151]
Switch input board (several required)
1 double-sided PCB coded 08107268, 54.5 × 38.5mm
1 2×5-pin boxed IDC header (CON70)
2 3-pin polarised vertical headers, 2.54mm pitch (CON71, CON75)
6 2-pin polarised vertical headers, 2.54mm pitch
(CON72-CON74, CON76-CON78)
General Input board (one or more required)
1 double-sided PCB coded 08107269, 49 × 38.5mm
1 2×5-pin boxed IDC header (CON60)
8 2-pin polarised vertical headers, 2.54mm pitch (CON61-CON68)
High-current interface board (one required)
1 double-sided PCB coded 08107260, 38.5 × 66.5mm
8 2-way vertical pluggable terminal blocks, 5.08mm pitch
(CON91-CON98)
4 1N4004 400V 1A diodes (D4-D7)
Rollover interface board (one or more required)
1 double-sided PCB coded 08117261, 65.5 × 38.5mm
1 2×5-pin boxed IDC header (CON80)
8 3-pin polarised vertical headers, 2.54mm pitch (CON81-CON88)
Bumper driver board (one required)
1 double-sided PCB coded 08117262, 93.5 × 77.5mm
1 2×5-pin boxed IDC header (CON110)
11 2-pin polarised vertical headers, 2.54mm pitch (CON111-121)
10 2-way vertical pluggable terminal blocks, 5.08mm pitch
(CON131-CON140)
5 1N4004 400V 1A diodes (D11-D15)
3 390W ±5% 1W resistors
siliconchip.com.au
By Steve Mansfield-Devine for PCBWay
The benefits of quality
Inspection Reports
for PCBs
However much you test your product designs, there
will always be factors outside your control that affect
your final product. One of the most important of these
is the quality of the PCBs you receive from your chosen
fabrication house.
A
ll PCB manufacturers make promises about quality control and
standards. It’s crucial for you to know
how well they live up to these assurances. That’s where quality inspection
reports play a vital role – they are the
proof that the PCB manufacturer is
meeting its promises.
Leading PCB fabs commission periodic, independent laboratory testing
of their laminate materials and finished boards. These reports provide
you with peace of mind and are also
invaluable for ongoing process monitoring, quality assurance, regulatory
compliance and certification.
PCBWay has published 14 quality
inspection reports from tests carried
out by Centre Testing International
(CTI), an accredited third-party testing laboratory (see the bottom of
the page at www.pcbway.com/oem/
quality-control.html).
Each examination is carried out
with industry-standard methods so
that customers can compare the results
from fabricators worldwide. This also
makes them directly applicable to
compliance demonstrations for IPC
acceptance standards.
As a product designer or electronics
engineer, you can use these reports to
ensure that the physical hardware of
the end product will conform to your
36
Silicon Chip
stack-up and material set, delivering
the necessary reliability, safety and
longevity.
Thermomechanical tests
For example, it’s essential to know
how boards will respond to heat, both
during assembly and when in use.
The glass transition temperature
(Tg) is arguably the most important
laminate specification for engineers
designing boards that will be soldered
with lead-free processes or that will
operate at elevated temperatures. It’s
the temperature at which the resin
binder in the laminate stops being
rigid, like glass, and changes to a viscoelastic state.
This happens over a transition
range, but the test results are usually reported as the midpoint. The
higher the Tg temperature, the better,
because exceeding it can mean the
board loses dimensional stability and
becomes susceptible to delamination
and mechanical damage.
The common Tg figure for standard
FR4 boards industry-wide is 130140°C. However, PCBWay significantly
exceeds this, with a figure of 169.61°C.
Similarly, time to delamination
(T260, T288 and T300) measures how
long a laminate can withstand a specific temperature before the layers
Australia's electronics magazine
separate. It is a better predictor of
assembly survival than Tg alone.
The most commonly cited specification is T288, which tests the time to
delamination at 288°C. The industry
standard is typically 5-10 minutes for
high-reliability boards, but PCBWay’s
tests show times consistently above
the top end of the scale.
High temperatures also cause
decomposition of the resin in the
board, resulting in loss of mass and
weakness. Most PCB fabricators aim
for a decomposition temperature (Td)
of 325°C, while PCBWay achieved just
over 345°C in its most recent tests.
Related to this is the coefficient of
linear thermal expansion (CTE) – how
much the board will expand or contract for each degree of temperature
change, relative to Tg.
As the laminate is reinforced with
glass cloth, expansion in the in-plane
axes (X and Y) are largely constrained.
However, expansion in the Z-axis (the
thickness of the board) can place significant stress on plated through-holes
(PTH), vias and solder joints under
reflow and thermal cycling, causing
barrel cracking, pad lifting and intermittent open-circuits.
For temperatures below Tg, the typical figure for CTE is 50-70ppm/°C.
Again, PCBWay significantly improves
on this, with a test result of 37.4ppm/°C.
These better-than-usual results
mean much greater safety margins in
both manufacturing and end-use for
PCBWay customers.
Dimensional and structural
integrity
Heat is not the only factor. There are
also mechanical and structural concerns, such as board flatness (bow and
twist), the integrity of inner-layer copper and interconnects, which can be
checked by microsection inspection,
and solder mask adhesion, which is
verified by lattice tests.
These are physical aspects of the
PCB that are often taken for granted.
However, with bow and twist, for
example, any board with SMDs that
has distortion of more than 0.75% can
experience problems such as tombstoning (components that should be
flat on the board sticking up, attached
only at one end) or the failure of solder joints on ball grid array (BGA)
packages.
This is something that needs to be
kept well under control, and PCBWay’s
siliconchip.com.au
tests show twist results of only 0.16%
and bow of 0.12%; well below the
threshold where problems typically
start.
Dimensional tolerance is another
factor that seems simple but can have
subtle implications. You might expect
that the board will be the exact size,
with drill holes in the precise locations, as specified in your Gerber files.
However, all manufacturing processes
have certain tolerances, and you need
to know that these are acceptable for
your design.
The size report covers finished
board dimensions, hole locations, pattern shrinkage or expansion and, in
some cases, layer-to-layer registration.
This helps confirm that the PCB will
fit the mechanical envelope, align with
mounting hardware, suit its enclosure
and mate correctly with connectors,
card edges and components.
In addition to reliability and manufacturing problems, poor sizing can
also create signal integrity and soldering problems.
There can be compliance and certification implications, too. Factors
such as safety spacing – for example,
between high-voltage and low-voltage
sections of the board – need to exceed
the minimum allowed values in the
final product.
Typical industry standards allow a
±0.1mm tolerance for the outline of
the board, ±10% for the thickness, and
±50–75µm for drill position, finished
hole size tolerances and layer registration tolerances.
Electrical and chemical
performance
One key metric that may be on the
minds of many engineers is how well
their boards will stand up to high
voltages.
The voltage resistant test (also
known as the dielectric withstanding
voltage, or hi-pot test) verifies that the
PCB laminate (or solder mask over conductor pairs) can sustain 1000V DC at a
controlled ramp rate of 100V/s for one
minute without breakdown, flashover,
sparkover or excessive leakage current.
It is a simple pass/fail test.
This is an important test for the certification of mains-connected equipment. With medical devices, it’s essential to ensure compliance with Means
of Patient Protection (MOPP) and
Means of Operator Protection (MOOP)
requirements.
siliconchip.com.au
Related to this is the breakdown
voltage. An AC voltage is applied
across the test sample, ramped at
500V/s, until there is a catastrophic
increase in leakage current or visible
arc discharge. It provides an upper
limit to the laminate’s dielectric
strength under AC excitation.
For power electronics designs, such
as motors, uninterruptible power supplies, inverters and other cases where
high-voltage conductors must be isolated on the PCB surface, solder mask
breakdown voltage is a critical parameter. A designer can use these figures
to derive the maximum allowable
electric field strength under the solder
mask and determine the minimum safe
conductor spacing.
Stable layers
A PCB is far from simple. It is a sandwich of laminate substrates, traces and
copper layers. How well those layers
remain together is obviously crucial.
The bond strength is a measure of
laminate-to-foil adhesion quality. Low
adhesion is a risk that manifests as
lifted pads during hand soldering or
rework, delamination under thermal
shock and trace peeling under mechanical vibration—all of which can result
in product failures in the field.
The test measures the force required
to maintain the peeling of a copper foil
from the laminate, the result being the
average of multiple tests. For standard
FR-4 (fibreglass) boards, the general
standard is 100-120N, but PCBWay’s
test samples averaged around 220N.
The bond strength degrades at high
temperatures, which is another reason that having a high Tg value is
important.
Moisture absorption also creates
problems for manufacturing and longterm reliability. For instance, moisture
trapped in the laminate can flash to
steam during reflow, creating internal
vapour pressure that causes popcorning (components flying off), delamination and blistering.
In RF and microwave PCBs, moisture absorption can be a primary
material-selection criterion because
absorbed water changes the laminate’s
dielectric properties. This can alter
controlled impedances, detune RF
structures such as filters and antennas, increase dielectric loss and affect
phase stability, particularly in equipment exposed to humidity or temperature cycling in the field.
When a PCB absorbs water, its mass
increases. The IPC-4101 maximum for
standard FR-4 is a 0.32% increase,
although PCBWay’s figures are four
times better, at 0.08%.
Production quality
There are also tests that relate
directly to the production quality of
the PCB. The first of these is porosity,
an important factor for any board with
a gold surface finish like ENIG (electroless nickel immersion gold), especially those that might be exposed to
harsh environments.
Microscopic pinholes in the gold
surface can expose the underlying
nickel or copper, opening up a pathway for corrosion, possibly leading to
‘black pad syndrome’, causing poor
solder joints and BGA interconnect
failures that may not be detectable
until deployment.
Sample boards are exposed to nitric
acid vapour and then dipped in a
An operator applies solder paste
to a PCB panel using a stencil in
preparation for assembly.
Australia's electronics magazine
June 2026 37
Above: a multi-head automated PCB
drilling machine.
Left: AOI (Automatic Optical
Inspection) of assembled panelised
PCBs.
reagent solution. The latter reacts with
any exposed copper or nickel to produce visible corrosion spots. These
are counted and grouped into three
diameter categories: ≤0.05mm, 0.050.51mm and ≥0.51mm. The lower the
number, the better. PCBWay’s most
recent report shows a perfect result
of zero in all categories.
Finally, the cleanliness test measures the total quantity of ionisable
(ionic) contaminants on the PCB surface. These are the products of flux
activators (organic acids, halide activators), electroplating chemicals, etching solutions and handling contamination. They can result in electrochemical migration (ECM), also known as
conductive anodic filament (CAF) formation and dendritic growth.
In the presence of moisture and a
DC field, dissolved ions move under
electromotive force and form conductive metallic filaments between adjacent conductors, causing leakage currents, intermittent short circuits and
ultimately failure.
The board is washed with a solvent
mixture, after which its conductivity is
measured, the result being normalised
to the mass of salt per unit board area.
The IPC requirement is a figure of
less than 1.0µg/cm2. PCBWay’s report
shows a significantly better value of
0.19µg/cm2. This is the result of a
well-controlled cleaning process and
minimal-residue flux due to high process control standards.
How to use the reports
These reports are not obscure technical documents but tools that exist
to provide real-world data to back up
assumptions engineers must make
during the design process. Engineers
can compare Tg, Td, CTE, thickness,
38
Silicon Chip
dielectric data and weave structure
against their simulation and reliability assumptions about power dissipation, impedance and via life, validating their stack-up assumptions.
Size, bow/twist and micro cross-
section dimensions confirm that the
fabricator can meet the mechanical
tolerances necessary for connectors,
enclosures and heavy components.
The reports also help engineers select
suitable laminates.
The size, micro cross-section, CTE/
Tg, bond strength and cleanliness
reports provide essential data when
seeking to qualify a new PCB or new
supplier, especially in the automotive
and aerospace sectors. The data can
also support reliability assessments
by helping engineers justify assumptions about PCB-related failure risks.
Signal integrity (SI) engineers frequently make use of the water absorption and micro cross-section reports to
be certain that the dielectric thickness
doesn’t vary too much from the design
specification. If it did, the trace impedance may shift, causing signal reflections and data errors in high-speed
buses such as PCIe or DDR4.
OEMs can share these reports
between design, quality and procurement teams to maintain a documented
quality history and to justify changes
in materials or suppliers during regulatory audits. Evidence of such tests
may be required as part of supplier
qualification or periodic audits (for
example, for ISO 9001 quality management documentation).
Even when the final product is in
production, the reports can aid in
ongoing process monitoring. Periodic cross-sections, cleanliness and
bow/twist measurements are used as
process control metrics and logged in
Australia's electronics magazine
inspection reports to show statistical
stability and trigger any necessary corrective actions.
Regulation and certification
Arguably the most significant benefit of these reports is in regulatory compliance and certification. For example,
UL 796 (the Underwriters Laboratories
standard for PCBs) requires fabricators
to track Tg and bond strength.
Automotive and aerospace projects need hard evidence for thermal
cycling, vibration, humidity bias and
high-temperature storage. PCB-level
CTE, Tg, Td, bond strength, bow/twist,
voltage and cleanliness measurements
are key elements in qualification
reports and control plans.
Cleanliness reports are mandatory
for Class II/III medical devices under
ISO 13485. Ionic contamination can
lead to leakage currents that interfere with sensitive bio-signals or, in
extreme cases, affect patient safety.
Similarly, safety standards such
as IEC 62368-1 (IT/AV), IEC 60601-1
(medical) and their UL counterparts
rely on factors such as voltage resistance/breakdown, dimensional accuracy and more to ensure that the PCB
portion of the design is robust.
The micro cross-section report is the
primary evidence that a board meets
Class 3 requirements (such as minimum copper wrap-around at the knee
of a hole) for AS9100 certification in
the aerospace and defence sectors.
Conclusion
For engineers, quality inspection
reports offer confirmation of technical standards. They also provide confidence that the customer’s design will
succeed, which is why PCBWay strives
SC
to exceed industry standards.
siliconchip.com.au
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Test & Measure
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Q 1089
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Human Comfort
Indicator
Whether it’s a couch or the environment, comfort is
often subjective. That is true of temperature, too;
you will feel a lot less comfortable on a warm day
if the humidity is high. Thus, this Human Comfort
Indicator is much more useful than a mere
thermometer because it tells you how hot it feels.
By Tim Blythman
T
his project comes about due to a request
from a magazine contributor. He
said it would be handy to have a device
that shows whether an environment
is comfortable or not, not just the raw
ambient temperature.
While comfort is subjective, this
device deals with parameters that can
be easily measured and quantified. It
is well known that certain combinations of temperature and humidity can
be uncomfortable to humans. Naturally, this can also apply to animals
and plants.
You would have no trouble identifying conditions that feel uncomfortable for yourself, but it’s handy to be
able to put a number on it, so you can
be alerted when others might not be
comfortable. One suggestion we heard
is that the Human Comfort Indicator
would be well-suited to monitoring the
conditions in a greenhouse.
Comfort and dew point
The parameter we are tracking with
the Human Comfort Indicator or HCI
is the ‘dew point’. This is the temperature to which air must be cooled for
liquid water to start condensing from
it. Being a temperature, it is measured
in °C or °F, but it relates to both the
raw temperature and the relative or
absolute humidity.
Let’s look at some theory to explain
why dew point is important.
If you are in a warm environment
that makes you perspire, the dew point
has come into play. As the perspiration
(sweat) evaporates, it cools your skin,
Features
Displays temperature, humidity and dew point
Historical displays for the last day, week and month
Configurable units, display orientation and update frequency
Battery-powered with USB charging for uninterrupted operation
The ultra-low-power e-paper display is unobtrusive and easy to read at a distance
Optional analog (voltage) dew point output
Open-drain alarm output
Specifications
Displays temperature/dew point in °C or °F to the nearest degree
Relative humidity shown to nearest %
Based on the excellent BME280 sensor
Average battery draw of around 300μA gives months of operation on a single charge
Screen update interval: every five minutes
siliconchip.com.au
Australia's electronics magazine
but it cannot cool any lower than the
dew point, since that is the temperature at which the air is saturated with
water. In this case, ‘saturated’ is used
in the scientific sense; it means that
the air is at 100% relative humidity.
Intuitively, as the dew point
approaches the ambient temperature
(due to the dew point rising or the
ambient temperature falling), the relative humidity rises. This can be an
indicator of changing weather conditions such as rain.
You might see some weather forecasts report a ‘feels like’ temperature.
This takes into account the dew point,
as well as factors like wind and sun.
For indoor conditions, the sensation
will be dominated by the dew point.
At very low dew points, evaporation
from the skin increases, which can
cause problems like skin drying out
and cracking.
Important, this is not necessarily
something you would notice, unlike
high humidity. So it’s handy to have
a device that can alert you to this condition, allowing you to do something
like switch on a humidifier.
Table 1 shows some typical ranges
of interest for dew point. It can be
quite subjective; if you live in a tropical area, you may be comfortable at
ranges higher than those suggested.
Measurements
Dew point sensors are not common,
but a figure can be easily derived if
June 2026 43
the relative humidity and temperature
are known. Thankfully, many modern
sensor modules can read both.
Historically, an arrangement known
as a wet-bulb thermometer would be
used. This is a glass thermometer that
has its bulb surrounded by a piece of
cloth soaked in water.
The water evaporates, cooling the
bulb and reducing the indicated temperature below ambient. It would often
be used in conjunction with a drybulb thermometer to give the true air
temperature.
The ‘sling psychrometer’ is a device
fitted with a wet-bulb and dry-bulb
thermometer. It is spun around above
one’s head for a minute or so, quickly
bringing the wet-bulb thermometer to
equilibrium. A chart was then used to
determine the dew point from the two
temperatures. Thankfully, you don’t
need to swing the HCI around above
your head!
The equations for converting temperature and relative humidity to
dew point are complex but well-
established, so it is a simple case of
performing readings from our sensors
and then a few calculations to produce
the desired figures.
Design
As you can see from the photos, the Human Comfort Indicator
has a simple design that would suit
being used around the home, similarly to a weather station. The case
is 3D-printed, although the PCB is
designed to be easily mounted inside
any suitable enclosure with a few
holes in it.
Table 1: Dew point interpretation
Dew point
Subjective condition
<5°C
Very dry
5-10°C
Dry
10-15°C
Comfortable
15-20°C
Mostly comfortable
20-25°C
Muggy
>25°C
Uncomfortable
Original source: https://media.bom.gov.au/social/
blog/1324/feeling-hot-and-bothered-its-not-thehumidity-its-the-dew-point/
We use an e-paper panel to display
the readings. These draw close to zero
power except when they are actually
updating, so they are a good choice
for a battery-powered device. They are
also easy to read under a wide range
of light conditions as they are similar
to ink on paper.
We have written a feature article
with more details on e-paper in this
issue. It includes some background on
the technology and how we came to
choose a specific panel.
The person who suggested this project also asked for some extra outputs
on the device. The first is an analog
voltage that reflects the dew point
temperature, which can be used as
an input to another system, such as
a data logger.
The other is an open-drain output
that can be triggered when certain
conditions are met, such as the temperature or dew point falling outside
preset ranges. It is controlled by a
small Mosfet capable of sinking a few
hundred milliamperes,
so it can
After the SMD parts have been fitted and
the micro has been programmed, you
can test the e-paper panel by supplying
power via the USB socket. You will see
this error message since the sensor has
not been fitted.
44
Silicon Chip
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directly drive a buzzer or even a small
relay if a larger load needs to be controlled.
Circuit details
Fig.1 shows the circuit diagram of
the Human Comfort Indicator. The circuitry around CON4 and the MOD2
e-paper panel is virtually identical to
that described in the feature article. It
differs from the breakout boards we
tested mainly in using larger components to simplify soldering.
This part of the circuit generates
the necessary voltages to drive the
display panel. Mosfet Q1 is driven
by the display controller on the e-paper panel to provide ±20V rails. BS1
is tied low to force the controller into
8-bit SPI mode.
The circuit is driven by a 16-bit
PIC24FJ256GA702 microcontroller
(IC1) boasting 256kiB of flash memory and 16kiB of RAM. The large
amount of flash allows us to store
graphics, such as font data, while the
RAM allows us to create a buffer large
enough to store an entire screenful for
display, something that would not be
possible with most 8-bit microcontrollers.
We’ve established that the PIC24
FJ256GA702 is capable of low-power
operation, having used it in the ESR
Tweezers project from the June 2024
issue (siliconchip.au/Article/16289). It
also has hardware multiply and divide
functions, which will help performing
the mathematical operations needed
to process our readings. On top of all
that, it’s relatively inexpensive.
IC1 is supplied from the 3.3V rail
and also has two 100nF supply rail
bypass capacitors plus the necessary
10μF capacitor on its VCAP pin (pin
20). This bypasses an internal regulator used to power the processor core
at between 1.2V and 1.8V.
Pins 1, 4 and 5 are ICSP (in-circuit
serial programming) pins connected
to CON1, along with 3.3V and ground,
allowing it to be reflashed after soldering. Pin 1 has a 10kW pullup resistor
to allow normal operation unless a
programmer is connected.
IC1 controls the e-paper panel via
six lines: three for the SPI interface
and three more control signals. The
PPS (peripheral pin select) feature of
IC1 allows most peripherals (like the
hardware SPI interface) to be directed
to most pins, simplifying the PCB layout. One exception is the Vout signal,
siliconchip.com.au
Fig.1: the circuitry around Q1 and connecting to the e-paper display via CON4 is driven by the controller on the e-paper
panel. These components generate the various supply rails needed to drive the display. Our feature article in this issue
(see page 66) covers this in more detail.
which is provided by the analog CVref
peripheral, which is fixed at pin 25.
The CVref output comes from a 5-bit
DAC. When using the 3.3V supply rails
as its inputs, we get 32 steps over 3.3V,
or near enough to 0.1V resolution for
the Vout signal. This is simply made
available, along with a ground connection, at pin header CON5. The opendrain output is provided at CON6, is
implemented using Mosfet Q2, driven
from pin 11 of IC1.
A bi-colour LED, LED2, is driven
from another two I/O pins via a 1kW
series resistor. The two pins allow it to
be lit up red or green, or off entirely.
Three tactile pushbutton switches
are connected to three more I/O
pins on IC1. These are configured
as inputs with internal pull-up
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currents, allowing the switch states
to be detected. Each pin is pulled to
ground by the associated switch when
it’s closed, or held high by the pull-up
current the rest of the time.
The last component is sensor module MOD2, which is connected at
CON3, a six-way header to suit its
pinout. This module includes a Bosch
Sensortec BME280 humidity, pressure and temperature sensor.
We have chosen it because it contains only the bare minimum circuitry
needed to operate the sensor chip. Specifically, it lacks a voltage regulator, so
we don’t need to worry about a poorly
designed module wasting power in an
inefficient regulator.
The sensor IC itself is designed for
3.3V operation, so it can run from the
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same rail as the microcontroller. It consumes just 0.1μA in sleep mode. The
chip and module can work in either
SPI or I2C mode; we are using I2C in
this case.
The module includes bypass capacitors and pullup resistors for the communication lines. It is an updated version of the GY-BM module described
in our review of Pressure/Temperature
Modules (December 2017; siliconchip.
au/Article/10910). The similar circuit
of that module is shown on p82 of
that article.
Power supply
Like the e-paper controller, IC1 is
a nominally 3.3V device (3.6V maximum), so the main logic and supply voltage is set at 3.3V. This comes
June 2026 45
from REG1, an MCP1700-3302 LDO
(low dropout) regulator. Helpfully,
it also has a low quiescent current of
around 2μA.
This is in turn fed from one of two
sources by a common-cathode dual
schottky diode, D1. One anode connects to a Li-ion battery, while the
other is a 5V supply from USB-C socket
CON2. CON2’s CC1 and CC2 pins are
connected to the requisite 5.1kW resistors to ground. These indicate that the
device should be treated as a sink and
be supplied with 5V when connected
to a source.
Two alternative locations are provided for CON2 so that the PCB can be
constructed to suit one of two particular orientations. 5V from CON2 also
supplies the charging circuitry based
on IC2. The 10kW resistor sets the
charging current to 100mA, the minimum permitted by this chip, while
LED1 is another bi-colour LED that
shows red while charging is occurring
and the STAT pin is low.
When charging completes, the STAT
pin goes high and LED1’s green element lights. The arrangement of the
two 1kW resistors allows this to work.
While it might appear inefficient to
have the resistors connected across the
supply, they will only draw current
while 5V is present at the USB socket
and won’t drain the battery.
The diode arrangement means that
there is no current draw from the
battery while charging is occurring,
so the battery can charge fully.
Software
Software operation is focused on
minimising power consumption
where possible. This mostly consists of setting the external modules
to low-power modes. The BME280
is checked every 5 minutes and the
screen is updated at the same rate. A
low-power RC oscillator (LPRC) in the
microcontroller keeping time means
that the processor can spend much of
its time sleeping.
The LPRC is configured to provide
an interrupt at around 5Hz, quick
enough that it can provide timing
down to one second with reasonable
consistency. Several counters are
updated with this interrupt. Some
counters keep rough track of hours,
days and weeks, allowing daily,
weekly and monthly averages to be
accumulated.
Another counter sets LED2 to light
up for about one second every minute;
it consumes a few milliamperes when
on, so operating it with a low duty
cycle reduces the average current consumption. The colour that LED2 shows
when lit matches the alarm state; if red,
then the alarm is active, Q2 is on and
the ALARM output is pulled to GND.
Otherwise, LED2 is green and Q2 is off.
The sensor readings require a bit
of processing. There are a total 18
Scope 1: the idle current of the Human Comfort indicator
is around 100μA, with a peak below 5mA (during a full
refresh, shown here).
46
Silicon Chip
calibration parameters that are unique
to each chip; they are used for compensating the raw 16-bit humidity
readings and 20-bit temperature and
pressure readings.
The humidity and pressure readings are further compensated based
on the measured temperature. Fortunately, Bosch Sensortec provides
sample code to do this. The results
are displayed according to user preferences, such as temperature display
units. There is also a menu system that
allows the preferences and settings to
be changed.
Since the e-paper display takes
so long to refresh, we have kept the
options and thus the menus fairly
simple to prevent them from being
unwieldy to use. We’ll explain more
about the operation once construction
is complete.
