This is only a preview of the September 2014 issue of Silicon Chip. You can view 35 of the 104 pages in the full issue, including the advertisments. For full access, purchase the issue for $10.00 or subscribe for access to the latest issues. Items relevant to "Create Eerie Music With The Opto-Theremin, Pt.1":
Items relevant to "A Wideband Active Differential Oscilloscope Probe":
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September 2014 1
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Ref: Silicon Chip Magazine June 2004
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Ref: High Performance Electronic Projects for Cars Silicon Chip Publications
Adjustable switching temperature
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Ref: High Performance Electronic Projects for Cars Silicon Chip Publications
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Ref: Silicon Chip
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Ref: Silicon Chip Magazine July 2013
An easy way to test a USB port to see if it is dead,
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Ref: Silicon Chip Magazine September 2014
Can deliver more than 10W per channel or
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Test Kits
• 12VDC automotive ignition coil and case not included
• 12V car battery, 7Ah SLA or
>5Amp DC power supply required $
95
• PCB: 170 x 76mm
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Ref: Silicon Chip Magazine July 2014
Switches a relay when its input voltage crosses
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Suits 5V, 12V or 24V applications. PCB,
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components included.
See
website for
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Ref: Silicon Chip Magazine August 2014
Convert a 240VAC
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or control 12V or
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49
Jacob's Ladder High
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Threshold Voltage Switch Kit
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Kit for Ni-Cd & Ni-MH
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connected cells
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charge options.
• Adjustable charging time-out
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change rate cut-off)
• Adjustable charge current
7995
$
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label and electronic components. Requires a power supply.
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Contents
Vol.27, No.9; September 2014
SILICON
CHIP
www.siliconchip.com.au
Create Eerie Music with The
Opto-Theremin – Page 20.
Features
12 How Omega Ruled The World Before GPS
What was the main global real-time radio navigation system before GPS took
over in 1997? The answer is “Omega”. Here’s a look at how the system worked
– by Dr David Maddison
32 Review: Incus Bluetooth Hearing Aid Programmer
Blamey & Saunders’ latest programmer for their great-value hearing aids
makes them even better. You can program them yourself to suit your hearing
loss and Bluetooth connection makes it easy – by Ross Tester
57 The Sydney Electronex 2014 Show & PCB Design Tips
Our preview to the Electronex 2014 show (September 10-11) with an emphasis
on PCB design and manufacturing
90 The Canberra RadioFest: All Types Of Vintage Radios
Want the opportunity to view or purchase an impressive collection of vintage
radios and spares? The Canberra RadioFest from September 19-20 is the
place to be – by Kevin Poulter
Pro jects To Build
20 Create Eerie Music With The Opto-Theremin, Pt.1
Completely new Theremin design uses an optical distance sensor to control
volume, making it easier to play and easier to build and adjust than earlier
designs. A metal antenna is used for pitch control – by John Clarke
Wideband Active Differential
Oscilloscope Probe – Page 40.
40 A Wideband Active Differential Oscilloscope Probe
Using a scope to measure high-speed/high-frequency circuits can be tricky
with a passive test probe. This high-performance active differential probe costs
much less than commercial units, has very little circuit loading and has a usable
bandwidth of more than 80MHz – by Jim Rowe
74 Mini-D Stereo 10W/Channel Class-D Audio Amplifier
This Class-D audio amplifier module delivers more than 10W/channel in stereo
mode or 30W into a single speaker in mono mode and features over-current,
over-temperature, short circuit and speaker protection – by Nicholas Vinen
Mini-D Stereo 10W/Channel
Class-D Audio Amplifier – Page 74.
86 An Improved Tweeter Horn For The Majestic Loudspeaker
The Majestic loudspeaker in the June 2014 issue has created lots of interest but
the Etone tweeter horn has become unavailable. We’ve located a Celestion horn
which looks and sounds even better – by Allan Linton-Smith & Leo Simpson
Special Columns
34 Serviceman’s Log
Cameras can be tricky to repair – by Dave Thompson
84 Circuit Notebook
(1) Micromite-Based Controller For 230VAC LED Downlights; (2) Safely
Measuring The Frequency Output Of The Induction Motor Speed Controller
92 Vintage Radio
Pye’s excellent C-2 Jetliner transistor radio – by Ian Batty
Departments
2 Publisher’s Letter
4
Mailbag
siliconchip.com.au
31 Subscriptions
98 Ask Silicon Chip
102
103
104
104
Online Shop
Market Centre
Advertising Index
Notes & Errata
Improved Tweeter Horn For the
Majestic Loudspeaker – Page 86.
September 2014 1
SILICON
CHIP
www.siliconchip.com.au
Publisher & Editor-in-Chief
Leo Simpson, B.Bus., FAICD
Production Manager
Greg Swain, B.Sc. (Hons.)
Technical Editor
John Clarke, B.E.(Elec.)
Technical Staff
Ross Tester
Jim Rowe, B.A., B.Sc
Nicholas Vinen
Photography
Ross Tester
Reader Services
Ann Morris
Advertising Enquiries
Glyn Smith
Phone (02) 9939 3295
Mobile 0431 792 293
glyn<at>siliconchip.com.au
Regular Contributors
Brendan Akhurst
Rodney Champness, VK3UG
Kevin Poulter
Stan Swan
Dave Thompson
SILICON CHIP is published 12 times
a year by Silicon Chip Publications
Pty Ltd. ACN 003 205 490. ABN 49
003 205 490. All material is copyright ©. No part of this publication
may be reproduced without the written consent of the publisher.
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in Australia. For overseas rates, see
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E-mail: silicon<at>siliconchip.com.au
ISSN 1030-2662
Recommended and maximum price only.
2 Silicon Chip
Publisher’s Letter
Debate on the MEN system
Well, well, well. My Publisher’s Letter and article on
the dangers of Australia’s Multiple Earth Neutral (MEN)
system in the August issue has certainly triggered a lively
discussion, as I thought it might. Some of the ensuing correspondence is featured in the Mailbag pages of this issue.
No doubt we will have more next month.
As you would expect, most of the correspondence
has come from electricians who are very familiar with
the MEN system and wiring practices as specified in the
SAA wiring rules (AS/NZS3000:2007). Typically, these
tradesmen are conscientious and concerned about any deviation from what they
perceive as standard practice. As you will see, some readers were concerned about
the standard of wiring shown in the photos of the meter box/switchboard in the
article and claimed that it was not “up to scratch”.
To be honest, the sight of the bundle of Earth wires behind the hinged-out panel
on my switchboard was a surprise to me. If I had thought about it at all, I would have
assumed there was an Earth link for all these connections. Prior to taking the photos
in the article, I had never looked at it. But I am assured that it does meet the relevant
clauses in the wiring rules. If you think about the number of connections necessary
for an Earth link bar, it would be quite a long bar and a lot of screw connections, all
of which can gradually come loose over time, due to the effects of creepage. So the
soldered bundle is probably the better approach for long-term safety.
Other readers were concerned with the fact that I found considerable current
flowing in the Earth. Some were adamant that no current at all must flow in the
Earth. If you think about it, there must always be some current flowing in the Earth.
Consider an installation in which the Neutral circuit back to the power pole is 300
milliohms, a fairly typical value. Now the Earth circuit should also have a very low
resistance and what if it, too, is 300 milliohms? This means that regardless of how
much current flows in to the Active connection, half flows back to the distribution
transformer (or sub-station) via the Neutral and the other half will flow via the Earth.
Other readers maintained that the consumer’s Earth should only be a copperplated stake driven into the ground and no connection to the water pipes. Well good
luck with that idea if you live in a hilly area where most of the houses are built on
rock. That describes my house and while I do have an Earth stake, it was buried in
concrete years ago and even then it must have been in a small pocket of shallow
soil over solid sandstone.
And good luck with the idea of keeping the area around the Earth stake wellwatered to keep soil conductivity high. How many people even know where their
Earth stake is or what it is for, let alone the idea that it should be watered in periods
of dry weather? This is why the water pipes become part of the consumer’s Earth – it
is bound to be a better long-term connection.
And that is the way it has been for a very long time. If not, why are plumbers
generally aware of the hazards of removing a water meter? It must be bridged with
a heavy jumper lead to provide an alternative path for the Earth currents while
the water meter is removed. In that respect, plumbers seem to be more aware than
electricians, even though they might not know the reasons why hazardous currents
(or voltages) could be present.
Finally, a couple of readers wanted to know if Energy Australia had subsequently
made efforts to find out where the apparent Neutral fault in my immediate locality
was. The answer to that is “no” and that was the subject of some discussion between
the inspector who checked out my installation and his supervisor. The problem is
that it could be anywhere or it might be the result of a number of less than optimum
consumer Neutral connections, in their switchboard, at the pole or wherever.
Overall, the reaction to the article has been very favourable and everyone agrees
that if any person ever gets a tingle from water taps or pipes within their home, they
should immediately contact their electricity supplier.
Leo Simpson
siliconchip.com.au
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MAILBAG
Letters and emails should contain complete name, address and daytime phone number. Letters
to the Editor are submitted on the condition that Silicon Chip Publications Pty Ltd may edit and
has the right to reproduce in electronic form and communicate these letters. This also applies to
submissions to “Ask SILICON CHIP” and “Circuit Notebook”.
Valve amplifier has
more detailed sound
I read with great interest your project article to build a Nirvana Valve
Sound Simulator in the August 2014
issue. Since I rekindled my interest in
valve amplifiers nearly 10 years ago,
I and my partner are of the opinion
that listening to our favourite music
through valves is superior.
For many years we have had a reasonably good hifi system, built around
solid-state technology. This all began
around the 1980s and 1990s when we
invested in the following components:
Yamaha A960 integrated stereo amplifier, Yamaha CDC 635 5-disc CD player
and Monitor Audio MA 100 bookshelf
speakers with Monitor Audio WA 200
passive subwoofer. This combination
gave us many years of splendid listening pleasure.
Then around 2005, I came back from
a trip to Hong Kong, where I purchased
a hand-made Class-A valve stereo amplifier. This is based on 300B, 12AU7
and 12AX7 valves, with 5Z4P rectifiers. Upon hook-up at home, using
the same speakers and sound source,
we were amazed at the additional fine
detail in the music, comparing this to
what we had been regularly listening to through the Yamaha amplifier
(for example, we could now hear the
musicians turning music sheet pages
Ground conductivity is
important for MEN system
The August Publisher’s Letter and
the article on the MEN system has reminded me of two situations. First, if
the earth connection is solely via an
Earth stake, the value of the ground
conductivity is obviously very important. I have seen an example in
which dry weather resulted in very
low ground conductivity and effectively no Earth. The solution was to
water around the ground stake.
The second situation has been
4 Silicon Chip
in the background). So much so that
we preferred to shelve the Yamaha
amplifier which is 100W per channel
with THD figures of 0.005% whereas
the 300B valve amplifier is 10W per
channel with harmonic distortion
figures of 0.3%.
Then some 12 months ago “The
Tube CAD Journal” on the web ran an
article on “Restoring Lost Harmonics” – see www.tubecad.com/2013/06/
blog0265.htm
In the light of your current article
on the Nirvana Valve Sound Simulator, I was wondering if you might be
interested in seeing this and maybe
commenting?
Brian Collath,
Moss Vale, NSW.
Leo Simpson comments: while not
denying that your valve amplifier may
reveal more detail than the Yamaha,
I would want to know precisely why
the latter was supposedly so inferior.
Possibly, the Yamaha really is inferior,
especially at low signal levels where
its distortion performance is likely to
be nowhere near .005%. After all, it
was a 1980s design.
I did look at the article in the “Tube
CAD Journal”. The idea that you can
recover lost detail from a recording by
using an amplifier that adds distortion is nonsense. The Nirvana Valve
Simulator project is actually an exerseen a few times. Some of the switch
mode power bricks use a 2-pin plug
for the power lead. If the Neutral
connection is not made and the Active is, a person can receive a mild
shock from the low voltage side. This
is because there is a small capacitor
connecting the primary and secondary sides of the circuitry. The fault
only lies partially with the switchmode design.
The major fault is with the moulding of the plastic around the plug.
The Neutral (and Active) brass ring
cise in adding distortion, as noted in
the article. It certainly cannot reveal
lost detail but it will make a modern
semiconductor amplifier sound more
like a valve amplifier.
Your Yamaha A960 was a fine
looking amplifier. If it belonged to me
I would investigate if I could update
its electronics with our Ultra-LD Mk3
amplifier circuitry.
Problems with
ceiling lights
Most of the ceiling lights in my
house are recessed “oyster cans”. A
few years ago I was alarmed about
fires caused by quartz-halogen lamps
in ceilings, so I had them changed to
compact fluoros (CFLs). Apart from
the slow ‘warm up’, they seemed to
be doing the job. More recently, I tried
changing to LEDs, with a view to even
greater economy, longer life, and less
time spent on ladders (one of the commonest causes of injury in older men).
As reported earlier in correspondence to SILICON CHIP (January 2012),
LEDs in recessed cans overheated and
failed quickly. An editorial note commented that CFLs also require good
ventilation and will have a short life
in recessed cans. Replacing all oyster
is bonded to the plastic and cannot
grip the pin on the power supply.
George Ramsay,
Holland Park, Qld.
Comment: your point about ground
conductivity is most important. It is
for this reason that the domestic installation should also connect to the
home’s copper water pipes. Clearly,
long periods of very dry weather
will prejudice ground conductivity
and there can be no reliance on the
area around the Earth stake being
regularly watered.
siliconchip.com.au
cans in my ceiling was going to be a
big job, so I went back to CFLs and
hoped for the best.
Recently I had to get back up a ladder and replace a CFL. I found blackening due to overheating and started
wondering about the next move. A
discussion at the American EDN website was very informative, but not very
comforting – see www.edn.com/electronics-blogs/led-insights/4423570/
That-60W-equivalent-LED--Whatyou-don-t-know--and-what-no-onewill-tell-youHere’s what I learned:
(1) The much-vaunted long life-time of
LEDs does not apply if they overheat,
and overheating is very common.
(2) Recessed fittings are very bad for
both CFLs and LEDs.
(3) “Base up” installation for LEDs and
compact fluoros is much worse than
“base down”, and is likely to result
in overheating and poor lifetime for
both LEDs and CFLs. In my experience
this even applies for globes suspended
from cords.
(4) The best solution may be track
siliconchip.com.au
silicon chip add.indd 1
Novel use for
old hard disks
Recently, I needed to upgrade
my 5-year-old desktop computer
and then had to dispose of it. It had
a lot of personal data that I really
didn’t want to be trawled by someone wanting to steal my identity
and just dumping it at the local
council recycling collection centre
didn’t appeal. So I removed the old
HDD, dissembled it (Philips and
flat-bladed screwdrivers were the
only tools necessary) to remove the
lighting or (although not very practical) long strips of multiple LED chips
glued into a U-shaped aluminium
channel which acts as a heatsink, so
they run very cool and have a long
lifetime.
(5) All mains-type LEDs have switching power supplies built into the
base of the globe, and these generate
electromagnetic ‘fog’ that can make
AM radio reception unusable. Now I
know why my AM reception at home
shiny platter itself and I now have an
interesting-looking and very shiny
coaster for my coffee mug.
My data is secure and probably
by now unreadable following spills
and scratches. A few weeks later, I
did the same for a 90-year old friend
who was upgrading from Windows
XP. Her HDD was a twin-platter job
so she now has a pair of coasters.
Keep up the good work with the
magazine.
Jacques Fievez,
East Ivanhoe, Vic.
is getting worse and worse.
(6) Chinese manufacturers take the
view that “as long as the product
meets the ‘specs’ it is OK” while USA
engineers talk about “good engineering
practice”.
We seem to be in a transition phase
where the old is out but we don’t
have generally accepted solutions for
the new.
James Goding,
Princes Hill, Vic.
September31/07/14
2014 5
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6 Silicon Chip
Majestic speaker system with substitute drivers
I have just built the Majestic Speaker project from
your June 2014 issue and it sounds absolutely fantastic.
I used separate sheets of timber for the inside box as
it was cheaper than buying the Bunnings shelf kit. I
also used laminated pine panels for the outside so I
could stain it the same colour as the rest of our pine
furniture. This also worked out much cheaper than
the Kaboodle panels.
As I could not get the Etone horn assembly I decided
to do a bit of research and came up with an Eminence
PSD2002s-8 HF driver fitted to an Eminence H290s
flare. I also used Selenium 15PW3 woofers. All in all,
the speaker prices were comparable to the ones that
your magazine suggested.
Although I don’t have the instruments to measure
the performance of the speakers as such, I can tell you
that my ears were very pleased with the end result and
that’s the best measuring instrument of them all. I drive
the speakers with a Denon PMA-1060 stereo amplifier.
After being in the trade of radio and TV repairs for over
40 years and now retired, I just loved getting my teeth
into this project. Many thanks.
Neville Bell.
Wangaratta, Vic.
Comment: you certainly have made a nice job of the
cabinets. However, without instruments it is not possible to know just how well your substitute drivers will
perform, compared to those specified for the Majestic.
The free-air resonance of 37Hz for the Selenium woofer
and its much larger Vas figure probably means that it
could not achieve the very low bass response that we
claimed for the Majestic.
Furthermore, the Eminence compression driver appears to have a significant fall-off in response above
10kHz and this could not be easily fixed by a boost
circuit in the crossover network. There also appear to
be two tweeter resonances, at 540Hz and 1.8kHz and
these may require additional compensation measures.
Finally, it’s possible that the output from your tweeter
needs some tweaking to match that of the woofer.
Having said that, we have no doubt that your speakers do sound impressive.
siliconchip.com.au
Misunderstanding of
VA and watts
In the letter entitled “Problems With
Isolation Transformer Article”, SILICON
CHIP July 2014, I wish to correct some
factual errors in your correspondent’s
explanation of current with respect
to VA and Watts. Your correspondent
writes, “For a VA of 920 and a load PF
of 0.6, we obtain a power of 522W or a
current of 2.27A, not 4A as suggested”.
This statement is wrong for the following reasons. VA or volt-amperes
is the “apparent power” in the circuit
and is derived (as the name implies) by
multiplying the circuit voltage directly
by the circuit current. This value is
independent of the circuit power factor. Thus for a device rated at 920VA
operating at 230VAC, the current will
be always 4A, irrespective of the power
factor.
“True power” is a value derived by
combining the voltage and current
‘vectorially’ where the voltage and
current are not ‘in phase’. In the case
mentioned by your correspondent, the
circuit power factor is quoted as 0.6.
Since power factor is the mathematical
Beware of Asian
wiring conventions
Readers working on imported
Asian-manufactured electrical and
electronic equipment should be
aware of the fact that the wiring
colours for these devices can be different to the Australian standard.
In these imported devices, Black
is sometimes Active and White is
Neutral.
While it would be logical to ascosine of the angle of lag in an inductive circuit (or lead as in the case of
capacitive circuits), the current waveform in this circuit will be lagging the
voltage by 53.13° (cos-1 0.6).
Thus to calculate true power, we
multiply 230V by 4A (the result of
this is the VA), then multiply by the
power factor of 0.6. The result is 552W.
Note that the current is still 4A, not
the 2.27A he stated.
For a load of 552W to draw 2.27A,
the circuit voltage and current would
be in phase and the Watts and VA
would be equal in value for a circuit
sume that White is Active (as in
3-phase power or twin active for light
switches) and Black is Neutral, according to Australian standards, this
is not the case with these imported
devices.
Anyone changing plugs from 2-pin
EU or US to 3-pin AU could easily
wire the plugs incorrectly if they are
not aware of this wiring convention.
Bruce Pierson,
Dundathu, Qld.
power factor of 1, ie, unity.
The fact that the current stays high
is the prime reason that power supply authorities insist on high values
of consumers’ load power factors.
The supply authorities must design
installations to cope with the values
of current as per the apparent power
(VA), but consumers only pay for true
power (W), since consumers’ meters
only measure the vectorial combination of currents and voltages no matter
how far out of phase they may be.