Power
Scopes 1 & 2 show typical current
consumption. Scope 1 shows a full
refresh occurring on the main page,
with the low levels on each side of the
peak representative of the normal idle
state below 100μA. The refresh is no
more than 5mA for no more than five
seconds and occurs about once every
five minutes, giving an average contribution of less than 83μA.
Scope 2 shows a partial refresh
occurring upon entry to the setting
screen. Note that the current peak
Scope 2: a partial screen refresh requires less current. The
1.5mA draw seen here is due to LED2 being lit while the
settings screens are active.
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siliconchip.com.au
Fig.2: we designed this 3D-printed case
(above) to suit the Human Comfort
Indicator. It comes in two variants,
with this render showing the landscape
version, with the USB socket coming out
the side. Vents allow the sensor to sample room
air. The portrait version is shown in the adjacent photos.
is slightly lower due to the partial
refresh. The higher level on the right
is due to the LED2 lighting up and consuming 1.5mA. During normal operation, the LED is on for approximately
one second per minute, contributing
an average of 25μA.
So we expect the long-term average
consumption of the Human Comfort
Indicator to be around 210μA. Given
that the self-discharge of Li-ion cells
is typically around 2% per month, a
typical cell will lose 40mAh per month
or around 53μA; a significant chunk
of the usage!
We have quoted 300μA to take into
account some time spent on the settings or viewing different pages. With
a nominal 2000mAh lithium cell, this
equates to 6600 hours or around nine
months of operation on battery power.
Considerations
Since the e-paper display panel
includes look-up table (LUT) options
for both full and fast refreshes, we
have included an option to set how the
refreshes occur. Broadly speaking, the
full refresh will use more power, but
will provide a clearer display.
The fast refresh appears less distracting when it happens, but the
resulting display has slightly poorer
contrast. The above calculations
assume that full refreshes occur at
all times, so using partial refreshes
should provide even longer operation
than quoted.
The outputs at CON5 and CON6
are nothing more than pin headers,
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since we expect they may not be used
in most cases. The analog output on
CON5 is a voltage (in volts) that is one
tenth of the dew point (in degrees).
So a dew point of 16°C will result in
an output of 1.6V; naturally, this is
capped between 0V and around 3.1V,
the upper limit of the CVref peripheral.
It is not buffered and has an estimated output impedance of around
30kW. Unless you are connecting it
to a high-impedance input, you may
need to buffer it. We have chosen not
to provide a buffer, since it would draw
extra power that would be wasted if
this output is unused.
E-paper’s ability to show a display
while using no power also has a subtle
downside in that it can be hard to tell
if the device is working or frozen. The
main way we show the health of the
Human Comfort Indicator is through
the flashing of LED2.
If you don’t see LED2 flash occasionally, the Human Comfort Indicator may have shut down due to a flat
battery. The voltage of the regulated
3.3V line is also shown on the main
page. If this gets near 3.0V, the battery may be overdischarged. There is
no built-in overdischarge protection,
so a protected cell must be used. That
will prevent significant cell damage if
you forget to recharge it.
Any unit like the Human Comfort
Indicator that measures ambient temperature is at risk of being affected by
self-heating, where the heat dissipated
by the unit’s own operation drives up
the measured temperature.
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Thankfully, it has very low power
consumption, and most of its power
consumption occurs immediately after
a reading has been taken (when the
display is refreshed with the updated
readings). So that should not be a probably, provided that the chosen enclosure does not trap heat.
Enclosure
We have designed a 3D-printed
enclosure to suit the Human Comfort Indicator with a vent to allow air
exchange. That should not only eliminate self-heating concerns, but it’s also
necessary so that the humidity sensor
(and to a lesser extent, temperature
sensor) can respond to the ambient
conditions properly.
It will probably take a few hours to
print, so we recommend that you start
that while assembling the PCB. The
two parts simply snap together, and
they are designed to be printed without supports.
There are two variants of the case,
one to suit each position for the USB
connector, CON2. One variant suits a
portrait layout, with the hole for the
USB socket on the long side. The other
variant suits a landscape display and
has the USB socket on the short side.
Make sure that you choose two matching halves before printing them. The
render in Fig.2 shows the two halves
of the landscape version.
We printed our prototypes on an
Ender-3 V3-SE and, to ensure the
best appearance, used a 0.08mm layer
height and low speed, about 50% of
June 2026 47
Fig.3: all the SMD parts are on one side of the PCB, with many of the through-hole parts mounted on the back. Try to keep
the area under the e-paper panel clear on the back of the PCB. The entire Human Comfort Indicator is just under 9cm tall.
It is fully self-contained and is powered from a rechargeable battery that should last close to a year between charges.
normal speed. The job took about six
hours in total: two hours for the front
and four hours for the back half.
The result should be usable with
minimal post-processing. At most, you
might need to remove small burrs or
file down the parts if they have been
heavily over-extruded. The bezels on
the front half of the case (where the
display mounts) are quite thin, so take
care when removing them from your
print bed. The vent holes are nominally 2mm in diameter if you wish to
clean them up with a drill bit.
The PCB also has mounting holes,
allowing it to be fitted to just about
any enclosure that is large enough
and can have suitable holes made (see
Fig.4). The PCB simply mounts to the
front panel of such an enclosure using
screws and spacers. A UB3 Jiffy box
should be a good fit. The view shown
in Fig.4 is from the outside of the
enclosure.
If you are using such an enclosure,
we suggest using the bare PCB as a
template for the mounting and switch
holes. The USB socket will probably
not align with the edge of the case, so
you will likely have to cut a hole to
allow a cable to pass through the case.
Options
The charging components are inside
a white box printed on the PCB. Leaving these parts off will disable the
charging feature. You could do this
if you don’t want to use an internal
48
Silicon Chip
battery; in this case, it will only operate when powered from CON2.
We’ll describe the assembly including all components. Simply leave off
the battery, battery holder and all parts
in that box if you wish to pursue this
option. You can also see this outline
in the overlay diagram (Fig.3).
We recommend using the battery,
since this will allow the Human Comfort Indicator to operate during brief
power interruptions. Importantly, it
will be able to retain its long-term
average readings in RAM.
PCB assembly
There are a few fine-pitch devices on
the board, so you will probably need a
magnifier and good lighting as well as
the usual SMD gear such as flux paste,
tweezers and solder-wicking braid.
Start by fitting the SMD components,
which are all on one side of the PCB.
IC1 and CON4 have the finest lead
pitches. Apply flux to the pads and
rest these components in place, adding more flux on top of the leads.
Carefully align the pins to their pads,
then check they are correctly orientated before tacking one or two pins
in place, making sure that they are flat
against the PCB.
We’ve made the pads quite long, so
you can try applying the iron to the
pad only; this should be sufficient to
cause the solder to run onto the lead
and form a proper joint. Check for any
bridges and use the braid to remove
Australia's electronics magazine
excess solder, adding more flux as
needed. When you are sure that CON4
is properly soldered, apply a solid fillet to each of the larger end pads for
mechanical strength.
Next, solder IC2. It has five pins, so
it will only fit properly in one orientation. Follow with the three-lead SOT23 parts. Note that this includes a regulator, two Mosfets and a dual diode,
which all look similar, so don’t get
them mixed up. There are also three
single diodes to be installed; solder
them next, making sure to place the
cathode stripes near the K symbols,
as shown in Fig.3.
Follow with the capacitors; they
will not be individually marked. The
1μF parts are the most numerous, so
we recommend starting with these.
Ten are at the lower left near CON4,
while two are near REG1. Most of the
1μF parts are in a single row that also
includes a solitary 100nF capacitor, so
watch out for the interloper.
Two of the 10μF capacitors are near
IC2, with the third near IC1. These
will probably be thicker than the other
capacitors, so you might be able to tell
them apart. Follow with the single
4.7μF capacitor (or 10μF as supplied in
the kit) and the two remaining 100nF
capacitors, near IC1 and the interloper
in the row of 1μF parts.
The solitary inductor has large
pads, but it doesn’t have a huge thermal mass, so soldering it should be
straightforward; it is not polarised.
siliconchip.com.au
Follow with the 11 resistors, checking
their markings (1003 or 104 = 100kW
etc). To complete the SMD parts, fit
CON2 to your preferred location. Be
sure to add solid solder fillets to CON2
so that it is mechanically secure.
That completes the SMD components, so clean up the residual flux
with a suitable solvent and check for
any bridges or dry solder joints. If you
need to reflow any joints, repeat the
cleaning process in that area. When
finished, allow the board to dry.
You can perform a brief check by
applying USB power to CON2. You
should see 3.2-3.4V on the second pad
of CON1 relative to ground. Ground is
the middle pad of CON2, or the marked
pads on CON5 or CON6. If you do not
see this voltage, disconnect power
immediately and investigate before
proceeding.
Programming IC1
If you purchased the chip from the
Silicon Chip Online Shop, it will be
programmed and you can skip to the
next step. Otherwise, fit a vertical
pin header to CON1. The reverse of
the PCB is where the e-paper module
will sit, so it is best to minimise the
amount by which components protrude into this area.
Inside our 3D printed enclosure,
the display panel sits 1.5mm from the
PCB, so this is the absolute maximum
by which items should extend behind
the PCB in this area. One way to do this
is to mount the header with its plastic
block sitting off the PCB slightly. There
should be enough clearance so that
CON1 can be left in place afterwards.
Connect your programmer to CON1;
a Snap, PICkit 4, PICkit 5 or PICkit
BASIC should all be suitable. You can
use the CON2 USB socket to provide
power. Open the Microchip MPLAB
IPE program and use it to program
the 2110526A.HEX file into IC1 and
verify it.
Checking the display
Disconnect any power supply
before proceeding. You can now
check that the display panel is functional by plugging it into CON4. Pull
the grey tabs outwards, parallel to the
PCB, to release the catch. Slot the FFC
(flexible flat cable) into CON4 with
the gold contacts facing upwards. The
gold part should not be visible when
the FFC is fully inserted. Then carefully push the tabs back in.
siliconchip.com.au
Parts List – Human Comfort Indicator
1 double-sided 50 × 80mm PCB coded 21105261
1 3D-printed case (alternative parts listed at the bottom) [SC7453/SC7684]
1 single AA (14500 size) PCB-mount cell holder
1 Li-ion rechargeable 14500 (AA-sized) cell with built-in protection
1 5-pin header, 2.54mm pitch (CON1; optional, for ICSP)
1 SMD USB-C power-only socket (CON2) [eg, GCT USB-4135-GF-A]
1 6-way right-angle header, 2.54mm pitch (CON3)
1 24-way SMT FFC top-connect ZIF socket (CON4)
[EastRising ER-CON24HT-1; www.buydisplay.com/24-pin-0-5mm-pitchtop-contact-zif-connector-fpc-connector]
2 2-way headers, 2.54mm pitch
(CON5 & CON6; optional, for external signal connections)
1 47μH 6×6mm SMD inductor (L1) [LSXBD6060WHL470M from DigiKey]
1 3.3V 6-pin BME280 module (MOD1) [Silicon Chip SC5482]
1 EastRising ER-EPD029-2B 2.9in EPD module with 24-pin FFC connector
(MOD2) [www.buydisplay.com/serial-2-9-inch-e-paper-screen-128x296for-electronic-shelf-label-lcd]
3 6×6×7mm through-hole tactile switches (~3mm actuators) (S1-S3)
1 piece of foam-backed double-sided tape or similar to secure e-paper panel
to main PCB
4 small self-adhesive rubber feet (optional)
Semiconductors
1 PIC24FJ256GA702-I/SS microcontroller programmed with 2110526A.HEX,
SSOP-28 (IC1)
1 MCP73831T-2ACI/OT Li-ion charge controller IC, SOT-23-5 (IC2)
1 MCP1700-3302E/TT LDO 3.3V linear regulator, SOT-23 (REG1)
2 AO3400 30V 5.8A SMD N-Channel Mosfets, SOT-23 (Q1, Q2)
1 BAT54C 25V 200mA dual common-cathode schottky diode, SOT-23 (D1)
3 MBR0540 50V 0.5A schottky diodes, SOD-123 (D2-D4)
2 3mm bi-colour red/green 2-lead LEDs (LED1, LED2)
Capacitors (all SMD M2012/0805 MLCCs)
3 10μF X5R 16V
1 4.7μF or 10μF X5R 16V
12 1μF X5R 50V
3 100nF X7R 50V
Resistors (all SMD M2012/0805 ±1% ⅛W)
1 100kW
4 10kW
2 5.1kW
3 1kW
1 0.47W
Alternative parts for non-3D-printed case
1 UB3 Jiffy box (see Fig.4 below)
2 M3 × 10mm panhead machine screws
2 M3 hex nuts
2 3mm-long, >3mm inner diameter untapped spacers
CL
Fig.4: if you don’t
plan to use our
3D-printed case
design, use this
34.5
34.5
diagram to cut and
22.5
drill a UB3 Jiffy
69
box lid instead.
32
DISPLAY
Find the centre of
WINDOW
your panel by
marking where
9.5
the two diagonals
cross; this should
2
help to centre
8
12
7.5
5
12
12
Ø3
Ø4 Ø4
Ø4
Ø3
Ø3
the display and
controls. Use the
blank PCB to mark
ALL DIMENSIONS IN MILLIMETRES
the panel first.
CL
Ø3
10
SCALE: 100%
SC7646 Kit ($60 + postage): includes everything except the case and battery
Table 2: Settings summary
Number Setting
Options
Notes
1
Dew point
minimum
Alarm on or
Alarm off
If this is off, the alarm is not
triggered by a low dew point
2
Dew point
minimum
-10°C to 30°C or
14°F to 86°F
Increments in steps of the
currently selected units
3
Dew point
maximum
Alarm on or
Alarm off
If this is off, the alarm is not
triggered by a high dew point
4
Dew point
maximum
-10°C to 30°C or
14°F to 86°F
Increments in steps of the
currently selected units
5
Sensor fail
Alarm on or
Alarm off
If this is set off, then the alarm
is not triggered by sensor
failure
6
Units
°C or °F
All temperature settings and
figures are shown in these units
7
Orientation
Portrait,
Adjust to suit the case or
landscape,
installation
reverse portrait or
reverse landscape
8
Text
Black text or
white text
The background is the opposite
of the text colour
9
Refresh
Always, Hourly
Daily
This is how often a full refresh
occurs; otherwise, a fast
refresh happens
10
Flash options
S3: Save to flash
S2: Restore from
backup
The “Ready” message will
change when a save or restore
has completed
This board has all the SMDs fitted but
none of the through-hole parts (yet).
The completed PCB is shown on the
left before installation in the case.
50
Silicon Chip
Australia's electronics magazine
In use, the flexible cable bends 180°
to put the display on the back of the
main PCB, but for now, the whole
assembly can lay flat on your workbench. These panels are quite fragile,
so handle with care.
Applying USB power at CON2
should cause the display to operate.
If it flickers but turns solid black or
remains white, it could be that one
of the leads for CON4 or one of the
components in that area of the PCB
is soldered incorrectly. Disconnect
the power and remove the display by
pulling out the grey tabs, then investigate the fault and rectify it before
proceeding.
Last components
Finish assembling the PCB by soldering the last few components. The
three tactile switches and two LEDs
should be soldered flat against the
PCB. These are all on the opposite side
to the previously fitted SMD components. The LEDs should be fitted such
that the green cathode (shorter lead) is
towards the nearest edge of the PCB.
You can easily test this by applying
power to the USB socket and carefully
connect the LED between pins 1 and
3 of CON1, avoiding contact with pin
2. Whichever pin is connected to pin
3 when the LED lights up is the cathode – see Photo 2.
The battery holder should also be
on the same side as the SMD components. Trim its leads short so they
don’t protrude too far into the area
where the display panel will sit, and
double-check the polarity. The AAA
markings were intended to allow a
pair of 1.5V AAA cells to power the
Human Comfort Indicator, but we have
not tested this configuration, and you
should use the AA markings.
The last component to solder will be
the sensor module, connected via the
CON3 header. Ideally, this should be
spaced off the PCB as far as possible
and near the vents in the rear of the
3D-printed case.
Use the right-angle header to achieve
this, being sure to maintain clearance
from the battery and its holder. You can
rest the PCB on the posts in the back
half of the base to check the position
and clearance.
You can test these components similarly to before, by connecting the display panel and USB power. Check that
the display updates to show our splash
screen with an “OK” message below
siliconchip.com.au
it. If it says “Sensor error”, it has not
been able to communicate with the
sensor and you should check the circuitry around CON3.
You should see LED2 flash red or
green within a minute if all is well.
LED1 might flash momentarily, but
will probably not show a true indication until the battery is fitted.
Completion
Now is a good time to add the foambacked tape. We opted to attach some
pieces to the PCB and leave the backing sheet on the side facing the display panel. This was still sufficient to
hold the panel in place without having to worry about aligning the two
permanently.
Slot the display panel into the bezel
window, with the FFC cable curving
around at the notch near the USB
socket. Carefully attach the display
panel to the PCB and rest the PCB in
place above it. The tape should apply
just enough pressure to keep the display panel in place. Install the battery and check that the display operates as previously. Snap the back of
the case on.
You might like to add some small
rubber feet to the lower four corners
Screen 1: the default main
screen shows information
in portrait. This design was
tested in late February and
it is a bit sticky, as the dew
point suggests!
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If a bicolour LED, connected as
shown here,
lights
up
then the
lead on the
middle pad is
the cathode
(for the green
element, in
this case).
of the case, since it is quite small and
light. This should prevent it sliding
around when connected to a USB
cable.
Using it
For the most part, the Human Comfort Indicator should be working as
intended from power-on. Screen 1
shows a typical display.
As noted earlier, the Human Comfort Indicator can also show the daily,
weekly, or monthly average statistics.
This is done on the main page by pressing S3 or S2. The screen will refresh
and show the respective averages if
it has recorded enough valid values.
Screen 2: one page of
settings is for configuring
display preferences. The last
item allows all settings to be
permanently saved to flash
memory.
If you see dashes displayed instead
of numbers, there may not have been
enough values recorded to make up
the average. As expected, you will not
see a monthly average until a month
has expired. You might also see dashes
if there is a problem with the sensor
module.
Changing settings
Screens 2-5 show the settings and
other options. All setting changes are
effective immediately. They can also
be permanently saved to flash memory, which will mean that those settings are restored after a power cycle.
The main choices for the display
are the orientation and colour scheme:
black text on a white background or
vice versa. The portrait and landscape
settings should suit the two different
3D printed case variants. You can also
choose a reversed (rotated 180°) option
if you prefer.
Another setting is a choice between
°C and °F for temperature displays.
Internally, all temperatures are stored
as units of 0.01°C and converted where
needed. You can also choose whether
a full screen refresh occurs every five
minutes (always), every hour, or every
day (see Screen 2).
Screen 3: the other settings
page relates to the alarm
outputs. Whether the alarm
is triggered for a low or a
high dew point can be set
independently.
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Screen 4: the white text on
a black background looks
striking; it would be very
impressive if used with a
black 3D-printed case.
June 2026 51
Screen 5: the landscape
format lays out the
main data screen in
this fashion; the settings
screens put the items
into two columns.
There are also some alarm settings:
the minimum and maximum dew
point and whether either threshold is
enabled (or neither, or both). You can
also set the alarm to trigger if a problem is detected with the sensor. Screen
3 shows these; they are all enabled by
default.
Because of the slow update rate of
the e-paper panel, the settings menus
operate slightly differently to those
you might have seen in our other
projects.
Pressing S1 (closest to LED2) enters
the settings menus and the alarms are
shown first. LED2 is lit solidly while in
the settings menus. Each button press
is followed by a one-second delay
before being acted upon. This allows
multiple button presses to occur before
the screen is refreshed, so it is easier to
make bulk changes. LED2 switches off
to indicate that a refresh is pending.
Screens 2 and 3 show the cursor
marker that indicates which item is
being edited – S1 skips to the next
option. For numeric values, S3 decrements them and S2 increments them.
For binary options, either S2 or S3 will
toggle the state.
For example, to change the dew
point maximum from 20°C to 15°C,
you would press S1 once to enter
the settings, then allow the screen to
refresh. Press S1 three times quickly
to jump to the DP maximum setting.
Allow the refresh to happen to make
sure you are changing the right item.
Then press S3 five times to drop the
setting by 5°C.
Let the refresh occur and check that
the value is correct. Then press S1
six times to jump forward to the flash
memory options, then press S3 to save
and check that you see the “Save done”
message. Finally, press S1 to return to
the main screen. Table 2 summarises
the settings.
If the settings appear to be corrupted, you can use Restore (S2) on
the last settings item to reload the initial settings from flash memory. You
should immediately use S3 to save
these to flash memory to be sure that
everything is as new.
Since LED2 is on for the settings
screens, it uses much more power
than the main screen. So if 30 seconds elapses without a button being
pressed, the Human Comfort Indicator
returns to the main screen displaying
temperature, humidity and dew point.
Summary
The Human Comfort Indicator will
be a great addition to any household
that needs to keep track of the local
humidity and dew point. We’re sure
readers will find interesting applications for the alarm and analog voltage
outputs. The firmware and STL files
can be found at www.siliconchip.com.
SC
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Installing a
Whole-House
Sound System
Feature by Julian Edgar
W
hen my wife and I decided to
build a new home, there were
lots of decisions to be made – literally, hundreds of them. From décor
to bathroom design, where to put
power points and how high the ceilings should be.
As part of the research to answer
those questions, my wife and I went to
a huge number of new display homes,
looking at what features were available and how they were implemented.
Unexpectedly, one display home
really caught my eye – or more accurately, my ears. This home had ceiling-
mounted speakers throughout the
house, and additional speakers in an
outdoor living area. They were playing
quietly, and as we walked through the
house, it started to change my mind
about music in a home.
Previously, in all five houses we’ve
lived in, the main sound system has
been in the lounge room – a traditional
stereo hifi system. To get the best quality sound, you sat in a designated area
and listened to the music.
Except, we never actually did that!
Instead, it was more likely that we’d
crank up the system while entertaining
or even when cleaning the house. We’d
not be sitting in one place but instead
moving around. It was bad for stereo
imaging, and even for hearing tweeters, but it was how the sound system
was actually used.
So the idea grew in my mind: in
the new house, let’s make the sound
system a whole-of-house design.
There would be inevitable trade-offs
in sound quality – but the sound system would be much more practical
and useful.
Choosing the speakers
Three amplifiers, one preamp, thirteen speakers,
hundreds of metres of wiring – it all sounds a nightmare!
So why do it? There are plenty of good reasons...
Having decided that there would
be speakers located throughout the
house, the next decision was on the
type of speakers to use. To minimise
the use of floor space and to be aesthetically acceptable, the interior speakers
needed to be mounted either in the
ceiling or in the walls.
These days, with home theatre systems often requiring numerous speakers, speakers designed to be mounted
in walls and ceilings are widely available. Most have a glaring deficiency:
they comprise bare drivers mounted
on a faceplate, with that faceplate then
fitted to the plasterboard. The resulting
speaker ‘enclosure’ is just the random
volume behind the faceplate.
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Image source: https://unsplash.com/photos/a-room-filled-withlots-of-different-types-of-speakers-vAHw2myA0EM
54
Silicon Chip
Photo 1: seven Bose DS 100F ceiling
speakers are used throughout the
house. They use a ported enclosure
with a 133mm long-throw woofer and
a 57mm mid-range/tweeter and suit
both 8W and 70/100V systems. These
are of much better quality than Bose
consumer speakers.
Photo 2: the wall in the lounge/kitchen backs onto the roof loft space. From left
to right, you can see one Bose speaker, an air intake grille, the two vents for
the subwoofers (with a ventilation intake grille in between), another (currently
unused) air intake grille, and the second Bose speaker. Another five Bose
speakers are distributed throughout the house. I would have chosen white
speakers if I had bought them new, but I don’t mind the contrast.
With wall-mounting, that volume
might be quite small; just the volume
between the noggins and studs. With
ceiling mounting, that volume might
be effectively infinite – the whole
volume of the roof space! Thus, such
speakers need to be designed with
huge compromises, and they cannot
use the most efficient common enclosure design: ported bass-reflex.
Therefore, I resolved that any
speakers would need to have their
own acoustic enclosures, meaning
that, because of the resulting greater
depth, they would usually need to be
mounted in the ceilings.
I figured I needed up to ten high-
quality ceiling speakers, and looking
at new prices showed that this could
very quickly become a huge cost.
At this point, I started searching for
what was available second-hand, and
I found someone selling a complete
ex-restaurant sound system.
It comprised seven Bose DS 100F
ceiling speakers (Photo 1), six Bose
DS 16F ceiling speakers, a large Bose
DXA 2120 amplifier, three smaller IZA
190-HZ Bose amplifiers, a line-level
audio splitter box and various remote
controls and cables. The price was
very good – in fact, less than the new
price of just the big amplifier! (As it
later turned out, that was just as well.)
To put it mildly, Bose has a variable
reputation amongst audiophiles; many
hate the brand due to its heavy reliance on processing and compensation
to make small speakers sound good.
However, in professional sound
reinforcement, the story is different.
I’ve had a lot of experience with different Bose gear, and I find two things.
First, their professional gear is better-
built than their consumer gear. And
second, if you buy their upper-tier
products, they can sound quite good.
In this case, before committing the
gear to the new house, I extensively
tested the larger DS 100F speakers
working with the DXA 2120 amplifier
– and I was impressed. The speakers
use a ported enclosure with a 133mm
long-throw woofer and a 57mm midrange/tweeter.
With a relatively small enclosure
volume, and with those drivers, the
speakers were never going to sound as
good as full-size, dedicated hifi speakers – but then again, in this application they didn’t need to. Still, they
had bass down to about 100Hz (more
on bass in a moment) and the treble
was adequate, although not wonderful.
This was with the speakers tested
not mounted in a ceiling: if mounted
in a ceiling near to a wall, you’d expect
the bass to be better due to the resulting acoustic loading.
In addition to the ceiling speakers, we also wanted a pair of speakers mounted outside to service a large
undercover deck. This area could also
have used ceiling speakers, but the
Bose speakers are not weatherproof,
and while such speakers wouldn’t be
subjected to direct rain, they would be
subjected to fog and dew.
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Australia's electronics magazine
So I decided to keep an eye out for
good quality exterior speakers. I eventually found a pair of second-hand
Niles OS7.5 wall-mounted speakers
for an excellent price.
The amplifiers
The Bose DXA 2120 amplifier was
going to be used to drive the DS 100F
speakers. But how many speakers
could it power? These speakers have a
rated impedance of 8W; the minimum
impedance this amplifier is happy
working with is 4W. Thus, each of the
two stereo channels can drive two
speakers in parallel, giving a total of
four speakers.
After a bit of thought, this worked
out well. The rectangular-shaped
house has two large rooms, one at
each end of the house. These rooms
have cathedral (raked) ceilings, with
internal walls that back onto a roof loft
space (Photo 2). If two of the speakers
were placed through these walls, we’d
have a stereo pair in each room.
Within the previously discussed
constraints, at least if sitting in these
rooms, the stereo imaging should then
be good.
What about the other speakers? The
two end rooms are joined by a wide,
open corridor that passes down the
middle of the house. Locating the
remaining three DS100F speakers in
this space would largely cover the
rest of the house – there wouldn’t be
speakers in every room, but you’d be
able to hear sound everywhere.
June 2026 55
But how do you drive three speakers from a stereo source? It didn’t make
much sense trying to do so!
So back to the remaining three
Bose IZA 190-HZ amplifiers (Photo
3). These amplifiers all have 70/100V
outputs. If you’re not familiar with this
approach, each speaker to be driven
from such an amplifier is equipped
with a transformer with multiple taps,
with each tap giving a different power
rating (and so speaker loudness).
The DS100F speakers were equipped
with such transformers, and different
power ratings could be selected by
turning a knob. A conventional 8W
speaker impedance was one setting,
explaining how these speakers could
also be used with the main amplifier.
Multiple speakers can be driven
from each output with such a 70/100V
system; rather than worrying about
impedance, you just need to ensure
that the total selected speaker power
ratings do not exceed the power output of the amplifier. The IZA 190-HZ
amplifiers are also able to be configured with a mono output from a stereo source, making them suitable for
driving the three speakers.
Only one amplifier was needed to
drive these speakers – which is just as
well, as it turned out that two of the
three second-hand IZA 190-HZ amplifiers were defective!
A 70/100V system has a reduced
frequency response, but in our case,
where these speakers are used to ‘fill
the hole’ between the speakers in the
end rooms, their more limited frequency response is well masked by
the 8W speakers, which are still audible from those locations.
All about the bass
Now, back to the topic of bass.
For our previous house, I’d built
two large subwoofers. Each used a
JBL 15-inch (380mm) driver and a
200L ported enclosure (Photo 4). I’d
mounted them beneath the floor of
the lounge room, firing through floor
grilles. They’d worked exceptionally
well, so I resolved to move them to
the new house.
There, they could be mounted in the
loft space, passing their sound through
two wall-mounted openings. As they
would also be used for the lounge
home theatre sound system (not covered in this article), they would provide bass at only one end of the house
– an acceptable trade-off as bass is
largely non-directional.
But what to power them with? In
the previous house, I’d used a four-
channel amplifier I had built. It had
an output of 68W/channel and drove
the subs and two full-range speakers.
In that small lounge room, the subs’
output had been fine, despite the relatively low amplifier power.
However, testing in the new house
soon showed that the much bigger
room seemed to suck all the bass away
– the huge subs sounded quite anemic. So I then built a 200W per channel amplifier, and the subs came alive.
Photo 3: a 90W Bose IZA 190-HZ amplifier drives three speakers using a 100V
system.
Photo 4: two subwoofers are used, each with a 200L custom-built enclosure and
a 15-inch, 300W JBL driver. There is audible bass down to 25Hz and strong bass
from about 35Hz.
56
Silicon Chip
Australia's electronics magazine
Photo 5: one of the two outdoor
subwoofers for the deck; it is built
inside a fibre cement stool. They
provide bass support for two Niles
wall-mounted speakers.
siliconchip.com.au
However, in all of this, I had forgotten the outside speakers – surely
I didn’t need yet another amplifier to
drive them, did I? Instead, I decided to
use relay switching to select between
driving the inside or outside speakers
from the same amplifier.
About this time, I developed the
Outdoor Subwoofer published in
the June 2025 issue (siliconchip.au/
Article/18313) and the improvement
it gave to the outdoor sound system
audio quality was major. So much so
that I decided to build two of these
subs (Photo 5).
Now things were getting complicated – to switch from inside to outside sound, I needed to simultaneously
switch the output of three different
amplifiers! But again, Silicon Chip
came to the rescue, and we developed
the Remote Speaker Switch that was
published in the January 2026 issue
(siliconchip.au/Article/19561). It’s a
very flexible system and does this job
neatly using three interlinked switches
(Photo 6).
Photo 6: the Silicon Chip
Remote Speaker Switch is
used to simultaneously switch the
output of three amplifiers between different
speakers, with three modules required.
The preamp
The next step was to consider how
the amps were to be fed signals, and
where all these amplifiers were going
to be mounted. Looking at the second
point first, I decided to place the three
amplifiers on a shelf in the roof space
loft. The loft is accessed by a dropdown ladder, with the area used primarily for storage.
If the amplifiers were remotely
switched, and if volume control was
also able to be achieved remotely,
there was no need to have the amplifiers located in the living space. Making this decision easier was the fact
that we would stream music from our
phones via Bluetooth, with the volume
also controlled by the phone.
So, a series of plywood shelves
were made, and the three amplifiers
installed in the loft.
How to feed signals to all these
amps? The ex-restaurant sound system
installer had faced the same dilemma
and had used the powered line-level
signal splitter to divide the source
signal between the amplifiers. However, he or she had not had an extra
subwoofer amplifier to contend with.
Not only did the audio signal have
to be sent to the different amplifiers,
but a subwoofer crossover needed to
be implemented as well. Here I took
a step that is unusual in home sound
siliconchip.com.au
Photo 7: unusually in a home
system, a Clarion EQS755 car
sound preamp is used. This drives the three
amplifiers from a single Bluetooth streaming input
adaptor, provides the subwoofer crossover and allows
frequency equalisation on seven bands. It runs from a 12V DC plugpack.
systems and decided to use a preamplifier designed for a car: a Clarion
EQS755 powered by a 12V plugpack
(Photo 7). I’d used it in our previous
house, and it had worked well.
Now out of production, it has surprisingly good audio specifications,
unbeatable at the price. It has a 7-band
equaliser and a variable-level subwoofer output, with the sub crossover
frequency able to be set at either 60Hz
or 90Hz. In addition, it has a further
two full-range outputs, for car use,
dubbed ‘front’ and ‘rear’.
However, in my application, I could
use these outputs to feed the two Bose
amplifiers. As a bonus, using the preamp would give me a seven-band EQ.
Disaster!
As an owner-builder, a lot of the
house was being built by me, and I
Australia's electronics magazine
wanted to listen to music as I toiled.
Therefore, the whole-of-house sound
system was running quite early in the
house build process – as soon as the
house was made weatherproof. The
ceiling speakers were mounted temporarily on plywood panels.
It’s just as well the system was trialled before the house was completed,
because I started experiencing major
amplifier failures!
First to go was the home-built subwoofer amplifier. It used two offthe-shelf modules, each comprising
a switch-mode power supply and a
Class-D audio amplifier. This amplifier lasted just weeks before it started
blowing supply fuses at switch-on. I
could have attempted to fix it, but truth
be known, I was a bit suspicious of
the quality and design of these modules, anyway.
June 2026 57
Photo 8: two LD Systems amplifiers are used to drive the main and subwoofer
speakers – an XS-400 (2 × 200W) for the main speakers and an XS-700 (2 × 350W) for the subwoofers.
These fan-forced commercial amplifiers were purchased after multiple amplifier failures – the demands of providing a lot
of power and working in a hot loft space proved to be extreme.
When John Clarke saw them, he was
scathing about their design layout! So
I replaced this amplifier with another,
more conventional design I’d built
long ago, an amplifier that I was sure
was of good quality.
Next to go wrong was the big Bose
DXA 2120 amplifier. This one developed a ‘splat! splat!’ in the audio output, then just died completely.
What on earth was going on? My
replacement amplifier for the subwoofers gave me the clue. Despite this
amplifier having run in my previous
home office for years, and despite my
having used it to occasionally test
loudspeakers at quite high power levels, the passively cooled heatsinks had
never run warm.
But here in the loft, driving the subwoofers, it was getting darn hot – over
55°C external heatsink temperatures...
and still rising.
Two aspects were at play. The first
is that the ambient temperatures at
which the amplifiers were working were high. In a normal domestic
setting, ambient temperatures are seldom very high; after all, that’s why
people have air conditioning! But in
the loft, within the roof space, temperatures were up to 35°C; potentially even higher in some weather
conditions.
The second aspect was that the
amplifiers were working really hard.
Especially with the house unfinished,
and so without plasterboard walls
and ceilings in place, the house volume was very large. To get adequate
sound levels in such a large volume
meant using a lot of power. Put those
two things together, and the amplifier working conditions were extreme.
So I decided to buy two new amplifiers, both fan-cooled and both aimed
at commercial (rather than domestic) use. After an extensive search, I
found two LD Systems amplifiers – the
XS-400 and XS-700. The XS-400 has
an output of 2 × 200W into 4W, and
the XS-700 develops 2 × 350W into
4W – see Photo 8.
Both are Class-D amplifiers that have
a maximum distortion of less than
0.1%. Not hifi, but good enough for
a whole-of-house sound system. The
amplifiers were bought second-hand,
and while it was an additional cost I
wish I didn’t have to outlay, they were
much cheaper than buying similar
quality amplifiers new.
As you can imagine, I tested these
amps very thoroughly, only to find
that certain internal components were
running very hot! However, a simple
modification to the airflow path within
the amplifiers, as described in my articles on amplifier cooling published in
the August & September 2025 issues,
improved this greatly (siliconchip.au/
Series/444).
To give you an idea of the required
power levels, I found that the 350W/
channel amplifier driving the two subwoofers was quite near clipping at
times. The amp has a clipping indicator on its front panel, so it’s easy to
see how hard it is working.
The final system
Fig.1: a Bluetooth adaptor feeds a preamp/subwoofer crossover that in turn
feeds three amplifiers. These power internal and external speakers, both
main and subwoofers, with inside/outside selection via three interlinked relay
switches. A mixture of 8W and 100V systems is used for the main speakers.
Fig.1 shows the layout of the final
system. A Bluetooth adaptor feeds the
Clarion EQS755 preamp. The preamp
also drives the LD Systems XS-400,
XS-700 and Bose IZA 190-HZ amplifiers. These power the four 8W speakers as two stereo pairs, and the three
mono 70/100V speakers located down
the middle of the house.
The preamp’s subwoofer output also
drives the LD Systems XS-700 subwoofer amplifier, which powers the
two 15-inch subs.
The speaker switch turns off all
the interior speakers and swaps the
XS-400 output to the outside wall
speakers; simultaneously, the XS-700
amplifier’s output is switched to the
two outside subwoofers.
Power to the Bose IZA 190-HZ,
LD Systems XS-400, preamp and the
switching relays is controlled by a
single wall-mounted conventional
switch in the living area, with one
LED indicator showing when they are
active. That is, this part of the system
is powered by a remotely switched
power point.
Australia's electronics magazine
siliconchip.com.au
58
Silicon Chip
Lessons learned
Test at every step! Without testing, you cannot be sure what you’ll end up with.
For example, until I had temporarily mounted the speakers in the half-built
house, I wasn’t sure that seven interior speakers would be sufficient. Until I had
tested over a period of many weeks in summer, I had no idea that amplifier cooling would prove to be so critical – and that so much power would be needed.
Would the Bluetooth adaptor continue to work if I took my phone out onto
the exterior deck? (It did.)
Did all the gear purchased second-hand actually work? It took me many
hours to discover that two of the Bose amplifiers were defective – I was chasing down blind alleys with their remote switching and volume control functions,
sure that their lack of output was something I was doing wrong! (Their power
LEDs came on and then slowly went off – the amps weren’t totally dead.)
Finally, consider how you actually use a sound system in a house and develop
a system to suit that application.
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need to refer to?
Photo 9: this is a mock-up design shot of what I hope the finished house will
look like, with the landscaping done.
Another wall plate switch operates
the LD Systems XS-700 subwoofer
amplifier – it’s on a separate switch,
so only this part of the system can be
switched on for home theatre use.
Finally, all the speaker wiring was
made using 3.4mm2 cross-sectional
area low-voltage garden lighting cable
– the cheapest cable I could find that
had plenty of copper cross-section.
It was much cheaper than dedicated
speaker cabling of the same gauge.
The results
So, are we happy? Yes, we are.
The interior system doesn’t have the
subtle nuances of a good hifi system
being listened to from the sweet spot
– but then, with seven distributed
speakers, it never could have. But it
fills the house (or outside deck) with
quality sound and has enough power
to listen at ‘party’ levels. Conversely,
it still sounds good at very low listening levels.
siliconchip.com.au
Despite the presence of the large
subwoofers (and their 700W amplifier), the bass is set to give body and
depth to the sound, rather than bump
thump. In the two main rooms, the stereo imaging is clear, and when walking from these rooms to the hallway,
the transition from stereo to mono is
unnoticeable.
The ability to balance the output
levels of the separate amplifiers also
means that the sound volume doesn’t
change throughout the house.
The outside speakers are ideal
for listening at normal levels and, if
required, can work at much higher levels (however, even in this semi-rural
valley, that can annoy neighbours).
The best aspect of the system is that
operation is seamless; you just flick
the wall switches, connect your phone
via Bluetooth, and play music. The
system was complicated in development and implementation, but in use,
SC
it just works.
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*see website for delivery prices.
June 2026 59
USB Power Monitor Kit (SC7683, $50): includes the PCB and all onboard parts
U Simple
S Power
B Monitor
By Richard Palmer
This circuit uses just a handful of parts but it can
measure USB voltage, current and power over a wide range (up
to 36V, 3A & 108W). It displays the readings on an OLED screen.
Displays USB bus voltage, current, power and energy delivered
Simple and detailed display formats
Supports USB 2.0 and 3.0 power delivery up to 3A/36V
Display settings remembered between sessions
±0.3% voltage and ±1% current accuracy
Display rotation at the touch of a button
Resolution: 100μA, 10mV Serial data logging
W
hile USB-C is slowly taking over,
there are still many devices using
USB-A plugs and sockets.
While our recent USB-C Power
Monitor (August 2025; siliconchip.au/
Series/445) is also capable of measuring USB-A devices with appropriate
adaptors, this project is substantially
simpler – it is basically an update on
the December 2012 USB Power Monitor (siliconchip.au/Article/460) with
higher resolution, modern components and the ability to measure the
wider range of voltages and currents
when the device uses a USB power
delivery (PD) mode.
The monitor has two display modes.
The default shows the USB bus voltage and current flow in large characters. A second mode, with smaller text,
adds the power and the energy that has
been delivered while the unit has been
powered on. The display can also be
flipped upside-down, if required for
more convenient reading.
The unit also provides a TTL-
compatible serial logging output,
shown in Screen 1, which avoids the
need for copying down a long series
of readings when monitoring over an
extended time period.
the many variations and how they
evolved.
In summary, a standard 4-pin USB
1.0 port can supply up to 500mA at
5V. USB 2.0 upgraded the 4-pin standard to 1A. USB 3.0 introduced power
delivery and a 9-pin USB-A connector, which is backwards-compatible
(ie, four of the nine pins are in the
same locations and have the same
functions).
USB-C PD can deliver up to 5A at
20V after negotiation between the
source and sink over the CC (Configuration Channel) pin using BMC signalling. When no negotiation occurs,
Component selection
USB connectors and power
delivery
There are a range of USB port types,
each with its own power capabilities.
The Wikipedia article on USB hardware (https://w.wiki/3oc8) details
60
Silicon Chip
5V is supplied. With USB 3.1, which
is exclusively delivered via USB-C
connectors, up to 5A at 48V can be
delivered.
In suspend mode, when the PC
or laptop is asleep, the host controller stops sending keep-alive (Start of
Frame) signals to devices. This tells
the connected device to go into idle
mode, with a reduced allowable current draw.
A USB device may adopt very different power profiles, depending on
which kind of power source and cable
are used, and whether the host is active
or asleep.
Screen 1: example output of the serial
logging feature in the Arduino Serial
Monitor.
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The monitor uses just three ICs, an
OLED display and a handful of passive components.
The SSD1306 128×64-pixel 0.96inch (24.4mm) I2C OLED screen’s footprint determines the size of the PCB,
with additional strips at the edges to
accommodate the tactile switch (S1)
and USB connectors.
The USB connectors, CON1 and
CON2, are soldered directly to the
PCB. The 9-pin USB-A plug and
socket are compatible with USB 1.0,
2.0 and 3.0 devices. SMD connectors
were selected because very few 9-pin
through-hole versions are available,
making reliable component sourcing
difficult.
Voltage and current measurements
are made by an INA237 power monitor
siliconchip.com.au
USB 3.1 PD Warning
The unit may be damaged with USB
3.1 power delivery modes sourcing
more than 36V. This can occur
when connected to a USB-C power
source designed to deliver more
than 180W, which permits up to 48V
to be supplied.
chip, which has an internal 16-bit
analog-
to-digital converter (ADC),
offering better than ±0.3% accuracy
and providing up to 85V high-side
voltage and current measurements.
The higher-priced INA238 chip
can be substituted, as it is pin- and
code-equivalent. It has better (±0.1%)
current accuracy, which will not
increase the overall accuracy of the
unit, as the shunt resistor’s 1% tolerance is substantially greater.
Through-hole power resistors with
resistances of less than 1W and tolerances better than ±5% are rare and
expensive, so a 1W ±1% M6332 (2512
imperial) low-resistance metal alloy
(LRMA) SMD resistor is used for the
current shunt (R1).
LRMA resistors use a cupro-nickel
alloy and have a very low temperature
coefficient, in the range of ±75ppm
(±0.0075%) per °C, which translates
to less than 0.4% variation across
a working range of 10-40°C. As the
stated temperature coefficient allows
for either a rise or fall in resistance
when the temperature rises, we have
not included temperature compensation in the current calculations.
The shunt resistor value is determined by the 3A maximum current
requirement and the 163.84mV full
scale of the INA237’s ADC. A value
of 0.025W results in 75mV across
the shunt and ¼W dissipation at 3A.
While 0.05W could have been used, the
lower value resistor means reduced
power dissipation and a lower V+ voltage drop without significantly affecting the overall accuracy.
To minimise the effect of any temperature rise on current readings, we
have connected the resistor’s terminals
to as substantial a PCB copper area as
the USB signal traces allow.
As USB 3.0 power delivery mode
can negotiate anything from 5V to 20V
on the V+ USB pin, a 3.3V regulator
with a wide input range is required
to reduce the voltage to drive the circuitry. While both the microcontroller
siliconchip.com.au
The INA237 DC power monitor IC
The INA23x series of DC power monitors offer current, voltage, power and die
temperature measurement (see the diagram below). It has a 16-bit ADC that
is shared by voltage, current and temperature measurements.
The chip can operate at 3.3V or 5V, is controlled over an I2C serial bus and
consumes less than 1mA. Two address pins allow up to four chips to coexist
on a single I2C bus.
Other products in the INA2xx series come with higher-accuracy 20-bit ADCs
or SPI control interfaces rather than I2C.
The current shunt resistor can be located on the high or low side of the load,
as the current input’s common voltage range is -0.3V to +85V. The chip has two
ranges for measuring the shunt voltage, 42mV and 164mV full-scale, providing
flexibility in choosing the shunt resistor’s value to best balance measurement
accuracy and heat generation.
As the chip has a very low input bias current, accurate current measurement from microamperes to kiloamperes is possible anywhere in the permitted input voltage range.
A digital filter rolls off the ADC response at half the sampling frequency to
avoid aliasing measurement errors. The sampling time is individually adjustable for the voltage, current and temperature measurements, ranging from
50μs to 4ms. The chip can average up to 1024 samples, further reducing noise.
Any necessary calculations are undertaken in the background to minimise
measurement lag.
The INA237 also has an alert pin, which changes state when any desired
combination of current, bus voltage, power or die temperature goes outside
set limits.
The INA237 chip includes a shared ADC that measures voltage, current and
temperature. The embedded processor can average up to 1024 readings and
calculate the power figure.
and power monitor chip can operate
at either 3.3V or 5V, 3.3V was selected
to provide headroom for this regulator when operating from a 5V supply.
The MIC5233-3.3 regulator was
selected as it has a small SOT-23-5
footprint, can handle the required
input voltage range and is readily
available. It is connected to V+ on the
upstream USB connector to avoid the
unit’s current consumption being registered by the INA237.
Like with the December 2012
design, no case is required. Instead,
the unit is protected by enclosing it
in a length of clear heat-shrink tubing.
Circuit description
The USB Power Monitor circuit
is shown in Fig.1. Regulator REG1
reduces the input USB input voltage,
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V+ on CON2, to 3.3V for the ICs and
display. Its heatsinking requirements
are not substantial, as the circuit only
draws a few milliamps. It can be disconnected at JP1 while the microcontroller is being programmed.
Power and data signals travel
between the two USB connectors,
CON1 and CON2, with the V+ line
interrupted by shunt resistor R1
(25mW). This resistor translates the
current consumed by the device under
test to a voltage, which is captured
by the power monitor chip’s Vin+ and
Vin− terminals.
The USB V+ voltage is measured
on the CON2 (output) side, so that the
voltage available to the device under
test is correctly displayed.
An ATtiny85 microcontroller operating at 16MHz drives the power
June 2026 61
A TTL serial-to-USB
adaptor (with
the black
PCB) can be
connected
to the Power
Monitor for
logging power-on time,
bus voltage, current
and more.
monitor chip and display. It has a Universal Serial Interface (USI) that can be
configured as an I2C or SPI port. During
device programming, the SPI mode is
used, while under normal operation,
the USI is in I2C mode to communicate
with the OLED and INA237 ADC chip.
The ATtiny85’s I2C interface has
SCL on pin 7 and SDA on pin 5.
Pull-up resistors for these pins are provided by the OLED display. The I2C
bus runs at 400kHz, at which speed
all the required traffic is completed
well within the two-second display
update cycle.
The I2C pins are shared with the
SPI interface used for in-circuit programming (via CON3), which is initiated when pin 1, RESET, is pulled low
by the programmer. When the unit is
booted normally, the code sets the pins
to I2C mode.
Once programming is complete, the
MISO SPI signal (PB1 at ATtiny85 pin
6) is no longer needed in I2C mode.
It is re-assigned as the unused RxD
(receive) serial pin for serial log data,
with the TxD (transmit) logging data
coming from pin 2 (PB3).
Software
When power is applied, the microcontroller initialises the OLED display, which is expected at I2C address
0x3C. The power monitor chip, IC2,
has an address of 0x40 with its A0 and
A1 pins tied to ground.
The resistance of the shunt and the
maximum current to be measured are
provided to the power monitor chip’s
driver software, which calculates
the calibration value for the chip’s
SHUNT_CAL register using the value
of the shunt resistor. Voltage calibration is inbuilt.
The chip is set to sample the current and voltage every 280μs and average them over 1024 readings, which
provides a final set of readings at
approximately 300ms intervals. It provides measurements in signed 16-bit
integer format, which are converted
into floating-point measurements in
software. The display updates once
every two seconds.
Fitting the display driver and font
into the available memory proved
challenging. The microcontroller only
has 8kiB bytes of flash memory program space and 512 bytes of RAM. A
full font would consume more than
the total flash, but for this project, we
don’t need the full ASCII character set.
So large and small fonts were created that contain only the characters
0-9 plus the decimal point, space, “V”,
“A”, “W” and “m” characters.
The usual practice of creating a bitmap in memory and then copying it
to the display would have taken 1024
bytes of RAM. Instead, each line of
characters is converted to bitmap format and written directly, in rows of
eight pixels at a time, to the display.
These 8 × 128 pixel ‘pages’ create
a restriction that a new line can only
start at the top of a new page if the previously written data isn’t to be overwritten. In practice, this means eight
rows of tiny characters, four rows of
medium-sized characters, or two rows
of large characters. Only the two- and
four-row options are used.
The tactile switch (S1) is sensed by
the ATtiny85 on pin 3 with the GPIO
port’s pull-up current enabled. It is
checked once per display cycle. A
press lasting one display cycle changes
between the two display modes, while
a two-cycle press rotates the display
by 180°.
Fig.1: the device uses three integrated circuits, one OLED display module, a shunt resistor and not much else. The circuit
simplicity is mainly due to the features of the INA237/238 being a perfect fit for our needs in this application.
62
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
Serial logging is accomplished by
driving the serial port in software
(bit-banging) as the hardware USI is
occupied with I2C communication for
the OLED screen.
The signal is at 4800 baud with 3.3V
TTL-compatible levels. A TTL serialto-USB adaptor and a suitable terminal
program can be used to view and save
the data. Only the RxD and GND pins
on the serial adaptor need to be connected to the USB monitor. The data is
comma-delimited, including the time
since power-on, USB bus voltage and
current written in the same format displayed on the screen.
PCB design
To ensure minimal voltage drop in
the USB ground return path, the USB
GND pins are connected to the PCB
ground plane as well as having pointto-point copper traces.
The ground plane has been removed
under the USB signal traces to minimise parasitic capacitance, which can
degrade high-speed signals. All the signal traces are of equal length to minimise relative phase shifts.