These quantities may be further explained by the power triangle, where
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September 2014 7
Mailbag: continued
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8 Silicon Chip
MEN means
‘Multiple Earth Neutral’
My August 2014 copy of SILICON
CHIP arrived and as usual I dived into
the Publisher’s Letter first. Oh dear,
Leo, you nearly got my subscription
cancelled on the spot. In talking
about domestic power supplies,
you incorrectly bracketed M.E.N.
as “Mains, Earth, Neutral” but all is
forgiven, since you got it right in the
main article.
I do not know a local ‘sparky’
with whom I would trust to even
discuss your article. I built a new
house about 12 years ago and had
the wiring done by a ‘sparky’ I had
known for probably 30 or more years
at the time. All the cables were run
and the sparky himself installed the
Earth stake and made the necessary
connection, explaining that the water
pipes could not be used because (a)
they might not be deep enough to get
a good earth and (b) there could be
(and were) plastic bits.
He didn’t know why but that was
what the regulations said (I hate
regulations which say “do”, without
an explanation as to “why”). Good,
the only thing that concerned me
was that in due course I laid concrete
Watts lies horizontally at the bottom,
VA is the hypotenuse, the Power factor
is the cosine of the angle between the
two quantities.
Thanks for a great magazine.
Terry Ives,
Penguin, Tasmania.
A climate of chaos?
Has a climate of chaos affected the
letters to the Editor? Unless I have
been asleep while emailing, I have
been wrongly credited with a letter
on climate change, on page 10 of the
August 2014 issue.
Although I am mainly interested
with the other side of the climate/
energy debate, from my university
lectures on the subject I think the
writer was pretty near the mark when
he used the word “complex”. Perhaps
another word that should be added
when dealing with the Earth’s climate
paths all around the house meaning
that the Earth stake was at least 1.2m
from any hope of being watered.
I suppose all is OK since we have
since been converted to smart meters.
I use the plural deliberately, because I
have two of the darn things but that’s
another story. I assume that if there
was a problem the large number of
installers who turned up to look at
my different system should have
spotted any problem.
Graeme Burgin,
Arafat, Vic.
Leo Simpson comments: I obviously
had a brain snap when I wrote “Mains
Earth Neutral” in the Publisher’s Letter. The really annoying aspect is
that at least five other people read
that editorial and did not see that
mistake! Oh, the frustration of it!
I well remember that the editor of
another magazine, on being criticised
for making a mistake, claimed that
he “was only human, after all”. I do
not make that admission or excuse,
even though it might be true!
We have since corrected the error in the on-line edition at: www.
siliconchip.com.au/Issue/2014/August/Electricity+is+a+boon%3b+ele
ctricity+is+a+killer!
is “chaotic” (as in Chaos Theory?).
Even with powerful climate cycles
such as the ocean conveyor system,
there is so much chaos acting on the
global main weather engines; it is a
semi-stable system.
Such systems can be provoked into
new semi-stable states by short-term
external influences. It also does not
have to be that powerful (the famous
butterfly effect). Just because global
temperatures have not risen since 1998
does not mean any extra retained energy from global warming is not affecting other and unobserved susceptible
parts of the globe and repercussions
arise unexpectedly later.
On the personal observation aspect
mentioned in the letter, in 1975 the
WA annual rainfall suddenly halved
when compared to known records to
that date. It has remained so to my
knowledge to the present time which
siliconchip.com.au
I am sure many older WA residents will attest to. It is a
measured fact, which has seriously influenced the fresh
water supply situation of Perth. It does not mean by itself
that global warming is taking place but does contribute
to measured collective knowledge which may indicate a
trend to climate change. Personal observations need to be
checked against hard data.
Modelling such a system is not for the scientific and
maths faint-hearted, as indicated by Dr Bob Lile’s letter
in the July 2014 issue of SILION CHIP – particularly since
the science community in this country is beholden to the
politicians for their funding. Politicians are notorious for
wanting absolute facts and then tend to shelve facts and
the funding for results that are not compliant with their
current ‘ideology’.
Kelvin Jones,
Kingston, Tasmania.
Comment: we must apologise for wrongly attributing a letter from Alan Wilson, of Glen Iris, Victoria, in the Mailbag
pages of the August issue, to Kelvin Jones.
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I have a number of comments regarding the switchboard
manufacturing in 3 or 1 days
shown in the article on the Multiple Earth Neutral system
in the August 2014 issue.
It is considered good practice for the tunnel screw terminals of Earth cables to be double-screw terminal conFrontPanelExpress.com
nectors; not single tunnel screw as shown in the picture
1(800)FPE-9060
(people might know them as “blue points”). While it’s
true that a single screw terminal is permissible, according
to AS3000 clause 3.7.2.11 b (ii), many electricians will
always use double-screw connectors when connecting
connectors is common in electrical installations, unlike
Earth cables for the reason that unless you have actually
that shown in the pictures of the switchboard. Tunnel
measured whether the single screw connector satisfies
screw connectors are also normally very lightly wrapped
b (ii) ,you don’t know if it meets specifications. With many
with some PVC to cover the exposed screw heads. It’s
parts coming from overseas, it would be unwiseSilicon
to simply
considered
good practice and this would apply to Earth,
Chip ad 120mmx87mm.indd
1
rely on an assumption that it will be OK to use a single
Active and Neutral connections.
screw connector.
Another thing I noticed in the picture was the use of a
By using a double-screw connector you are assured of
soldered connection of some 15+ Earth cables. Given that
a legal connection without any measurement of the conall of those cables also seem to be soldered into a small
nector. I have a suspicion that an old rule in AS3000 said
volume, I would have some misgivings about the integrity
that double-screw connectors were the only ones you could
of the soldered joint if we consider that the combined
use and this is another reason that the use of double-screw
cross sectional area of that soldered connection would be
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siliconchip.com.au
September 2014 9
11/14/12 7
Mailbag: continued
Earth stakes
can corrode
The Multiple Earth Neutral (M.E.N)
article in the August 2014 issue
was most interesting. All plumbers
should read it.
In the mid-1970s, the Earth stake
became the mandatory method for
earthing electrical installations in
all new residential and commercial
buildings, alterations, extensions
and repairs to existing electrical installations. It’s also my understanding that the building earth must have
two attachment points – Earth stake
AND water pipe. These Earth connections must also be sprayed with
zinc-loaded paint to protect them
from the elements and the earth wire
itself must face down to minimise
water ingress.
The accompanying photos tell
the story.
15mm2 (at the very least) wide and
all of those wires would need to be
thoroughly heated for a soldered joint
to have a good integrity.
Haven’t we all had problems when
not heating even very small, narrow
cables properly and the soldered joint
becoming a “dry joint”? You might
need a blow torch to heat all those
cables in that small volume to the right
Earth stakes also need replacing;
they are a copper-plated mild steel
rod. In my case, the Earth rod had
become a 3-5mm bit of rusted steel
temperature. The other thing about the
soldered Earth connection is that once
the whole bundle is soldered together,
exactly how would anyone else who
comes along actually inspect the connection visually, other than having to
physically peel all the PVC tape off
the connection?
All things considered, can you see
why it is more commonplace to use
after being staked in heavy clay soil
for about 30 years.
Cyril Kosorok,
Minchinbury, NSW.
an appropriate Earth bar that can accommodate a larger number of Earth
cables?
Who knows, the bar might even be
numbered so that the cables are associated with the Neutral cables leading
into the Neutral bar (you are meant to
label the protective device, eg circuit
breaker with the associated cable on
the Neutral bar – CB1 is marked N1
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siliconchip.com.au
Tenants saved from injury
by electrical inspection
The Publisher’s Letter in the August 2014 edition
of SILICON CHIP should be given wide distribution.
Some years ago, one of my tenants in a Darwin
property reported receiving “tingling” when using
the taps. I had the matter investigated and it turned
out to be the loss of Neutral through corrosion as well
as a badly wired hot-water service. I had lived at the
property for three years beforehand with my family
and without any problems.
The cost of the inspection and repair was a small
price to pay to prevent a possible loss of life; not to
mention the litigation which would inevitably follow
a tragic outcome.
A ‘tingle’ is a sure sign that more is to come; don’t
ignore it.
Graeme McKenzie,
Thuringowa, Qld.
to tell you that the associated Neutral of the Active is
screwed under number 1).
Using an Earth bar allows easy expansion of the circuit
by the next electrician, as they can simply screw down onto
a spare terminal (double screw connection). An Earth bar
can also be visually and physically inspected by simply
testing the screw tightness. AS3000 seems to allow for a
bird’s nest of Earth cables to be soldered but with some
insight into the subject of earthing I myself would not recommend soldered Earth connections in this case. Another
thing is that some character might come along, see these
soldered connections and then shove the whole thing into
a large tunnel screw connection if it were smaller – bad
because screwing down onto a soldered joint is considered very bad form, as it creates high resistance joints (I
stopped someone from doing it a number of years ago).
Another thing missing from the equation in the picture
is a label telling anyone which of those yellow/green cables is the MEN link. According to AS3000, this is now
another requirement under the new rules.
On the whole though, the article is very good if an
interested party wants to get an idea of how the earthing
system really works. It should be required reading for
every electrician.
Guy Reece,
Kelso, Qld.
Leo Simpson comments: as far as I know, the switchboard
is completely legal, conforms to AS:NZS3000 and has been
inspected on at least two occasions. The first was about
15 years ago when I had the house completely rewired,
a new switchboard and box installed and new mains out
to the pole. At the time I insisted on having a complete
inspection. Then, as reported in the August 2014 article,
the entire switchboard was thoroughly checked by an
Energy Australia inspector. He even checked the tightness
of all Earth and Neutral connections. The Earth bundle is
soldered and is legal.
However, it does seem as though energy authorities
SC
around Australia do maintain different standards.
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September 2014 11
How
OMEGA
Ruled
The
World
Before
GPS
By Dr DAVID MADDISON
12 Silicon Chip
Question:
What was the main
global real-time radio
navigation system before
GPS took over in 1997?
If you answered
“Omega”, you are
correct.
And where is the tallest
man-made structure
in the Southern
Hemisphere?
The answer is the nowobsolete 427m high
Omega tower near
Woodside in Victoria.
Here’s how the Omega
system worked – and was
used for more than 20
years.
siliconchip.com.au
O
The US Navy had
mega is now obsolete
a very specific and
but the huge antenna
specialised need for
mast still stands as
Omega, apart from it
an imposing landmark in
being a general purthe Gippsland area in southpose, global, real-time
eastern Victoria.
navigation system.
The tower is 427.45 metres
In 1964 it was introhigh (1,402.4 feet) and when
ducing a fleet of naviit commenced operation in
gation satellites called
1982 it was the fourth highTRANSIT (also known
est structure in the world. It
as NAVSAT – Navy
is also said to be the world’s
Navigation Satellite
tallest Very Low Frequency
System). These would
(VLF) radio antenna.
allow global high acSince the tower is close to
curacy position fixes
the sea, it is used by fishermen
of around 120 metres
as a visual guide to their loca(decreased to 3m by
tion. Assuming a 472 metre
1980 with software
height (the base of the tower
improvements and betis about 45m above seal level) To get to the top, you have to climb that ladder seen in the foreand a fisherman with his eyes ground – there is no lift or hoist. The person you can (perhaps!) see ter geodesy models)
which would origi2 metres above the water, the is an abseiler, probably illegally descending from inside the top of
top (bright red during the day the Woodside Omega Tower. There has also been at least one death nally be used to reset
the inertial navigation
and illuminated at night) can amongst daredevils using the tower for illegal BASE jumping.
be calculated to be visible Attribution: “Woodside Omega Transmitter” by Nickinator – Own work. systems on submarines (later TRANSIT
from about 83km away.
became widely used elsewhere).
The tower was originally intended to be built in a more
Ground stations used the Doppler effect from signals
optimal location in New Zealand but this did not happen,
transmitted from these satellites to determine their position
because of opposition by protest groups against military
much like (but in reverse of) how the Argos satellites (see
infrastructure, even though it could be used by civilians.
SILICON CHIP, July 2014) determine the position of some
There were seven other stations around the world, used
models of the Argo floats.
in conjunction with the tower in Victoria.
TRANSIT satellites were in use for more than 30 years,
The Omega Navigational System preceded GPS as a
from 1964 to 1996, for both civilian and military use and
global navigation system and operated between 1971 and
these seemingly indestructible satellites remain in use
1997, transmitting VLF radio signals between 10kHz and
today, as part of the US Navy’s Ionospheric Monitoring
14kHz to provide navigational fixes.
System.
The system was developed by the United States, although
A problem with this Doppler navigational technique is
a US court subsequently determined that it was based
that it results in two position
on work by the British Decca
fixes, one real and one
Navigator company. It refalse and it is necesceived US Governsary to distinment approval
guish befor go-ahead
NORWAY
tween
in 1968.
NORTH DAKOTA
FRANCE
JAPAN
HAWAII
LIBERIA
ARGENTINA
siliconchip.com.au
AUSTRALIA
Omega stations were located in Bratland, Norway (Station A), Paynesville, Liberia
(Station B), Kaneohe, Hawaii (Station C), La Moure, North Dakota (Station D),
Chabrier, France (Station E), Trelew, Argentina (Station F),
September
September
2014 13
2014 13
Woodside, Victoria, Australia (Station G)
and Tsushima, Japan (Station H).
After the Omega System shut down, some of
the equipment was transferred to the Maritime
Museum in nearby Port Albert
(http://yarrampa.customer.netspace.net.au/pamm.html).
This is just one of the items on display: an Omega
receiver (although there were many types).
the two. Traditional navigation techniques were not always
accurate enough to do this but Omega could provide the
correct one.
Omega’s design accuracy was 2 to 4 nautical miles (3.7 to
7.4km) but this was largely dependent upon the accuracy
of tabulated radio propagation predictions.
TRANSIT positions were more accurate than Omega’s
so they were used but Omega’s fix was good enough to
distinguish between the real reading and the false one.
And although TRANSIT position fixes were more accurate than Omega’s, another problem with TRANSIT was
that it took several hours before a fix could be obtained at
the equator and one or two hours at mid latitudes. Thus it
was not a real-time system, unlike Omega.
So despite the better positional accuracy available with
TRANSIT, Omega soon became an accepted navigation
system in its own right.
And before GPS, Omega was the state-of-the-art realtime global navigation system. Other navigation systems
were available and more accurate but were not global in
scope, having only limited range or regions where they
could be used.
Very low frequencies
Omega antennas were so large because they operated
at very low radio frequencies; from 10 to 14kHz. The
wavelength of these frequencies is 21km to 30km so the
antennas have to be very large to be even moderately efficient. Even so, they are only a fraction of the wavelength
in height. One quarter wavelength would be ideal but a
This Omega Aerial Tuning Relay was one of five units and is
shown with cutaway sections. Each of the five relays might
switch twice in each ten second cycle to change the frequency
of the signal (see table overleaf) meaning that each relay would
have to operate around 6,000,000 times per year. The noise of the switching relays could be heard up to 400 metres away,
even though housed in a heavily built concrete building. The white objects inside the relay are vacuum switches designed
to prevent arcing as voltages as high as 200,000 volts may be present. The vertical copper tubes were designed to prevent
electrical losses as AC currents tend to be conducted on the surface (skin effect) rather than deep inside a solid conductor.
The donut-shaped rings were designed to prevent corona discharge and arcing as they offered a smooth surface and the
black spheres on the right were spark gaps to allow a harmless discharge of any electrical arcing that was to occur.
14 Silicon Chip
siliconchip.com.au
Woodside Omega Tower Facts
The Australian Department of Transport built the station for
a cost of $12 million (1982 dollars) not including land. The
tower itself was built by the Sydney-based Electric Power
Transmission company for a cost of $1.1 million.
The tower weighs around 500 tonnes and the base of the
tower is in the form of a ball joint which allows the tower to
move under wind load. The tower is designed to withstand
wind loads of 228km/h at the top and 145km/h at the bottom.
Beneath the tower is embedded an extensive copper wire
earth system or “counterpoise”.
Woodside Station G was the eighth and last station in the
Omega System but was subject to an eight month delay
because of union industrial action.
quarter wavelength of 10kHz is 7500 metres so the size
cannot be anything like that. Because of this the efficiency
is very low, perhaps only a few percent .
Due to the low efficiency of VLF antennas a very high
input power and drive voltage is required for a much
smaller output power, however the output power of this
Omega antenna was 10kW, as it was for all other Omega
installations around the world.
VLF frequencies were chosen because (a) the VLF signals
would be propagated globally with little attenuation in
the natural wave-guide created between the earth and the
bottom of the ionosphere, which would also minimise the
number of stations required, (b) the stability of VLF signals
as they are not subject to much fading and (c) the relatively
great distances between lines of zero phase difference
within which vessels would locate themselves, provided
by the long wavelength of the radio waves.
Coast Guard in partnership with Argentina, Norway, Liberia, France, Japan and Australia.
Conspiracy theories abound
As with most technical subjects that have any military
connection, conspiracy theories abound regarding the actual use of the Woodside Omega Tower (just as they still
abound regarding North West Cape).
And who could forget the crackpot claims which came
Top guy wires driven elements
In the case of the Victorian installation, the tower itself
is not an active antenna element. Instead, the uppermost
guy wires are the electrically active elements.
These radiating elements are electrically insulated from
both ground and the mast and are arranged in a pattern
akin to the ribs of an umbrella.
“Umbrella” antennas radiate vertically polarised waves
which is appropriate for the atmospheric wave-guide mode
of propagation with wave-fronts oriented vertically between
the ground and the bottom of the ionosphere.
Other towers may have had different designs depending
upon local circumstances.
The eight Omega stations were installed around the
world, distributed in such a manner that a receiver would
be able to receive signals from at least five transmitters. In
addition there was a testing station in Forestport, New York.
The Omega system was operated by the United States
siliconchip.com.au
This enormous helix coil is part of the matching circuitry
in the antenna feed, required because the wavelength of the
antenna is very much shorter than even a quarter-wave of
the signal wavelength. The gauge of the coil “wire” and the
size give some idea of the powers involved. (Photo courtesy
Catherine McAloon, ABC Gippsland).
September 2014 15
Omega’s “Hyperbolic” Navigation System
LOP-2
A hyperbolic navigation system involves measuring
the timing or phase difference for the reception of two
X
OBSERVER
radio signals from different places to establish the rela(Hyperbolic Fix)
tive distance from each station. One way these timing
differences can be determined is through looking at
the phase difference between the received signals. If
the transmitted signals were perfectly synchronised
with each other and if the receiver was equidistant
between two stations, there would be zero phase difP-1
LO
ference between the two signals. If the receiver was
closer to one station than the other, there would be
a phase difference, indicative of the relative distance
to each station.
Plotting on a map the location for all possible positions corresponding to the observed timing or phase
Y
M
differences results in a hyperbolic line called the Line
of Position (LOP). The receiver could be anywhere
along that line so another measurement is made with
Hyperbolic Lines of Position (solid lines). The dashed green lines
a different (third) transmitter. This results in another show zero phase contour lines between station M and X and the
Line of Position. The point at which these two lines dashed red lines show zero phase contour lines between station
intersect corresponds to the position of the receiver.
M and Y. These dashed lines correspond to “lanes”. The Lines of
The reality is a little more complicated though, as Position (LOP) for the observed timing or phase differences have
there are multiple points where zero phase difference been plotted by the observer for both stations X and Y and the
can occur. As one travels away from a point of zero intersection of these lines gives the position of the vessel.
phase difference going closer to one transmitter and
away from the other, the phase difference increases from
At the lowest frequency of 10.2kHz used by Omega, the
zero to 360°. A phase difference of 360° is the same as a lane width was around 14.7km or 8 nautical miles (correspondzero phase difference. The distance between these points ing to half the wavelength). Different frequencies resulted in
of zero phase difference (or zero phase contour lines) cor- different lane widths and different frequencies could also be
respond to one half of the wavelength of the radio signal.
combined to generate very wide lane widths for purposes
Since the distance between stations is much greater we shall see later.
than half the wavelength of the transmitted signal, there
The position of these lanes was plotted on reference maps.
are multiple zero phase contour lines. These zero phase For reference purposes the lane midway between stations
contour lines are known as “lanes” which are shown as the was numbered 900 and with the lane numbers decreasing
dashed lines on the diagram above
toward the station with the lower letter designation and increasing toward the station with
TRANSMISSION DURATION (s)
0.9
1.0
1.1
1.2
1.1
0.9
1.2
1.0
the higher letter designation
(eg, decreasing toward StaStation A: Bratland, Norway
10.20 13.60 11.33 ------ ------ ------ ------ -----tion A and increasing toward
Station B: Paynesville, Liberia
------ 10.20 13.60 11.33 ------ ------ ------ -----Station H).
In addition, it was possible to
Station C: Kaneohe, Hawaii
------ ------ 10.20 13.60 11.33 ------ ------ -----determine the relative position
Station D: LaMoure, ND, USA
------ ------ ------ 10.20 13.60 11.33 ------ -----within these lanes by examinStation E: Chabrier, France
------ ------ ------ ------ 10.20 13.60 11.33 -----ing the proportion of phase
difference corresponding to the
Station F: Trelew, Argentina
------ ------ ------ ------ ------ 10.20 13.60 11.33
relative position within the lane
Station G: Woodside, Vic, Australia 11.33 ------ ------ ------ ------ ------ 10.20 13.60 (from zero to 360° representing
Station H: Tsushima, Japan
13.60 11.33 ------ ------ ------ ------ ------ 10.20 from zero to 100 percent of
the lane width), so the lanes
Each Omega station transmitted three different frequencies in a unique order and
could be further divided into
duration and could be identified on that basis. For example, Station A transmits
100 equal parts for greater
10.2kHz for 0.9 seconds, then 13.6kHz for 1.0 seconds, then 11.33kHz for 1.1 seconds.
accuracy.
Between each transmission there is a 0.2 second delay. Note that for any point in the
The big question was, which
transmission sequence there were always three different frequencies being received,
lane
was one within? As it
10.20, 11.33 and 13.66kHz from three different stations. For example, when Station A
turned out, it was not possible
transmitted its 0.9 second 10.20kHz signal, Station G was transmitting on 11.33kHz
to directly determine what lane
and Station H was transmitting on 13.6kHz with a total transmission cycle takes of 10
one was within. It was necesseconds, endlessly repeated. All stations were synchronised via Caesium beam atomic
clocks. Note that throughout Omega’s service life some frequencies were changed and
sary to count the lanes a vessel
also each Omega station transmitted an additional frequency as an aid to identifying
crossed from the time it began
the station; not for navigational purposes.
16 Silicon Chip
siliconchip.com.au
its voyage from the port whose position was accurately
known. This lane count was related to a map showing the
lanes for a particular geographic area.
A problem arose if the lane count was lost for any reason,
such as due to power or equipment failure, adverse radio
propagation conditions or transmitter failure. In the event
of a loss of lane count it was easy enough to re-determine
the position within lanes but the actual lane numbers were
not known and had to be determined.
This inability to directly determine a lane number if the
initial lane count was lost was known as “lane ambiguity”. It
was therefore necessary to know one’s approximate position
using navigation techniques such as maintaining a vessel
track with dead reckoning. But the accuracy of the vessel
track determined by dead reckoning or other traditional
means was less than the spacing of the lanes so it was not
possible to accurately locate the vessel within any particular
lanes with certainty. In reality, a proper location fix within the
lanes required that the other navigation method (eg, dead
reckoning) be accurate to half a lane width.
Lane width could be increased by changing the transmitting frequency but 10.2kHz was already the longest
wavelength in use and therefore the widest lane width. But
as shown in the table at left, there were three transmission
frequencies, at 10.20kHz, 11.33kHz and 13.60kHz. The
13.60kHz signal gave a lane width of 11.0km or around 6
nautical miles; unfortunately an even narrower lane width.
But here is the clever part. These frequencies were carefully selected so that four 13.6kHz lanes (4 x 11.0 = 44km)
equal the same width as three 10.2kHz lanes (3 x 14.7 =
44km ignoring rounding errors). When these frequencies
are electronically subtracted in the Omega Navigation
equipment, 13.60 – 10.20 = 3.4kHz, we get a much lower
frequency with a correspondingly greater lane width, the halfwavelength of this frequency being 44km, ignoring rounding
errors. This is exactly triple the width of the 10.2kHz lanes.
Then to establish lane count it was only necessary to
establish one’s position by dead reckoning or other means to
within half the lane width or 22km instead of around 7.35km,
as with the 10.2kHz signal. This is within the capability of
dead reckoning and other means. Having established one’s
position within the 44km wide lane the position within that
lane is determined (on a scale of zero to 100 percent of
width).
Recalling that this 44km wide lane corresponds to exactly
three 10.2kHz lanes it is then possible to establish which
of those lanes the vessel is located within by reference
to Omega navigational charts. The frequency is reset to
10.2kHz and lane counting can then resume. The 11.33kHz
frequency can be utilised in a similar manner and wider lane
widths of 133km can be established.
Of course, in matters maritime, the original measurements
were in nautical miles.
All Omega readings had to be adjusted according to
correction tables which related the propagation of the VLF
radio signal in relation to changes in the ionosphere related
to time of year, location on the globe, time of day etc. The
corrections may change the percent of lane readings and
may even change the lane count number.
siliconchip.com.au
Above is a Google Earth image of the tower with the ground
plane clearly visible, along with the many guy wires.
out about the HAARP research station (see SILICON CHIP,
October 2012).
One story about the Tower in particular and Omega in
general, which was published back in 1994 in the “Green
Left Weekly”, had all sorts of claims and ‘statistics’ (see
www.greenleft.org.au/node/7434).
Now, we’re not saying we subscribe to ANY of the conspiracy theories in that story but “reading between the lines”
does give a few more insights, despite its sensationalism
and outright bias.
For example, they query the “10kW” radiated power of
Omega, maintaining there is also a half-million watt “ground
wave” transmitter also associated with the installation.
(We believe that the very high input power – perhaps even
approaching 500kW – is required because of the very low
efficiency of the antenna. But why ruin a good story with
facts?).
Omega shutdown
The Omega Navigation System was shut down worldwide
at precisely 0300Z on September 30, 1997. All navigation
users, having been given appropriate warning, were as-
Visiting the Tower
The Woodside Omega Tower is well worth a visit, particularly if
you’re in the Gippsland area. To get there, go a short distance to
the east of Woodside on the South Gippsland Highway, A440.
You can’t miss it! It can be seen from the side of the road (make
sure you park safely). You can also see it on Google Earth: its
specific location is at 38° 28’52” S, 146° 56’ 7” E or -38.481111,
146.935278. There is also a YouTube video by the author showing
the installation at http://youtu.be/S_T7hd0oXUE
September 2014 17
Warsaw Radio Mast
While the Woodside Omega Tower remains one of the
largest radio masts in existence, it is a pygmy compared to
the long-wave AM radio mast which once stood in Warsaw,
Poland. This was 646 metres (2,120 feet) tall and was the
world’s tallest structure until its collapse in August 1991.
Its two megawatt, 227kHz broadcasts could be heard around
the world.
This equipment rack contains the following instruments: 1) a
synchronometer, which kept the signal correctly timed with
others around the world, deriving its timing pulses from a
caesium beam atomic clock; 2) an Omega monitor, receiving
signals from a remote site at Blackwarry for self-monitoring
purposes; 3) Omega Format Display showing which stations
were transmitting and when; 4) Omega Signal Controller –
provided computer control of the signal and also monitoring
capabilities; 5) Power supply, one of several required to
provide voltages of 12, 28 and 11,000 volts DC and 115, 240,
415, 480 and 9,000 volts AC; 6) Frequency Counter to check
the signal or do other system checks; 7) Relay Driver to
switch high voltage relays; 8) a modem to communicate with
the remote monitoring site mentioned in (2); 9) a high voltage
relay to switch 100,000 volts for aerial tuning purposes.
sumed to have migrated to GPS by that time.
While GPS has replaced most radio-navigation systems,
they were much more difficult to jam by enemy or terrorist
activity than is GPS, which is relatively easy to jam. They
were also likely to be more resistant to the effects of electromagnetic pulses from nuclear explosions than are satellites.
Today, we take GPS for granted and it is built into numerous devices such as phones, tablet computers, cameras, cars,
collars to track pets and other animals and there are even
dedicated GPS units! It is highly accurate (typically within
3 metres) and simple to use. In fact, the typical consumer
experience goes no further than seeing one’s location on
a map or planning a trip route. Navigation technology has
come a long way in a very short time.
Use by the Royal Australian Navy
After the Woodside Omega station was shut down it
was acquired by the Royal Australian Navy (RAN) for use
in submarine communications. VLF signals are useful for
submarine communications because unlike other radio
frequencies, VLF waves penetrate between 10 and 40 me18 Silicon Chip
tres into seawater. For this purpose the station had to be
converted from operation at 13.0kHz to 10-14kHz and other
significant equipment changes had to be made to support the
2-channel constant envelope minimum-shift keying (MSK)
required for unidirectional submarine communications.
California-based company Hi Q Engineering, who specialise in LF and VLF communications, was contracted to
make these changes. Changes included: adding a phase shift
network and converting some existing tuning variometers
to T-network coils plus adding a capacitor bank, removal
of the existing matching transformer and adding another
tuning variometer, reducing the inductance of remaining
tuning variometers, modifying the main helix and tapping into it with fewer turns, major changes to the helix
network; and adding digital antenna current metering and
an automatic antenna tuner.
After these modifications the station supported 100 baud
two channel MSK transmission with 150kW antenna input
power and a radiated power of 36.5kW. Its station designation was VL3DEF.
It was shut down for Navy and all other use on December
31st 2008, as it was no longer considered viable for use.
Incidentally, there is another large VLF transmitter still
in use in Australia. The Naval Communication Station
Harold E. Holt at North West Cape is a joint facility of the
US Navy and RAN. With 13 towers ranging in height from
304 to 387 metres it operates at 19.8kHz, with an input
power of around 1MW. A counterpoise comprising a mat
of 386 kilometres of copper wire is buried underneath the
antenna array.
The Omega tower’s future?
The future of the Woodside tower is uncertain, depending on who you ask. Some say it should be removed as even
ongoing maintenance is no longer justifiable (there are numerous reports of its aviation hazard lights failing and not
being replaced as quickly as they might).
But many others say it represents an important part of
Australian and international navigational history.
Let’s hope an appropriate alternate use is found for this
tower, such as for amateur radio groups or scientific organisations (or even legal BASE jumpers or tourist operators) and
it is not demolished just because some bureaucrat deems it
convenient, economic or politically correct to do so.
SC
Want to know more?
There’s a wealth of information on the ’net – including a US Navy movie on Youtube showing how ships
and planes can work out their position and much more.
Enter “Omega Navigation” in YouTube’s search panel.
siliconchip.com.au
Create eerie musical
sounds with the:
Opto-Theremin,
Create your own electronicallysynthesised music or produce
eerie science fiction sounds with
our new “Opto-Theremin”. This
completely new design uses
an optical proximity sensor to
provide a more effective volume
control plate which adds the
possibility of rapid tremolo,
while vibrato can be applied in
the normal way with the vertical
pitch antenna.
By JOHN CLARKE
Unlike conventional Theremins, the new Opto-Theremin uses an optical
distance sensor to control the volume, making the unit easier to build and
adjust. A metal antenna rod is used for pitch control.
20 Silicon Chip
T
HIS LATEST THEREMIN from
SILICON CHIP merges the traditional
with the modern. As well as the optical proximity control plate, it includes
a touch of ‘bling’ in the form of blue
LEDs and polished aluminium tubes.
Even the top of the pitch antenna is
illuminated with blue light.
For those who don’t know what a
Theremin is, it is an electronic musical
instrument designed by Leon Theremin in the early 1900s. Pitch and volume are varied by moving your hands
near two antennas and a wide range of
tones covering several octaves can be
produced. Just do a Google search for
Theremin to see a selection of YouTube
videos of Theremin performances. All
of those demonstrations involve Theremins of largely traditional format.
The Theremin owes its popularity
to its extreme versatility and to its
unique sound compared to conventional instruments. Even a simple
combination of hand movements can
lead to interesting effects. Theremin
passages can comprise a smooth gliding tone (glissandi) or can be separate
notes (staccato), or a combination of
both. It really is a versatile instrument,
limited only by the skill of the player.
Our Opto-Theremin operates in a
radically different manner to traditional Theremin designs. The ‘Opto’
prefix refers to its use of an optical
volume control and to the blue LEDs
which add visual interest – the ‘bling’.
Before anyone starts worrying that
our new Opto-Theremin may have lost
its heritage, be assured that it sounds
just like a traditional Theremin and is
played in exactly the same way. For
example, the Opto-Theremin still has
a vertical antenna for pitch control just
siliconchip.com.au
Pt.1
like a traditional Theremin, whereby
the right hand is moved horizontally
to change pitch.
The big difference compared to a
conventional Theremin is the volume
control. As with the original, the left
hand is moved vertically to control the
volume but this movement is sensed
using an optical proximity sensor
rather than the traditional horizontal
loop-shaped antenna.
Why use optical sensing?
This solves a number of problems.
Traditional Theremins use RF (radio
frequency) oscillators to feed the antennas for both pitch and volume control. Without careful tuning, there can
be all sorts of interactions between the
volume and pitch oscillators, leading
to unwanted ‘squawks’ in the sound or
pitch changes when the player is only
trying to adjust the volume.
By using optical sensing for the volume control instead, there’s no chance
of any interaction with the pitch control circuitry. Additionally, the volume
action is always predictable and does
not drift with temperature changes.
Plus it makes the set-up procedure
much easier.
We’re still mixing two high-frequency oscillators to produce the audio
signal as this results in sounds with
the required waveform to imitate musical instruments, such as a cello. So
although this new Opto-Theremin has
a different method for volume control,
it still uses RF techniques to generate
the pitch, allowing it to produce the
classic Theremin sound.
Features
In order to play a Theremin, the
siliconchip.com.au
musician must be able to accurately
position one hand near the antenna,
to produce the required pitch. The
generated tone has to be set ‘by ear’,
just as for a violin or a trombone. This
is because the Theremin does not have
a fixed set of notes but instead deliv-
ers a continuous range of tones over
several octaves.
Correct linearity of pitch variation
in response to hand movement is a
critical feature of the design. In this
case, ‘linearity’ means that there is a
similar range of hand movement for
September 2014 21
FOR HAND PITCH CONTROL
ANTENNA
L1
EQUALISING
COIL
VOICING
VC1
HAND
VOLUME
SIGNAL
BUFFER
•
•
•
•
•
•
•
•
VOLUME
VR1
INVERTER &
LEVEL SHIFTER
(IC2a, VR4)
External pitch adjustment control
Linear pitch change with hand
movement over four octaves
Linear volume control with hand
movement
Adjustable hand volume range
Voicing adjustment (internal)
Integral loudspeaker with volume
control
Minimal pitch drift during warm-up
No volume control drift during
warm-up
9VAC or 12V DC operation <at>
250mA (eg, from AC plugpack or
12V battery)
Line output level: 250mV RMS
Frequency range: <40Hz to >5kHz
22 Silicon Chip
Vref
Q4
Main Features
•
LOUDSPEAKER
CARRIER
each octave. It’s important that no
octave is compressed into a very small
hand movement range, as this would
make the instrument difficult to play.
The Opto-Theremin is designed
to avoid this and it includes a test
circuit to assist in correctly adjusting
the linearity. An adjustment is also
included to modify the tonal quality
or ‘voice’ of the Opto-Theremin. This
allows it to be adjusted from producing
a sinusuoidal (or pure) tone through to
a sound that’s reminiscent of a cello at
low frequencies and a soprano voice
at higher frequencies. In addition, an
externally adjustable pitch control
provides compensation for changes in
pitch due to the unit’s location and its
surroundings and/or due to temperature variations.
The unit contains an in-built ampli-
•
•
LINE OUTPUT
CON3
MIXER
IC1
VR2
ADJUST PITCH
DISTANCE
SENSOR
(SENSOR1)
BUFFER
IC2b
Q3
REFERENCE
OSCILLATOR
(T2, Q2)
V+
LOW PASS
FILTER
BUFFER
PITCH
OSCILLATOR
(T1, Q1)
IC3
AUDIO
AMPLIFIER
Fig.1: block diagram of the Opto-Theremin. The pitch and
reference oscillators are mixed together in mixer IC1 and
filtered to provide the tone, while Sensor1 controls the
volume by adjusting the output level from the mixer.
fier and loudspeaker but it also has a
“Line Out” socket on the front panel
so it can be connected to an external
amplifier and loudspeaker system. The
loudspeaker volume is independently
adjustable so it can be silenced when
using an external amplifier or alternatively, used as a monitor speaker
during on-stage performances.
Appearance & controls
As shown in the photos, the SILICON
CHIP Opto-Theremin is housed in two
plastic cases, one to accommodate
the main PCB (and support the pitch
antenna) and a smaller one to house
the distance sensor PCB for the volume
control. They are connected by threaded rods housed within aluminium
tubes and the whole assembly mounts
on a timber pedestal via another set of
aluminium tubes and rods.
The vertical pitch antenna is also
made from aluminium tube and is
easily detached for transportation. The
volume control box is translucent and
lights up during operation to make it
look ‘cool’. A translucent dome at the
base of the pitch antenna is also lit
using blue LEDs, while a separate blue
LED illuminates the transparent cap
at the top. These blue LEDs not only
give the Opto-Theremin an impressive
appearance but also reflect from the
player’s hands when the instrument is
being played, for even greater visual
effect.
The three external controls (power,
volume and pitch) are arranged along
one side of the case, together with the
line output socket. Power can come
from a 9VAC supply or from a mainsderived 12VDC supply or battery.
Note that a switchmode DC supply
(eg, a switchmode DC plugpack) is
not suitable for use with the OptoTheremin. That’s because noise from
a switchmode supply would find its
way into the two onboard oscillators
and upset the operation.
Operating principles
Fig.1 shows the block diagram of the
Opto-Theremin. It uses two oscillators:
(1) a pitch oscillator and (2) a reference
oscillator. Both oscillators are set to
run at close to 455kHz. The reference
oscillator includes pitch adjustment
VR2, to precisely trim the frequency.
While the reference oscillator basically runs at a fixed frequency, the
pitch oscillator is varied via the attached antenna. Any hand movement
adjacent to the pitch antenna alters its
coupling to ground and this changes
the frequency of oscillation.
Both oscillator outputs are buffered
to isolate them from the following
mixer stage, an MC1496 balanced
modulator (IC1). As shown, the signals
are fed to the SIGNAL and CARRIER
inputs of IC1.
Its output comprises several frequencies, including the sum and difference frequencies of the reference
and pitch oscillators.
If the two oscillators are almost
at the same frequency, eg, 455kHz
and 454kHz, then the sum of the two
frequencies will be 909kHz while the
difference frequency will be 1kHz. The
low-pass filter on the mixer’s output
removes all frequencies above 3.3kHz,
leaving only the difference frequency;
in this case, 1kHz.
The resulting 1kHz audible tone is
then fed to unity gain op amp stage
IC2b which buffers it and provides the
siliconchip.com.au
Volume control
As mentioned, we use an optical
distance sensor (made by Sharp) for
the volume control. It comprises an
siliconchip.com.au
OBJECT AT ~ 300mm
LE
C
TE
D
LIG
HT
SCATTERED
LIGHT
RE
F
line output signal. This also drives a
small internal power amplifier (IC3)
and loudspeaker.
So far, we haven’t mentioned the
equalising coil that’s connected between the pitch antenna and the pitch
oscillator. This vastly improves the linearity of the pitch oscillator’s response
as it changes frequency due to hand
movements near the antenna. Without
it, relatively small hand movements
would cause large frequency changes
at the higher octaves.
The equalising coil works by forming a tuned circuit in conjunction with
the capacitance of the antenna. Its
resonant frequency is set to just below
the pitch oscillator’s frequency by its
9mH inductance and the antenna’s
~14pF capacitance. Moving a hand
closer to the antenna increases this
capacitance, thereby reducing L1’s
resonant frequency.