Parts List – Simple USB Power Monitor
1 double-sided PCB coded 04104261, 44 × 29mm
1 128×64-pixel monochrome 0.96-inch I2C OLED module [SC6176/SC6936]
1 Würth 692112030100 9-pin USB 3.0 SMD plug (CON1)
1 Switchcraft RAHUA30E 9-pin USB 3.0 SMD socket (CON2)
1 2×3 pin header (CON3; optional, for ICSP)
1 3-pin header (CON4; optional, for serial logging)
1 4.5 × 4.5mm, 5mm tall SMD tactile pushbutton switch (S1)
[Altronics S1112A]
1 6-pin vertical 2.54mm-pitch pin header (for mounting OLED module)
1 50mm length of 35-50mm wide (measured flat) clear heatshrink tubing
1 USBasp programmer with 6-pin adaptor and IDC cable
(optional; for ICSP) [Jaycar XC4627 + XC4613]
Semiconductors
1 INA237 or INA238 power measurement IC, VSSOP-10 (IC1)
[Mouser 595-INA237AQDGSRQ1, DigiKey 296-INA237AQDGSRQ1CT-ND]
1 ATtiny85V-20PU microcontroller programmed with 0410426A.HEX, DIP-8
(IC2) [Altronics Z5105, Jaycar ZZ8721 (both supplied blank)]
1 MIC5233-3.3YM5 or MIC1793-330OT LDO 3.3V linear regulator,
SOT-23-5 (REG1) [Mouser MIC5233-3.3YM5-TR]
Capacitors/resistors
2 4.7μF 25V SMD M2012/0805 X7R multi-layer ceramic capacitors
1 100nF 50V SMD M2012/0805 X7R multi-layer ceramic capacitor
1 0.025W ±1% 1W+ M6332/2512 LRMA SMD current-sense resistor
[Mouser LRMAP2512-R025FT4]
Construction
All components mount on the 44 ×
29mm PCB, which is coded 04104261
– see Fig.2. The OLED screen, tactile
switch and USB connectors fit on one
side, with the remaining components
on the other.
The ATtiny85 chip comes in an
8-pin DIL package. While it could be
socketed, that is not recommended
as it will produce a bump in the heatshrink cover on the bottom of the unit.
Leave mounting the OLED until last,
as the USB connectors and in-circuit
programming pins can’t be soldered
in once it is in place.
If you are programming your own
ATtiny85, solder it in and follow the
instructions below. Programming may
be done at this point or after other components have been mounted. If the regulator is in place when programming,
JP1 must be broken to prevent the regulator being reverse-powered and possibly damaged.
Next, install the surface-mount
parts. Begin with the three ICs and
then follow with the passive components. Most of the SMD parts are big
enough not to present too many difficulties. We’ve covered SMD soldering
on many occasions in the past, so we
won’t go into detail here.
siliconchip.com.au
Fig.2: like the circuit, the PCB is simple and assembly is straightforward. Make
sure to mount the screen last, and carefully check all the SMD solder joints,
especially on IC1, before moving on to the through-hole parts.
The INA237/8 power monitor chip
is in a VSSOP package with 0.5mm pin
spacing. If you accidentally bridge any
of the pins, simply use solder wick to
clean it up. A dab of ‘no-clean’ flux
paste applied to the bridge beforehand
makes clean-up easier.
Solder in USB connectors CON1
and CON2 next. I had to lever up the
shield on CON2, as the pins were
unreachable with a soldering iron.
Don’t worry if the shield breaks off.
Once testing is complete, it can be
clipped back on and a couple of dabs
of solder on the top edge will hold it
firmly in place.
At this stage, plugging the unit into
a USB power source should produce
3.3V between JP1 and either of the
grounded USB connector cases.
Mount the OLED display using a
pin header for the connections and
two single pin pieces of header strip
Australia's electronics magazine
soldered through the mounting holes
at the other end of the display to
anchor it. Before soldering, make sure
that the pins on CON3 don’t foul any
components on the OLED module.
Cut all the OLED pins off flush on
both sides.
If logging is required, trim off any
protruding leads from pins 2 and 4 of
the ATtiny85. Remove the middle pin
from the three-pin header and mount
it on the underside of the PCB, parallel to CON2. Extra solder pads have
been provided to make the connections more robust.
Programming the ATtiny85
If you haven’t purchased a pre-
programmed ATtiny85, you will need
programming hardware and software.
While there are many options available, I have found the following to
be straightforward and reliable on
June 2026 63
Screens 2 & 3: the main Zadig screen with the USBasp device selected and libusbK as the target driver (shown at left).
Device Manager showing that the USBasp driver has been successfully changed to libusbK (shown at right).
Windows. For Mac and Linux users,
there are several good online tutorials
for ATtiny85 USBasp programming.
First, purchase the USBasp programmer (see www.fischl.de/usbasp)
from your favourite source. Make sure
it has a 6-pin socket and IDC cable or
includes a 10-pin to 6-pin adaptor.
For Arduino users, complete code is
also included in the download pack.
Board and device settings are listed
at the top of the main program. The
programmer to select is the “USBasp
(ATTiny Core)”.
Otherwise, download and install
AVRDUDESS (siliconchip.au/link/
acb4), which includes the AVRDUDE
command-line programming software.
Next, download and install Zadig
(https://zadig.akeo.ie). Plug in the
USBasp programmer and run Zadig
(Screen 2).
If USBasp doesn’t show in the
device field, click on Options → List
All Devices and select it from the list.
Select libusbK from the dropdown
list that the green arrow points to,
and click on the Install (or Reinstall)
Driver button. Wait for the process to
complete.
Now if you open Windows Device
Manager, you should now see an entry
for libusbK USB devices, similar to the
one in Screen 3.
Programming is undertaken with
the ATtiny85 mounted on the PCB
and the programmer connected to the
ICSP header. No USB cables should be
connected to the USB Power Monitor
while programming.
Everything is now ready to program the ATtiny85. If your USBasp
programmer has a voltage selector
jumper, choose 5V. Open link JP1 on
the Power Monitor board to prevent
reverse-
powering REG1 during programming.
Connect the USBasp and Monitor
boards via the 6-pin connector. Pin
1 (red stripe on the cable) is marked
with a white dot on the PCB. Plug the
USBasp into a USB port on your computer and run AVRDUDESS (Screen 4).
Select “usbasp-clone” from the list of
programmers and select “ATtiny85”
from the microcontrollers list.
Locate the HEX file from the
download package (siliconchip.au/
Shop/6/3621) using the “…” button
to the right of the Flash field. Leave
the EEPROM field blank but change
the “Fuses & lock bits” settings to L =
0xF1, H = 0xD7, E = 0xFF, LB = 0xFF.
The AVRDUDESS window should
look similar to Screen 4.
Click on the Write button next to the
Fuses & lock bits settings, then click
Program! The console panel should
show progress, ending with a message indicating that the flash memory
or fuse bytes have been verified. Disconnect the programmer and re-solder
JP1 to restore the power supply from
REG1. The Power Monitor is ready
for use.
Testing
The unit can now be fully tested.
Plug it into a power source. The display should light up after a second or
so, displaying close to 5V and 0.0A.
Screen 4: this AVRDUDESS window shows the programmer type, target
microcontroller and HEX file selected. Note the values in the “Fuse” and “lock
bits” settings. These need to be written to set the clock speed correctly.
The larger
PCB is one
version of the
USBasp-based
AVR programmer.
Since this one has a
10-pin socket, you’ll need a 10-pin to
6-pin adaptor (shown adjacent), or to
purchase one with a 6-pin socket.
Australia's electronics magazine
siliconchip.com.au
64
Silicon Chip
Press and hold the tactile switch; the
display should change format after a
display cycle.
Plug any USB device into the measurement port. The displayed voltage
should drop marginally, and the current reading should show a non-zero
value. Calibration is not required.
If all is well, the heatshrink sleeve
can be added and shrunk on the outside edges. If header pins were fitted
to CON3, the pins should be trimmed
down to the plastic retainer before fitting the heatshrink tubing.
While large-bore clear heat shrink
tubing isn’t readily available from
the main Australian suppliers, eBay
and AliExpress both have suitable
products. Be careful not to shrink the
tubing too tightly, as the screen rotation switch can become permanently
depressed. If this happens, cut a circle
in the heat-shrink tubing around the
switch’s plunger.
Operation
Operation is straightforward. Simply connect the monitor to a USB
power source and the device to test
into the USB socket on the monitor.
Initially, the unit will display the
USB bus voltage and the load current
in large characters. If the button is
pressed for a display cycle (approximately two seconds), the display will
change to also show the instantaneous
power flow and the total energy that
has been delivered since the unit was
powered on.
The display automatically switches
between amps, watts and amp-hours
and their milli- equivalents when the
current/power/energy reading is low.
If the text on the display is upside
down, hold the switch down for two
display cycles and it will flip.
When logging, always connect
the Power Monitor to its USB power
source before connecting the TTL
serial adaptor. Otherwise, the monitor
may not operate correctly.
The USBasp programmer
connected to the
underside of the Power
Monitor (with a red
colour PCB for the
6-pin adaptor this time.
While an IC socket was
used for IC2 here, we do
not recommend
using one, as it will
produce a bump in
the heatshrink.
The Monitor attached to my
vintage decade resistance
box during testing.
Conclusion
The INA237 power monitor chip
enabled this project to be developed
with a high level of accuracy using
only a few components.
The ability to calculate the energy
consumed and log readings on a
computer extends its usefulness for
devices such as power banks and battery chargers where the load varies
SC
over time.
Here is the Power Monitor connected to my mobile phone from a power
delivery capable charger.
siliconchip.com.au
Australia's electronics magazine
June 2026 65
We have recently started using e-paper displays in our projects. We have looked at
some modules incorporating them before, but this is the first time we’ve integrated
a bare e-paper panel into a design. It was more involved than expected; this article
explains what we did to make it work.
By Tim Blythman
F
or our Human Comfort Indicator project, we decided to use an
e-paper display to achieve low power
consumption with a screen that can be
read at any time. e-paper is readable
in ambient light, so it does not require
a backlight, which could otherwise
have a substantial power requirement.
These screens might also be called
eInk or EPD, where EPD stands for
electronic paper display or electrophoretic display. ‘Electrophoretic’ refers
to the motion of charged or polarised
particles in a liquid medium due to
an electric field.
The laboratory technique known
as electrophoresis involves separating different molecules based on their
size and electrical charge. The common factor is the presence of an electric field affecting charged or polarised particles.
We reviewed a small e-paper module in the June 2019 issue (siliconchip.
au/Article/11668) with a resolution of
200×200 pixels, measuring 1.54 inches
(39mm) along its diagonal. It had an
IL3820 controller and was configured
to use an SPI (serial peripheral interface) bus. We created some demonstration code for the Arduino and
Micromite.
Display controller ICs for e-paper
most operate similarly to LCD and
OLED controllers. They have numerous internal registers to configure the
device and some RAM (random access
memory) that holds a representation
of what needs to be displayed.
The big difference with e-paper
displays is that they are not constantly refreshed, like other display
types. Instead, an explicit command
is required to perform the refresh.
It can take a second or longer, so it
needs to be done under the control of
the software.
Since e-paper needs no power to
maintain its display, the proportion
of time it spends updating will dictate the total and average power consumption. The downside is that it is
difficult to tell the difference between
an e-paper device that is working and
one that has not updated.
Nearly all the e-paper modules we
have seen use an SPI interface. Like
many LCD and OLED controllers,
many can also support I2C or parallel
interfaces, although these may not be
available due to the circuitry used on
the module; they are usually designed
for just one interface type.
With low power consumption being
an important aspect of the Human
Comfort Indicator, we found that many
modules included circuitry that made
this target difficult to achieve, since
they often contained unnecessary circuitry that would waste power. Thus
we had to base our design on a bare
display panel and provide the support
Subcapsule addressing enables
high-resolution capability
Transparent
Top Electrode
Positively
Charged
White
Pigment
Negatively
Charged
Black
Pigment
Clear Fluid
Bottom
Electrode
Fig.1: the operation of an e-paper display with particles having different colours, sizes and charges in a clear medium.
Source: https://w.wiki/7qVD
66
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
Photo 1: the panel we selected includes a controller IC and a display panel
integrated into a COG assembly. It connects via the FFC on the right. Source:
www.buydisplay.com/serial-2-9-inch-e-paper-screen-128x296-for-electronicshelf-label-lcd
circuitry needed to operate the controller.
Fig.1 shows the operation of an
e-paper display. With an electrode on
each side of the panel, it’s easy to set
a pixel by simply setting the electrode
polarity. In practice, the electric field
is pulsed and reversed several times to
ensure that all the particles (which are
smaller than the pixels) are not stuck.
The type of display shown in Fig.1
uses particles with different colours,
sizes and charges moving through a
clear medium; some displays may use
a coloured medium to further expand
the range of colours that can be displayed. There are also variants that use
multi-coloured, polarised particles.
Since the panel uses electric fields
to control the display, the support
circuitry involves generating voltages
above normal logic levels; the panel we
are using spans +20V to -20V. Fortunately, the movement of the tiny particles in the display does not require
much current.
Controller operation
Typically, once the circuit is powered up, you need to initialise the
display controller with some configuration commands, then fill its RAM
with data indicating what to display.
Performing a refresh then sends the
data to the panel.
For low-power designs, the controller can be put to sleep between
refreshes to ensure it uses the least
amount of power. This requires it to
be initialised again before the next
refresh.
The refresh process is controlled by
a look-up table (LUT). This is effectively a simple program that describes
how the panel electrodes are strobed,
for how long, and with what voltages.
siliconchip.com.au
The values in the table depend on the
characteristics of the panel. Some controllers can work with two-colour and
three-colour panels; they will need different LUTs than monochrome panels.
For the module that we reviewed in
2019, the LUT was stored by the microcontroller and sent to the controller
over the SPI bus, as is fairly common.
Some panels also have OTP (one-time
programmable) memory that contain
one or more LUT programs, which can
be used directly by the controller or
automatically loaded.
Sometimes the controller is attached
to the panel glass using a COG (chipon-glass) process. Connecting traces
are made with transparent, conductive ITO (indium tin oxide) material.
In this case, the OTP LUT parameters
are typically programmed by the panel
manufacturer, with the LUT optimised
for the specific panel the controller is
connected to.
Many controllers that we investigated had multiple LUTs, each optimised for a specific temperature range.
An onboard temperature sensor allows
the controller to automatically pick the
correct LUT. This is important because
the temperature of the medium in the
panel affects its viscosity and thus
the rate at which the coloured elements move.
Some (but not all) controllers also
include LUTs for full and fast refresh.
As the name suggests, a fast refresh is
quicker than a full refresh, but it may
show remnants of the previous display
(a phenomenon known as ‘ghosting’).
One trick that we saw in some epaper software libraries is to override the internal temperature sensor
to make it use a faster LUT. In practice, we found this made a negligible difference to the speed we could
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achieve. Suffice to say that there are
many factors involved in refreshing
e-paper displays.
The website www.buydisplay.com
sells a wide range of bare display panels of various types, including LCD,
OLED and e-paper, plus breakout
modules. They also sell many of their
items on eBay. Notably, they provide
detailed data sheets and sample code
for all their modules and panels, so
we found it quite easy to get things
working.
We ordered several panels, breakout boards and modules from them to
suit Arduino and Raspberry Pi boards.
Many of the e-paper panels are fitted
with a 24-pin flat flexible cable (FFC)
connector, so they can be interchanged
with other panels. With this option,
we were able to try several panels easily to see what might work best in our
application.
Best-laid plans
Several three-colour and four-colour
e-paper displays are now available,
and we thought they might be handy
to show different states or conditions.
However, these displays can take up to
15 seconds to perform a refresh, which
we decided was too long.
A multi-colour display consists of
particles with different sizes or charges
that move at different rates through
the liquid layer. Thus, the controller must set each colour in turn and
make sure that the other colours are
not affected, significantly slowing the
refresh process.
A full refresh of a multi-colour panel
typically involves the display flashing
rapidly for a long period before settling on its final output, which would
be quite distracting for a device that
should sit unobtrusively in a home.
Such a long refresh would also tend
to use more power than a simpler
panel. In the end, we decided to keep
things simple and use a monochrome
(black and white) display.
The ER-EPD029-2B is a 2.9-inch
(74mm) e-paper display using the
SSD1680 controller IC. The panel
has a resolution of 296 × 128 pixels,
ample for the information we want to
display. This controller has support
for two sets of LUTs, allowing either
a full or fast refresh without having to
tweak any parameters.
A 2.9in/74mm display is large
enough to be clearly visible, with a 67
× 29mm display area (see Photo 1), and
June 2026 67
the panel is quite well priced relative
to its size. This controller can support
multi-colour displays, but we are using
the monochrome variant.
There is also the ER-EPD029-2R
version that supports a black, white
and red display, which looks otherwise identical.
e-paper circuitry
The glass e-paper panel consists of
the controller IC connected to the display matrix. There are 24 lines brought
out via a 0.5mm pitch FFC. This is connected to a ZIF (zero insertion force)
socket on both the commercial modules and our PCB. As well as providing
the SPI interface for communication,
there are some extra lines that need to
be provided to the controller.
Nine of these lines connect to 1μF
capacitors and bypass various voltages for the controller. There are a
few other components, too. The main
reason they are connected this way is
that it would not be easy to provide
that amount of capacitance on the
glass substrate.
Fig.2 shows the circuit that is
used on the breakout modules that
we tested. This is about the minimum needed to support the display
panel; the modules also include level-
conversion circuitry that is not shown,
so that the module can interface with
Scope 1: the blue trace is the PREVGL line, the red trace is the PREVGH
line, the green trace is the VGH line and the yellow trace is the VSL line (all
shown in Fig.2) during a 1.5-second refresh period.
microcontrollers running at different
voltages.
The circuit around the Mosfet and
inductor is used to generate dual rails
with voltages of up to ±20V. Scope 1
shows the measurements on some of
these lines during a full refresh cycle
on the panel.
This circuitry is managed by the
controller IC, including the drive to
the Mosfet. The GDR line signal (not
shown in Scope 1) starts out at around
300kHz with a duty cycle lower than
Fig.2: the SSD1680 e-paper
controller requires some support
circuitry that can’t easily be
mounted on the panel. That
includes capacitors, a Mosfet and
an inductor.
68
Silicon Chip
Australia's electronics magazine
10%. Once the voltages have stabilised, the driver starts skipping pulses,
presumably to limit and regulate the
voltages.
The PREVGH line is arranged in the
standard boost configuration, with a
0.47W resistor allowing the controller to sense the rising current in the
inductor to limit it safely. The PREVGL
line is created by coupling the switching node to a point between the two
diodes, acting as a charge pump, which
brings the PREVGL line to -20V.
Several internal regulators supply
lines such as VSL (the yellow trace
in Scope 1). You can see the various
regulated voltages remaining steady
despite PREVGL sagging under load.
The data sheet for the SSD1680
controller indicates that the voltages
are as expected and the internal regulator currents are less than 1mA. We
noted that the total 3.3V supply current jumped up to about 5mA, which
seems reasonable. With several internal regulators needing input and output bypassing, it’s easy to see why so
many capacitors are needed.
Fig.2 also shows the six control
lines needed. As well as the three
pins needed for a unidirectional SPI
bus (SCK, MOSI and CS), there is a
reset line and a data/command (D/C)
selector. This is used to differentiate
between commands and display data
when addressing the controller. These
are all common to other display controllers, such as those used for graphics LCDs.
The sixth line is a BUSY signal that
the controller drives when it is busy
siliconchip.com.au
Photo 2: nowadays there are even colour e-paper displays
available. Some, like the Waveshare display shown here,
only provide a select few colours, while others have access
to the full spectrum. Source: www.waveshare.com/product/
raspberry-pi/displays/e-paper/3.97inch-e-paper-hat-plus-g.
htm
Photo 3: Amazon’s Kindle is one of the most well-known
e-paper devices. e-paper devices like the Kindle have very low
refresh rates, typically at 10Hz or less. Source: www.amazon.
com.au/dp/B0CFPL6CFY
refreshing the display and should not
be interrupted. Once the refresh is
completed, the controller can be shut
down by taking its reset line (RES) low
or sending a sleep command.
While it might appear that the controller supports an I2C interface via
the TSDA and TSCL lines, this is not
used by a host to talk to the controller.
Instead, these pins allow an external
I2C temperature sensor to be read by
the controller IC.
The BS1 line can be used to select a
9-bit SPI mode that removes the need
for a separate D/C pin, since the D/C
bit is sent as the ninth bit. We have
no shortage of pins, and the 8-bit SPI
mode is much easier to implement, so
that’s what we used.
Summary
Our experience with the Arduino
display module gave us the knowledge
and experience we needed to design
the hardware and software to work
directly with e-paper display panels.
While it would have been nice to use a
multi-colour display, we did not think
they were suitable for our application;
thus, we chose the monochrome panel
seen in Photo 1.
In another situation, such as a price
tag in a shop, a slower/flickering
refresh would not really be a problem
as it would be updated so infrequently.
A splash of colour would be nice there
(eg, to separate the price from the product name), so colour e-paper displays
clearly suit some applications.
By designing our own hardware, we
have been able to achieve our target of
very low quiescent power consumption. You can see the result of this in
the Human Comfort Indicator project,
SC
which starts on page 43.
Dual-Channel Breadboard
Power Supply
Our Dual-Channel Breadboard PSU
features two independent channels each
delivering 0-14V <at> 0-1A. It runs from
7-15V DC or USB 5V DC, and plugs straight
into the power rails of a breadboard, making it
ideal for prototyping. Photo shows both the Breadboard
PSU and optional Display Adaptor (with 20x4 LCD) assembled.
Both articles in the December 2022 issue – siliconchip.au/Series/401
SC6571 ($40 + post): Breadboard PSU Complete Kit
SC6572 ($50 + post): Breadboard PSU Display Adaptor Kit
siliconchip.com.au
Australia's electronics magazine
June 2026 69
Background source: https://unsplash.com/photos/silhouette-of-trees-under-starry-night-O7FxxiZr-Hk
By Andrew Woodfield, ZL2PD
Micropower
SSB
Single
Side
BAND
Transmitters
This project is an attempt to see how small an HF SSB
transmitter can be made with a minimal parts count. One
of the three versions uses just three transistors while
generating a surprisingly clean signal!
D
uring one of our local radio club meetings a little while ago, someone
tossed a PTT microphone over to
me. “Here, maybe you can use this!”,
they joked. Lacking the usual curly
cord and connector, it had clearly
seen better days. Nevertheless, I took
it home with me and overnight, an idea
came to mind.
The Pixie range of CW (continuous
wave, ie, Morse Code) transceivers is
very well known, as is Doug DeMaw’s
March 1976 Tuna Tin Two CW
70
Silicon Chip
transmitter and George Burt’s “OXO”
three-transistor CW transmitter. Having more interest in QRP SSB transceivers (www.zl2pd.com), I wondered
if an SSB transmitter could be shoehorned inside that microphone shell.
Naturally, only a very low-power
SSB transmitter would be possible,
a design using an absolute minimum
number of parts. As an extra challenge,
I decided to avoid using SMD components or ICs.
The result, for the cost of one more
Australia's electronics magazine
transistor than the famous OXO transmitter, is a small milliwatt-level LSB
transmitter operating close to 3.7MHz
on the 80m band.
Named the “Mike-One”, it uses just
four general-purpose NPN transistors
and a set of low-cost crystals.
In its present form, it will never
achieve transoceanic communications. Instead, covering short distances
across the shack or at the radio club,
it’s intended to be a lighthearted example of minimalist analog design. It’s
also quick and easy to build, so it can
be used as a teaching aid to illustrate
the generation of conventional SSB
signals at a very low cost.
Circuit description
This transmitter is cut to the bone.
As Fig.1 shows, it features a microphone amplifier (Q1), a carrier generator (Q2), a balanced modulator
(diodes D1 and D2), a three-crystal
ladder-type SSB filter, an unusual
‘autodyne’ oscillator-mixer (Q3) and a
single radio frequency (RF) amplifier
stage (Q4). All stages use the generic
BC548 NPN small signal transistor or
one of its equivalents.
The relatively high level audio
signal from the electret microphone
allows a single transistor amplification stage (Q1) to generate sufficient
audio from the microphone to directly
drive the balanced modulator. The
18.432MHz carrier, set by a small 22pF
series capacitor (Cx), is balanced out in
the mixer using VR1, a 100W trimmer.
This arrangement saved several
bypass capacitors that are usually
required in such stages.
siliconchip.com.au
The autodyne converter stage (Q3)
allowed a further useful reduction
in the parts count. This mixer is a
14.7456MHz Colpitts crystal oscillator, amplitude modulated by the
18.4320MHz SSB signal. The output
includes the desired 3.7MHz lower
sideband (LSB) output, the difference
between these two frequencies.
This type of mixer was very common in the first stage of cheap transistor AM broadcast receivers, and
it was also briefly popular in a few
early commercial and amateur radio
VHF FM transceivers. While it saves
a few parts, the output of this mixer
demands a good bandpass filter (L1,
L2 etc) to remove the other unwanted
products, including the 14.7456MHz
oscillator output.
A single π filter at the transmitter
output also contributes to the low spurious and harmonic products of the
design. It serves a secondary purpose
– the output load is unlikely to be a
perfect 50W load. I’ve mostly demonstrated it with just a length of hookup
wire, perhaps half a metre long.
Of course, it will work perfectly
into a good load, but the useful feature of a π filter is that it transforms
the output impedance of awful loads,
such as the very low impedance of my
50cm of hookup wire (less than 1W) or
an off-resonant long wire (possibly a
few thousand ohms) to an impedance
of 25-200W at the collector of Q4. Q4
is most unlikely to suffer damage as
a result.
The bandpass filter (BPF) is designed
to be as flexible as possible to allow for
a variety of crystals, as the following
Photo 1:
MikeThree
(40m
band) is
even less
complex
than the others,
with just three
transistors.
sections will show. In the Mike-One,
the BPF is arranged in a series-parallel
arrangement to reduce the loading on
the autodyne mixer.
The choice of carrier, filter and
mixer crystals is dictated by the current selection of readily available crystals. If your parts bins are well-stocked,
you may prefer to use other crystals.
In the days of analog TV, 6.552MHz
crystals were widely available, as
were 10.245MHz crystals for converting 10.7MHz intermediate frequency
(IF) signals to a second IF of 455kHz.
This combination will also produce
an 80m LSB signal close to 3.685MHz.
In this case, the carrier frequency sits
at the lower corner of the crystal filter passband. This means that capacitor Cx in Fig.1 is replaced by a 15μH
RF choke (RFC1 in Fig.2). This lowers the carrier crystal frequency to
6.5500MHz. I’ve named this version
the Mike-Two.
The different array of outputs generated by the autodyne mixer requires
a slightly different BPF, but the output
LPF remains unchanged.