In practice, changes to the equalising coil’s resonant frequency will be
much greater than any corresponding
frequency changes in the pitch oscillator. This is because hand capacitance
effects of just few picofarads will have
a far greater effect on the antenna’s
14pF capacitance (and hence the resonant frequency of the equalising coil)
than on the much larger 220pF capacitor that’s in parallel with the 560µH
pitch oscillator coil (both contained
within a 455kHz IF transformer).
So, with the equalising coil, hand
capacitance changes have a greater
effect on the pitch oscillator for hand
movements further away from the
antenna than closer in. This nonlinearity counteracts the non-linearity
of the pitch oscillator’s sensitivity to
capacitance changes and results in the
required linear response.
For further information on this, see
www.element14.com/community/
thread/1802/l/theremin-linearity
Trimmer capacitor VC1 adjusts the
coupling between the pitch and reference oscillators. This is the ‘Voicing’
adjustment and it affects the waveshape of both oscillators due to intercoupling, thus also affecting the output
waveform shape.
In practice, it’s just a matter of setting VC1 to obtain the required sound
from the Opto-Theremin.
OBJECT AT ~ 40mm
RE
LENS
C
FLE
TE
D
LIG
HT
SCATTERED
LIGHT
PULSED INFRARED LED
CHARGE-COUPLED
IR SENSOR ARRAY
DISTANCE SENSOR
Fig.2: how the optical distance sensor works. As the object moves away from
the pulsed infrared LED, the angle of the reflected light passing through the
lens changes and this changes the position of the light spot focussed onto a
charge-coupled sensor array (or CCD).
infrared transmitting LED, a receiving
lens and a sensor array. The LED and
the receiving lens are spaced about
20mm apart, while the sensor array
is a Charge Coupled Device (CCD)
consisting of numerous light sensors
arranged in a single row.
In operation, the LED is pulsed so
that it produces high-intensity flashes
of infrared light focused as a small
dot. If an object is within the sensor’s
range of measurement, the infrared
light will be reflected and some of it
focused by the lens.
If the reflecting object has an uneven
surface, the infrared light will tend to
be scattered – see Fig.2. However, part
of the light will be reflected back to the
lens which then focuses it on the CCD.
The exact position of the light spot
on the CCD will depend on several
things: (1) the spacing between the
IR LED and the lens, (2) the distance
between the focal point of the lens
and the CCD’s light-sensitive surface,
and (3) the distance from the reflecting
object to the sensor.
The first two distances are fixed by
the sensor itself, leaving the distance
between the sensor and the reflecting
object as the variable.
If the object is close to the sensor,
the reflected light will be focussed
towards the outside edge of the CCD.
However, as the object moves further
away, the reflected light angle becomes
progressively shallower. As a result,
the reflected light progressively moves
towards the other end the CCD. The
sensor includes circuitry to detect
where the light is focussed on the
CCD and processes this information
to produce a voltage output that varies
with distance.
Note that the object does not need to
be perfectly flat or parallel to the sensor. The sensor will detect the object
as long as there is sufficient scattered
light from the object to reach the lens.
Sharp makes several different versions of the distance sensor, each with
different optics that set the range of
distance measurements. The OptoTheremin uses the GP2Y0A41SK0F
sensor which has a range of 40-300mm.
For further information on this device, refer to the data sheet at www.
sharp.co.jp/products/device/doc/opto/
gp2y0a41sk_e.pdf
The output from the distance sensor
drives IC2a which inverts and level
shifts the signal. IC2a’s output then
supplies bias current to mixer stage
IC1, to control the volume. Inverter
September 2014 23
Background To The Theremin
In 1919, Russian Physicist Lev Termen (or Leon Theremin as he is called in the
western world) invented an electronic musical instrument called the “Theremin”.
At that time, the Theremin was innovative and unique in the musical world
and was essentially the first electronic instrument of its kind. Playing it relied
solely on hand movements in the vicinity of two antennas to control two electronic oscillators – one antenna to vary the pitch of the sound and the other to
change the volume.
The Theremin was subsequently further developed and manufactured by
the Radio Corporation of America (RCA) around 1929. General Electric (GE)
and Westinghouse also made Theremins in the 1920s. However, the number
of units produced was quite modest, totalling about 500.
Today, the Theremin is hailed as the forerunner to modern synthesised music
and was instrumental in the development of the famous Moog synthesisers. There
is also a website devoted to Theremins (www.thereminworld.com). Because of
its unique sound, it has been popular with music producers for both film and live
performances. The sound is ideal for setting the scene for supernatural events
and for close encounters with extraterrestrial beings in science fiction movies.
A Theremin was used to produce background music in the feature film “The
Ten Commandments” by Cecil B DeMille (1956). Its eerie sounds have also
made it ideal for science fiction movies such as “The Day the Earth Stood Still”
(1951), “Forbidden Planet” (1956) and “Mars Attacks!” (1996).
The Beach Boys also used an instrument similar to the Theremin – called an
Electro-Theremin (also named a Tannerin) – in their 1966 hit, “Good Vibrations”.
More information on Theremins is available at www.thereminworld.com/
Theremin-Models
Finally, SILICON CHIP has produced four previous designs for home construction: a basic Theremin in August 2000, a MIDI Theremin in April/May 2005,
the Mini Theremin in July/August 2006 and the Mk2 Theremin in March 2009.
stage IC2a is necessary because the
output voltage from the sensor reduces
with distance but we want the volume
to increase as the hand is moved further away (ie, upwards).
Circuit details
Fig.3 shows the full circuit details
of the Opto-Theremin. As well as the
distance sensor (SENSOR1), it uses
three low-cost ICs (IC1-IC3), four JFETs
(Q1-Q4), several coils and sundry
other parts.
Both the pitch and reference oscillators utilise pre-wound 455kHz IF
(intermediate frequency) transformers
(T1 & T2), as commonly used in AM
radio tuners. Each of these stages is
connected as a common drain Hartley
oscillator, with T1 & Q1 forming the
pitch oscillator and T2 & Q2 making
up the reference oscillator.
T1 has a tapped primary winding
with a parallel-connected capacitor
to form a tuned circuit. Its resonant
frequency can be varied using a ferrite
slug which screws into the core. Q1
drives a portion of the tuned circuit
winding via the tapping at pin 2, while
the signal at the top of the tuned wind24 Silicon Chip
ing is coupled to the self-biased gate
of Q1 via a 68pF capacitor. This arrangement provides positive feedback
to maintain oscillation at the tuned
frequency.
The second winding inside T1, at
pins 4 & 6, provides a low-impedance
output signal. This signal is fed to the
gate of JFET Q3 via a 330pF capacitor.
Q3 is wired as a source follower stage,
buffering the signal from T1 and feeding it to pin 1 (SIG IN+) of mixer IC1.
Current is fed to Q1’s drain via a 680Ω
resistor connected to the 9V DC supply
rail, while Q3’s drain current is set by
a 100Ω resistor to ground.
The reference oscillator is very
similar to the pitch oscillator, the difference being that JFET Q2 is powered
via 1kΩ potentiometer VR2 and a 220Ω
resistor. VR2 varies Q2’s drain-source
current to provide pitch adjustment
since altering this current affects Q2’s
gate-source capacitance. This in turn
alters the reference oscillator’s tuned
frequency. Q4 buffers the signal from
the reference oscillator, feeding it to
pin 8 (CARRIER IN+) of IC1.
Equalising coil L1 is connected directly to pin 1 of T1 by placing jumper
link LK1 in its NORMAL position.
Moving LK1 to the TEST position
means that the equalising coil is in
series with a 100kΩ resistor.
Diode D1 connects to the junction
of the equalising coil and the 100kΩ
resistor, while its cathode goes to test
point TP1. In test mode, the equalising
coil is sufficiently isolated from the
pitch oscillator to allow the resonance
of the coil and antenna to be monitored
by a DMM set to read DC volts, connected between TP1 & TP GND.
In operation, the DMM filters the
rectified RF signal from D1 due to
both lead capacitance and internal
capacitance, and it discharges this
stray capacitance via its own loading.
Once the DMM is in place (and LK1 set
to TEST), the slug in T1 is adjusted to
alter the frequency of the pitch oscillator to give the lowest voltage reading.
This sets the pitch oscillator to the
resonant frequency of the equalising
coil and antenna. The frequency is
then adjusted slightly away from this
resonance point.
Mixer stage
As mentioned, the signals from JFET
buffer stages Q3 & Q4 are applied to
pins 1 & 8 of mixer IC1 via 1nF capacitors. The signal level applied to pin
1 is around 180mV, while the level
applied to the carrier input at pin 8 is
reduced to around 50mV by the resistive divider at Q4’s source, preventing
carrier overload.
The signal inputs at pins 1 & 4 and
the carrier inputs at pins 8 & 10 are
all DC biased from a voltage divider
connected across the 9V supply. This
divider comprises the 1.2kΩ, 820Ω and
1kΩ resistors and each input is connect
to the divider via a 1kΩ resistor.
Note that the SIG IN- and CARRIER
IN- inputs (pins 4 & 10) are only DC
biased, with any AC shunted to ground
via 100nF capacitors.
The 680Ω resistor between pins 2
& 3 of IC1 sets the gain of the mixer,
while the bias voltage applied to pin 5
(from IC2a) sets the signal level at the
two output pins (6 & 12). As shown,
these outputs are biased using 2.2kΩ
pull-up resistors (to the 9V rail) and
filtered using 22nF capacitors to remove ultrasonic signals.
Unity gain op amp stage IC2b buffers
the low-pass filtered audio signal from
pin 6 of IC1. The signal is AC-coupled
via a 100nF capacitor to IC2b’s noninverting input (pin 5), while a resissiliconchip.com.au
siliconchip.com.au
September 2014 25
68pF
10 µF
100k
G
2
3
1
IN
470Ω
LED6
GND
OUT
K
K
λ
A
4
6
4
6
K
A
470Ω
λ LED7
A
1000 µF
25V
K
MAX
NORMAL
39Ω
100Ω
G
+9V
1.2k
100Ω
G
CON5 CON2
100k
330pF
100k
330pF
TP
GND
TP1
D3 1N4004
T2 (WHITE)
T1 (WHITE)
100k
A
D1 1N4148
THE OPTO THEREMIN
DISTANCE
SENSOR
GND
Vcc
GP2Y0A41SK0F
Vout
3
2
1
VC1
2-10pF
100pF
3
2
1
NRML
LK1
TEST
REG2 7805
68pF
220Ω VOICING
PITCH
ADJUST
100k
G
SENSOR1
S
D
S
D
~9mH
L1
EQ. COIL
+9V
S
D
S
D
A
D1
TPS
LK2
47k
1nF
Q4
2N5485
1k
820Ω
1nF
Q3
2N5485
K
OUT–
IC1
MC1496
VOLUME
SPAN
VR4
10k
1
100k
100nF
+9V
A
2.2k
1k
IC2: TL072
K
VR1
1k
K
K
A
100nF
K
A
S1
D
2N5485
S
470nF
–
+
3
1
VP
100nF
GND
IN
8
+~~–
OUT
K
560Ω
LED2
λ
λ
K
560Ω
λ LED4
A K
λ LED3
A
1
2
3
GP2Y0A41SK0F
A K
A
10 µF
100nF
8Ω
LOUDSPEAKER
+9V
CON4
GND
OUT
GND
W04
IN
REG1 7809
–OUT
5
10 µF
CON3
LINE OUT
10 µF
LED1
150Ω
100k
+OUT
7809, 7805
6
PWR GND
100nF
10 µF
470 µF
25V
~
470nF
SIG G ND
POWER
G
7
IC3
TDA7052A
2 INPUT
~
4
+9V
4 DC VC
+11V
8
IC2b
100nF
6
5
BR1
W04
LEDS1–7
CON1
9VAC OR
12V DC
INPUT
D2
1N5819
(BODY)
VOLUME
VR3
5k
100k
MAX
VOLUME
SET
10k
100k
100nF
2.2k
22nF
22nF
D2, D3
A
LED5
λ
12
6
6.8k
8 CARRIER
IN+
GND BIAS
5
14
CARRIER
IN–
4 SIG
IN–
10
IC2a
100nF
3
2
82Ω
100nF
1k
1k
100nF
100nF
1k
1k
3
OUT+
680Ω
2
GAIN
1 SIG
IN+
+9V
Fig.3: the complete circuit diagram for the Opto-Theremin. JFET Q1 & transformer T1 form the pitch oscillator, while Q2 & T2 form the reference oscillator. Their
outputs are buffered by Q3 & Q4 and mixed in IC1. Pin 6 of IC1 then drives the line output socket via buffer stage IC2b, while IC2b drives audio amplifier stage
IC3. Sensor 1 is the optical distance sensor. Its output is buffered and inverted by IC2a which then drives the BIAS input of IC1 to control the volume.
SC
20 1 4
HAND
VOLUME
VOLUME
CONTROL
BOARD
100nF
Q2
2N5485
(BODY)
VR2 1k
Q1
2N5485
680Ω
ANTENNA
SHARP
LED6
A
Vcc
GND
A
Vo
LED7
470Ω
3
2
1
10 µF
REG2
7805
RANGE SENSOR
SENSOR1
D3 1N4004
C 2014
23108142
470Ω
Fig.4: install the parts on
the two PCBs as shown
in this parts layout
diagram, starting with
the main PCB assembly
as shown below. If you
are using SMD ICs for
any of IC1-IC3, then these
should be installed on the
back of the main PCB as
shown in Fig.5. Note that
equalising coil L1 must be
secured to the PCB using
an M4 x 25mm Nylon or
polycarbonate screw and
nut (do not use a metal
screw).
GP2Y0A41SK0F
1000µF 25V
CON5
24180132
Vo
GND V+
82Ω
~
–
BR1
+
~
100nF
TP GND
VR4 10k 100nF100nF
A
The main PCB has been designed to accept either
DIP or SOIC (surface-mount) ICs (IC1 & IC3 are
SOICs on this assembly, while IC2 is a DIP IC).
D1
4148
10 µF
+
1
(SMD under)
1
100k
THEREMIN
C 2014
TEST
23108141
A
LED1
LED3
A
A
A
LED4
tive divider consisting of two 100kΩ
resistors across the 9V supply biases
this input to 4.5V.
IC2b’s output appears at pin 7 and is
fed to the Line Out socket (CON3) via
PITCH ANTENNA
560Ω
LED2
100nF 1nF
2N5485 330pF
Q4
T2
REFERENCE
OSCILLATOR
68pF 2N5485
Q2
39Ω
TP1
1k
1k
100nF
100Ω
14180132
L1
1
(SMD under)
1
100nF
M4 x 25MM NYLON
OR POLYCARBONATE
SCREW
1k
820Ω
PITCH ADJ
VR2 1k LIN
100k
100k
Right: a 3-pin header is
soldered to the distance
sensor’s output terminals
before installing it on its
PCB – see Fig.6 for the
mounting details.
LK1
2.2k
Normal
680Ω
T1
2.2k
Q1
100k
1k
560Ω
68pF
22nF
22nF
100pF 1nF
100nF
VOICE
VC1
2-10pF
1k
330pF
2N5485
GND
PITCH OSCILLATOR
2N5485
Q3
100nF
100k
150Ω
CON3
(WIRE TO
VR2 BODY)
100k
IC1 MC1496
26 Silicon Chip
680Ω
100k
100k
6.8k
1.2k
220Ω
470nF
TPS
100nF
IC2
TL072
SPAN
100Ω
CON4
10 µF
SPEAKER
VR3 5k
RANGE
LINE OUT
LED5
100nF
1k
(SMD under)
5819
10k
100nF 1 1
D2
VR1 1k LIN
IC3
470nF
470 µF 25V
LK2
MAX.
Normal
10 µF
100nF
GND
SPKR VOL.
100k
47k
TDA7052
10 µF
CON2
POWER
S1
VOL.
REG1 7809
GND V+
CON1
Vo
Above: the completed volume
control PCB. Note how the two electrolytic
capacitors are bent over so that they later
clear the case lid.
a 10µF coupling capacitor (to remove
the 4.5V DC bias voltage) and a 150Ω
resistor. The 150Ω resistor isolates the
op amp from any capacitive loads,
preventing oscillation.
IC2b’s output also feeds power amplifier IC3, a 1W bridge-tied load (BTL)
amplifier. Its volume is controlled by
a DC voltage at pin 4, with a range of
about -70dB to +35dB for 0.4-1.2V.
siliconchip.com.au
Volume control pot VR1 is connected
in series with trimpot VR3 and a 10kΩ
resistor from the 9V supply, with VR1
being the volume control and VR3
being the maximum volume preset.
VR3 allows the top of VR1 to be
adjusted from 0.75-1.0V, giving a maximum gain between about -20dB and
+20dB. In practice, VR3 is set so that
the loudspeaker produces sufficient
volume without gross distortion.
The bottom end of VR1 connects to
ground via Schottky diode D2. This
provides a fixed bias of approximately
0.2V at the bottom of VR1 and is necessary to set the minimum volume level.
Optical volume control
The Sharp GP2Y0A41SK0F distance
sensor (SENSOR1) forms the heart of
the optical volume control circuit. Its
output at pin 1 varies from about 0.4V
when the hand is 300mm above the
sensor, to about 2.8V at 40mm. The
sensor’s output is non-linear and must
be inverted and level shifted using op
amp IC2a to derive the correct volume
control function to drive the bias
input (pin 5) of mixer stage IC1.
As shown on Fig.3, the sensor’s
siliconchip.com.au
output is fed to the inverting input of
IC2a via LK2. IC2a operates with a gain
of just over -2, as set by the ratio of the
100kΩ and 47kΩ feedback resistors.
IC2a’s non-inverting input (pin 3) is
biased to about 1.7V by trimpot VR4
and this offsets the output by 1.7V x
the non-inverting gain, ie 1.7V x (1+
100kΩ/47kΩ) = 5.3V. VR4 allows the
volume control range to be set to suit
the degree of hand movement.
IC2b is configured in a rather unusual way, with its output driving a red (or
green) LED (LED5) and a 1kΩ resistor
to ground. The arrangement ensures
that the output at LED5’s cathode can
swing all the way down to 0V. This is
necessary because IC2a’s output can
only go down to 1.8V (it’s a TL072)
and we need 0V to set the minimum
bias on pin 5 of IC1.
So why not use an op amp that
can swing down to 0V, such as an
LMC6482 or LM358? The answer is
that these aren’t tolerant of RF signals
and produced high-frequency noise in
this circuit, even with extra compensation and filtering. The TL072 doesn’t
have this problem. In addition, LED5
acts as a volume indicator, displaying
full brightness at maximum volume
and dimming down as the volume is
reduced.
The output from LED5 drives the
bias input of IC1 via a 6.8kΩ resistor.
With 0V output, the lack of bias completely shuts down any signal at IC1’s
output to provide full attenuation.
The maximum output from IC2a is
around 7V. So after taking the LED voltage drop into account, the maximum
voltage that can be applied to IC1’s
bias input is about 5.2V, sufficient to
give full volume.
Link LK2 is included so that the distance sensor can be bypassed. When
it’s moved to the MAX position, pin
2 of IC2b inverting amplifier is tied
to 0V via a 47kΩ input resistor. As a
result, IC2b’s output goes high and the
distance sensor no longer has any effect, making pitch adjustments easier.
Power supply
As stated, power for the circuit is
derived from a 9VAC plugpack or from
a 12V DC linear (non-switchmode)
supply. RF is filtered from the incoming AC (or DC) rails by 470nF capacitors, while BR1 full-wave rectifies the
AC supply. BR1 also makes the unit
insensitive to DC polarity. A 470µF
capacitor filters the resulting DC, while
regulator REG1 provides the 9V rail to
power most of the circuit.
A 5V supply rail for the distance
sensor is derived via diode D3 and
regulator REG2. D3 provides reverse
polarity protection, while the following 1000µF filter capacitor is necessary
to supply the peak current for the
pulsed infrared LED inside the sensor.
An 82Ω resistor in series with the 11V
supply input limits the peak charging
current into the 1000µF capacitor. This
prevents unwanted noise in the output
due to the pulsing of the IR LED in
the sensor.
LEDs 5 & 6 illuminate the area
adjacent to the volume sensor with
blue light when power is applied. A
470Ω resistor in series with each LED
provides current limiting.
Construction
Virtually all the parts for the OptoTheremin are mounted on the two
PCBs. The main PCB (code 23108141)
is double-sided and measures 147 x
85mm, while the volume control PCB
(code 23108142) is single-sided and
measures 61 x 47mm. Fig.4 shows the
parts layout for both boards.
Start by assembling the main PCB.
This board has been designed to accept
either DIP or SOIC (surface-mount)
packages for IC1-IC3. DIP package ICs
are installed on top of the PCB, while
SOIC package ICs go on the underside,
as shown on Fig.5.
DIP ICs are somewhat easier to install but many types are now difficult
to obtain in this package, especially
the MC1496 and TDA7052. An SOIC
package is still quite easy to solder
though, even though its pins are closer
together.
If using one or more SOIC packaged (SMD) ICs, then these should
be installed first (see Fig.5). Begin by
placing a tiny amount of solder on
one of the corner pads, then coat the
remaining pads with some no-clean
flux paste. That done, place the IC in
position (with the correct orientation)
and hold it in place using tweezers.
Now solder the relevant corner pin
to its pad, then check that the IC is
correctly positioned, with all pins
centrally located on their pads. If
the IC needs adjustment, reheat the
soldered pin and slide the IC to its
correct position.
Once it’s correct, solder the remaining pins but don’t worry about solder
bridges between pins during this proSeptember 2014 27
Parts List
Main Theremin Section
1 double-sided PCB with platedthrough holes, code 23108141,
147 x 85mm
1 UB1 plastic utility box, 158 x 95
x 53mm
1 front panel label, 149 x 87mm
1 9VAC 250mA plugpack
1 PCB-mount DC socket (inner
diameter to suit plugpack)
(CON1)
1 3-way PCB-mount screw
terminal block with 5.08mm pin
spacing (CON2)
1 PCB-mount 3.5mm stereo
switched socket (CON3)
1 2-way polarised header, 2.54mm
spacing (CON4)
1 SPDT miniature PCB-mount
toggle switch (S1) (eg. Altronics
S1498)
1 75mm 8Ω loudspeaker
2 1kΩ linear 16mm potentiometers
(VR1,VR2)
2 knobs to suit potentiometers
1 5kΩ horizontal trimpot (VR3)
1 10kΩ multi-turn top adjust
trimpot (VR4)
2 2nd IF coils (white) (T1,T2) (can
be bought in a set of IF coils
from Jaycar Cat LF-1050. Two
sets required)
1 potcore pair and bobbin (L1)
(Jaycar LF-1060 cores/LF-1062
bobbin, Altronics L 5300 cores/L
5305 bobbin)
2 M205 PCB-mount fuse-clips for
antenna connection
1 2-way polarised header plug,
2.54mm spacing, with crimp
pins
2 3-pin headers with 2.5mm
spacing (LK1,LK2)
2 jumper shunts (for LK1 & LK2)
1 M4 x 25mm Nylon or poly
carbonate screw (to secure L1)
1 M4 x 10mm Nylon or
polycarbonate screw (for top of
pitch antenna)
2 4mm ID Nylon or polycarbonate
washers (spacer for L1)
3 M4 Nylon or polycarbonate nuts
(to secure L1 and for top of
pitch antenna)
3 M3 x 6mm machine screws
2 M3 x 10mm machine screws
3 M3 nuts
2 M3 x 9mm tapped spacers
1 100mm length of medium duty
28 Silicon Chip
hookup wire (to earth VR2)
1 200mm length of medium-duty
hookup wire or 100mm of
light gauge figure-8 wire (for
speaker)
1 12m length 0.25mm enamelled
copper wire (L1)
1 400mm length of 0.7mmdiameter tinned copper wire
(LED lead extensions)
1 400mm length of 1mm-diameter
heatshrink tubing (LED1-LED4
leads)
1 10mm length of 20mm-diameter
heatshrink tubing (L1)
7 PC stakes (TP, 3 x GND, TP1,
TPS, 2 x L1)
Semiconductors
1 MC1496P (DIP) or MC1496D
(SOIC) balanced modulator
(lC1)
1 TL072CP (DIP) or TL072CD
(SOIC) dual op amp (IC2)
1 TDA7052A (DIP) or TDA7052AT
(SOIC) BTL amplifier (IC3)
1 7809 3-terminal regulator
(REG1)
4 2N5485 N-channel JFETs
(preferably from the same
manufacturer & batch) (Q1-Q4)
4 3mm blue LEDs (diffused lenses
preferable) (LED1-LED4)
1 3mm red or green LED (LED5)
1 W04 bridge rectifier (BR1)
1 1N4148 signal diode (D1)
1 1N5819 Schottky diode (D2)
Capacitors
1 470µF 25V PC electrolytic
4 10µF 16V PC electrolytic
2 470nF MKT
12 100nF MKT
2 22nF MKT
2 1nF MKT
2 330pF NP0 ceramic
1 100pF NP0 ceramic
2 68pF NP0 ceramic
1 2-10pF trimmer capacitor (VC1)
Resistors (0.25W, 1%)
9 100kΩ
2 680Ω
1 47kΩ
2 560Ω
1 10kΩ
1 220Ω
1 6.8kΩ
1 150Ω
2 2.2kΩ
2 100Ω
1 1.2kΩ
1 82Ω
6 1kΩ
1 39Ω
1 820Ω
Volume Control Board
1 single-sided PCB, code
23108142, 61 x 47mm
1 UB5 translucent blue plastic
utility box, 83 x 54 x 31mm
1 Sharp GP2Y0A41SK0F 40300mm distance measuring
sensor (SENSOR1) (RS
Components Cat 666-6568P,
Littlebird Electronics DF-SEN0143, Digi-Key 425-2819-ND)
1 3-way PCB-mount screw terminal
block, 5.08mm spacing (CON5)
1 3-pin header with 2.5mm spacing
(for Sharp sensor)
1 M3 x 6mm machine screw
2 M3 x 10mm machine screws
3 M3 nuts
4 3mm ID washers
1 50mm length of 1mm clear
heatshrink tubing (central wire
between CON2,CON5)
1 300mm length of 1mm straight
steel or aluminium wire
(between CON2 & CON5)
1 120mm length of 6mm diameter
heatshrink tubing (packing
inside aluminium tubing)
Semiconductors
1 7805 3-terminal regulator
(REG2)
1 1N4004 1A diode (D3)
2 3mm blue LEDs (diffused lenses
preferable) (LED6,LED7)
Capacitors
1 1000µF 25V PC electrolytic
1 10µF 16V PC electrolytic
Resistors
2 470Ω 0.25W 1%
Extra hardware
1 800mm length of 10mm-diameter
(OD) x 1mm-thick aluminium
tubing (cut for 450mm antenna,
volume control attachment and
tripod stand)
1 350mm length of M5 or 3/16-inch
zinc-plated threaded steel rod
(cut to 2 x 62mm and 3 x 75mm)
10 M5 or 3/16-inch nuts to suit
threaded rod (eg, Nylon lock
nuts in preference to half nuts)
1 151 x 90 x 19mm DAR pine
timber
1 29mm-OD frosted halfhemisphere hollow plastic ball
(cut from ball salvaged from rollon deodorant) (optional)
siliconchip.com.au
23108141
IC2 TL072
(SMD)
IC1 MC1495
(SMD)
1
1
Fig.5: here’s how
to mount the
alternative SMD
ICs on the back
of the PCB. Our
prototype used
SMDs for IC1 &
IC3, as shown in
the inset photos.
1
1
IC3 TDA7052
(SMD)
1
cedure. Once all the pins have been
soldered, you can remove any excess
solder using solder wick.
If you’re not using SOIC ICs, or once
you’ve finished fitting them, install
the resistors. Be sure to push them all
the way down so that they sit flush
against the PCB before soldering their
leads. Table 1 shows the resistor colour
codes but you should also check each
one using a DMM before soldering it
in position.
Next, fit any DIP ICs, either by
soldering them directly to the PCB
or using IC sockets. That done, fit PC
stakes to the three GND positions (ie,
TP GND and the GND pads adjacent
VR1 and T1), then TP1, TPS (adjacent
IC2) and for the two wiring points for
coil L1. The two 3-way pin headers for
LK1 and LK2 can then go in.
Diodes D1 and D2 are next on the
list, taking care to ensure that they are
correctly orientated. Bridge rectifier
BR1 can also be installed at this stage,
with its ‘+’ pin positioned as shown.
Follow with JFETs Q1-Q4 and trimpots VR3 and VR4. Note that VR4 is
orientated with its adjustment screw
adjacent to LED5. The capacitors can
then all go in but be sure to orientate
the electrolytic types correctly. Table
2 shows the codes used on the lowvalue capacitors.
LED3 is installed next and must be
pushed all the way down onto the PCB
before being soldered. Its anode (A)
lead is orientated as shown.
siliconchip.com.au
1
Once it’s in, the two adjacent
M205 fuse clips (used to connect the
antenna) can go in. These must have
their end-stop tabs broken off before
installation, by bending them back and
forth using small pliers.
These fuse clips are both mounted
slightly proud of the PCB and their
pins soldered on both sides of the
board, to make a secure mounting
receptacle for the antenna. Do not
push the fuse clips all the way down
onto the PCB as they could short to
LED3’s pads.
The two oscillator coils, T1 & T2,
can now be installed. These are both
white-cored IF transformers and only
go in one way, since they have three
pins on one side and two on the other.
Push them all the way down onto the
PCB before soldering their pins and
don’t forget to solder the mounting
pins on either side of the metal cans.
Once these parts are in, install
switch S1, power socket CON1, 3-way
screw terminal block CON2 and
3.5mm jack socket CON3. Note that
the wire entry side for CON2 must go
towards the adjacent edge of the PCB.
9V regulator
Regulator REG1 mounts horizontally, with its leads bent by 90° so that
they go through the PCB holes. Secure
its tab to the PCB using an M3 x 6mm
screw and M3 nut before soldering
the leads. Don’t solder the leads first;
if you do, the PCB tracks could crack
as the screw is tightened.
Next, cut the shafts of VR1 & VR2
to suit the knobs that will be used and
clean up the ends with a file. That
done, snap off the small lug next to
the threaded shaft bushing on each pot
and install the two pots on the PCB.
The metal body of each potentiometer must be earthed to the PCB via
a GND PC stake. For VR1, the GND
stake is immediately adjacent and
the pot’s metal body is connected to it
using a short length of tinned copper
wire. Note that it will be necessary to
scrape or file away a small section of
the passivation layer on the pot’s body
to allow the solder to adhere.
By contrast, VR2’s GND stake is
some distance away, to the left of
coil L1. It should be connected using
medium-duty hookup wire. This earth
position was necessary to remove
background hiss from the Opto-Theremin’s audio outputs.
Front-panel LEDs
The remaining LEDs (LED1, LED2,
LED4 & LED5) must all be mounted
on 35mm lead lengths, so that they
later protrude through the lid of the
box. This means that you will have to
extend their leads using short lengths
of tinned copper wire.
Keep the anode leads slightly longer
than the cathode leads, to make it easy
to check the polarity when the LEDs
are installed. It will be necessary to
sleeve at least one lead of each LED
September 2014 29
Table 1: Resistor Colour Codes
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
No.
9
1
1
1
2
1
6
1
2
2
1
1
2
1
1
M3 x 10mm
SCREW
2 x 3mm ID
WASHERS
PCB
Value
100kΩ
47kΩ
10kΩ
6.8kΩ
2.2kΩ
1.2kΩ
1kΩ
820Ω
680Ω
560Ω
220Ω
150Ω
100Ω
82Ω
39Ω
RANGE SENSOR
SHARP
GP2Y0A41SK0F
M3 NUTS
with heatshrink tubing after attaching
the wire extensions, to prevent them
from shorting.
Once the extensions are in place,
mount the LEDs on the PCB (red for
LED5, blue for the others), taking care
to ensure that they are orientated correctly. It’s a good idea to slide a 35mmwide strip of cardboard between the
leads of each LED when mounting
it in position. It’s then just a matter
of pushing it down onto this spacer
before soldering its leads.
Equalising coil
Equalising coil L1 consists of a bobbin and two ferrite core halves. The first
step is to jumble-wind (ie, randomly
wind) 260 turns of 0.25mm enamelled
copper wire onto the bobbin. When the
winding is complete, lightly twist the
two free ends together for about 2mm to
prevent the winding from unravelling,
then cut the leads to 20mm and scrape
away the insulation from each end.
Next, cover the winding with a
layer of insulation tape. Alternatively,
shrink some 20mm-diameter heatshrink tubing around the bobbin. The
coil can now be assembled onto the
PCB, as follows:
(1) Position one ferrite core section on
the PCB and fit the bobbin in place.
30 Silicon Chip
4-Band Code (1%)
brown black yellow brown
yellow violet orange brown
brown black orange brown
blue grey red brown
red red red brown
brown red red brown
brown black red brown
grey red brown brown
blue grey brown brown
green blue brown brown
red red brown brown
brown green brown brown
brown black brown brown
grey red black brown
orange white black brown
M3 x 10mm
SCREW
2 x 3mm ID
WASHERS
Fig.6: this diagram
shows the mounting
details for the Sharp
optical distance
sensor. Note the 3mm
stacked washers used
as spacers.
(2) Slide two 4mm-ID Nylon or polycarbonate washers inside the bobbin,
so that they rest on top of the inner part
of the bottom core (these are needed
to provide a 2.5mm spacing between
the two cores).
(3) Place the top core in position and
secure the entire assembly to the PCB
using an M4 x 25mm Nylon or polycarbonate screw and an M4 nut. Be sure
to orientate the coil as shown on the
parts layout diagram (Fig.4).
(4) Solder the coil wires to the adjacent
PC stakes.
Volume control PCB
That completes the main PCB assembly – now for the volume control
board. Start by installing the two 470Ω
resistors and diode D3, then fit regulator REG2. As before, be sure to secure
the regulator’s tab to the PCB using an
M3 x 6mm screw and M3 nut before
soldering the leads
Next, fit the 10µF and 1000µF electrolytic capacitors. As shown, the
latter must be installed with its body
lying horizontally and its leads bent
down through 90° to go through its
solder pads. The 10µF capacitor will
also need to be bent over slightly so
that it later clears the case lid.
The two blue LEDs can go in next.
5-Band Code (1%)
brown black black orange brown
yellow violet black red brown
brown black black red brown
blue grey black brown brown
red red black brown brown
brown red black brown brown
brown black black brown brown
grey red black black brown
blue grey black black brown
green blue black black brown
red red black black brown
brown green black black brown
brown black black black brown
grey red black gold brown
orange white black gold brown
Table 2: Capacitor Codes
Value
470nF
100nF
22nF
1nF
330pF
100pF
68pF
µF Value
0.47µF
0.1µF
0.022µF
0.001µF
NA
NA
NA
IEC Code
470n
100n
22n
1n
330p
100p
68p
EIA Code
474
104
223
102
331
101
68
These are mounted with their bodies
close to the PCB and are bent slightly
towards the 470Ω resistor, so they do
not later directly shine into the player’s
eyes. If you are not using a translucent
case, then the LEDs will need to be
mounted about 10mm proud of the
PCB, so they later protrude through
the case.
The distance sensor is installed by
first soldering a 3-way pin header to
the pins of the right-angle 3-way connector on the underside of its PCB.
This is clearly shown in one of the
accompanying photos. The sensor is
then mounted on the volume control
PCB and secured using M3 x 10mm
screws and nuts, with two stacked M3
washers serving as spacers on each
side – see Fig.6.
Tighten the screws down firmly
before soldering the 3-way pin header
to the PCB.
That’s all we have space for this
month. Next month, we’ll describe
how the two boards are assembled into
their boxes, give the final mechanical
assembly details and detail the simple
SC
test and adjustment procedure.
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New Bluetooth
Hearing Aid
Programmer
Blamey & Saunders’ latest
programmer for their
already amazing value
hearing aids makes
them even better!
by
ROSS TESTER
R
egular SILICON CHIP readers will recall two reviews of
new Hearing Aids from Australian company, Blamey &
Saunders. We originally purchased some hearing aids
back in 2011 and couldn’t quite believe the difference they made
to a severe case of industrial deafness which occurred some
30+ years earlier (‘Australia Hears – and So Do I!’ – July 2011).
Later, we had the opportunity to trial some of their new digital
hearing aids and found they were even better, even if more
expensive. (SILICON CHIP, March 2013).
While a little outside the normal ‘fare’ you might expect to see
in an electronics magazine, feedback from readers has been
most enthusiastic and quite a few have told us that as a result
of those articles, their new Blamey and Saunders hearing aids
have “cured” hearing problems they have had for years.
There were two major points of difference between the B&S
hearing aids and others we had considered in the past:
(1) They were significantly cheaper than the vast majority of “fair
dinkum” hearing aids on the market. (There are some el-cheapo
units available on the internet – and they are very cheap – but that
old adage really does apply here: you gets what you pays for!)
However, despite the B&S hearing aids being around half the
price of most quality hearing aids on the market, in this case half
price does not equate to half quality. We reckon they’re better!
(2) You can program these hearing aids to suit your requirements – so you don’t need to spend money to visit an audiologist to have hearing aids programmed – or “tailored” to suit your
particular loss. No two cases are the same; in fact it’s highly likely
that one of your ears has different characteristics to the other, so
the ability of being able to individually program your B&S hearing
aids yourself is a real boon.
Of course, if you have visited an audiologist and have a copy
of your audiogram (ask for it!) then B&S will supply your hearing
aids programmed with that data. Incidentally, there are quite a
few websites which will also provide you with something of an
audiogram – perhaps not up to “professional” audiologist standards, but a good starting point nevertheless.
NEW SCREEN GRAB
TO COME
Assuming you’ve managed to make the Bluetooth connection
(!) programming the hearing aids is so simple, even an
octogenarian could do it! Choose the hearing aid type . . .
32 Silicon Chip
. . . then it’s simply a matter of adjusting the slider bars to
suit your particular requirements and save the profile. You
can play around without the risk of damaging anything.
siliconchip.com.au
But using the hearing aid programmer from Blamey and
Saunders, you can build several individual programs within your
hearing aids to suit various situations without any professional
intervention at all.
New Programmer
Recently, Blamey & Saunders introduced a new, improved
programmer. The Incus programmer, in conjunction with their
‘IHearYou” software, is both similar and quite different to the old
(AHPro3) model – it’s similar in the way it works but it is even easier
to use. The biggest difference is that it operates via a Bluetooth
connection, so it doesn’t even need to be wired to the computer.
I’ll be honest, at first I had no joy whatsoever in connecting it.
After a judicious amount of weeping and wailing etc, this turned
out to be a faulty Bluetooth dongle – as soon as I swapped to a
laptop with inbuilt Bluetooth and downloaded the new programming software, it connected and worked exactly as it should.
Later, I went back to the original notebook PC with a different
Bluetooth dongle attached and presto! away it went.
The software is particularly intuitive – you don’t really need
to have any computer knowledge to run both the software and
programmer.
Connecting to the hearing aids themselves for the first time
is a little problematic – there is a “shiny” and a “dull” side on the
connector which is a little difficult to pick unless you’re in pretty
bright light. But once connected, it’s all child’s play (or in my case,
senior’s play!).You simply work your way through the menu items,
adjusting levels to suit your hearing level.
Following my ‘road test’ of the programmer, I was talking to
Blamey & Saunders about my Bluetooth problems and then the
success I had.
I mentioned that the one bugbear I had with my new program
was the traffic indicators on my new car were so damned loud
– really annoyingly so. Their response: “Why don’t you create a
new program for the hearing aids – call it ‘car’ – and reduce the
levels at those frequencies?” Well, durrr – why is the answer so
blindingly obvious you can’t see it?
So I did. And the solution was perfect – when I get into the car,
I switch over to program 2 (a push-button on these aids) and the
problem ceases to exist.
If you have more than one problem (eg, the TV sound must be
up too high or you can’t understand people in a crowd) you can
create separate hearing aid programs to suit those situations.