The Mike-Three
By this stage, I could see a way to further reduce the number of parts used
in these first two versions. Mike-Three
is an example of an ‘on-frequency’ SSB
transmitter that avoids the need for the
mixer stage. This time, it produces a
7.2MHz LSB signal on the 40m amateur band (Fig.3) with just three transistors. These crystals are also very
widely available.
Mike-Three uses the same PCB as
the others, but with fewer components,
as shown in Photo 1.
Construction
All three versions can be built on the
same small single-sided PCB, which
was designed to fit into the prototype
push-to-talk (PTT) microphone case
(see Photo 2). This style of PTT microphone has been made in very large
numbers by many manufacturers over
Photo 2: an
otherwise
useless PTT
microphone
lacking a
cord was the
inspiration
for this
tiny SSB
transmitter.
Fig.1: the Mike-One circuit features a basic three-crystal SSB filter, along with
an unusual autodyne oscillator-mixer stage to minimise the parts count.
siliconchip.com.au
Australia's electronics magazine
June 2026 71
the years. It’s fairly likely you can lay
a hand on a suitable microphone without much difficulty.
In case you can’t, I’ve created STL
files so you can 3D-print one!
To fit everything in the limited
space, almost all resistors are mounted
on-end. The PCB is coded 06103261
and measures 44.5 × 76.5mm. Refer to
the overlay matching whichever version you are building – Fig.4 for MikeOne, Fig.5 for Mike-Two or Fig.6 for
Mike-Three.
Start by fitting all the resistors and
capacitors, then proceed to fit the
parts to complete each stage, one by
one, testing each completed stage as
you proceed.
T1 is made by twisting three 120mm
lengths of 0.25mm enamelled copper
wire (ECW) together. Two or three
twists per centimetre is all that is
72
Silicon Chip
required. Wind eight turns of this ‘trifilar’ triple wire arrangement onto an
FT37-43 toroidal core. The toroid may
be replaced by a similar-sized toroid
recycled from an old fluorescent lamp.
I found a less expensive approach
to winding T1: wind four trifilar turns
of 0.25mm ECW on a low-cost ferrite
bead. Avoid ferrite beads with a small
1.5mm hole. They can be used, but
it’s quite difficult to get all that wire
through the small centre hole. I had
some ferrite beads with a 2mm hole,
which allowed for the required turns
to be achieved far more easily.
The material used to make these
ferrite beads can vary enormously, so
this may not work for you with your
parts and your carrier frequency. Using
the FT37-43 toroidal core is the most
reliable option.
When the toroid or ferrite bead has
Australia's electronics magazine
been wound, identify the start and end
of each winding. These are numbered
on the circuit diagrams and PCB overlays to help with construction. Solder
one set of three wires into the holes
marked 1, 3 and 5 in any order. Now,
using a continuity tester or ohmmeter
with an audible continuity (‘buzzer’)
function, identify each of the matching ends for each wire, one by one, and
solder them into the correct matching
holes, marked 2, 4 and 6.
L1 and L2 are inexpensive 7×7mm
unshielded variable inductors. These
have 26 turns and a range of 3-6μH.
The similar-looking inductors with
only about 12 turns (0.6-1.7μH) cannot be used here. However, if you buy
them by accident, just rewind them
with the required number of turns.
They will work just fine.
The BPF has been designed to allow
siliconchip.com.au
Fig.2: Mike-Two uses a 6.552MHz
carrier and filter crystals, along
with a 10.245MHz mixer crystal to
give SSB on 80m. Besides the crystal
changes, some capacitor values have
been altered, and the BPF has been
reconfigured.
Fig.3: the circuit of the ultra-simple
40m Mike-Three SSB transmitter.
The crystals change again, plus
some capacitor and inductor values.
In addition, the autodyne mixer and
its associated band-pass filter have
been removed and bypassed.
either a series-parallel BPF (Mike-One)
or a coupled BPF (Mike-Two). The relevant PCB overlays show the location
of the wire added to configure these
correctly. Other arrangements are possible with this PCB layout for those
wanting to experiment further.
L3 is made by winding 27 turns
(Mike-One or Mike-Three) or 15 turns
(Mike-Two) of 0.375mm enameled
copper wire onto a T37-6 core. However, a less expensive solution is to
use a 2.2μH RF choke (Mike-One or
Mike-Three) or an 820nH RF choke
(Mike-Two). Both methods gave similar results for me.
In the case of Mike-Three, no mixer
or bandpass filter components are
fitted or required. This time, a short
jumper wire connects between two
empty capacitor pads, as shown in
Fig.6. However, the output pi filter
siliconchip.com.au
Figs.4-6: the PCB overlay diagram for ▶
the Mike-One (top), -Two (middle)
and -Three (bottom) variants; use the
component values and locations shown
here to build each version. There are
some small component differences
between each diagram such as the
crystals and lack of mixer circuitry.
should still be fitted to ensure any
spurious and harmonic products are
minimised, and to deliver some useful impedance matching.
The PCB mounts component-side
down in the case, with the electret
microphone (MIC1) soldered on the
solder side of the board. I used several
drops of hot-melt glue at the top edge
and the PCB corners to hold it in place.
3D-printed microphone shell
While the microphone shell shown
is readily available, it’s likely some
readers will still find it difficult
to locate or expensive. For that
reason, I’ve also designed a lowcost 3D-printed version, shown in
Figs.7(a)-(d). In this version, the electret mic capsule mounts on the same
side of the PCB as the other components. You can download the STL files
from siliconchip.au/Shop/11/3582
The case is in four parts: lower,
middle and upper sections, plus the
‘pressel’ lever. The lever’s hinge fits
into the mating slot in the middle section. I used a 10mm-long scrap of copper wire to hold the lever in place on
one version, and a cut-down 1.6mm
panel pin (ie, a small nail) on another.
This assembly is then placed on the
back shell of the microphone. Three or
four drops of hot glue will hold these
together. Avoid getting any glue near
the pressel.
Australia's electronics magazine
June 2026 73
The transmitter PCB can then be
inserted into place – component-side
up this time – and a drop of hot glue
applied at the top edge to hold it in
place. The battery, LED and related wiring can now be added, and the length
of wire to be used for the antenna also
connected to CON2 and fed through
the antenna hole in the shell.
The upper shell of the microphone
may then be placed on top of the
assembly. Three 20mm-long self-
tapping screws hold the microphone
case together.
Alignment
Depending on the crystals you use
and the version of the transmitter you
are building, you will need to mount
either a small capacitor, Cx/Ca, or an
RF choke, RFC1, in the top-right corner
of the PCB. Nominal values for these
parts have been shown in Figs.1-6. This
allows the carrier crystal frequency to
be at the upper or lower corner of the
SSB crystal filter respectively.
The values shown (22pF, 15μH
or 18pF) were found to be best for
the prototypes, and are likely to suit
most applications, but your crystals
may require slight changes. Values
are likely to be in the range from 4.722μH for RFC1, and 10-33pF for Cx/
Ca. You can listen to your signals on
an SSB receiver to confirm the audio
quality is reasonable and the opposite
sideband is nearly inaudible.
L1 and L2 should be adjusted for
maximum transmitter output. These
have a reasonably broad tuning
response. Of course, this step is not
required for the Mike-Three.
VR1 in the balanced modulator
should be adjusted to give minimal
carrier output in the absence of modulation. This setting is very sharp and
will be close to the midpoint of the
adjustment range of the trimmer.
I built all the prototypes using a variety of crystals, which delivered about
0dBm into 50W with a carrier suppres-
Photo 3: this version uses Cx to set the
correct carrier frequency (PCB upper
right), a ferrite bead for the balanced
modulator (PCB centre), and an RF
choke for the LPF (PCB lower edge).
Photo 4: Mike-One uses more crystals
than transistors! The narrow bandpass
filter required for SSB demands at
least three crystals, while the carrier
oscillator and mixer add two more.
sion of 40dB or better, and 30-40dB of
unwanted sideband rejection. This latter value depends on the audio modulation frequency. All spurious and
harmonics were attenuated by 50dB,
and many by as much as 60dB.
The second method I tested used
a small A23 or A27 12V alkaline battery. An A27 battery has a diameter of
just 8mm and a length of 28mm. The
capacity of an alkaline A27 battery is
about 30mAh. While modest, it proved
ideal for the original microphone shell.
I also tried fitting a slightly larger
A23 battery (the holder is visible in
Photo 3).
The higher A23 or A27 battery voltage of 12V is perfectly OK for the transmitter. Usefully, it also allows a blue or
red LED to be fitted in series with the
supply wiring to CON1. The supply
voltage at the transmitter is dropped
by almost 3V by a blue LED and by
about 2V by a red LED. The LED is lit
during transmit mode and its brightness gives an approximate indication
of the battery level.
Power supply options
If you are building the Mike-One
in a small box rather than in a microphone, you can use a standard PP9
type 9V battery. The transmitter only
draws 15mA, so the battery will last
for quite a long time.
Fitting a battery in the limited space
available inside the microphone shell
presented a challenge.
One approach tested used a small
recycled 3.7V 70mAh Li-Po cell and
a tiny boost converter module. This
gave a very reliable 9V supply.
Figs.7(a)-(d): this 3D-printed
microphone shell has been
designed for those unable to
locate a suitable microphone shell.
74
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
A23/A27 battery holders
Battery holders for these tiny A23
and A27 batteries are not always
readily available. Faced with this,
I designed and printed a simple
3D-printed holder for each type,
shown in Fig.8.
The battery contacts were fabricated
from a pair of M2.2 solder tags. I filled
the hole normally used for a bolt with
a film of solder.
These were pressed through the
3D-printed battery holder from the
inside and held in place by the battery
and the slight tension of the holder.
I placed some clear adhesive tape
around the battery before inserting it
to make it easier to replace.
Parts List – Micropower SSB Transmitter
Fig.8: the 3D-printed 12V
battery holders provide a
low cost solution to fitting a small
battery inside the microphone shell.
1 single-sided PCB coded 06103261, 44.5 × 76.5mm
1 electret microphone (MIC1) [Altronics C0170, Jaycar AM4011]
1 PTT microphone shell, salvaged or 3D-printed
3 M3 × 20mm self-tapping screws (for 3D-printed case)
1 A23 or A27 12V battery
1 3D-printed battery holder
2 2.2mm solder lugs (for 3D-printed battery holder)
1 2-pin header (CON1; optional)
1 PCB-mounting right-angle tactile pushbutton, 6×6mm, 6mm-long actuator (S1)
[Jaycar SP0607 or AliExpress 1005007559876628]
1 FT37-43 toroidal core (T1)
[www.minikits.com.au/FT37-43, AliExpress 1005009245292057] OR
1 4mm OD, 2mm ID, 5mm-long ferrite bead (T1) [Altronics L5250A]
1 360mm length of 0.25mm diameter enamelled copper wire (T1)
1 100W top-adjust trimpot (VR1) [Altronics R2605]
3 BC548 30V 100mA 300MHz NPN transistors (Q1, Q2, Q4)
1 red or blue 3mm LED (LED3)
2 1N4148 75V 200mA signal diodes (D1, D2)
various lengths of light/medium-duty hookup wire
Capacitors (all 50V radial ceramic)
6 100nF
2 10nF
3 1nF
2 100pF
2 33pF
Resistors (all ¼W axial ±5% or better)
1 1MW
1 2.2kW
1 220kW
1 1kW
3 10kW
1 470W
1 3.3kW
1 47W
Extra parts for both Mike-One & Mike-Two
2 3-6μH 5-pin variable inductors on 7×7mm formers (L1, L2)
[AliExpress 1005008114591102]
1 2.2μH axial RF choke (L3) [Jaycar LF1514, Altronics L7014] OR
1 T37-6 toroidal core (L3)
[www.minikits.com.au/T37-6, AliExpress 1005005686909567] AND
1 400mm length of 0.375mm diameter enamelled copper wire (L3)
1 BC548 30V 100mA 300MHz NPN transistor (Q3)
1 100nF 50V radial ceramic capacitor
1 100pF 50V radial ceramic capacitor
2 56pF 50V radial ceramic capacitors
1 22kW ¼W axial resistor (±5% or better)
1 6.8kW ¼W axial resistor (±5% or better)
1 4.7kW ¼W axial resistor (±5% or better)
Extra parts for Mike-One only
4 18.432MHz HC-49 crystals (X1-X4)
1 14.7456MHz HC-49 crystal (X5)
2 330pF 50V radial ceramic capacitors
2 47pF 50V radial ceramic capacitors
1 10-33pF 50V radial ceramic capacitor (Cx, nominally 22pF; see text)
Extra parts for Mike-Two only
4 6.552MHz HC-49 crystals (X1-X4)
1 10.245MHz HC-49 crystal (X5)
1 4.7-22μH axial RF choke (RFC1, nominally 15μH; see text)
2 680pF 50V radial ceramic capacitors
1 330pF 50V radial ceramic capacitor
1 150pF 50V radial ceramic capacitor
1 22pF 50V radial ceramic capacitor
Extra parts for Mike-Three only
4 7.2000MHz HC-49 crystals (X1-X4)
1 820nH axial RF choke (L3)
2 47pF 50V radial ceramic capacitors
1 10-33pF 50V radial ceramic capacitor (Ca, nominally 18pF; see text)
siliconchip.com.au
Australia's electronics magazine
Wiring
The wiring is straightforward; it’s
shown clearly in all three circuit diagrams, Figs.1-3. In brief, run a red wire
from the battery + to the LED anode
(longer lead), an orange wire from the
LED cathode (shorter) lead to the + terminal on CON1 and a black wire from
the – terminal on CON1 to the battery
– terminal. Also refer to Photo 3.
Operation
This is not a complicated transmitter
to use! Just press the PTT button and
talk. Your LSB signal will appear very
close to 3.7MHz or 7.2MHz, depending
on the version you’ve built.
While the range is not massive when
using a short length of hookup wire
for the antenna, the signal is quite
audible in nearby receivers. Usefully,
the design is such that many popular
data modes can also be tested with
the transmitter, and further amplifier
stages can be added if desired.
In short, Mike-One (or Two or
Three) will allow you to quickly, easily and inexpensively enjoy a short yet
rewarding voyage on the QQRP ultralow-power HF seas. I hope you enjoy
making and using one (or more!) of
SC
these little SSB transmitters.
June 2026 75
SOnline
ilicon Chip
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Rotating Lights
April 2025
USB-C Power Monitor
August-September 2025
USB Power Adaptors
May 2025
SMD LED Complete Kit
SC7462: $20
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SC7463: $20
Short-Form Kit
SC7489: $60
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This kit includes everything needed to build
the Rotating Light for Models, except for a
power supply and wire.
This kit includes all non-optional parts, except
the case, lithium-ion cell and glue. It does
include the FFC (flat flexible cable) PCB.
You can choose from one of four USB sockets
(USB-C power only, USB-C power+data, mini-B
or micro-B). The kit includes all other parts.
DCC Base Station
Short-form Kit
SC7539: $90
Complete Kit
with choice of USB socket
SC7433: $10
PICKit Basic Power
Breakout Board
September 2025
January 2026
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Mic the Mouse
Complete Kit
SC7508: $37.50
August 2025
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everything
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one Mic the
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solder, glue and a
CR2032 cell.
Complete Kit
SC7512: $20
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Includes the PCB, all onboard parts and a
length of clear heatshrink tubing. Jumper wire
and glue is not supplied.
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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.
The iClap intelligent multi-clap switch
I spent some time searching for a
simple yet efficient clap switch circuit
to build for some rooms in my house.
I finally surrendered to the old proverb, “on n’est jamais mieux servi que
par soi-même” (you are never better
served than by yourself).
It isn’t that I found no clap light
circuits, but many had the same pitfall: false triggering from accidental
sounds. Adding a microcontroller
gives some intelligence to the whole
circuit, as it provides more flexibility
to adjust parameters without changing the hardware. Sensing more than
one clap also reduces the probability
of false triggering.
One may expand this idea to use
different numbers of claps to perform
multiple functions.
The circuit uses a small electret
microphone, fed into a minimalist (yet
very sensitive) discrete amplifier. The
output of that amplifier drives the GP3
input of the PIC10F200, which has no
analog-to-digital converter (ADC) or
siliconchip.com.au
comparator; it’s just a digital microcontroller.
The PIC micro is normally in sleep
mode and wakes up on a pin level
change if the clap produces a pulse
with an amplitude greater than 2.4V
(as GP3 is a TTL-type input). Within
the next two seconds, if another clap
is detected, the light is switched on
using relay RLY1. The same sequence
is used to switch it off.
Digital output GP2 drives the coil
of the low-power 24V relay through
transistor Q2, a general-purpose NPN
bipolar transistor. The rest of the circuit is a classic transformerless capacitive power supply to produce the 24V
and 5V rails. Capacitor C1 must be an
X2 (or X1, Y2 or Y1) type for safety
reasons. As it is somewhat bulky, we
have chosen to use a 24V DC coil relay,
rather than 12V or 5V, to reduce the
coil current, hence reducing the current that C1 must supply.
We may choose a relay with NO/
NC contacts to switch between a
Australia's electronics magazine
high-power bulb (active state) and a
much lower power bulb (idle state)
if we don’t like dark rooms. Another
option is that, after activating the relay,
an internal countdown starts, and after
45 minutes, it will automatically deactivate the relay (in case someone leaves
the room and forgets to switch it off).
The fully commented assembler
source code takes less than 100 words.
It is not optimised to make it easier to
understand, in case it is worth being
translated to another type of microcontroller. You can download the software
from siliconchip.au/Shop/6/3567
Hichem Benabadji,
Oran, Algeria. ($85)
Note: this project operates at mains
potential and must be fully isolated
from contact. That includes the
microphone that needs to be located
well inside an enclosure and the LED
shouldn’t protrude through the enclosure without a fully covering bezel.
The enclosure must be Earthed if it
is metal. For a plastic enclosure, no
metal parts should be exposed on the
outside of the enclosure.
June 2026 77
Interruptible NiMH battery trickle charger with memory
This circuit uses discrete parts to
trickle charge a pair of AA NiMH cells
from a USB source. One of its interesting features is that it remembers the
charging time if you unplug it from
the USB source but don’t remove the
cells. If you plug it back in again, it
resumes charging, meaning the total
charge time will still be limited even
if you charge the cells across several
sessions.
The timer is reset when you remove
the cells and insert a different set, or
re-insert the same ones later. It could
be adapted to suit AAA cells by adding extra PCB mounting points for a 2
× AAA cell holder and changing the
value of the 10W resistor that determines the charging current.
It’s designed to be plugged into a
USB socket for power (no data connection), and charges whenever that
USB socket supplies power (as shown
78
Silicon Chip
in the photo at upper right). After
27.5 hours of charging, it stops supplying current to the cells and flashes
the LED.
The timer has two chips that function as ‘memory’, remembering how
long the cells have been charging for
(IC3 & IC4). These two chips can be
‘battery backed’ by the cells being
charged since they are 74HC logic
chips that can operate with a supply
as low as 2V.
When plugged into USB, current is
supplied to the cells via NPN transistor Q10. A 10W resistor in its collector
circuit senses the charge current and
the voltage across that is fed to the base
of Q7, while similar transistor Q6 has
its base set to the divided output of a
2.5V reference (REF1) that’s connected
to the USB supply. The result is that
the voltage across the 10W resistor is
regulated to 1V.
Australia's electronics magazine
That means the charge current is
limited to 100mA (1V ÷ 10W). Since
the emitters of Q6 & Q7 are connected
to ground through Mosfet Q9, charging
only occurs when Q9 is switched on.
That’s controlled by logic gate IC3b.
Its output is high as long as either pin
5 or 6 of IC4a is low. IC4a is the end
of a counter chain.
When USB power is applied, IC1 is
clocked by a 32,768Hz crystal oscillator. It divides that by 16,384 to produce
a 2Hz signal at pin 3, which is used
to flash the LED. However, the LED
can’t flash during charging because it
is forced on by Mosfet Q8, so it only
flashes when the charge current has
been switched off.
Pin 1 of IC1 divides the crystal frequency by 4096 to produce an 8Hz signal that’s fed to the clock input of IC2.
IC2 divides it by 4096 again, producing a signal at its pin 1 that has a cycle
siliconchip.com.au
Ideal Bridge Rectifiers
Choose from six Ideal Diode Bridge
Rectifier kits to build: siliconchip.
com.au/Shop/?article=16043
28mm spade (SC6850, $30)
The charger PCB uses a Type-B USB socket as they are robust. You can see the
cell holder underneath the board.
time of 512 seconds. This is gated by
the cell charge voltage and then fed
to IC3c and IC3d, into pin 13 of IC4b.
This pin only toggles every 512 seconds if charging is occurring.
IC4b divides this signal by 16 times
to give a cycle time of 8192 seconds or
about 2¼ hours. That’s fed into another
counter, IC4a, and with the way IC3b
is configured, the signal from its pin
6 to stop charging will go low after 27
hours and 18 minutes.
Once charging stops, you have to
power cycle the circuit by removing
the cells and USB power before it’ll
charge again.
Russell Gurrin,
Highgate Hill, Qld. ($100)
siliconchip.com.au
21mm square pin (SC6851, $30)
Compatible with PB1004
10A continuous (20A peak),
72V
Connectors: solder pins on
a 14mm grid (can be bent
to a 13mm grid)
IC1 package: MSOP-12
Mosfets: TK6R9P08QM,RQ
5mm pitch SIL (SC6852, $30)
Compatible with KBL604
10A continuous (20A peak), 72V
Connectors: solder pins at
5mm pitch
IC1 package: MSOP-12
Mosfets: TK6R9P08QM,RQ
IF signal injector
To align certain radios (eg, the
Sailor 66T navigation radio on
p88), you need a way to connect an RF sweep generator to
the first IF transformer without
damping its primary coil. This
injection needs to be done in a balanced/differential manner. The
circuit shown here does just that,
allowing you to sweep and check
the IF bandpass frequency response.
For many transistor radios, a
sweep generator is not required
because all the coils can be peaked
on the centre IF frequency (455kHz
in most transistor radios).
The radio is often designed to
have the correct overall bandpass
response in that condition. However, this is not always the case for
radios with double-tuned IF transformers, such as the Sailor 66T.
The circuit for the adaptor I made
uses a Jaycar LO1234 25mm toroidal ferrite core with two 12-turn
windings made using enamelled
copper wire approximately 0.5mm in diameter. Each winding has
an inductance on the
order of 200μH.
In the unloaded condition (without the
Compatible with KBPC3504
10A continuous (20A peak),
72V
Connectors: 6.3mm spade
lugs, 18mm tall
IC1 package: MSOP-12
(SMD)
Mosfets: TK6R9P08QM,RQ (DPAK)
mini SOT-23 (SC6853, $25)
75W termination resistance on the
secondary), the loading on the generator’s 75W output resistance at
470kHz is negligible.
The 75W termination resistor on
the secondary makes sure that there
are no spurious resonances. The
high-value series resistors ensure
that the primary of the first IF transformer is not damped or affected by
the connection of the adaptor.
One thing that helps significantly
with winding toroidal cores is to
wrap Scotch 27 cloth (fibreglass)
tape around the core. It stabilises
the position of the wires and makes
for a much better result.
Dr Hugo Holden,
Buddina, Qld. ($80)
Width of W02/W04
2A continuous, 40V
Connectors: solder
pins 5mm apart
at either end
IC1 package: MSOP-12
Mosfets: SI2318DS-GE3 (SOT-23)
D2PAK standalone (SC6854, $35)
20A continuous, 72V
Connectors: 5mm screw
terminals at each end
IC1 package:
MSOP-12
Mosfets:
IPB057N06NATMA1
(D2PAK)
TO-220 standalone (SC6855, $45)
40A continuous,
72V
Connectors:
6.3mm spade lugs,
18mm tall
IC1 package: DIP-8
Mosfets:
TK5R3E08QM,S1X
(TO-220)
See our article
in the December
2023 issue for more details:
siliconchip.au/Article/16043
Australia's electronics magazine
June 2026 79
SERVICEMAN’S LOG
Music to my ears
Dave Thompson
It may seem obvious to many regular readers that I am ‘into’ music.
Or perhaps it isn’t that obvious, but rest assured, I am into it! So, not
surprisingly, a lot of the gear I’ve fixed over the years has been related to
musical instruments and hifi equipment.
I both listen to and play music, and I have done so since I
was eight years old, when I was taught piano by an elderly
Hungarian Jewish man who lived just around the corner.
He was a very good player and a very good teacher. He had
some stories to tell about the war years – which were likely
heavily sanitised for my tender young ears!
Sadly, he passed away a few years after I started, so I
changed teachers. That killed my piano-playing career. What
it did teach me is that having the right teacher is crucial.
While I still play instruments today, I don’t play any of
them anywhere near as much as I used to, or should.
As for listening to music, I have my favourites, of course,
but am not averse to listening to anything new coming along.
I know what I like (usually within seconds of starting), so
these days I stick with what I know, or I check out recommendations from others I know who have similar tastes
(that includes some of the folks producing this magazine).
All that said, I am definitely not one of those guys with
a library-sized collection of vinyl, playing them on an
audiophile-
level home audio system.
You know
80
Silicon Chip
the ones, with those thousand-dollar-per-metre speaker
cables made from unobtanium and Mars dust.
My earliest dabbling in electronics – with a lot of help
and encouragement from my dad – was with simple oscillators, crystal radio sets and very basic amplifiers. It fast
became a keen interest, and the more I got into it, the more
I saw music-related potential.
I don’t think I was alone with these interests either, if
the number of music-related projects in the magazines of
the day was anything to go by. I took it as a sure sign that
others were as keen as I was, and I was proven right.
There was even a relatively short-lived magazine out of
England that featured just that: electronics, current music
technology and really cool projects for musicians. I have
every copy stored away somewhere, but there weren’t that
many with that first-generation theme before it morphed
into something that wasn’t of much interest to me. Publishing is tough in any field, time period, or country!
It seemed every month, one magazine or another would
have an interesting music project. I must have built many
dozens of them (mostly on prototype boards); some useful,
some just gimmicks. Still, it was all educational and much
grist for my mill back then.
Making projects kept me busy while I should have been
practising, but I had a lot to learn, and so I was very eager
to do both as much as I could.
I saved all my newspaper delivery money (then my parttime after-school job earnings) to buy these magazines and
then the relevant components for projects. I still have
large stacks of the mags in storage (and components!).