There’s not much more I can say about the new programmer,
except that it works! The kidney-shaped device is about 75 x
50 x 20mm so it’s smaller than the old one and operates from a
single AAA cell. Battery life is about three hours. (That’s where
I thought the problem was initially – but no, it was the Bluetooth
link). Typical of Bluetooth, it will operate up to 10m from your
computer and a (new, improved!) Bluetooth dongle is included
with the Incus programmer.
On the top side are three LEDs – red and blue show you when
the right and left (respectively) hearing aids are connected, while
on the right side is a green LED which is inside the (fiendishly
cleverly disguised!) power button.
This Incus/IHearYou package normally sells for $295 but
is included with new hearing aid purchases from Blamey and
Saunders. The software includes lifetime updates and support.
Blamey & Saunders Hearing is based in Melbourne (364 Albert St, East Melbourne, Vic 3002) but operates Australia (and
world) wide via the ’net. For more information and a free on-line
hearing test, visit www.blameysaunders.com.au or call them
on (03) 9008 6371.
SC
siliconchip.com.au
September 2014 33
SERVICEMAN'S LOG
Cameras can be tricky to repair
Many people think that there isn’t a lot inside a
camera. However, there’s a surprising amount
of electronic jiggery-pokery lurking inside even
the most basic unit. And as with other electronic
devices, things can and often do go wrong but
fixing them requires the skill of a brain surgeon.
Cameras can be awkward devices
for a serviceman to repair, mainly
because there are so many different
types. There are also lots of different
systems used and this makes them
particularly challenging, especially for
a novice. Just pulling them to bits can
be a lesson in frustration and a test of
dexterity and skill.
For starters, cameras contain electromechanical systems to control or adjust
(among other things) focal length, shutter speed, exposure, white balance,
zoom and flash intensity. Some even
include circuitry to make fake shutter
sounds. But it doesn’t stop there; just
about every function on a modern
camera is electronically controlled or
guided using a complex arrangement
of electric motors, sensors, switches,
displays and other components.
In my opinion, some modern cameras, especially state-of-the-art, topof-the-range models, are more sophisticated than just about any other
consumer electronic device. And they
not only boast all this wizardry but it’s
also packed into the tiniest of spaces.
I clearly recall the first camera I
opened up many years ago. It was a
Yashica FX-D SLR camera (purchased
from my brother) and I couldn’t believe
the places they’d managed to cram
circuit boards bristling with transistors
and ICs. And that was long before the
advent of microscopic, surface-mount
components. That old Yashica was my
introduction to camera repairs and
though I’ve not seen many others of this
type since then, the lessons I learned
were well worthwhile.
The first thing I learned was that it
is imperative to have the right tools for
the job. A set of Fathers’ Day screwdrivers, a hammer and a set square are not
going to help you disassemble a camera
body. Many cameras are held together
with a weird and wonderful assortment
of clips, safety screws and other fasteners, and some of them require specific
driver bits to undo.
In short, the old trick of using a
small, flat-bladed jewellers’ screwdriver to see if you can fluke undoing a ‘weird-headed’ screw usually
doesn’t work. Instead, you’ll likely
end up wrecking both the screw and
the screwdriver blade and trying to
drill out damaged screws from a $1000
camera body is not something I want
to experience.
Another essential item is one of
those fabric aprons watchmakers
and jewellers use to tuck into the
workbench when seated. These catch
anything you drop and my trick is to
use a makeshift apron fashioned from
an old sheet. It may look a bit naff but
Servicing Stories Wanted
Do you have any good servicing stories that you would like to share in The Serviceman column? If so, why not send those stories in to us?
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.
34 Silicon Chip
Dave Thompson*
Items Covered This Month
•
•
•
Cameras can be tricky to repair
The snake in the air-conditioner
Beyonwiz PVR repairs
*Dave Thompson runs PC Anytime
in Christchurch, NZ.
Website: www.pcanytime.co.nz
Email: dave<at>pcanytime.co.nz
believe me, grubbing around the floor
looking for a screw the size of a pinhead
looks a lot less dignified. And if your
workshop floor is anything like mine,
chances are you’ll never find what you
are looking for anyway.
An apron like this can also save the
day if you drop something breakable
– the falling item simply lands in the
apron like a trapeze artist falling into
a safety net. Again, this is preferable
to it hitting the floor; lenses and filters
especially don’t like the sudden stop
at the bottom.
So the right tools are essential. But
that will get only you half-way to completing the job; technical ability, skill
and luck are necessary to complete the
other half.
Even so, unless one is used to repairing cameras, they can be intimidating
devices. Part of the problem is that if
a circuit board is dead, then unless
you have a circuit diagram and you’re
good at working with surface-mount
components on tiny PCBs, the repair
involves replacing the entire module.
Getting replacement parts for many
cameras can be difficult however,
especially older models. What isn’t
available new may have to be scavenged from salvaged units at a repair
shop but either way, they’ll probably
be quite expensive.
In short, whatever it is that’s killing
your camera, you’d better hope that it’s
something that doesn’t involve swapping out major parts.
As mentioned, my first camera
repair job involved my Yashica FXsiliconchip.com.au
D, a highly-regarded unit in its day.
Unfortunately, I’d managed to drop it
while taking photos of anything and
everything, as you do when you first
get a new camera. That was in the
days when photos were on film and
you typically had 12 or 24 shots before
having to change the roll. Not only that,
once you’d taken the photos, you then
had to take the roll to an agency to have
it developed and the photos printed.
All this cost about the same as a small
house, so you very quickly learned to
ask yourself “do I really need to take
this photo?”
The accident itself was simply due
to carelessness on my part. I’d put the
camera up on a shelf about 2m high for
safe keeping and turned to walk away.
Unfortunately, as I did so, the padded
shoulder strap I’d added that very day
caught my wrist and the following few
seconds played out in slow-motion.
I’d swear I had time to stroll back
and catch the camera but in reality, I
stood transfixed and could only watch
helplessly as it fell all the way to the
carpeted floor.
I couldn’t believe it; I’d owned this
expensive camera barely 72 hours
and it was probably already ruined. I
gingerly picked it up and turned it on
and was relieved to hear the camera
come to life. A quick look through the
viewfinder revealed no broken lenses,
mirrors or other optics, so I took a
quick test photo and all seemed OK
except for one problem – a small spot
had appeared in the field of view. It
wasn’t on the lens or on the outside of
siliconchip.com.au
the viewfinder, so it had to be inside
somewhere.
Now being an 18-year-old, secondyear avionics apprentice flush with
newly-acquired technical skills, I
thought that I was able to repair anything. As a result, I quickly developed
a burning need to pull the camera apart
to see what that the spot was and to
determine if it was an indicator that
something had broken. And so my first
foray into camera repair was to check
out and hopefully remove the only
visible consequence of that fall, the
spot that appeared in the viewfinder.
I’d already determined that whatever was causing the spot wasn’t on
the outside of the optics. The lens
was connected to the camera with a
bayonet-style fitting and a quick twist
soon had it off the body. I immediately
took a good look through it but that
didn’t reveal anything either.
Just to be sure, I gave everything a
quick going over with a lens-cleaning
wipe but the spot remained. So whatever the foreign object was, it was definitely somewhere inside the camera
body and that meant taking it apart.
At that stage of my engineering career,
I would happily (and yes, recklessly)
open up anything without fear of not
being able to put it back together again.
What’s more, I had by then acquired an
awesome set of very high-quality tools,
including some pretty cool instrument
repair hardware (most of which I still
have). I also had access to some of the
most advanced workshop equipment
available anywhere at the time (and
some serious engineering talent to go
with it should I come unglued), so I
was confident that fixing my camera
wouldn’t be a problem.
At the time, it was quite acceptable at
the airline’s workshops to work on ‘foreign orders’ in our spare time. These
were mainly jobs that we brought in
from home and so, one lunchtime, I set
about disassembling the camera with
the intention of locating and (hopefully) resolving the problem.
The first thing I noticed was just how
small and fine everything was, so I had
to utilise a desktop magnifier almost
from the beginning. Fortunately, the
workshop I was seconded to as part of
my apprenticeship had high-quality,
back-lit magnifiers fitted to most of
the workbenches so I was in business.
Well, almost – there was no YouTube, Google or even a publicly-access
ible Internet in those days, so searching
for a ‘walkthrough’ on disassembling
and repairing a Yashica FX-D wasn’t
even a distant dream back then. With
no information to hand, I was going
to have to wing it and rely on the experience of those around me if things
turned sour.
This camera was very well-engineer
ed and there are similarities with the
way Apple products are now put
together. Where a sturdy plastic clip
would suffice to hold something inplace, one or more tiny screws are used
instead. But while these products are
undoubtedly well-made, they can also
sometimes be over-engineered. It can
be a servicing nightmare when it comes
to remembering where each screw goes
and while some manufacturers use the
same-size tiny screws throughout their
devices, many do not. As a result, the
average serviceman ends up with a
parts bin full of many different types
of screws and has the enviable task of
remembering where each one goes in
a particular job.
The last thing we want to do as
repairers is install a long screw where
a short one should go. During the last
few years, I’ve seen many laptops come
into my workshop where an amateur
repairer has put a ‘too-long’ screw in
to hold the case together, only to see it
go right through to the keyboard side.
Punching holes in a laptop chassis
is bad enough but screwing the wrong
fastener through someone’s LCD panel
is even worse! And since this is something I really want to avoid when concontinued on page 37
September 2014 35
Serviceman’s Log – continued
The snake in the air-conditioner
The dead snake after it had
been removed from the
compressor unit. No wonder
it didn’t move when prodded
with a broom handle!
Servicemen frequently encounter
dead rodents, cockroaches and other
nasties inside electrical equipment.
A. F. of Kingscliff, NSW recently
encountered a large snake and it was
really on the nose. Here’s his story . . .
Did the snake eat the rat before
the snake died or did the snake die
by electrocution on an empty stomach? That was the thought running
through my mind as I recently surveyed the damaged wiring inside a
faulty air-conditioner.
This little saga had started four
days earlier, when a neighbour complained to me of a foul smell in her
garden. I took a quick sniff and the
smell was certainly unpleasant but I
fobbed her off by saying that another
neighbour had probably spread some
organic fertiliser around. And besides, it was too hot to do anything!
Unfortunately, by the fourth day,
the smell had become unbearable
and in spite of the heat, it was time
for a search to track down the source
of the problem. The smell seemed
to be coming from the side of her
house but it was difficult to tell as
the wind kept gusting. There was
nothing along the side of the house
except a strip of grass and the outside
compressor unit of a split-system
air-conditioner.
This was the area where the smell
was strongest but there was only the
compressor box that could hide anything. I then spotted two large black
horse flies sitting on the top of the
compressor unit. Was that a clue as
to the origin of the smell?
There was only one way to find
out. The compressor unit had a small
cover on one end, which allowed
the electrical cables to enter the
casing. I thought that removing this
might give me some quick insight as
to what the problem was, as it was
easier to remove this than the eight
self-tapping screws which held the
top down. As a result, I removed
the cover, took a peek inside and
quickly stepped back when I saw a
snake’s skin.
Now when I left school, I was
conscripted straight into the army.
We were young and green and were
not smart enough to question any
authority. Of course, there was lots
of training and one of the basic questions which you had to get right was
“what steps would you take, if you
saw the tail fins of a mortar bomb
sticking out the ground?”
The correct answer was “large
ones sir and to the rear”. I was
glad that I’d remembered my basic
training when I saw that snake; my
memory must still be OK!
Keeping my distance, I waited
for the snake to slither out of the
compressor unit but it stayed there.
After waiting some time, I cautiously
advanced and rapped on the top of
the box but still the snake did not
appear. I then gave the box a mighty
thump to dislodge any living thing
that might be inside but still there
was no movement
Eventually, I plucked up my courage, removed the screws from the
lid and gently lifted it free, holding
it in front of me as a shield. A large
carpet python (which later measured
1.65 metres long) was lying across
a circuit board near the top of the
compressor and its extremities disappeared down into the lower parts
of the unit. And it wasn’t moving.
I took a long-handled broom and
poked the snake but still it did not
move. It certainly appeared to be
dead but were there others lurking
inside? I cautiously examined every
nook and cranny that I could see but
nothing seemed to be alive in there.
I now had the unpleasant task
of removing this creature from the
compressor unit while hoping that
it didn’t return to life. Fortunately,
there wasn’t much chance of the
latter occurring – after four days in
the summer heat, the snake was well
and truly maggot-ridden and it was
stinking to high heaven.
Extracting this 1.65-metre snake
The carpet python measured 1.65 metres (5-feet 5-inches)
long and really wasn’t in the best condition! Was that bulge
in its body, near its tail, the remains of a rat?
36 Silicon Chip
siliconchip.com.au
This view inside the compressor unit shows the wiring and
control PCB section where the snake was found.
The damage caused by the rat chewing through the wiring
insulation can be seen here. It set a deadly trap for the snake.
from the intricacies of the compressor unit was an extremely unpleasant task but eventually the job was
done and the carcass disposed of.
The smell inside the compressor
unit then quickly lessened and I was
able to closely inspect it for damage.
It was just as well I did because
next to the circuit board that the
snake had been draped across was
a large rat’s nest. And the rat had
shown a fondness for the plastic insulation around the electrical cables
and spade connectors. It had chewed
away quite a lot of the insulation,
leaving lots of exposed copper wires.
What’s more, as the rat had chewed
at the insulation, it had pulled
strands of the copper wire out from
the insulating sheaths, creating a
nest-like web. It was a real mess.
Closer examination revealed that
the rat had chewed the leads that led
to the fan motor, which I assumed
must have been powered down when
ever it did this (probably at night).
Unfortunately for the snake though,
the fan motor relay must have energised while it was crawling through
bared copper wires to get at the rat
and so the snake was electrocuted!
What amazing timing!
Well, that was my first impression
when I started the repair. But was it
“amazing timing”? Several weeks
later, when I was at home at my desk,
I looked at the damage to one of the
cables using a magnifying glass. And
I spotted the telltale signs of three
blackened copper strands with balls
of melted copper at the ends.
That threw a different angle on the
grisly scene. I now believe that the rat
chewed through the insulation of the
Neutral wire without being shocked.
However as the strands of copper
broke with the chewing, eventually
there were only three strands left and
these subsequently melted with the
inevitable current overload.
When these strands melted, the
strands of copper on the fan motor
side suddenly jumped from Neutral
potential to Active potential, ie,
230VAC. Some time later, the python slithered past and was electrocuted when it brushed against these
230VAC strands on the fan motor
side – an electrocution aided by the
fact that other parts of the snake’s
body would have been touching the
sheet metal housing which was at
ground potential.
What irony! The snake was hunt-
ing the rat but the rat had unwittingly
set up a fatal ambush.
The repair involved much more
work than just replacing the chewed
cables and the damaged connectors. I
also had to remove most of the unit’s
side panels, to get at the numerous
rats’ nests that had been built around
the compressor motor and piping. It
was necessary to remove these, otherwise they would be a fire hazard.
The circuit boards were cleaned
by pouring hot water over them
and lightly scrubbing them with a
brush. They were then thoroughly
dried before being refitted. The airconditioner was then tested and it
worked perfectly.
I’m still wondering whether the
rat was eaten by the snake before the
latter was electrocuted or whether
the rat got away, to wreak havoc on
another piece of electrical gear.
fronted with lots of different screws, I
always draw out a plan of the board
or chassis and make decent notes as
to what goes where.
The Yashica camera was the first repair job that I made such notes on and
I’ve done it as a matter of course ever
since. It also pays to make very clear
and understandable notes; it could be
weeks before you put a device back together and there is nothing worse than
SC
thinking you’ve got it covered with
siliconchip.com.au
September 2014 37
Serviceman’s Log – continued
Beyonwiz PVR repairs
Goods damaged in transit are one
of the risks when buying online.
Fortunately, regular contributor B.
P. of Dundathu, Qld was able to
straighten out a dented PVR (personal video recorder) he bought
recently via eBay. Here’s his story . . .
PVRs have now replaced VCRs
for recording TV programs for later
viewing. This change came about
because PVRs are easier to use and
was also prompted by the introduction of digital television. Analog
TV transmissions have now been
switched off in most areas, making
VCRs much less useful than before
as they cannot receive digital TV.
Recently, I decided to update our
SD PVRs to HD PVRs. My daughter
already had a Beyonwiz FV-L1 HD
PVR and liked it, as it’s capable of
recording two channels at the same
time. As a result, I thought I would
try eBay to see what was available
in this brand. There were several
brand new units listed, along with
a few used models. After some
thought, I decided to bid on some of
the used models, as this would save
a substantial cash outlay. I initially
obtained an older “DP-S1” model
with an in-built DVD player, which
arrived safely and worked well. I
then purchased a “DP-Lite i” which
again worked well.
Some time later, I found a “DP-P2”
model being advertised and I was
again successful with my bidding.
It duly arrived but you can imagine
my dismay when I opened the box
and found that the bottom of the unit
had been stoved in.
The seller had done what I would
call an adequate job of packing the
unit, so what had gone wrong? It
appeared that a very heavy weight
had been placed on top of the box,
resulting in damage to the bottom of
the unit. Fortunately, that the seller
had packed the unit upside-down,
otherwise the top of the unit would
have been damaged instead.
I pondered what to do. I didn’t
want to power up the unit at this
stage because if the bottom of the case
was contacting the PCB, doing so
could result in irreparable damage.
I thought of contacting the seller but
in the end decided to see if I could
repair the unit. I was almost certain
that the internals were undamaged
and I decided to take a chance that
this was indeed the case.
The first step was to break the
warranty seal. I then removed the
lid by removing the four screws from
the back and the single screw from
each side.
Once inside the unit, it was apparent that I would need to remove the
HDD (hard disk drive) before I could
remove the PCBs. After unplugging
all the cables, I removed the four
screws securing the HDD, extracted
diagrams and hand-written records
only to find that the notes you made
are inadequate.
It’s also a good idea to take lots of
digital photos, especially with complex repair jobs or those held together
with dozens of different screws.
As mentioned, my Yashica was extremely well made. I suppose all goodquality cameras are made that way
but this was my first experience with
cameras and I was impressed. I ended
up using a few specialised tools to get
into the thing but it all went smoothly.
First, I removed the front housing of
the camera, exposing all the internal
workings. Then, after removing every
visible screw, I removed the plastic
framework, along with the mirror and
shutter assembly which came out in
one piece. That was about as far as I was
comfortable taking things, though. Any
further and I seriously doubted that I’d
be able to reassemble it, despite my
youthful naivety and bravado.
When I inspected the mirror and
the now-exposed lenses, prism and
viewfinder assemblies it didn’t take
long to spot the spot. It was very small
and appeared to be a piece of rubber
or something of a similar texture. The
fragment was stuck to the face of the
prism inside the top of the body and
it took a bit of picking at it to dislodge
it from the glass.
Under the magnifier, it had a defi-
38 Silicon Chip
it from the case and put it aside. I
then removed the power supply and
logic boards, after which I removed
the rear panel.
It was then just a matter of straightening the bottom panel. This was
done by hand since the metal was
fairly thin and easily bent back to
into position. Once it was all done,
I reassembled the unit, connected it
to a TV set, plugged it in and turned
it on. Fortunately, it was still in good
working order and none-the-worse
for its ordeal.
Non-working unit
When I purchased that last unit on
eBay, I also noticed a Beyonwiz “DPLite i” that was listed as “not working
or for parts”. The seller described it
as having a hard drive issue and had
initially thought that the hard drive
could not be formatted.
Suspecting that the original HDD
was faulty, he had replaced it with
a brand new HDD only to find that
the fault persisted. He’d then researched various internet forums
and the popular opinion was that it
was a power supply problem, so he
had decided to sell the unit as “not
working or for parts”.
This unit had been listed on two
previous occasions and I had already made an offer which had been
rejected. Offers from several other
bidders had been rejected as well.
This was getting the better of me,
as I wanted to see if the unit could
be repaired. Even if it wasn’t repairable, I would still end up with a spare
500GB hard drive and a spare remote
nite edge to it on one side and looked
like it could have been part of a seal,
washer or mounting bush that had
come adrift on impact. However, even
after a very close inspection, I couldn’t
see anywhere obvious where it could
have come from.