Sadly, the magazines will likely end up in the recycling bin if I can’t give them away.
I’ve seen many people trying to pass on complete
collections of magazines and libraries worth of books
over the years, but the modern age, with much of it digitised retroactively anyway, what’s the point in keeping
vast collections, other than just that – collecting them? It
seems such a waste, but it’s just reality.
Years ago, as a wee tacker, I made everything from tone
boosters, fuzz boxes, wah pedals and metronomes until,
after a while, I was making increasingly complex projects such as my own stereo amps, preamps, full-blown
PA amps, speaker cabinets, mixing consoles, guitar/bass/
keyboard amps, microphones, wireless systems and guitars themselves.
I wanted to be able to record music at home, on a computer, and that’s where this music rabbit-hole led me.
Australia's electronics magazine
siliconchip.com.au
Back in those days, the go-to home recording device, if
you could afford one, was something like a Tascam or a
Fostex four-track, which recorded onto standard cassette
tapes. They were pretty good for their day, but as we know,
cassette tapes aren’t the best for audio quality, especially
if they were used to ‘dub’ or ‘bounce’ many tracks down
into one track a few times.
The step up from there was into a reel-to-reel four-track or,
if you owned a corporation, an eight-track reel-to-reel that
used half-inch tape. They had much better audio quality.
Fun fact: The Beatles’ album Sgt. Pepper’s Lonely Hearts
Club Band was recorded on just two Studer J37 four-track
recorders (using one-inch tape), synched together electronically by audio engineers, at what later became Abbey
Road Studios. This shows what could be accomplished in
1966 with some very good gear and much lateral creative
thinking, producing and mixing.
Those cassette-based four-track recording machines
were very much a 1980s child and, as they were relatively
affordable, they launched the imaginations of many and
the possibility of a viable home recording studio.
All was well then, but recording at home is not just a
matter of grabbing some digital audio workstation (DAW)
software from the interwebs, plugging in your microphone,
keyboard or guitar to your computer and laying down a
new number-one hit single.
While you’d think that the computer already has analog
inputs to allow instrument/microphone/line connections,
the CPU has to work hard to crunch that signal into a digital
form so the computer can process, store and manipulate it.
You might be surprised to know that most built-in
‘sound cards’ - while most are built onto the motherboard
now, people still call them sound cards – are pretty much
useless for doing any studio-level sound processing. Yes,
they can record speech and basic mic audio, but there are
inherent problems.
For example, if you want to monitor recorded audio
through headphones while multitracking, there is a delay
between input and output signals as the computer struggles to keep up. This is called latency and makes onboard
sound unsuitable for multitrack recording, where there
must be minimal latency between in and output signals.
So, an external sound interface is usually the way to go.
These typically connect via USB or Thunderbolt, operating
similarly to an accelerated graphics card in that the interface handles all the audio heavy-lifting for the computer.
To do this, a special driver is needed, called an ASIO
driver (Audio Stream Input/Output). This was developed
by the Steinberg company in the late 1990s specifically to
Items Covered This Month
• Musical instruments and USB ASIO card repair
• Repairing a Simpson Contessa washing machine
• A powerless Li-ion charger
• Small replacements for a Dyson fan
• Fixing a Samsung TV
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
siliconchip.com.au
reduce latency and allow the processing of multiple concurrent audio streams.
Usually, these drivers are supplied with the interface, or
available as a download or, at a push, a generic freeware
ASIO driver. Interfaces cost anywhere from under a hundred bucks to several thousand, depending on what you
want. My Line 6 Toneport UX2 is almost vintage now, yet
still cost me 500 bucks second-hand in 2003. It still works
perfectly for my needs – or it did until recently.
It is connected permanently to my PC and acts as a normal sound card when just listening to music or watching
YouTube, but it’s when all the audio inputs are utilised
with a DAW that we really see and hear the difference.
The problem now is its age. All the pots are scratchy, some
of the sockets are intermittent, and it is just not right. So I
decided that it was finally time to do something about it.
The beauty of this era of music gear is that it really is
‘analog’ and it was designed with repair in mind. Typically,
clamshell plastic or metal cases were screwed together with
normal screws, meaning easy disassembly. All the sockets
utilised in most pedals and music gear are standard components, most of which are still available.
However, this unit is interesting in a few different ways.
Disassembling it was odd from the start; after turning it over
multiple times (no doubt with a puzzled look on my face),
I simply couldn’t see how it was held together. There are
no obvious screws underneath. I even popped one of the
four glued-on rubber feet off to check for hidden screws
(as is typical of many laptops) but I found none.
I thought maybe that the four rotary controls (two independent mic input gains, headphones volume and output
level) located on the top half of the case might actually be
holding it all together. However, when I popped the knobs
off, I saw that Line6 had simply extended the pot shafts up
through the top of the case, so they actually didn’t hold
down anything at all. Interesting...
It turns out there are no screws and no clips; just a friction fit that holds the top half of the case to the bottom,
although the front and back panels also play a vital part.
Australia's electronics magazine
June 2026 81
It’s always a little scary when applying pressure to something that might be clipped or screwed (oh for a small X-ray
machine!) but it eventually let go and eased apart with gently increasing pressure.
This left the top of the PCB exposed, with the front and
back panels still engaged in a slot that runs around the
edges of both halves of the case. It’s a purposely tight fit
and, when the case is assembled, it all holds itself together.
Given that this is designed to sit on a desk and not go on
the road, this is an elegant (and likely cheaper) way of
holding it all together.
Both the front and back panels are an odd but very cleverly implemented two-layer lamination. These consist of
the screen-printed, outward-facing coloured fascia, and
behind it, a very thin metal laminate, which is no doubt
added for shielding and grounding. Between them, they
fill the slot around the case edge perfectly, with a pleasing, ever-so-snug interference fit.
It has obviously been carefully thought out by the designers and well-implemented by the manufacturers (what we
pay the bigger dollars for, I suppose).
The back panel is held onto the PCB by a raft of 6.35mm
82
Silicon Chip
(¼-inch) jack sockets and a sole RCA socket. These are
the line in, footswitch, S/PDIF and analog output sockets.
I never use those anyway, except for the USB connector
(which utilises the older, but still widely used USB-B type
connector), so I left that panel alone; there was no point
in taking it off.
The multi-layer PCB itself is packed with assorted sockets, pots, a couple of backlit, olde-worlde analog VU meters
and what looked to be about a million SMD components
distributed in between the bigger parts. I decided to remove
the front panel, mainly for easier access to some of the sockets and switches that live right behind it.
The PCB was held to the panel by the barrel nuts and
black plastic washers of three 6.35mm jack sockets and four
(surprisingly long) machine screws holding on to two Canon
XLR sockets. Both socket types are the universal standard
for plugging instruments and microphones into audio gear.
There are two guitar inputs (one normal and one ‘padded’
for hotter inputs) and a headphone jack output. Removing the barrel nuts on the jacks exposes some interesting,
thick, multi-pinned plastic locating washers that hold the
jack sockets fast into the front panel without any risk of
Australia's electronics magazine
siliconchip.com.au
the socket turning (as often happens with chassis mounted
versions of these same sockets), as shown in the photo.
More importantly, this locking system prevents the transference of any cable pressure or tension directly onto the
fragile PCB. One common mistake I’ve made myself many
times before is to forget I’m plugged into something and
walk away, blissfully unaware that when the length of the
cable runs out, some huge stresses are going to be inflicted
on those poor sockets at either end.
I’ve done this with power tools, laptops, mobile phones,
headphones and guitars. We’ve likely all done it!
The two XLR connectors are solely for microphone inputs
and have two screws per socket. The only other control
on the front panel is a push-on/push-off phantom power
switch for sending 48V DC to the microphones (if needed).
They must have a decent DC/DC converter in there to
take 5V from USB and be able to send 48V (admittedly only
up to a maximum of 10mA of current) to power up to two
connected active microphones.
Once it was all open, I sat it on a plastic box, plugged the
USB cable into my workshop computer, and my headphones
into the output to monitor what was happening. Then I
worked on the potentiometers. All four were scratchy and
felt gritty, so I gave them a good squirt of contact cleaner
while rotating them from end to end, making sure the entire
track got a decent wet wipe.
They quietened down a lot, and as there is no obvious
dust inside the interface, it was likely worn pot track debris.
I gave them another few blasts once this lot had dried.
I moved on to the jack sockets. These are mostly enclosed
by hard plastic mouldings, so getting access to the contacts inside was a problem. The barrel nuts on the outside
of the socket are easy enough to tickle up, as they need to
be taken off anyway, but I replaced them before cleaning.
If these ferrules aren’t electrically clean, there’s not a lot
of point doing the rest.
What I needed was a means of cleaning the contacts inside,
at least where jack plugs would touch. To this end, I took
a timber dowel and glued very fine (1200 grit) wet and dry
sandpaper around it, making it a snug fit inside the socket.
After spraying the sandpaper with contact cleaner, a few
gentle ins-and-outs and a twist or two cleaned the relevant
surfaces, at least as much as I wanted to use abrasives on
them. Then I blew out any debris after the cleaning rod work
and sprayed with more contact cleaner to flush things out.
Left: a Line
6 Toneport
UX2 audio
interface.
Removing
the barrel
nuts on the
headphone
jacks reveals
multi-pinned
plastic antirotation
washers.
siliconchip.com.au
Australia's electronics magazine
June 2026 83
I repeated this on all the sockets and manually polished anything I could see and access with my diamond
contact file.
I cleaned the XLR connectors (not that I use them) with
a bamboo skewer soaked in contact cleaner. It was the perfect size to fit in the holes in the socket. The probe came
out clean anyway, so I considered that done.
That was about as far as I could go with it. Other than the
pots and sockets, there really are ‘no user-serviceable parts
inside’. The audio tests after that were a lot better, but not
perfect as far as the pots went. However, I wasn’t too keen
on the prospect of desoldering anything from this circuit
board, especially a through-the-board pot.
For the amount of use this device gets now, I can live
with it. At least now I know that if the pots continue to give
me trouble, I can get the device apart easily enough and
replace them. Fingers crossed it doesn’t come to that. The
sockets all seem to be working well now, so I reassembled
everything in reverse order for a final test. All was good,
which was music to my ears!
Simpson Contessa 425 washing machine repair
I refurbished a Simpson Contessa 425 washing machine
about four years ago. Since then, it has worked well. I had
to repair the spin solenoid around two years ago (described
in Serviceman’s Log, October 2022).
Lately, it has been leaking water. This was not a major
drama, as the machine is on the back verandah and the
small amount of water just ran off the concrete onto the
grass. It was more of an annoyance than anything.
I had been meaning to check where the water was leaking,
but every time I noticed it leaking, the machine was in use
with water in it. I finally co-ordinated troubleshooting with
my wife. I needed to pull the machine out and remove the
back panel so that I could see exactly where the leak was.
With the machine pulled out and the back panel removed,
we added some water, and I could see that it was the water
pump that was leaking. Water pumps are one component
that I do have spares of, so I was confident I could find a
replacement.
I recalled that we had previously used a Simpson 7.5kg
machine that was computer controlled. We used it for several years until the computer failed, so that was not economically repairable and it went to the boneyard.
I located the machine and removed the pump. I then
removed the pump from the 425 and compared them; they
were completely different. The original pump was much
longer and had the inlet on the top, whereas the possible
replacement pump was much shorter and it had the inlet
on the end. Therefore, the original drain hose was too short.
But maybe I could use the hose from the 7.5kg machine.
I went back to the boneyard and retrieved the inlet hose.
Then it was time to see if the later-model pump and hose
would fit in the older machine. I first checked to see if the
bolt holes in the pump would line up with the holes in the
back of the machine where the pump mounts.
On the 425, there were four holes for mounting the pump;
two of them lined up with the bolt holes in the replacement pump, so that was OK. After bolting the pump into
the machine, I fitted the inlet hose to the pump and then
to the bowl. It fitted correctly, with plenty of clearance to
the pulley on the bottom of the bowl, so the pump transplant was a success.
I decided to change the outlet hose at the same time, as
the old hose had previously had some leaks in it, which
had been repaired with duct tape. While this had been
successful, I thought that the newer hose looked better, so
I would use it.
I connected the replacement hose to the pump and
noticed that the new hose was a slightly smaller diameter, so I had to change the fitting where the outlet end of
the hose is connected to the grey water disposal pipe, but
that was easy and I then replaced the back panel. With
the machine back in use, there were no more water leaks.
The reason these old pumps leak is that the seal where
the motor shaft enters the pump wears out. This is a special type of seal that is not available as a spare part. I have
previously repaired these old pumps by swapping parts
between them, like swapping a good motor onto a good
pump, but there’s only so much I can do without being
able to obtain spare parts.
Bruce Pierson, Dundathu, Qld.
Ozito QL09009A 5-cell lithium-ion battery charger
The original (longer) Simpson Contessa 425 washing
machine pump is shown above. The replacement pump is
below, with the inlet located at the end.
84
Silicon Chip
This Ozito battery charger had no output. It is a conventional flyback design using an AP8263 IC. The secondary
side has an LM358 dual op amp that monitors the charging
current and alters the drive to the feedback optocoupler to
vary the output voltage of the charger.
Australia's electronics magazine
siliconchip.com.au
From left-to-right: the AM05 & AM07 motor control boards; a brushless DC hair dryer motor; the drive signal from this
hair dryer motor.
There is a P-channel Mosfet in series with the output,
which was not being switched on, hence the lack of output.
There is also an unmarked 8-pin IC that seems to monitor
the battery charging and drives a three-pin LED, giving a
red or green light. Another output of this IC drives an NPN
transistor that should switch on the Mosfet.
I decided that the mystery IC was faulty, so I forced the
Mosfet on by shorting out the NPN transistor. That got the
charger working again. I assume the Mosfet was supposed to
be turned off if the charging current got too high or charging
took too long. It would help if the IC could be identified.
Roger Sanderson, Fig Tree Pocket, Qld.
Dyson bladeless fan faults (AM05 & AM07)
The brushless DC motor circuit drive boards in these
Dyson fans use a Power Integrations LNK304D buck regulator to produce 15V or 5V for the control ICs from the 350V
DC rectified mains. Unfortunately, this part fails, feeding a
destructive voltage through to the low voltage parts, particularly the microprocessor.
Power Integrations now has an LNK3204D, which hopefully is more reliable.
Replacement boards for these fans cost around $200, so
it is questionable whether it is worth repairing them. Of
course, the microprocessor that holds the software is not
available as a spare part.
I am looking at using an alternative brushless DC motor
control board to power the fans. There are low-cost controller boards available, but they are designed to drive
low-voltage motors. They have a built-in switch-mode
converter to provide a low voltage for the motor and drive
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
the story is about as long as it’s in some way related to the
electronics or electrical industries, to computers or even to
cars and similar.
We pay for all contributions published but please note that
your material must be original. Send your contribution by
email to: editor<at>siliconchip.com.au
Please be sure to include your full name and address details.
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circuit from the AC mains. To use them, the motor would
also need replacement.
Attached are photos of the AM05 and AM07 control
boards. The AM05 uses an SMA6823 to drive the motor,
while the AM07 uses individual Mosfets.
I am also investigating using a brushless DC hair dryer
motor from AliExpress to replace the motor and driver in
a Dyson bladeless fan.
Note that the drive signal on one of the three phases is
not continuous, but is in bursts. The driver board provides
three levels of airflow. As the airflow is increased, the driver
pulse width increases, but the pulse rate stays the same.
Roger Sanderson, Fig Tree Pocket, Qld.
Samsung TV fixed the IT way
We have a Samsung TV (UA55CU8000) and sound bar
(HW-Q600C). One evening, as my wife settled down to watch
one of her programs while I was occupied in another room,
she called out that the sound was “not working properly”.
When I came to check, I could see that using the remote
would bring up the numerical data on-screen for the volume setting but it was obvious that the volume was not
changing. As a quick fix, I jumped into the TV menu and
enabled the TV speakers while disabling the sound bar. This
worked, seemingly indicating a problem with the sound bar.
The next day, I switched on the TV and re-enabled the
sound bar. The remote still had no effect, but now the volume was changing, slowly upwards, without me doing
anything! As part of my fault-finding process, I decided
to transfer the sound bar to the small TV in the kitchen
and see what happened. Well, of course it worked properly, didn’t it!
I put the sound bar back while glaring sideways at the
now-suspect TV. While I was doing this, the old computer
adage of “Have you tried turning it off and on again?” came
to mind. Since no modern piece of electronics is ever turned
completely ‘off’, I pulled the power cord out of the back of
the TV, waited a while and plugged it in again.
When I turned it on again, everything worked correctly
and has continued to work since. When we thought about
it, earlier that evening we had a momentary mains power
glitch, probably a little less than half a second. This appears
to have addled the TV set’s brain, and a full power reset
got it straightened out again.
SC
Ian Malcolm, Scoresby, Vic.
Australia's electronics magazine
June 2026 85
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$10 MICROS
$15 MICROS
ATmega328P
ATtiny45-20PU
ATtiny85-20PU
110dB RF Attenuator (Jul22), Basic RF Signal Generator (Jun23)
2m VHF CW/FM Test Generator (Oct23)
Graphing Thermometer (Mar26), Simple LC Meter (May26)
Simple USB Power Monitor (Jun26)
PIC12F617-I/P
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-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), Human Comfort Indicator (Jun26)
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
HUMAN COMFORT INDICATOR (SC7646)
(JUN 26)
Kit: includes all parts, except the case and battery (see p49, Jun26)
- white 3D-printed case: portrait (SC7453) or landscape (SC7684) version
- 3.3V GY-BME280 module (SC5482)
PINBALL MACHINE KITS
(JUN 26)
$60.00
$12.50
$10.00
(JUN 26)
Kit: includes the PCB and all onboard parts (see p63, Jun26)
- 0.96in 128x64 cyan OLED screen (USB Power Monitor, Jun26; SC6176)
- 0.96in 128x64 white OLED module (USB Power Monitor, Jun26; SC6936)
μDCC DECODER KIT (SC7617)
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)
$50.00
$10.00
$10.00
(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)
$25.00
$45.00
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
STEPPER MOTOR DRIVER KIT (SC7601)
(APR 26)
CALLIOPE AMPLIFIER PARTS (SC6021)
(APR 26)
DCC BOOSTER / REVERSE LOOP CONTROLLER KIT (SC7579)
(MAR 26)
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)
(FEB 26)
MAINS HUM NOTCH FILTER (SC7598)
(FEB 26)
Includes all required parts, except for the case and wire/cable (see p63, Feb26) $35.00
Includes everything except for the case and power supply (see p53, Feb26)
$150.00 DCC BASE STATION KIT (SC7539)
Control Board (SC7659): includes the PCB and all non-optional onboard parts
Power Supply (SC7680): includes the PCB and all onboard parts
$50.00
Cable & Connector Set (SC7681): includes 17 10-pin box headers, 34 10-pin IDC
connectors, 10m of 10-way ribbon cable, 30 2-way pluggable terminal blocks
and 20 2-way polarised headers
$65.00
SIMPLE USB POWER MONITOR (SC7683)
siliconchip.com.au/Shop/
DCC REMOTE CONTROLLER KIT (SC7552)
$35.00
$15.00
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
RGB LED STAR KIT (SC7535)
(DEC 25)
DCC DECODER KIT (SC7524)
(DEC 25)
EARTH RADIO KIT (SC7582)
(DEC 25)
RP2350B COMPUTER
(NOV 25)
Includes the mostly-assembled board and all non-optional components
except the power supply (see p43, Dec25)
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)
$80.00
PICKIT BASIC POWER BREAKOUT KIT (SC7512)
(SEP 25)
RP2350B DEVELOPMENT BOARD
(AUG 25)
Includes all parts except the jumper wire and glue (see p39, Sep25)
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)
MIC THE MOUSE KIT (SC7508)
(AUG 25)
USB-C POWER MONITOR KIT (SC7489)
(AUG 25)
Includes all non-optional parts except the case, cell & glue (see p39, Aug25)
*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.
$25.00
$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)
Includes all parts except a CR2032 cell (see p64, Aug25)
$45.00
$7.50
$50.00
(JAN 26)
$90.00
$7.50
$5.00
$20.00
$30.00
$1.00ea
$37.50
$60.00
PRINTED CIRCUIT BOARDS & CASE PIECES
PRINTED CIRCUIT BOARD TO SUIT PROJECT
SECURE REMOTE SWITCH RECEIVER
↳ TRANSMITTER (MODULE VERSION)
↳ TRANSMITTER (DISCRETE VERSION
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)
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
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PCB CODE
10109231
10109232
10109233
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
01111241
01103241
9047-01
07112234
07112235
07112238
04111241
9049-01
09110241
09110242
09110243
09110244
04108241
9015-D
15109231
Price
$5.00
$2.50
$2.50
$2.00
$2.00
$2.00
$1.00
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$2.50
$2.50
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$2.50
$20.00
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$15.00
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$5.00
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$2.50
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$5.00
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$2.50
$2.50
$10.00
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$10.00
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$2.50
$2.50
$7.50
$7.50
$5.00
$15.00
$5.00
$10.00
$7.50
$5.00
$5.00
$2.50
$2.50
$5.00
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$2.50
$2.50
$2.50
$2.50
$5.00
$5.00
$2.50
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PRINTED CIRCUIT BOARD TO SUIT PROJECT
POWER LCR METER
WAVEFORM GENERATOR
PICO 2 AUDIO ANALYSER (BLACK)
PICO/2/COMPUTER
↳ FRONT & REAR PANELS (BLACK)
ROTATING LIGHT (BLACK)
433MHZ TRANSMITTER
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TOOL SAFETY TIMER
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USB POWER ADAPTOR (BLACK, 1mm)
HWS SOLAR DIVERTER PCB & INSULATING PANELS
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433MHz RECEIVER
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DUCTED HEAT TRANSFER CONTROLLER
↳ TEMPERATURE SENSOR ADAPTOR
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MIC THE MOUSE (PCB SET, WHITE)
USB-C POWER MONITOR (PCB SET, INCLUDES FFC)
HOME AUTOMATION SATELLITE
PICKIT BASIC POWER BREAKOUT
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GRAPHING THERMOMETER
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Price
04103251
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$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
09111247
$1.50
04103261
$2.50
01304261
$2.50
01104261
$15.00
PINBALL MACHINE CONTROL BOARD
↳ POWER SUPPLY
↳ PLAYER LED BOARD
↳ SCORE LED BOARD
↳ LED OUTPUT BOARD
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↳ GENERAL INPUT BOARD
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SSB TRANSMITTER (MikeOne/Two/Three)
SIMPLE USB POWER MONITOR
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JUN26
JUN26
08107261
08107262
08107263
08107264
08107265
08107266
08107267
08107268
08107269
08107260
08117261
08117262
06103261
04104261
21105261
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$5.00
$2.50
$5.00
$5.00
We also sell the Silicon Chip PDFs on USB, RTV&H USB, Vintage Radio USB and more at siliconchip.com.au/Shop/3
Vintage Radio
The Sailor 66T Navigation Radio
This radio was very popular in the 1960s, 1970s and 1980s. Primarily,
it was deployed for radio navigation in the North Sea between Norway
and Scotland, as well as being used in the North Atlantic prior to
modern GPS navigation systems. It was made by Danish company SP
Radio Aalborg.
By Dr Hugo Holden
T
his article is more about the radio
itself than its radio direction finding (RDF) applications. However,
numerous radio navigation and radio
direction finding systems existed in
the past that no longer do because satellite navigation (eg, GPS) has taken
over.
The RDF system briefly discussed
here was called Consol. The navigator takes a direction reading by rotating their radio’s direction finding (DF)
antenna to receive and null signals
emanating from a specific fixed radio
beacon on land. By taking bearings
from only two known radio beacons,
then plotting those on a chart, the
navigator can determine the vessel’s
position.
The DF antenna typically consisted
of a ferrite rod and tuned coil that
could be rotated manually. Loops can
88
Silicon Chip
also be used. When the long axis of
the ferrite rod is aligned with the axis
of the beam from the beacon, there is
a signal null. This is called a ‘relative
bearing’. However, the rod could be
pointed either towards or away from
the beacon due to its figure-8 sensitivity pattern.
To get around this 180° ambiguity
and make a ‘relative determination’,
there is a “Sense Switch” on the radio’s
front panel. When deployed, the
switch combines some of the received
signal from the main antenna, which
is omni-directional. This creates a cardioid sensitivity pattern.
Therefore, when the ferrite rod is
rotated 90° to a signal maximum, the
combined result is more sensitive in
one direction than the other. The navigator can combine the information
with compass readings too.
Australia's electronics magazine
For North Sea navigation, one radio
navigation beacon was on 266kHz in
Bushmills on the north coast of Northern Ireland, and another on 319kHz at
Stavanger, on the coast of Norway – see
Fig.1. They had a typical transmission
range in the order of 1000 nautical
miles (about 1850km).
The beacons transmitted their carrier waves as dots in one sector (sector A) and dashes in another (sector
B) during the direction-finding transmission period.
The transmission period for direction finding is 60s with a one-second
pause, then the station call sign is
transmitted for six seconds. Most of
the remainder is a long dash (heard
as a long tone due to the radio’s BFO)
for 50 seconds, followed by a three-
second pause.
The DF information repeats again,
siliconchip.com.au
Photo 1: the connection panel for the
radio is utilitarian, but it provides
everything you need.
Photo 2: when the optional speaker
box is mounted, the connection panel
is inside it.
Photo 3: the loudspeaker is a quality
unit.
so the entire cycle takes 120 seconds.
The speed of the rotation is one sector
width per 120 seconds.
For example, if you were in the position marked × in Fig.1, you would hear
48 dots of the remaining A sector and
12 dashes from the B sector from the
Stavanger Beacon in Norway as the
beam passes by your location. On the
other hand, you would hear 28 dashes
and then 32 dots when the beam from
the Bushmills beacon passes.
Aside from the internal battery pack,
three more DC power options can
be selected using an internal rotary
switch for 12V, 24V or 32V operation
– see Photo 4 overleaf.
The radio sports a nice audio amplifier with two good-sized Philips
transformers, each with a 10 × 10mm
cross-sectional core area, visible below
the switch. Just beside the upper
(output) transformer on each side
are the two AC128 output transistors
mounted to heat-conducting fins. The
audio output is rated at 1.8W.
Also in Photo 4, at the bottom, is a
large power stud-type 9.1V zener diode
(BZZ19) mounted on a 4mm-thick, 6
× 8cm black-painted aluminium heatsink. This is because the voltage regulator design for the external power
Features of the 66T receiver
Apart from its RDF capabilities, it is
a highly sensitive and capable superheterodyne radio receiver. It can be
powered from an internal battery pack
of six D cells in a battery box on the
right side of the radio housing.
When the attached speaker box
option is not used, the radio’s power
input panel, shown in Photo 1, is simply screwed onto the left-hand side of
the radio. However, when the accessory speaker box is used, this panel
sits on standoffs that attach the speaker
housing to the radio’s housing and is
attached with thumb nuts, as shown
in Photo 2.
To remove these, the speaker and
the front panel retaining it must be
removed.
The speaker box has a hole in its
rear to allow the main antenna connection to pass through. The speaker
is a high-quality four-inch (102mm)
unit – see Photo 3. Interestingly, it
is mounted on a timber baffle, which
likely improves the damping in the
cabinet a little.
siliconchip.com.au
×
Fig.1: the locations of the two main radio beacons for the North Sea area. The
radial sectors provided a way to determine the ship’s location based on the
signals received from both stations.
Australia's electronics magazine
June 2026 89
Photo 4: from top
to bottom, you
can see the power
selector switches,
output transformer
flanked by the output
transistors, phase
splitter transformer
and power regulator
zener diode.
Photo 5: the dial is
large and clear. Note
the index mark and
calibration marks.
option for this radio is a shunt regulator design. The excess input voltage is
dropped across a substantial ceramic
wire-wound power resistor.
While that might seem inefficient to
some, the beauty of it is that it makes
the power supply and radio highly
resistant to electrical abuse such as high
voltage transients on the DC supply,
because the zener diode snubs them
off. It also prevents accidental reverse
polarity accidents because it conducts
in the forward direction in that case.
More complex series pass voltage
regulator circuits are more easily damaged, often requiring TVS protection
devices or other protective parts.
The radio can operate on four bands:
• Long-wave (LW): 150-285kHz
• Navigation band (NW): 255425kHz using the DF antenna input
• Medium-wave (MW): 5251600kHz
• Short-wave (SW): 1.6-4.2MHz
The 66T has a very attractive glass
dial with a well-calibrated scale for
each band (see Photo 5). The dial
contains some additional markings
that are very helpful in performing an
alignment (calibration) of the radio.
While the calibration frequencies were
mentioned in the manual, I could not
find any mention of the critical index
mark in the text. Having said that, I
did not have a fully translated manual.
The index mark controls the
mechanical relationship of the dial
pointer to the three-gang variable
capacitor. That relationship in my
radio was badly off, making calibration
90
Silicon Chip
and tracking impossible until it was
corrected.
Photo 6 shows the general architecture of the radio. The rear section
of the 3-gang variable capacitor is the
one that tunes the set’s local oscillator and its associated inductances for
each band. The middle section tunes
the inductances associated with the
RF stage, and the front section tunes
the inductances associated with the
antenna circuit.
Notice the bends in the outer adjustment wings of the rear (oscillator) section of the variable capacitor; these are
discussed later.
Another notable feature of this radio
is the 470kHz intermediate frequency
(IF) amplifier board. This uses double-
tuned IF transformers.
On some versions of this IF board,
the first IF transformer had an additional small coil added to its primary.
It was a signal injection point labelled
H. This was so that a low output resistance sweep generator could easily be
connected without damping the tuning on the first IF coil.
However, in later versions, such
as my radio, that coil was dispensed
with, and instead, two test points, corresponding to “Test point H”, were
provided across the first IF transformer primary. This is a very high-
impedance zone. I had to make a special adaptor to drive it, as will be discussed briefly in the alignment section.
There was a note in the manual:
“Never touch the intermediate frequency alignment unless proper
Australia's electronics magazine
measuring equipment is available” (by
this they mean a sweep generator and
scope). In this radio, if the IF tuning
slugs are simply peaked at 470kHz,
the overall bandwidth is far too low
and the recovered audio modulation
is therefore very muffled and lacking
in high-frequency components.
General specifications
The radio weighs in at 8kg. The
sensitivity of this radio is very good
on the SW band, giving 50mW output
for only 3μV RF input, specified with
30% audio modulation.
The IF bandwidth is specified as
6.5kHz. This can only come about with
correct tuning of the double-tuned IF
transformers, as will be outlined in
the alignment section. The image suppression was specified as an excellent
50dB or better at 2.2MHz.
The audio frequency response is
stated as 100-3000Hz (without the
filter switched in). I found this a little
restrictive. I reduced the value of a filter capacitor to widen the frequency
response in the audio section, which
made music listening better.
In keeping with many transistor radios like this, the current consumption is amazingly low at around
40-150mA depending on the volume
setting. The six D cells in the battery
carrier have a very long life. On external power, due to the nature of the
shunt zener voltage regulator, the current consumption is 400mA.
The radio’s signal-to-noise ratio was
specified in the manual. To measure
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this requires an output signal from a low-impedance
source (25W) and the use of
a dummy antenna. This will
be described in a later section.
The radio also contains five
quartz crystals for fixed-frequency
reception. In my radio, the crystals
fitted were for 2182kHz, 1792kHz,
1834kHz, 1841kHz and 1848kHz. The
crystals are housed in a row on the
lower rear chassis (see Photo 7).
Circuit details and factory
modifications
There were a number of revisions of
the circuit by the manufacturer. The
first 66T set was series A, then going
all the way to series K with small
changes. After series A, most of the
schematics are very similar except
that after series A, an extra switch
gang was added to switch the two
local oscillator signals (crystal versus
the four tuned bands) as separate signals into the mixer circuit.
After series B, the RF amplifier was
modified. It turned out that either electrostatic discharges (lightning) or RF
output power from the ship’s transmitter via the antenna could fry the BF115
RF amplifier transistor. The general
approach to this sort of problem is to
use diodes to protect the transistor.
Interestingly, in some of their earlier versions, they had a diode in
series with the base of the RF amplifier transistor, likely to augment the
AGC rather than to protect the transistor. Although a large positive signal
impulse would tend to reverse-bias
the diode, the diode’s reverse breakdown voltage is not enough to protect
the transistor from very high voltages.
No such diode was used in series
B. Then they added a diode across the
base-emitter junction of the BF115, as
explained in the manual (translated
from the original Norwegian):
“Since we have received complaints
that the RF transistor in some receivers burns out due to static electricity
on the antenna or RF voltage from the
transmitter, we have introduced protection for the transistor in future production runs. The protection consists
of a silicon diode mounted across the
base-emitter junction of the RF transistor.”
The RF sections of the series C circuit are shown in Fig.2. This one corresponds to my radio. I have highlighted
important sections with boxes.
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Photo 6: the chassis layout is neat. You can clearly see the three-gang variable
capacitor on the left; I bent some of the plates on the lower gang to improve the
tracking.
Photo 7: the five plug-in crystals for
fixed-frequency tuning. They have
matching coils and capacitors.
Photo 8: the capacitors that match the
crystals shown in Photo 7.
Potentiometer R2 is the “Sense–
Balance” preset, which is accessible
through a hole in the front panel, just
beside the Sense Switch. In my radio, a
green LED power light had been placed
in that hole. Its appearance and that
of the wiring to it suggest it was done
by the manufacturer, but it was only
operational on external power.
Australia's electronics magazine
June 2026 91
RF amplifier
Diode mixer
RF ▲
Sense preset potentiometer (R2)
▲ OSC
Channel selector switch*
92
Silicon Chip
Crystal oscillator
Oscillator for SW, MW,
NW & LW bands
Band selector switch*
I switched the LED over so that it
runs whenever the radio is powered
from any source. It is good to have,
because when the radio is powered
by batteries, it is all too easy to leave
it accidentally switched on.
As noted previously, the Sense system creates a mix between the signal
received by the DF antenna and the
main antenna to create an asymmetry
in the reception sensitivity so it can
be used for unambiguous direction-
finding. The Test H inputs are used to
couple in the sweep signal for aligning
the IF amplifier. This arrangement is
not as ideal as the earlier version with
the small coupling coil.
Fig.2 shows the whole circuit for the
66T. The left-hand of the circuit shows
the coil sets and the top end tuning
capacitor for the SW- band. The other
coil sets and tuning capacitors for the
other bands (three for each band: the
antenna coil, RF coil and oscillator
coil) are connected to the empty positions on the rotary switches.
For the fixed crystal reception frequencies, there are five crystals with
an antenna coil and RF coil associated with each crystal channel. In this
case, fixed polystyrene tuning capacitors are used for the antenna and RF
470kHz double-tuned IF amplifier and AM detector
stages. The arrangement here accounts
for 10 coils in total and 10 fixed tuning capacitors associated with them.
These capacitors, two for each of
the crystal channels, are mounted
vertically on the side of the chassis,
as shown in Photo 8.
BF115 silicon transistors are used
in both of the oscillators and the RF
amplifier. AF127 germanium transistors are used for the IF amplifier. The
specifications of both parts are excellent. The BF115 is a spectacularly good
silicon planar epitaxial transistor. Its
transition frequency is in the order of
230MHz, and it has a low noise figure
of 1.2dB at 1MHz.
The AF127 belongs to a family of
parts that replaced the AF11x series
of transistors, which are now prone to
failure from tin whiskers. Fortunately,
the AF12x series of parts does not suffer from these problems.
The AF127 is a diffused-alloy transistor, with a transition frequency of
75MHz. It is a very capable part for RF
and radio work, with a low noise figure
of 1.5dB. One of its very useful features
in IF amplifier applications is that it
has a very low feedback capacitance,
only in the order of 1.5pF. This means
it can work as a stable IF amplifier
Australia's electronics magazine
without requiring neutralisation.
On the other hand, older-generation
germanium RF parts, such as the OC45,
had feedback capacitances in the order
of 10pF and always required neutralisation feedback components added to
be stable in an IF amplifier application.
One would therefore expect the
performance (especially noise and
sensitivity figures) of a radio such as
the 66T to be very good on account of
the very capable RF, IF and oscillator
transistors.
Certainly, the sensitivity figure specified for the SW band being less than
3μV input for 50mW output is very
good. The signal-to-noise (S/N) ratio
is specified at 10dB below 1MHz with
a 10μV signal and a dummy antenna.
The AGC system is shown on the
right of Fig.2. It feeds a separate line
to the RF amplifier and the first IF
amplifier. A separate preset is used to
adjust the AGC for the RF amplifier.
The front-panel RF gain control affects
both the AGC to the IF and the RF
amplifier. The specified performance
is that an increase in RF input voltage
from 31μV to 100mV will increase the
output by less than 10dB.
The radio’s metal chassis is independent of the actual positive and negative
siliconchip.com.au
AGC amplifier and signal meter driver
Audio preamp and
audio output
see text
★
★
Front panel RF PCB preset
gain (R46)
(R49)
◀
★
◀
nfb
AGC RF
Signal meter
BFO
Shunt zener
regulator (D7)
Dial lamp
* Crystal array, select switches and
10 associated coils and five crystal –
two coils (L15 & L16) and one crystal
E shown
* three-gang 500pF variable capacitor,
nine coils and nine top-end tuning
capacitors: coils L1-L3 and capacitors
C1-C3 shown – SW band
supply power system, only bypassed
to those with capacitances. So the
radio could be mounted in a vessel
that had either a positive or negative
ground power supply system.
In my radio, I made some modifications to three capacitor values in the
audio system, shown with purple stars
in Fig.2. One problem I encountered
was a noisy volume control, which
persisted even after substituting in a
new control and renewing the coupling capacitors.
I changed both the capacitors
around the volume control to low-
leakage 1μF axial tantalum capacitors. I could have used film capacitors,
but I had no axial types of that value
that fit the PCB well. Reducing the
10μF capacitor, leading away from the
control, to 1μF substantially reduced
low-frequency noise with control
rotation. It did not degrade the audio
low-frequency response.
In this circuit, the resistances are
such that the frequency response, even
with a 1μF capacitor (rather than the
10μF value), does not reach -3dB until
it is below about 20Hz.
The 22nF capacitor in the base circuit of T9 resulted in fairly heavy
audio high-frequency roll-off, muffling
siliconchip.com.au
Input power conditioning
Fig.2: the radio’s circuit. It uses a 470kHz IF and has five sets of
crystals/coils/capacitors for quick fixed-frequency tuning. The audio
stages, AGC system, BFO and power supply regulator sections of the
66T radio are shown on the right-hand side of the circuit.
the sound somewhat. That may well
have been OK for voices but not so
much for music. For a better tone balance, I reduced that value to 1.5nF.
I could not find anything else that
required changing. In terms of faulty
parts, the only capacitor that I had to
replace was C100, a 400μF electrolytic
that I replaced with two parallel axial
220μF parts. The original had gone
high in ESR, resulting in a motorboating effect with low-frequency oscillations in the audio.
The audio amplifier in the radio is
quite capable and gives a good sound
with the speaker in the speaker box.
The amplifier has negative feedback
to reduce distortion, and audio transformers with good-sized iron cores.
Conveniently, SP Radio provided
the results of injecting signal voltages
at different test points in the radio,
under the condition that 50mW is
being produced with a 30% modulation at 400Hz. This is helpful in
verifying that the radio is working to
specifications.
Dial miscalibration
When I checked the radio initially,
I found that none of the received station frequencies were close to their
Australia's electronics magazine
Photos 9 & 10: after resleeving the
knobs, they are close to the original
but not identical. I made the sleeves
by boring out a plastic donor knob.
June 2026 93
Scope 1: if all the
IF adjustments
are tuned for
470kHz, the result
is a response
that’s too narrow
and peaked.
Scope 2: how
the IF response
should look like
with correct
alignment, with
each element
tuned to a slightly
different centre
frequency.
Mechanical repairs
One curio is that this model of radio
has a peculiar failure rate of the black
phenolic sleeves that were placed over
the chromed knobs. They have a habit
of splitting, falling off and getting lost.
They were all missing on this radio,
except one.
This required some donor phenolic knobs. I machined them out with
an internal taper to create a sleeve
or shell so they would slip over the
original chrome metal knobs to act
as a reasonable replacement. As can
be seen in Photos 9 & 10, these have
finer finger-grip grooves than the original sleeve, but they were as close as
I could find.
Another mechanical problem that
cropped up related to the signal meter;
it was sticking. Investigation revealed
that some rust crystals had projected
out of the side wall of the laminated
iron pole pieces and were catching on
the meter’s coil form.
I removed these by slipping in strips
of sticky tape to extract them. Some
people have attempted to blow debris
out of meter movements with compressed air. This is better avoided, as
it normally destroys the hairsprings
and movement.
Photo 11: I use this RF signal generator and this frequency counter for aligning
radios.
94
Silicon Chip
dial markings. Sailor went to the trouble of making a very precise-looking
dial, suggesting the unit should have
good calibration. This is unlike some
domestic radios with poor dial markings, without graduations between
them, and somewhat loosely spaced
dial legends.
On the SW band, it was not possible
to receive the frequencies at all above
about 3.6MHz. The radio was significantly out of alignment.
One of the true arts of radio restoration is in the radio’s alignment. It
might not be so important in some
radios, such as pocket transistor radios,
with single tuned IF transformers and
limited dial markings. Still, in commercial types such as communications
receivers, calibration is very important.
It is often clear from inspecting a
radio’s tuning dial whether the manufacturer thought of it as more of a
domestic product, or more of a scientific instrument, where the dial information was expected to be reasonably
accurate and meaningful.
Australia's electronics magazine
Alignment tools
I have several useful tools to help
siliconchip.com.au
with radio alignment. One is the
Philips PM5326 RF Generator, which
includes an accurate frequency
counter. It puts out exactly 50mV RMS
into a 75W load on 0dB attenuation. It
has an excellent shielded RF attenuator that goes beyond -80dB. A -80dB
output corresponds to 5μV RMS into
a 75W load.
In most radios, the local oscillator (LO) runs at the intermediate frequency above the received station
frequency. To examine the LO, I have
a frequency counter with a programmable offset value, in this case set to
subtract 470kHz, the set’s IF.
As Photo 11 shows, with no signal input applied to the counter, its
display reads 99.5300MHz. It has an
input sensitivity in the range of 10mV
to 40mV and its maximum counting
frequency is about 48MHz.
The input impedance is too low
(in common with many counters)
and its input capacitance is too high
to directly connect to a radio’s oscillator circuitry without loading it and
causing a large frequency shift. To
solve that, I designed a buffer circuit
that is described in Circuit Notebook
on page 79.
IF alignment
It is the gain and bandwidth of the IF
stages in a superhet radio that confer
much of the radio’s selectivity and sensitivity. There is less selectivity in the
RF and antenna circuits, as these need
wide enough bandwidth to accommodate tracking errors.
One basic principle of superhet
radio alignment is to make sure the IF
stages are correctly set up with the correct centre frequency and bandwidth
(if the latter is adjustable). With the IF
amplifier in the 66T, if all the IF slugs
are peaked to the same frequency, the
bandpass response is far too narrow.
The result is a muddy sound with a
loss of treble.
The sweep result shown in Scope
1 occurs when all the IF transformers
are peaked at 470kHz. The resulting
narrow bandwidth response has an
asymmetrical skirt.
The manufacturer specified a bandwidth of 6.5kHz, meaning that the
response should be 3dB down at
±3.25kHz around the 470kHz centre
frequency. This is easily achieved by
adjusting the IF slugs while using a
sweep generator, with the result shown
in Scope 2.
siliconchip.com.au
Indexing
Prior to any other alignment processes, as well as the IF being correctly adjusted, it is important that
when the dial pointer is pointing to a
specific legend at the low-frequency
end of the dial, the variable capacitor is in the correct position. This is
so that over the tuning range, capacitance varies over the correct range to
suit the coil set.
The question is, where is that position? It may not be explicitly stated,
or for that matter even present on
some dials.
It was once a custom for a manufacturer to put an index mark on the dial.
In most cases, the pointer should be
aligned with this mark with the variable capacitor fully meshed, or close to
that. I found no mention of this mark
in the Sailor 66T manual, although
one was evident on the dial.
This setting for my radio was so far
off that the variable capacitor had completely unmeshed by about 3.6MHz on
the shortwave band! It was therefore
impossible to tune in to any frequencies above that.
The dummy antenna
The Sailor 66T manual says to use
an IEC dummy antenna to interface the
RF generator with the radio. It says to
use it with a generator with a 25W output resistance (eg, a 50W output with
a 50W terminator applied to bring the
output impedance down to 25W). This
is to be used for the LW, NW and MW
bands but not the SW band, where
they suggested using the 25W signal
source directly.
A typical dummy antenna is meant
to be driven by a low
source resistance of 25W
or less, but there is little
practical difference in
using a 37.5W source, ie,
a terminated 75W source.
Fig.3 shows the American IRE dummy antenna
circuit. Its performance
is shown graphically in
Fig.4.
Unfortunately, the IRE
version of the dummy
antenna does not suit
the Sailor radio, especially on the LW band,
Fig.3: a standard IRE dummy antenna
circuit. It will work for the MW & SW
bands but is no good on the LW range.
150-280kHz. The IRE circuit mainly
suits radios with MW and SW bands.
Unfortunately, the circuit for the recommended IEC (not IRE) dummy
antenna is not readily available.
If attempting to align this radio
with the IRE dummy antenna, the
LW antenna coil would not come into
range on its tuning slug because, at
17kHz, the IRE dummy antenna does
not apply enough load to the primary
circuit of the antenna coil. Its load is
in the order of nearly 5kW capacitive
reactance at 170kHz, on account of the
220pF capacitor.
As a result of this, and the mutual
coupling, the tuned secondary resonant frequency of the LW antenna
coil was too low. Even with the ferrite slug removed from the former, it
still only came up to a maximum of
around 160kHz.
As a solution, I made an adaptor to
emulate the capacitance of the realistic
antenna system shown in Fig.5(a). This
capacitance is present regardless of
what band on the radio is being used,
so it is suitable to adapt the generator
to the radio for alignment purposes
on all bands.
Since the length of the wire antenna
is relatively short compared to the
Fig.4: an impedance
chart for the IRE dummy
antenna shown in Fig.3.
Australia's electronics magazine
June 2026 95
Obtaining The Best Possible Dial Calibration
Textbook alignment
Once the IF and dial alignments are
correct, the oscillator coil’s tuning slug
(or its adjustable padder capacitor, if
there is one) is set to receive the tone
modulated test frequency for maximum signal out of the IF’s detector
or the audio amplifier stages.
The dial pointer is then moved to
an instructed position near the high
end of the band, and the generator
set to that frequency. The oscillator’s
trimmer capacitor, which is in parallel
with the oscillator’s variable capacitor gang, is moved to tune that in for
a peak signal. These two steps are
then repeated a few times because
they interact.
After that, the antenna and RF coil
slugs can be peaked at the low end of
the band at the same dial locations,
and the trimmer capacitors associated with those coils are peaked at the
recommended high-end frequency.
With this common alignment
method, the tracking of the oscillator’s frequency is exactly correct at
the upper and lower points and at
some intermediate point. These three
frequencies are called ‘crossover frequencies’.
Photos 12 & 13: the oscillator tuning
gang in the radio as I received it (top).
The oscillator tuning gang in the
radio after I minimised the tracking
errors (bottom).
96
Silicon Chip
In the tracking zones around the
crossover frequencies, the local oscillator runs a little faster or slower than
ideal. These errors, shown in Fig.a, are
called ‘tracking errors’. They are intrinsic to a superhet radio where the variable capacitor’s gangs have the same
capacity and the oscillator gang has a
required padder capacitor in series to
reduce its overall capacitance.
When the padder capacitor is the
correct value, the magnitudes of
the + and – tracking errors, at their
worst, are about equal. If significant
enough, they can result in a reduction
in the sensitivity of the radio and/or
a reduction in the image rejection in
those zones.
Tracking alignment
There is an alternative method
to adjust a radio to ensure that the
dial markings match the received
frequencies as closely as possible
and that the tracking errors are minimised. No modulation is required on
the carrier from the RF generator in
this process.
This method does not rely on the IF
amplifier, and it can also be used to
measure the magnitude of the tracking errors. However, the IF amplifier
must be properly set up for a final
result.
Once the IF has been set up correctly with the sweep generator and
marker generator, and the mechanical relationship of the variable capacitor angle and dial pointer are set,
the oscillator transistor stage is disabled. I do this by shorting the base
to the emitter with a 100W resistor
in the case of a separate oscillator
transistor.
For designs with mixer/oscillator
stages, shorting out the oscillator’s
resonant coil also works.
Then, for each band, the cores in
the RF and antenna coils are peaked
on the manufacturer’s recommended
low frequency, and the capacitor trimmers at the upper band end in the
usual way, but in this case by monitoring the output of the antenna/RF
tuned circuit (if present) where it feeds
into the mixer, or on the RF amplifier’s
variable capacitor gang.
You need a low-capacitance (<1pF)
probe to monitor the RF output; I have
Australia's electronics magazine
designed one that is presented in Circuit Notebook this month, on page
79. This allows the tuned carrier to
be seen on a scope with negligible
detuning effects on the RF stage’s
resonant circuit. In essence, this
part of the radio is being treated as
a TRF circuit.
Once the upper and lower frequency points are set for the antenna
& RF stages, the positions of all other
dial markings with respect to the dial
pointer (representing the variable
capacitor’s angle) can be checked
to see how closely the dial markings
and pointer match the applied carrier
frequencies.
This is why an RF generator with
a built-in frequency counter is very
helpful. In the Sailor radio, it turned
out that the antenna and tuned RF
stages were closely correlated with
the variable capacitor’s pointer and
the dial markings. In this case, there
is no requirement to adjust the wings
on the variable capacitor gangs associated with those two radio frequency
stages.
The glass dial’s markings had
clearly been created from a law defining the tuned frequencies when a
straight-line wavelength (SLW) variable capacitor was used. Rather than
calibrating the dial in wavelength,
which would have more evenly spread
the values, it was calibrated in frequency.
This is very convenient because
any adjustments to the oscillator’s
fine tuning can be targeted to match
the dial markings as closely as possible too. This way, both tracking errors
and dial marking/pointer errors for
tuned stations can be simultaneously
minimised.
In the case that the dial markings
closely follow the oscillator’s tuning,
the wings of the oscillator’s variable
capacitor should never be altered
from standard. Only the wings of the
RF and antenna sections should be
adjusted (with the oscillator disabled)
if required, to better match the dial/
pointer relationship.
Setting up the oscillator
After re-enabling the oscillator,
adjust it at the low and high recommended frequency points on the dial
siliconchip.com.au
with the tuning slug and trimmer
capacitor, respectively. It pays to do
it a few times because they interact.
Then the points on the dial in the
tracking error zones can be checked
by disabling the oscillator and tuning the antenna and RF system for
a peak, then re-enabling the oscillator. If required, the adjustment vanes
on the oscillator gang of the variable
capacitor can be altered to improve
the tracking.
Due to the fact that the capacitance
of the variable capacitor gang can
only be reduced by bending the wing
outwards, to gain full control, all the
vanes will have to be bent outward initially. After that, you can bend one in
to increase the capacitance or bend
it out to decrease it further (see Photos 12 & 13). But this does not always
need to be done.
Every time the wings are adjusted,
both the oscillator’s tuning slug and
the trimmer capacitor have to be reset
at the upper and lower frequency
points to correct the upper and lower
set frequencies.
Ideally, before starting, you create a
tracking error map. This is done by disabling the oscillator, as noted above,
tuning the RF signal for a peak at
each major dial frequency step, then
re-starting the oscillator and inspecting its deviation. This is much easier
if you have a counter that subtracts
the intermediate frequency for you.
As one might expect, the ideal
adjustment of the wings would be an
S curve, reminiscent of the tracking
error curve itself. However, it is compressed due to the nature of the SLW
variable capacitor’s vane profile. To
get an actual curve, the vanes would
require twisting as well as bending
outward.
Another approach, as shown in
Fig.b, is to bend them directly outwards. There are not enough adjustment wings to acquire a super accurate result; 10 wings would be better.