Next, I gave the interior a good
blow-out with dried, low-pressure
compressed air. During this procedure,
I gently tapped and shook the body just
in case there were any other fragments
floating about inside but nothing else
fell out. All that was left to do was
reassemble the parts in reverse order
but first I gave the interior optics a good
going over with a lens-cleaning cloth.
It was a pleasure to have a spot-free
siliconchip.com.au
control, which would be worth having as this model’s remote operates
all the different Beyonwiz models
except for the DP-P2.
I decided to re-submit my previous
offer and this time, it was accepted.
The unit arrived a few days later and I
immediately hooked it up and turned
it on. When I did this, it displayed a
message stating that the hard drive
would be initialised.
I cancelled this operation, turned
the machine off and unplugged it. I
then removed the lid, expecting to
see several electrolytic capacitors in
the power supply with bulging tops.
However, at first glance, all looked
good. I then thought that I would
remove the power supply board and
test the capacitors. However, before
going to all that bother, I decided that
I would first try replacing the SATA
cable to the HDD.
I dug out an old PC SATA cable,
swapped it over and again powered
up the unit. This time, I opted to initialise the hard drive and the process
completed successfully. I then tuned
in the channels and all appeared to
be working correctly.
But was it going to be as easy as
that? I had an uneasy feeling that it
had all been too straightforward, so
I decided to reinstall the original
SATA cable to confirm that it was
indeed faulty but again, all was well.
And that meant that the fault lay
elsewhere.
Next, I removed the logic board
and inspected the SATA socket
carefully with a magnifying glass.
I wasn’t entirely happy with the
soldering on the socket’s pins, so I resoldered them and refitted the board.
I then decided to check the ESR
of the electrolytic capacitors on the
power supply board, as I suspected
that this was where the problem
really lay. As a result, I removed this
board and it was then that I noticed
an almost imperceptible bulge at the
top of C30, a 470µF 16V electrolytic.
When I tested its ESR, it was very
high at 1.6Ω, so it was obviously
faulty. I then checked the remaining
electrolytic capacitors on the power
supply board. All were OK except
for C38 (470µF 25V) which had an
ESR of 0.32Ω. While this wasn’t exceptionally high, it was high enough
to cause concern.
I replaced both faulty capacitors,
then reassembled the unit, set it up to
record several programs and left it to
do its thing for a few weeks. During
that time, I used it to periodically
watch live TV (ie, via its tuner) and
to view recorded programs and it
functioned flawlessly.
This was a ‘win-win’ situation.
The seller got a fair price for his
‘dead’ PVR and I paid less than I
would have had it been in good
working order. I was then able to
repair it for little more than the cost
of my time.
Once again, my trusty ESR meter
saved the day and a faulty piece of
electronic equipment was successfully repaired. I built my ESR meter
from a Jaycar kit many years ago and
it has proved invaluable over the
years for finding capacitor faults in
all sorts of equipment.
viewfinder again and thankfully, that
was the only time I ever had to pull
the camera apart. That camera subsequently took thousands of photographs
before being retired once digital cameras superseded it.
However, not long ago, it developed a
problem with the fold-out side screen,
the image on which recently began
slowly scrolling like Dad’s old black
and white TV used to do.
In Dad’s case, he’d just mutter
something unprintable and tweak the
knobs around the back of the set to stabilise the image. When it comes to the
Handycam though, there are no knobs
to twiddle. However, I did discover
that applying some gentle pressure
to the screen’s hinge area slowed the
scrolling down.
With that discovery, my serviceman’s nose began to twitch and I went
looking for a suitable screwdriver so
that I could start stripping the screen
Sony Handycam
Another camera that’s done the
hard yards with us is our trusty Sony
Handycam. Its not only travelled with
us but has also taken a few tumbles
in the quakes, with one long, deep
scratch in the housing evidence of
where something fell onto it after it
had fallen to the floor.
Despite these battle-scars, it still
takes excellent video and still shots.
siliconchip.com.au
MISS THIS ONE?
Published in Dec 2012
2.5GHz 12-digit
Frequency Counter
with add-on GPS accuracy
Wow! 10Hz - >2.5GHz in two ranges;
1us - 999,999s with a 12-digit LED display.
It’s a world beater and it’s the perfect
addition to any serious hobbyist’s bench –
or the professional engineer, technician,
in fact anyone who is into electronics!
You’ll find it one of the handiest pieces of
test gear you could ever own and you can
build it yourself.
All the hard-to-get bits (PCBs, micros,
LEDs, panels, etc) are available from
the SILICON CHIP PartShop.
You’ll find the construction details at
http://siliconchip.com.au/project/2.5ghz
PCBs, micro etc available from PartShop
down. A single screw and several plastic clips hold it all together so it wasn’t
rocket science to expose the screen and
associated internal connections.
Like Yashica, Sony has made an art
out of squeezing incredible amounts
of electronics into tiny spaces – and
space really is at a premium inside the
screen bezel. Several strips of Mylar (or
similar material) with embedded tracks
run from the camera’s logic boards
to the screen and my guess was that
one of them wasn’t seated properly. I
was praying it hadn’t split or cracked
because that would be a real can of
worms I didn’t want opened.
There were seven connections altogether where the straps terminated into
PCB-style ZIF (Zero Insertion Force)
connectors. I re-terminated each one
by flipping up the plastic tensioner bar
to release the strap, cleaning the strap’s
gold connections with isopropyl al
cohol, and then sliding it back into the
socket and clicking home the tensioner
bar to lock it in place.
Fortunately, my efforts paid off
because this completely resolved the
screen scrolling issue. I’m not sure
what I’d have done if it hadn’t! Tricky
SC
things, cameras.
September 2014 39
WIDEBAND,
ACTIVE DIFFER
OSCILLOSCOPE
Using your oscilloscope to examine and measure high speed and high
frequency circuits can be tricky if you use only the usual passive test
probes supplied. Here’s a design for a high performance, active differential
probe which costs much less than commercially available active probes. It
has very little circuit loading and usable bandwidth of more 80MHz.
The differential probe can be powered by any convenient USB – in this case,
the Agilent ’scope has a USB input which is more than capable of supplying
the <40mA required. If your ’scope doesn’t have a USB socket, you could
use a computer, laptop or even a USB plugpack. The trace shown on the
oscilloscope is actually the output of transformer T1 on the SiDRADIO PCB
(SILICON CHIP, October 2013), as measured by the differential probe (not the
point shown in the photo).
40 Silicon Chip
siliconchip.com.au
By JIM ROWE
RENTIAL
PROBE
D
o you know what is inside the ‘passive’ test probes
supplied with most oscilloscopes, and how to use
them to make reasonably accurate measurements
at high frequencies?
If not, have look at the excellent article on this topic by
Doug Ford in the October 2009 issue of SILICON CHIP. Doug
explains how complex these probes can be and how many
factors can result in their performance falling away, espe-
cially at high frequencies. In addition they tend to disturb
operation in the circuit being tested, making it difficult to
make proper measurements.
It’s because of the shortcomings of passive probes that
some of the big manufacturers produce ‘active’ probes to
provide a much higher input resistance together with a
much lower input capacitance.
Originally, active probes used valves (vacuum tubes) at
their input but then when semiconductor technology came
along, JFETs and MOSFETs made it possible to make active
probes that were much smaller and easier to use.
It also became feasible to make ‘differential’ active probes,
which overcame some of the remaining drawbacks with
conventional ‘single ended’ active probes. (More about
these shortly.)
The big problem with commercial active probes is their
price tags. Even the single-ended type can set you back well
over $700, while the differential type can cost over $2000
apiece – more than most of us paid for our digital scopes!
In short, the only way that most of our readers are likely
to be able to use an active probe with their scope is to
build one. Yet the last DIY active probe to be described
in Australia was way back in the September 1989 issue of
ELECTRONICS Australia – 25 years ago. That design is now
very dated.
This new active, differential scope probe design takes
advantage of modern surface-mount components to deliver
a high level of performance and it fits inside a compact case.
Best of all, it can be built for much less than the cost of any
currently available commercial active probes.
We estimate that you should be able to buy all of the
components and build it for about a quarter of what you’ll
pay for the cheapest commercial active probe presently
available.
Why differential?
Before we start describing the new probe and how it
works, perhaps we should look at why a differential active
probe tends to be better than a single-ended one.
A single-ended active probe is certainly a big improvement over most passive probes, offering high input resistance combined with very low input capacitance.
It tends to cause lower disturbance to the circuit under
test, particularly at high frequencies – where the higher
input capacitance of a passive probe causes increased
circuit loading.
The high frequency and transient response of the
probe-plus-scope combination also tends to be better and
smoother, due to better compensation and fewer reflections
in the cable between the probe output and the scope input.
But there can still be problems when you’re making HF
measurements with a single-ended active probe. These
problems are mainly associated with the ‘ground clip lead’,
which is used to make the connection between the probe’s
input and the earthy or ‘cold’ side of the circuit under test.
As you can see from Fig.1A, even when the ground clip
lead is quite short, it can introduce enough inductance
(Lg) to reduce the effective signal voltage appearing at the
actual input of the probe at high frequencies.
So the frequency response of the probe tends to droop
at high frequencies, reducing the measurement reliability.
As well, the ground lead inductance can interact with
the probe’s input capacitance (Cin), resulting in resonances
siliconchip.com.au
September 2014 41
R
FFE
BU P
AM
TO SCOPE
INPUT
+Vsig/2
Rin
TIP
Cin
L
TIA
EN )
FER =1
DIF MP (A
A
GROUND
LEAD (MAY
BE OPTIONAL)
Lg
POSITIVE
TIP
Cin
Rin
Rin
Vcom
Cin
Lg
Vsig
GROUND
LEAD
R
FFE
BU P
AM
2)
TO SCOPE
INPUT
50
+
(A=
–
+Vsig – (–Vsig)
= 2Vsig
(50 TERM.
AT SCOPE
END)
R
FFE
BU P
AM (A=2)
–Vsig/2
NEGATIVE
TIP
A SINGLE-ENDED PROBE
B
DIFFERENTIAL PROBE
Fig.1: Comparing a ‘single ended’ active probe (A) with a differential active probe (B). With a single ended probe the ground
lead inductance Lg can cause problems at high frequencies, but a differential probe solves these problems.
at specific high frequencies.
This can not only result in the probe
producing unwanted loading on the
circuit being measured but can also
produce spurious ‘peaks and dips’ in
the measurements.
It is possible to minimise these problems by replacing the ground lead with
a very short ‘ground blade’, providing
a somewhat lower inductance than
the usual 100mm-or-so long ground
lead and clip.
Many of the commercial singleended active probes come with this
type of ground blade as an accessory.
But a better solution is to change over
to a differential probe, as shown in
simplified form in Fig.1B.
As shown, the differential probe has
two tips and is designed to measure
the signal difference between the two
– rather than the signal between either
probe tip and ground.
In fact the ground lead (or blade)
is really only used to tie the circuit
under test’s ground to that of the probe
and scope, to keep the voltages being
measured within the probe’s common
mode input range.
This means that if there is no sig-
nificant voltage difference between the
two grounds, the ground lead or blade
may be regarded as optional.
Inside the differential probe there
are two virtually identical input buffer
amplifiers (one from each tip), each
of which feeds one input of a third
amplifier, the differential amplifier.
This is where one of the two signals
is subtracted from the other to send
only the ‘difference’ signal out to the
scope input.
This subtraction cancels out any
‘common mode’ signal present at both
probe tips, leaving only the ‘difference
Specifications
An active differential probe for oscilloscopes, housed in a compact handheld case and operating from +5V DC, derived from
any convenient source such as a USB port on a PC or digital oscilloscope. It provides tip area illumination via a white LED
and a choice of two switched gain settings: 1:1 or 10:1.
Input coupling:
AC
Input resistance, each probe tip:
1MΩ nominal on the 1:1 range (1.0023MΩ);
10MΩ nominal on the 10:1 range
Input capacitance, each probe input socket to ground:
3.15pF approximately
(So capacitance tip-to-tip is approximately 1.6pF)
Maximum DC voltage at probe tips:
±45V, both ranges
Maximum AC voltage input before overload, both probe tips: 2.0V peak-to-peak (700mV RMS) on the 1:1 range,
20.0V peak-to-peak (7.0V RMS) on the 10:1 range
Output impedance:
50Ω (Needs an output cable of 50Ω characteristic impedance,
terminated in 50Ω at the scope end)
Bandwidth (probe + output cable and termination): 25Hz - 80MHz +0.2dB/-3dB, both ranges
60Hz - 50MHz +0.2dB/-0.5dB, both ranges
150Hz - 40MHz +0.2dB/-0.3dB, both ranges
Overall transmission gain/loss:
On 1:1 range, 0.0dB ±0.6dB
On 10:1 range, -20dB ±1.0dB
Current drain from 5V DC supply:
Less than 40mA
42 Silicon Chip
siliconchip.com.au
This photo, close to life size, shows the
Active Differential Probe in its handheld
instrument case. It’s a comfortable fit in
the hand while applying the probe to the
circuit under test.
MEASURED RESPONSE (1:1 RANGE)
signal’ – the signal between the positive and negative probe tips, which
is what we are trying to look at and
measure.
As the common mode signal is essentially equal to the voltage VCOM
at the probe’s ground terminal, this
explains why any voltage difference
developed across the ground lead or
blade inductance LG is no longer a
problem. It’s simply cancelled out.
Before we leave Fig.1, you may
be wondering why we’ve shown the
output of the differential probe as having an amplitude of 2Vsig. Won’t this
cause a calibration problem, by giving
the probe a gain of 2?
Not really, because as shown in
Fig.1B, there’s a ‘source termination
resistor’ of 50Ω fitted in series with
the probe output. This is to match
the characteristic impedance of the
probe’s output cable (normally 50Ω).
Then at the scope end of the same
cable, another 50Ω shunt resistor
is used to ensure that the cable is
terminated correctly at that end too,
to avoid reflections and consequent
complications (like peaks and dips).
And the combined effect of the two
termination resistors is to introduce an
attenuation factor of 2:1 – bringing the
overall signal gain of the probe and
cable back to unity.
1F capacitor in parallel with a 10nF
capacitor.
This combination has been chosen
to give a lower input corner frequency
of less than 30Hz, together with the
smoothest possible upper frequency
response.
Following the DC blocking capacitors the signals each pass through 27Ω
overload protection resistors, before
reaching the gates of input buffer
transistors Q1 and Q2.
These are BSS83 N-channel MOSFETs designed especially for operating
from a 5V supply voltage. We’re using
them as near-unity gain wideband
source followers, to give high input
impedance combined with the lowest
possible input capacitance.
The gates of both Q1 and Q2 are
biased to +4.3V via the 1MΩ resistors.
This bias level is chosen to provide a
‘half supply voltage’ (+2.5V) level at
the sources, which are direct coupled
to the following ICs. The bias voltage is
The probe’s circuit
Now refer to Fig.3, which shows the
complete schematic of our new probe.
The two probe input tips plug into
CON1 and CON2 at left, from where
they each pass to the end contacts of
S1a and S1b – the two sections of range
switch S1.
Depending on the setting of S1, they
each pass into the two input buffer amplifiers directly or via a series 9.0MΩ
input divider resistor comprising three
3.0MΩ 1% resistors in series.
Then each signal passes through a
DC blocking capacitance comprising a
+1.5
+1.0
+0.5
0dB
–0.5
–1.0
–1.5
–2.0
–2.5
–3.0
10k
15
20
30
40 50
70
100k
150 200
300
500
700
1M
1.5
2
3
4
5
7
10M
15
20
30
40 50
70 100M
INPUT FREQUENCY (kHz/MHz)
Fig.2: The upper frequency response of the differential probe, as measured on the 1:1 range. At the LF end it rolls off quite
smoothly below 150Hz, with the -3dB point at around 25Hz.
siliconchip.com.au
September 2014 43
330
A
TIP
ILLUM
+5V
K
LED1
10F
(WHITE)
K
+ TIP
3.0M
3.0M
MMC
2.7k
1F
3.0M
27
OPTIONAL
GROUND
LEAD & CLIP
10:1
MMC
+4.3V
RANGE
SWITCH
K
8
D
G
A
Q2
BSS83
100nF
AD8038ARZ
BSS83
S
*B
6
47F
10nF
MMC
MMC
1.0k
1.30k
1.0k
3
2
IC1– IC3: AD8038ARZ +5V
7
IC3
4
10nF
+2.5V
D
MMC
SM5819A,
SS16
A
MMC
S*
G
10nF
3.0M
SM5819A
OR SS16
7
IC1
470
27
3.0M
+5V
47F
MMC
1.0M
1F
MMC
3.0M
1.0k
15k
S1b
MMC
4
MMC
3
2
7
IC2
6
1.0k
1.0k
4
1.0k
47F
1.30k
MMC
4
1
(SUBSTRATE)
ACTIVE DIFFERENTIAL RF SCOPE PROBE
derived via the 2.7kΩ + 15kΩ voltage
divider, with a 10F bypass capacitor
to provide filtering.
and Q2 – while also providing the
current drive capability to feed the
inputs of difference amplifier IC3.
The two 47F capacitors connecting
the 1.0kΩ ‘lower feedback’ resistors
to probe earth are to maintain the LF
response.
IC3 is also an AD8038ARZ device,
configured so that the positive-tip input signal is fed to its positive input
(pin 3) while the negative-tip signal is
fed to the negative input (pin 2).
The four 1kΩ resistors and 47F +
10nF bypass capacitors ensure that IC3
does perform the desired subtraction
10:1 attenuator
44 Silicon Chip
POSITIVE TIP
OUTPUT CABLE
TO INPUT OF
SCOPE/DSO
UT E
TP OP
OU SC )
TO (50
on
c
p
hi
.c
om
.a
u
DC R
5V WE
PO
N w.silic E
CO ww AL PROB
I
L
TI
SIHIPIFFERSECNOPES
C TIVE DSCILLO
O
0
AC R
FO
–
IN
PU
x1
The 1MΩ gate biasing resistors also
provide the main component of input
resistance for both input channels,
when switch S1 is in the ‘1:1’ position.
Then when S1 is moved to the ‘10:1’
position, they form the lower elements
in the 10:1 input dividers (in conjunction with the 9.0MΩ series resistors).
After passing through input buffer
transistors Q1 and Q2, the two input
signals pass through amplifiers IC1
and IC2.
These are AD8038ARZ wideband
amplifiers, specified for operation
from a single 5V supply and with a
bandwidth of better than 150MHz (for
a gain of 2.0).
Incidentally, we also looked at
several other devices, including the
AD818, MAX4414ESA and OPA356
but none performed as well as the
AD8038ARZ. So the 8038 it is!
We are using them
here as buffer amplifiers with a gain of 2.3, NEGATIVE TIP
to compensate for the
small loss in the input
source followers Q1
T
x1
SC
2014
470
10F
– TIP
K
A
3
2
S1a
SMA SKT
(STRAIGHT,
END ON)
LED1
+2.5V
S
1.0M
1:1
CON2
MMC
MMC
SMA SKT
(STRAIGHT,
END ON)
D1
10nF
D
*
G
10nF
10F
MMC
Q1
BSS83
MMC
CON1
100nF
+
IN
PU
T
OPTIONAL GROUND
CLIP LEAD (CLAMPED
TO THE FERRULE OF
EITHER TIP PLUG)
of the two signals, so a ‘2Vsig’ difference signal appears at its output
(pin 6).
The two paralleled 100Ω resistors
at the output of IC3 provide the 50Ω
‘source termination’ for the cable connecting the probe’s output at CON3
to the scope input and the paralleled
100F and 100nF capacitors provide
DC blocking.
LED tip illumination
Finally, LED1, located at upper left
is included to illuminate the area right
in front of the probe’s tips, to make
connections easier.
Many of the up-market commercial active
probes also provide this
‘tip illumination’, be5V POWER CABLE
cause when you are
(FROM USB SKT
making measurements in
ON DSO, PC OR
high frequency circuits
PLUG PACK)
you’ll almost certainly
be using very short tips on the probe
itself. This means that the probe body
will not only shield the immediate area
of the circuit being tested from a light
source, but will also tend to block your
view as well.