With the wings untouched and
matching those of the antenna and
RF stage gangs, in the zone between
1.8MHz and 2.7MHz, the oscillator
is running a little more slowly than
ideal and requires a little less capacitance; this is why the wings in that
zone are better bent outwards. In the
siliconchip.com.au
Fig.a: typical
tracking errors
across the dial of a
correctly adjusted
superhet.
Fig.b: by correctly bending the ‘wings’ on the variable capacitor, it is possible
to minimise the tracking errors.
Fig.c: the configuration of the
tuning capacitor wings in
this set.
zone between 2.7MHz and 36MHz,
the oscillator is running a little faster
and requires more capacitance.
With this radio, after adjusting the
wings on the SW band, tracking was
as ideal as possible on the other three
bands. The SW band was the most
convenient one to use for the tracking adjustment because the outer
dial scale and pointer have a larger
range of relative motion for a small
change in angle of the variable capacitor, and the dial marking details are
very helpful.
The maximum mechanical error
in the position of the pointer with
respect to a dial marking in the tracking zones in SW mode, when all is set
in proper alignment, is in the order
Australia's electronics magazine
of about 1-1.5 times the width of the
pointer.
Fortunately, in the scheme of
things, the effects of tracking errors
in single-conversion superhet radios
are generally small. This is because
of the relatively wide bandwidth of
the tuned RF and antenna stages,
being significantly broader than the
oscillator’s tracking errors, so there
is no significant loss of sensitivity or
image rejection.
It is the IF stage in the radio that
confers the selectivity to the receiver
as a whole. Still, it is good to have
the radio in good alignment, as well
as the dial pointer giving a good representation of the received station’s
frequency.
June 2026 97
Silicon
Chip
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wavelengths involved, there is no
requirement to model the antenna’s
inductance or the transmission line
properties of the coax. The antenna
system is essentially a capacitive load.
The relatively low load of 37.5W
(the terminated generator), placed in
series with the load capacitance, has
negligible effects on the total load, but
it allows signal injection in series with
the 680pF load capacitance. With this
arrangement, shown in Fig.5(b), the
antenna coil’s tuning slug positions
closely matched the manufacturer’s
slug positions (locked with red paint)
on all bands.
At 170kHz, the reactance of the
680pF capacitor is in the order of
1.4kW. At 4MHz on SW, it is quite low,
around 58W. This low load is as recommended on the SW band by Sailor.
Summary
The Sailor 66T is a remarkably wellmade radio. It lives up to its sensitivity specifications on testing and sports
a very attractive, well-calibrated dial.
Its direction-finding capabilities are
quite remarkable. In the days prior to
satellite navigation, it probably saved
a number of sailors’ livelihoods, and
lives too, in the treacherous North Sea.
It has a very satisfactory speaker
and audio system, and with only a
very small change to a capacitor value,
makes a very pleasant sounding radio
to listen to music stations on the MW
SC
band.
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98
Silicon Chip
Australia's electronics magazine
Fig.5: (a) the recommended antenna
for using the 66T radio on a ship; (b) a
dummy antenna circuit that provides
similar operating conditions for
aligning the set.
siliconchip.com.au
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
DCC Base Station likely
has a short circuit
I am building the DCC Base Station
from a kit (January 2026; siliconchip.
au/Article/19558). When testing the
REG1 circuitry using a 9V battery, as
per the printed instructions, I am only
seeing 4.00V DC at the anode of D1.
The instructions say to expect 5.2-5.4V
at this point. I have checked every solder point for dry joints, bridges etc.
Any advice on troubleshooting further? (J. L., Mudgeeraba, Qld)
● There isn’t anything that immediately comes to mind that would cause
it to be near 4V, as long as the 9V battery is, say, 8V or higher. So it seems
that there may be a short circuit on the
board, causing the 9V battery output
to sag. That can be easily verified with
a multimeter.
You say you’ve already looked for
bridges. We’d also check if any components have been reversed, although
we can’t think of any specific reason
why that would result in 4V at the
output. If you have already soldered
the Pico, you could try removing D1
to isolate the Pico and see if that narrows down which part of the circuit
is causing problems.
Building model trains
from scratch
to start or get an idea of the full process. I really appreciate any reply. (N.
G., Qld, via email)
● Model railways are a very broad
topic and people take an interest for
different reasons. Where to start will
depend on what you want to achieve
and what you enjoy doing.
Some prefer working with electronics, scenery, painting, construction or
operation (and probably other different things, too). Being an electronics
magazine, the most relevant articles
that we have are related to electronics
projects that can be used with model
railways.
The DCC (Digital Command Control) series is a good example of this.
You can view free previews of the articles in this series at siliconchip.au/
Series/455 – that might give you an
idea of what we have written about.
As far as building trains and tracks
from scratch, that isn’t something
we’ve heard of many people doing,
although it must be possible. We have
built (in HO and N scale) our own vehicles and some track items, but these
have all used commercially available
parts like motorised chassis and track
profiles, combined with 3D-printed
parts and then painted.
While researching this answer, we
found a few open-source projects that
are focused on making functional
3D-printed model railways.
We suggest making contact with a
local model railway club (they often
have their own layouts) or visiting a
model railway exhibition. The clubs
and exhibitions will have people with
different interests. If you have a specific question about how to use electronics, we might be better equipped
to help you with that.
Analog Devices placing
restrictions on parts
I have finally gotten around to gathering the parts to build the Versatile
Waveform Generator (March 2025;
siliconchip.au/Article/17792) but I
have run into a major problem!
I ordered the Analog Devices op
amps that are central to the project
from element14 and got a message
that they won’t send them to New Zealand. So I put together a big order from
Mouser, including all those devices
and switches etc. Back came a message
that the manufacturer will not allow
shipping to New Zealand. What?!
How did Silicon Chip obtain the
chips to build the project and how
can I obtain them? If I purchase them
Finding an LCD screen for the Graphing Thermometer
I would like to build my own model
railway from scratch. While I was able
to find a 1999 magazine issue that
appeared to have some relevant information, I was having trouble finding
where to start or if there is an existing kit. I’m generally a ‘techy’ person,
having studied game development and
computer science, but electronics will
be new to me.
I intend to build the trains and
tracks as well (not using off-the-shelf
products). I do miniature building and
painting, so I’m excited to bring that
together with some of my other interests. There’s a lot of information out
there on the internet, but even with AI
assistance, it’s difficult to know where
I want to build the Graphing Thermometer from the March 2026 issue (siliconchip.
au/Article/19833) and have bought the PCB and programmed ATtiny85 from your
web store.
Now I am collecting the other parts and I am having problems searching
AliExpress for the LCD screen, boost regulator and the 2-way barrier screw block
connector. Any assistance would be appreciated.
I have been a long-time subscriber and enjoy every issue. (D. M., Geraldton, WA)
● Maintaining current links for parts from these sources continues to pose
challenges despite checks shortly before publication, as AliExpress items often
change links or are discontinued by sellers. The LCD can be found by searching
for “GLX12864” on supplier websites. One current item number is AliExpress
1005006267035677 (try putting that number in the search box).
There are many equivalents for the boost converter module used in the design.
Search for “0.9 - 5V in / 5V out boost regulator”. One current item on AliExpress is
1005006809303748. Other supply options exist, as noted in the article.
The 2-way barrier strip used was a standard 7.62mm/0.3-inch pin-to-pin part
for which there are many equivalents. Other metric types can be readily adapted
to fit the PCB. One of many sources (for now) is AliExpress 1005003429295570.
siliconchip.com.au
Australia's electronics magazine
June 2026 99
directly from Analog Devices, it will
be an additional $52 in postage, making this an expensive exercise. (G. D.,
Burleigh, NZ)
● We have never had trouble getting
Analog Devices parts in Australia. We
suspect that Analog Devices has an
exclusive deal with some NZ distributor, so other vendors are restricted
from selling you those parts. However,
we don’t know who that is. You might
have to contact Analog Devices to try
to find out.
It will probably be easier to simply
select similar parts from another manufacturer. We haven’t tested these, but
we suspect they will work as they have
very similar specifications:
• Analog Devices AD8065ART
= Texas Instruments OPA810IDBVR
• Analog Devices AD8091ART
= Texas Instruments (National
Semiconductor) LMH6642MF/NOPB
or LMH6642MFX/NOPB
As for Analog Devices, the phrase
“shut up and take my money” comes to
mind. What do they have against New
Zealanders buying op amps?
with an extra row or two of width, but
have not been able to locate one. Can
you point me to a supplier, or am I mistaken? (K. W., Newport, Vic)
● We think the trick is to connect
two of those breadboards side-by-side
(some are designed to be expanded that
way). With the power rails down the
middle, the sets of five holes should be
further apart, so you will be left with
more rows to plug into.
Some larger breadboards come with
the power rail down the middle (or can
be reconfigured that way), for example, the one from Altronics shown in
the photo below.
Questions about the
Calliope Amplifier
I have some thoughts on the Calliope
Amplifier (April 2026; siliconchip.au/
Article/20084) as I’m looking at building some to use at a higher power. I
recognise that they’re already very
low distortion, but I can’t help myself.
Can I suggest that you look at the
KSA992FBTA (PNP) and KSA1845
(NPN) for the low-power stages? These
are going obsolete, but are still availUsing RP2350B Dev
able from the usual suspects. They
Board on a breadboard will allow the amplifier output to go
I have a question about the pre- up to possibly 150W into 8W, maybe
assembled RP2350B Development more if parallel output transistors
Boards (August 2025; siliconchip.au/ are used.
Article/18635). The magazine article
They are low-noise types, so will
states: “...designed to suit solderless have low Rbb figures. This means that
breadboards with two rows of 32 pins”. the amplifier should be fed from a low
If I try to plug it into my bog- source impedance, which can be prostandard breadboard, it is too wide to vided by an op amp used as a unity-
leave any empty pin holes along one gain buffer in the amplifier, or by an
edge. I have tried to find a breadboard active crossover.
100
Silicon Chip
Australia's electronics magazine
Your use of the BF722 has solved a
problem that I’ve had for a while, of
finding a good VAS transistor. Thank
you for that. I’ve tried finding KSC3503
units, but most I find are on eBay. I
have some doubts about them.
In the original Hummingbird, you
used bench power supplies for distortion testing. What are the figures when
standard power supplies are used?
I’m looking at running them in
Class-B only as I can measure the distortion and optimise the bias to minimise that distortion to meet the Oliver criteria (about 26mV across re +
Re where re is the transistor’s internal
emitter resistance and Re is the emitter resistor).
Douglas Self recommends the
MJL3281 and MJL1302 output transistors as they are ring emitter units and
thus suffer less beta droop than other
transistors. Your thoughts?
If they’re run in Class-AB, the amplifier will spend a lot of time switching
between Class-A and Class-B. Is this
a concern? The value for Cdom seems
to me to be high and could have a
significant effect on slew rate, particularly as the LTP current isn’t very
high. Thank you most kindly for the
work you’ve put into both the amplifiers and the digital preamplifier. (K.
J., Cleveland, Qld)
● The Calliope designer, Phil
Prosser, responds:
Regarding the KSA992/A1845 transistors, I have come across them before.
When I design projects, I go out of my
way to use parts that are commonly
available. I recall these being lownoise types; I had not looked at their
voltage ratings and did not consider
them over the ‘decent’ devices that can
be bought from the likes of Altronics
and Jaycar.
If we specified a hard-to-find part,
there would be a lot of people asking
how to get them and what else they
could use. We note that Mouser stocks
the KSA992, though. There is nothing
stopping you from using these; just
note that the pinout is different. The
voltage rating would allow higher voltage operation, but more on that later...
The lack of reasonable VAS devices
on the market is what drove me to go
back to the design. It is really frustrating that so few through-hole parts are
even half-decent. I am not fussed by
SMDs, but a lot of people are. I bought
a stack of various VAS devices from
eBay years ago and tested a bunch of
siliconchip.com.au
them to convince myself they were OK.
To be honest, the BF469/470 remain
a favourite, but these are totally
unavailable through normal channels,
and if I saw them online, I would not
buy them.
The tests I have performed on fully
built amplifiers with a conventional
power supply were totally consistent
with the measurements running from
the bench supply. The way a typical
audio amplifier works means it really
doesn’t care that much about the ripple on the power supply.
The caveat is that you get the
grounding right. That star ground is
critical; even minor errors on that
will noticeably increase the distortion levels.
As the article noted, even running the output wire over the input
stages causes havoc with the distortion numbers. There are similar problems if using cruddy connectors. The
truth is that you would still need test
equipment (not your ear) to detect the
problem, but that is kind of what it is
about, isn’t it?
Regarding Class-AB vs Class-B, I
played with the bias level a lot and
made many measurements. If the bias
is grossly maladjusted, you will get
substantially elevated distortion (from
memory about 10dB worse). Anything
in the ballpark of the recommended
bias point, which isn’t that different
to what you are shooting for, gives the
measured results.
I built about a dozen of these amplifiers in various configurations as part
of testing. In one set of tests, I couldn’t
work out why one amplifier module was giving more distortion than
I expected. I was checking parts and
wiring until I realised that the bias
was turned right down. It is surprising
how forgiving the ‘blameless’ architecture is.
On the output devices, the “Frankenamp” I mentioned in the article
used an MJL21193 on one side and
an MJL3281 on the other, making it
about as mismatched as you can get.
The input was a BC54x and a BC33x.
While the DC output offset was borderline dangerous, the distortion was
still very low indeed.
I was frankly surprised at this, but
the point is that there are many things
that are ‘technically better’, such as
matched output devices, but make a
surprisingly small difference to the
performance. Don’t get me wrong,
I match input devices, but it is less
important than many other aspects of
the design.
I would choose the MJL21193/4 for
the outputs if I were going to give the
amplifier a hiding. Those devices are
incredibly hard to kill. I have tried and
failed several times. I have a stack of
MJL3281/1302 devices, which I also
use. If I were pushing my luck and
wanted to wring every watt out of the
board at elevated voltages, I would
go with the MJL21193/4 as their SOA
is better.
If I were worried about getting
the distortion down, noting that the
measurements didn’t show a glaring difference, I would choose the
MJL3281/1302.
A less obvious thing is that the
MJL3281/1302 have an ft of 30MHz.
This is not a problem, but it is almost
10 times that of the MJL21193/4. Some
people see this difference and jump to
the conclusion that a higher ft is better,
but it is a double-edged sword.
The increased ft does mean that the
high-frequency gain is elevated, and
this can lead to oscillation on recovery from clipping, unlike the ‘slower’
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Complete kit for $50 (SC6952; siliconchip.com.au/Shop/20/6952)
The kit includes everything pictured, except the lithium coin cell and optional programming header (CON1). The
three resistors and single capacitor needed for calibration are included. See the article in the June 2024 issue for
more details (siliconchip.au/Article/16289).
For testing other components like capacitors and diodes, check out our Advanced SMD Test Tweezers from the
February & March 2023 issues (siliconchip.com.au/Series/396). We sell a kit for those Tweezers for $45 (SC6631).
siliconchip.com.au
Australia's electronics magazine
June 2026 101
Getting tachometer working with Ignition System
I recently built your Programmable Ignition System (March-May 2007; siliconchip.
au/Series/56). It works great except I can’t get my rev counter to work. The vehicle is
a 1987 Ford Courier ute with a points distributor. I have connected the programmable
ignition tacho output but the rev counter doesn’t work.
If I connect an external aftermarket rev counter to the tacho output, it works, so
I know I’m getting a signal. I have also tested the tacho in the ute, and it’s working
fine. I tried making an amplifier circuit that I found online, but that doesn’t work
either. Any help or advice would be appreciated. (G. N., Lincoln, NZ)
● Presumably, the original tachometer is an impulse type that relies on the
high primary coil voltage to operate rather than a low-voltage signal such as the
tacho output from the programmable ignition. Check the source of the original
tachometer signal. If it was at the points, then the tacho may work when connected
to the transistor coil driver that connects to the coil.
21193/4. The oscillations are usually
in the MHz region and not reflective
of the devices’ behaviour at audio frequencies.
When you roll back the frequency
to audio performance in an amplifier,
with that Miller capacitor providing
the dominant pole, the ft difference
is not significant.
So I agree with the preference on the
basis of distortion, but would advise
you to be careful with safe operating
areas if you want to crank the voltage.
You really ought to use extra output
devices and resistors, but then you are
basically building something like the
SC200 amplifier.
Keep that protection circuit in there,
as if your speaker dips in impedance,
as many do, you may find your nominal 8W load presents a problem at some
frequencies. In that case, the load-line
protection circuit would possibly save
you repair to the amplifier and/or your
speaker.
Unless you have a compelling reason that demands such a tiny amplifier board, if you want more than 100W
then go to one of the Ultra-LD amplifiers, as it saves you rat’s-nesting the
extra devices in, and also gives you
more separation of the input stages
from the high currents in the output
stage, which has distortion benefits.
I would prefer to run the amplifier
in Class-AB, as the notion of ‘being
exactly on the edge of Class-B’ sounds
both optimistic and not likely to be
true over temperature variation, voltage rail variation and the life of the
amplifier.
The expense of a bit more dissipation is fine by me, and the only argument I would easily accept is that
running a BJT amplifier in Class-A is
‘obviously’ going to result in lower
crossover distortion.
I have tried this, and I kind of liked
the massively hot heatsink, but was
unable to actually hear any difference
except for the very slight buzz of the
power supply cranking out hundreds
of watts into a big heatsink 24/7. At
night this annoyed me, so I turned that
bias down again.
Cdom is set higher than absolutely
necessary in the Calliope to allow a
ridiculous range of parts to be used
without the amplifier giving stability
problems.
The article makes brief mention of
me adding a two-pole Miller arrangement. This reliably and substantially
reduced high-frequency distortion,
but was really hard to squeeze in, and
when I started throwing random parts
in for output devices etc, I decided
that 220pF was a safer choice for your
average constructor.
There is nothing stopping you from
building and tuning your own Cdom or
even adding that second pole; it isn’t
hard to fit on the back of the board.
Just remember that you need to test
for stability not only at low power
levels; you really need to look at stability running into a low-impedance
load near clipping.
Watch the waveform as it goes into
and comes out of clipping near the
negative rail. Bursts of high-frequency
oscillation at this point are a characteristic of a marginally stable amplifier using this topology. It is seen in
pretty well every conventional BJTbased amplifier when you start pushing the slew rate.
So in the end, I went for a value of
Cdom that was reliable, safe and gave
good results. Reliability in my mind
trumps slightly better performance
when it comes to the range of readers
and constructors the magazine has.
One great aspect of this project is
that people can do what they want.
If you want to use the KSA parts, go
for it. I am confident they will work
well. The MJL1302 transistors are
known good too. Feel free to adjust
Cdom if you have the means to verify
the amplifier is still stable, and if you
want to try a two-pole version, that
definitely has benefits. A couple of
extra components on the back of the
board will not hurt.
Just be careful turning the voltage
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.
102
Silicon Chip
Australia's electronics magazine
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up, and if you do, then watch the SOA.
There is not a lot of ‘room’ there for
speakers that do surprising things, so
if you can’t resist the temptation, then
add an extra set of output devices. That
is a little untidy, but it is only six more
wires per amplifier. That buys you a
lot of SOA headroom.
● We published a white noise generator in September 2018 (siliconchip.
au/Article/11225). You could feed its
output into an amplifier and then to
speaker(s). You would probably want
very directional speakers, perhaps
using a parabolic reflector, to confound
the camera without making a racket.
White noise generator
wanted
Using a differential
ADC for Reflow Oven
My daughter unfortunately lives
next door to the area snoop and gossip. She recently discovered that the
neighbour’s security camera, which is
allegedly aimed at the footpath, actually points over their deck and picks
up what is said on the deck. It is probably illegal, but hard to prove, so I
thought a white noise generator will
probably solve the problem legally.
Have you produced a suitable circuit? (J. A., Healesville, Vic)
I am putting together all the parts to
build the DIY Reflow Oven Controller project (April & May 2020 issues;
siliconchip.au/Series/343). I have a
question regarding the thermocouple
amplifier section. I purchased the same
module you used from eBay. It looks
like it is a copy of an Adafruit design.
Why does CON10 not indicate an
input for the reference voltage? I would
have thought it better to use a differential ADC measurement (direct or two
siliconchip.com.au
Australia's electronics magazine
individual channel readings) so that
the reference/offset voltage did not
necessarily have to be known, as long
as it provided a large enough positive
temperature span.
As you mentioned, 2.5V would
be too large for a 3.3V system. What
CON10 pin would you use/suggest?
I will update the software to handle
this. I am going to make my own special board to take the CON10 ribbon
cable direct and have a separate twopin connector for the SSR connections.
(M. V., Taree, NSW)
● The designer, Phil Prosser,
responds: if I understand your intent,
you are asking about using a second
ADC channel to make the sensor temperature measurement independent
of the temperature sensor’s DC offset.
If your sensor output voltage range
does not saturate the ADC across the
full measurement range, you could certainly do that. You will need access to
June 2026 103
Advertising Index
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Blackmagic Design....................... 7
Dave Thompson........................ 103
DigiKey Electronics..................OBC
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Emona Instruments.................. IBC
Hare & Forbes........................10-11
Jaycar............................. IFC, 22-25
Keith Rippon Kit Assembly....... 103
LD Electronics........................... 103
LEDsales................................... 103
Microchip Technology.................. 9
Mouser Electronics....................... 3
PE Back Issues........................... 52
PCBWay....................................... 35
PMD Way................................... 103
SC Bridge Rectifiers.................... 79
SC ESR Test Tweezers............. 101
Silicon Chip Binders.......... 59, 103
Silicon Chip Kits........................ 76
Silicon Chip PDFs on USB......... 98
Silicon Chip Subscriptions........ 53
Silicon Chip Shop.................86-87
The Loudspeaker Kit.com............ 8
Wagner Electronics..................... 83
Errata and on-sale date
Airzone 6552A, Vintage Radio,
May 2026: in the circuit diagram,
C4 is pointed to the wrong
capacitor, it should point to the
capacitor directly below C3. Some
components also had incorrect
values, the correct values are –
R10 is 250kΩ; R12 is 500kΩ; R14 is
250kΩ; and capacitor C1 is 250nF.
Digital Vehicle Compass, Circuit
Notebook, April 2026: on p17, the
SDA and SCL connections going
down vertically from the Arduino’s
SDA and SCL pins are swapped.
All the SDA pins should be joined
together, and similar for the SCL
pins.
PicoSDR, April 2026: in Fig.3 on
p39, pin 39 of the Pico (VSYS)
should be connected to +5V.
Next Issue: the July 2026 issue
is due on sale in newsagents by
Monday, June 29th. Expect postal
delivery of subscription copies in
Australia between June 26th and
July 13th.
104
Silicon Chip
the reference voltage on the thermocouple interface, and would need to
pay attention to limit cases such as
low-temperature operation.
The current calibration process
zeroes out the absolute offset. The
actual precision of the thermocouple really limits what you should be
expecting to achieve; you probably
want to balance the effort you put in
with the benefit you would get.
The PIC microcontroller is hugely
programmable in its I/O capability. Look into the data sheet for your
options, which you need to configure
with the other inputs and outputs.
Depending on how you implement
this, you will need to check the temperature scaling, but I suspect will be
OK with the calibration.
To be honest, I wonder if the rework
of the code will deliver a great benefit.
Knowing how agricultural my coding
style is, you may end up tearing a few
handfuls of hair out, though.
Converting Nano Pong
to HDMI output
I built the Nano TV Pong kit a while
ago (August 2021 issue; siliconchip.
au/Article/14988) and it works well
plugged into a TV with component
inputs. But I want it to output HDMI.
I’ve tried to use a component-toHDMI converter (Jaycar Cat AC1722)
and the screen comes up, but it goes
away after a few seconds with “No
Signal” being displayed for a few seconds, then back to the game display.
I’ve tried different TVs, and the No
Signal is the same display on each of
them, so I assume it’s coming from the
converter box. The sound works fine
throughout. Any ideas?
I am a long-term reader back to
Radio, TV & Hobbies. (M. H., Parkinson, Qld)
● The signal from the Nano Pong
is composite video. Since the AC1722
Converter states that it supports composite video, it should work. It seems
like the converter thinks that the signal is going away and coming back for
some reason.
Have you tried changing the resolution setting on the Converter? We are
not sure that will help, but it would
be worth trying. We found some forum
posts that suggested the 720p setting
would work better (despite 1080p
sounding like it should be ideal). The
Converter may be a bit fussy about the
Australia's electronics magazine
signal it expects; we didn’t have any
trouble with any of the TVs or capture
cards that we tried.
The Converter mentions features
such as “black/white level expansion, color transition improvement,
dynamic range expansion”, so we
wonder if it is not handling the twolevel monochrome image well.
It may be better to produce a native
HDMI signal rather than try to convert
it. That could be done using one of our
small computers that have an HDMI
output, such as the RP2350B computer
project from November 2025. It would
just need software to play Pong.
We found a BASIC version that
seems promising, but we have not
tested it: https://github.com/jmdeejay/
mmbasic-picomite/blob/main/games/
pong.bas
Where to obtain
VOC sensors?
I have a query regarding the volatile
organic chemical (VOC) sensor mentioned on page 45 of the February 2020
issue for the Indoor Air Quality Monitor (siliconchip.au/Article/12337).
This MOX sensor worked very well.
In the University lab where I worked
previously, it notified our staff that we
had a methanol leak (odourless but
harmful), and also that a fume cupboard was malfunctioning (it used a
three-phase motor with two of its poles
inadvertently reversed, blowing down
instead of up).
In addition to these accomplishments, I used the ‘nose’ to estimate
the range of VOCs in pharmaceutical products, which we tested on a
gas chromatograph. There is a window in which to measure such a signal, thus the appropriate dilution was
employed, and it was spot-on every
time.
However, both the CCS811 with
onboard HDC1080 I have no longer
give readings on both Micromite BackPacks. My guess is that the heaters
have failed. Core Electronics has discontinued this line. Do you know of
any other more reliable VOC sensors
that are as good as that one? (G. A. D.,
PhD, Biochem).
● The sensor module is still available from sellers on AliExpress, see:
www.aliexpress.com/w/wholesaleccs811-hdc1080.html
w w w. a l i e x p r e s s . c o m / i t e m /
SC
1005006603898777.html
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