In other words, it’s a very worthwhile feature and one which was
easily provided at low cost.
siliconchip.com.au
6
F1 1A
L1 100H
Parts List –
Active Differential Oscilloscope Probe
POWER
VBUS
(FAST BLOW)
GND
1
2
3
4
5
1 ABS instrument case, 114 x 36 x 24mm
CON4
USB MICRO
TYPE B SOCKET
10nF
MMC
10F
MMC
100nF
MMC
CON3
100
100
100F
MMC
OUTPUT
TO SCOPE
INPUT
SMA SKT
(STRAIGHT,
END ON)
TERMINATE OUTPUT
CABLE IN 50
AT SCOPE END
Fig.3: The probe’s full
circuit schematic. All
components except range
switch S1 and LED1 are
SMD devices.
The whole probe runs from a +5V
DC supply which means that it can
be powered via virtually any standard USB port, such as the one on the
front of many recent-model digital
scopes, a USB port on your PC – or if
neither of these are available, one of
those low-cost ‘USB charger/power
pack’ devices you can pick up for less
than $15 (preferably not a dodgy “el
cheapo” from China!).
Since the total drain of the probe is
less than 40mA, this should be well
within the capability of most USB
ports on DSOs and PCs.
CON4 is used to bring the +5V DC
power into the probe. This is a USB
micro type-B socket, which allows you
to use a standard ‘USB type A-plug
to USB micro type-B plug’ cable (as
used to hook up tablet PCs and mobile
phones to a PC or charger) to provide
the probe with power.
100H inductor L1 is used to filter
the +5V input and remove any noise
from the USB port or charger, while
fuse F1 and diode D1 are used to protect against reversed-polarity damage.
These components do nothing if the
5V supply is connected with the correct polarity but if the polarity should
be reversed for any reason, D1 will
immediately conduct and cause F1
siliconchip.com.au
2
1
1
1
3
PCBs, 103 x 26mm, code 04107141 & 04107142
100H SMD inductor, 1.6A rating (L1)
1A SMD fuse, 0603 fast acting (F1)
DPDT/DIL slide switch, raised actuator (S1)
SMA socket, end launch, PCB edge mtg (CON1,2,3)
1 Micro USB type B socket, SMD (CON4)
8 Self-tapping screws, 6G x 5mm long
Semiconductors
3 AD8038ARZ SOIC8 video amplifier (IC1,2,3)
2 BSS83 MOSFETs, SOT-143 SMD pkg (Q1,2)
1 3mm white waterclear LED (LED1)
1 60V 1A Schottky diode, DO214AC SMD pkg (D1)
(Hammond 1593DTBU element14 code 187-7372)
(Murata 48101SC)
(Cooper Bussman 0603FA1-R)
(TE Connectivity ASE 2204)
(Emerson Connectivity
142-0701-806 or
Multicomp 19-70-4-TGG)
(FCI 10103594-0001LF or
Molex 105017-0001)
(RS Components order code
523-6872)
(element14 order code
108-1312)
(SS16 or SM5819A)
Capacitors
1 100F MLCC, SMD 1210, X5R dielectric 6.3V rating
3 47F MLCC, SMD 1210, X5R dielectric 6.3V rating
4 10F MLCC, SMD 1210, X7R dielectric 16V rating
2 1F MLCC, SMD 1206, X7R dielectric, 50V rating
3 100nF MLCC, SMD 1206, X7R dielectric 50V rating
6 10nF MLCC, SMD 1206, X7R dielectric 50V rating
(Code 107)
(Code 476)
(Code 106)
(Code 105)
(Code 104)
(Code 103)
Resistors (all 0.125W 1%, SMD 1206)
6 3.0MΩ
2 1.0MΩ
1 15kΩ
The codes shown here
1 2.7kΩ
are the two most common
2 1.30kΩ
but there are others! If in
6 1.0kΩ
doubt, check all SMD
2 470Ω
resistors with your
1 330Ω
multimeter as you would
2 100Ω
any doubtful resistor.
2 27Ω
(Code 3M0 or 3004)
(Code 1M0 or 1004)
(Code 15K or 1502)
(Code 2K7 or 2701)
(Code 1K3 or 1301)
(Code 1K0 or 1001)
(Code 471 or 470R)
(Code 331 or 330R)
(Code 101 or 100R)
(Code 270 or 27R)
to ‘blow’ – protecting both the probe
circuitry and the 5V source from significant damage.
Construction
All of the probe circuitry and components are fitted onto a PCB measuring 103 x 26mm (code 04107141).
This is designed to fit inside one half
of a small handheld ABS plastic case,
with a screening PCB of the same size
(code 04107142) fitted into the other
half of the case.
The case itself measures only
114mm long, 36mm wide and 24mm
high, so it can be held in your hand
very comfortably. In fact, the case has
been designed to house hand-held
equipment such as this. It comes from
NB: not
all SMD
capacitors
are marked.
If in doubt,
measure!
Hammond Manufacturing.
The small SMA sockets (CON1 and
CON2) used for connection of the
probe’s input tips are mounted at one
end of the case, along with the white
LED1, which illuminates the tip. Two
sockets are mounted at the other end,
SMA output socket (CON3) along with
CON4, the USB micro B socket for the
probe’s 5V DC power.
All of the components used in the
probe are mounted directly on the
main PCB and all but two of the components are SMDs (surface-mountdevices).
The two through-hole exceptions
are slide switch S1 and LED1. Switch
S1 is mounted under the PCB and
LED1 is mounted above it with its
September 2014 45
ACTIVE DIFFERENTL
SCOPE PROBE
UPPER SHIELD PLATE
4
330
Q2
2
1
27 BSS83
100nF
1.0k
47F
top of the board.
Your PCB assembly should now be
complete, with all that remains being
to connect the shield PCB copper to
the ground copper on the main PCB.
This can be done using a short
length of light hookup wire – baring
a few millimetres at each end so that
the ends can be soldered into the ‘via’
holes at the rear of each PCB, as shown
in Fig.4.
Preparing the case
Now prepare the case. This involves
drilling three 7mm holes in the removable ‘front’ end panel (for CON1, CON2
and LED1), together with another
round hole in the ‘rear’ end panel for
CON3.
Then there’s an 8 x 3mm rectangular
hole to be cut in the rear end panel as
well (for access to CON4), and finally a
10 x 7.5mm rectangular hole cut in the
bottom half of the case (which becomes
the top) for clearance around S1 and
access to its actuator.
The location and size of all of these
holes is shown in Fig.5. You might also
want to make a ‘dress’ front panel, to
give your probe a professional look and
TOP
L
1
2.7k
10nF
K
F1
SS16 1A
10nF
1.0k
10nF
100
C
2014
410
2 HC
1
5
1
100 100nF
1.0k
1.0k
100
1.30k
100F
help in using it. Artwork for a dress
front panel is also shown in Fig.7.
You can make a photocopy of
this, (or you can download it from
siliconchip.com.au and print it),
hot laminate it (or use self-adhesive
book cover film) for protection and
then attach it to the front panel using
double-sided adhesive tape – after cutting it to size and also cutting out the
clearance holes for the case assembly
screws and S1.
Assembly
Now slip the front end panel of the
case over CON1, CON2 and LED1 at
the ‘front’ end of the main PCB, and
the rear end panel over CON3 at the
rear end of the PCB.
Then lower the complete main PCBplus-end-panels assembly down into
the bottom half of the case (which
becomes the top), with the two end
panels passing into the moulded
slots and S1 passing down through its
matching slot.
Once this main board assembly is
down as far as it will go, you can secure
it firmly in position using four 5mm
long 6G self-tapping screws – mating
(NOTE: BECOMES TOP OF PROBE)
TOP
(REAR END
PANEL)
6
A
7.75
PWR IN
104107141
41L1
70140
8038A
IC3
10F
100H CON4
4800S
10F
L1
A
MURATA
10nF
D1
A
D
B
7.75
A
6.5
L
L
C
7.5
8
1.75
3
6
L
OUT
3
1.0k
10F 15k 10F
47F
1.0k
1206
1206
10nF
1
WIRE CONNECTING
SHIELD PCB WITH
GROUND
C ON
2014
MAIN
PCB
04107141b
CON3
1F
3.0M
1
Q1
1.30k
IC1
8038A
4
1F
47F
IC2
8038A
S1
3.0M
(BOTTOM HALF OF CASE – TOP VIEW)
(FRONT END
PANEL)
1206
1206
IN–
3.0M
10:1
(UNDER)
A
100nF
470
1:1
LED1
ACTIVE DIFFL
SCOPE PROBE
3.0M 10nF 27 BSS83
2
3
1.0M 1.0M
K
TIP
1206
1206
IN+
CON1
3.0M
3.0M
470
(SHIELD BOARD – FITS INSIDE UPPER HALF OF CASE)
CON2
leads bent forward by 90° so the LED’s
body can protrude through the ‘front
end’ of the case between the two input
sockets.
The component overlay diagram of
Fig.4 shows the location of all components, together with their orientation.
When assembling the PCB, use a finetipped soldering iron – preferably one
with temperature control.
We suggest fitting the components to
the PCB as follows: first fit USB micro
socket CON4, taking great care when
soldering its five very small contacts
at the rear. Then mount the resistors
and capacitors, followed by fuse F1
(which is very tiny). Then fit diode
D1, Mosfets Q1 & Q2 and the three ICs.
Next, fit the three SMA sockets
(CON1, CON2 and CON3), which
slide onto the front and rear edges of
the PCB, with their centre pin resting
on (and soldered to) the centre pad at
the top of the PCB.
Their ‘side prongs’ solder to the
matching pads on each side, on the
top and bottom of the PCB.
Inductor L1 comes next, followed
by LED1 on the top of the PCB and
switch S1 underneath it in the position shown.
When you are fitting LED1 make
sure you mount it vertically with the
underside of its body about 13mm
above the top of the PCB. After the
leads are soldered they can both be
bent forward (left) by 90°, so the LED
can protrude from the centre hole in
the case front end panel.
Finally fit slider switch S1. This is
in a 6-pin DIL package, which mounts
under the PCB with its pins coming
up through the matching holes. Make
sure you push the switch body firmly
against the underside of the PCB before
you solder its pins to the pads on the
10.0
31.5
HOLES A: 7.0mm DIAM. HOLE B: 3.5mm DIAM. HOLE C: 3.0 x 8.0mm HOLE D: 7.5 x 10.0mm
5.25
(ALL DIMENSIONS IN MILLIMETRES)
Fig,5: drilling and cutout details of the Hammond Manufacturing “Hand Held Instrument Case”, shown 1:1. The only
slightly difficult holes are the cutouts for the USB socket on the rear end panel and the switch on the lower half of the case.
46 Silicon Chip
siliconchip.com.au
Fig.4 (left): the component overlay for the main PCB with the shield
board (which contains no components) above. It is connected to the
main board by the short link as shown. The main board fastens to the
bottom of the case, which becomes the top, while the shield is secured to
the top of the case, which becomes the bottom!
Below is a same-size photo of an early prototype main PCB, actually
mounted in the case. Take no notice of the “AD818” labelling – we
actually used AD8038s as shown on the PCB overlay.
with the holes in the moulded standoffs underneath.
Then the shield PCB can be fixed
into the other half of the case, using
another four of the same screws.
The final assembly step is to invert
the case half with the shield PCB and
lower it down over the half with the
main PCB, so that each end panel slips
into the moulded slots as before.
Then you can upend it and fasten it
all together using the two countersinkhead self tappers supplied and your
active differential probe should be
complete.
Making the probe tips
The simplest way to make ‘basic’
probe tips for the project is probably to
base them on an SMA male connector,
as shown in Fig.6.
This is the way I made the probe
tips you can see in the photos, basing
them on an Amphenol Connex type
132113 SMA plug; only the plug body
and the centre contact are used – the
crimping sleeve and PTFE spacer are
not needed.
The steps in making the tips are
shown overleaf. The actual tips are
20mm lengths of 1mm diameter nickel
plated steel wire, cut from a large
paper clip.
You might like to make a second pair
of tips, fashioned in the same way but
with longer lengths of wire – say 30mm
The two ends of the case, with their
drilling/cutouts to suit the three SMA
sockets, USB socket and white LED.
long – with a ‘crank’ in the centre to
allow their tip spacing to be adjustable. This would be done simply by
loosening their plug bodies and then
rotating the tips as needed to set the tip
spacing before tightening them again.
Ground clip lead
As mentioned earlier, a ground clip
Here’s how it all goes together – the main PCB and the
shield PCB screwed into their respective case halves. The
SMA connectors and USB socket poke through the case ends.
siliconchip.com.au
September 2014 47
Fig.6:
MAKING
A BASIC
PROBE
USINGAN
ANSMA
SMA PLUG
MAKING
A BASIC
PROBE
TIPTIP
USING
(SCALE: 2x ACTUAL SIZE)
BODY OF SMA PLUG
CENTRE
CONTACT
20mm LENGTH OF 1mm DIAM.
NICKEL PLATED STEEL WIRE
(CUT FROM A LARGE PAPER CLIP)
GROUND TO A POINT AT FAR END
1 THE FOUR COMPONENTS YOU’LL NEED
(SMA PLUG’S CRIMPING SLEEVE & PTFE SPACER
ARE NOT NEEDED)
9.0mm LONG SECTION OF 3.0mm OD,
1.0mm ID PTFE DIELECTRIC FROM A
LENGTH OF COAXIAL CABLE
Close-up of ground clip construction.
2 APPLY FLUX TO THE BLANK END OF THE WIRE, PUSH IT INTO THE REAR OF THE
SMA PLUG’S CENTRE CONTACT AND SOLDER.
The close-up photograph above
shows the idea. By the way you don’t
have to make the ground clip lead particularly short, because its inductance
is not critical when you are using a
differential probe. So feel free to make
it any convenient length.
Other Uses
3 WHEN IT HAS COOLED, PUSH THE CENTRE CONTACT AND WIRE INTO THE
REAR OF THE SMA PLUG’S BODY UNTIL THE 0.8mm DIAMETER CENTRE PIN
EMERGES FROM THE FRONT CENTRE OF THE INSULATING PLUG BY
2.0mm AND ITS WIDENING SHANK JUST BECOMES VISIBLE
4 FINALLY, PUSH THE LENGTH OF DIELECTRIC DOWN THE WIRE AND INTO
THE REAR OF THE SMA PLUG’S BODY AS FAR AS IT WILL GO.
YOUR PROBE TIP WILL NOW BE COMPLETE.
48 Silicon Chip
matter which one).
Then a 3mm hole is drilled in the
centre of the flat sections of the clamp,
so a 6mm long M3 screw and nut can
be used to attach the solder lug of the
ground lead, while at the same time
fastening the clamp to the plug ferrule.
+ INPUT
x10
– INPUT
x1
lead is often not necessary when you
are using a differential probe of this
kind. However, you might like to make
one up, so it will be available in situations where you may need it – or at
least to see if it has any effect.
An easy way to make a suitable clip
lead is to connect a suitable clip to one
end of a length of flexible insulated
hookup wire and then fit a small solder
lug to the other end.
The solder lug can then be attached
securely to a small clamp made of thin
brass sheet and bent into a ‘P’ shape
with an inner loop diameter of 4.5mm,
so it will slip over the ‘crimp ferrule’ of
one of your probe tip plugs (it doesn’t
A differential probe can also be
handy for measuring signals which
are relative to other voltages in a
circuit. Both signals must be within the probe’s common mode input
range and given that the probe is
AC-coupled, you will only get the
AC component of that signal.
For example, if you have a circuit with a signal that’s relative to
a ‘half supply’ rail, there may be
ripple or signal injected into this
rail. So using the differential probe
would allow you to see the signal
with this unwanted component
removed.
Many scopes can perform this
function using ‘math’ mode but
that requires the use of two of your
precious scope inputs and the result is generally a lot better when
the subtraction is performed in the
analog domain.
With this method, the circuit
ground can remain earthed, allowing easy simultaneous measurement of the signal.
ACTIVE
DIFFERENTIAL PROBE
FOR OSCILLOSCOPES
SILICON
CHIP www.siliconchip.com.au
SC
OUTPUT
TO SCOPE
(50 )
5V DC
POWER
Fig.7: same-size front panel(FRONT
artwork
to photocopy and glue to the
PANEL ARTWORK)
hand-held instrument case for a professional finish.
siliconchip.com.au
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16 Smithfield Rd
Smithfield
NSW 2164
Compact size, high current, with variable output and fan cooling.
Thermal overload and short circuit protected. Individual current and
voltage backlit displays with LED fault indicator light.
• Analogue meter
• Size: 148(W) x 162(D) x 62(H)mm
http://bit.ly/TL-4020
IP67 True RMS DMM with
Smartphone App
View live measurements, trend graphs,
data log, and email your results or
upload them to the Cloud - all from your
Smartphone!
siliconchip.com.au
Filament
not included
FROM
149
$
PH: 02 9604 7411
Rolling Floor Base for
Magnifying Lamps
Mount a magnifying lamp to this base
and you can roll it around the floor
providing even greater flexibility in your
work. Heavy base so it doesn't easily
topple over.
• Suits QM-3548
• Size: 700(H) x 385(Dia)mm
QM-3549
89
$
19" Rack Mount Enclosures
Ideal for studios, PA, sound
reinforcement, IT, or phone
system installations.
Features 1.8mm solid steel
powder coated cabinets
with clear tempered glass
doors.
• 6U
• Key lockable
• Size: 530(W) x 360(H) x 450(D)mm
FROM
129
$
Flat Packed HB-5170 WAS $159 NOW $129 SAVE $30
Assembled HB-5171 WAS $189 NOW $149 SAVE $40
September 2014 49
www.jaycar.com.au
DAD’S CAR
12VDC Marine Grade Power Sockets
Marine grade cigarette power sockets rated up to
10A. Supplied with brackets for flush and
surface mounting.
NEW!
$
FROM
1495
Universal GPS Charger
with Dual USB
• Supplied with panel mount,
under dash bracket, and a
surface mount "hood"
• Connects via 6.3mm spade
terminals
• Size: 36(Dia.) x 50(D)mm
MP-3616
• 5-30VDC
• Connects via 6.3mm spade
terminals
• Size: 36(Dia.) x 26(D)mm
QP-5582
NEW!
2495
$
Simply connect the transmitter to your iPhone®, iPod® or
iPad®, select a frequency from 88.1 to 107.9MHz then
tune in using your FM car radio. It has a built-in mic for
hands-free communication and a USB port built into the
cigarette lighter plug for charging other popular electronic
devices.
• Working voltage: 5VDC
• Backlit LCD display
• Size: 100(L) x 30(W) x
12(D)mm
$
95
AR-3124
2995
$
29
• Streams music
via the car radio
• Size: 110(H) x
65.5(W) x 40(D)mm
AR-3125
iPhone® not included. Not
compatible with iPhone® 5S
• CREE® XLamp CXA1512 LED
• Ballast size:65(L) x 50(W) x 16(H)mm
• 12V 6000K
• 300% more light than halogen
H4 (High / Low Beam) Cree® Module
• 1600/1800 Lumens per LED bulb
SL-3498 WAS $169.00 NOW $149 SAVE $20
H1 Slim Ballast HID Kit
H3 Slim Ballast HID Kit
H4 Slim Ballast HID Kit
H4 Slim Ballast HID High + Low Kit
H7 Slim Ballast HID Kit
149
$
Warning: State road and traffic authorities do not allow retrofitting of these products to cars
with ordinary headlights - even if it’s really simple to do so.
Pen Light with COB LED
Nifty LED pen light with
magnetic pocket clip for handsfree operation. Very bright 90
Lumen COB (chip-on-board)
LED runs up to 20 hours.
NEW!
1295
$
4995
$
HID provides far greater light output than standard
automotive lights. This series of kits all feature a slim
ballast design for ease of installation
FROM
in engine bays and tight spaces.
$
4995
SL-3490
SL-3492
SL-3494
SL-3495
SL-3496
$49.95
$49.95
$49.95
$79.95
$49.95
Note: Please ensure your lights are angled correctly.
These lights are not ADR approved.
LIMITED STOCK
500 Lumen 10W LED Worklight
500 Lumen Mini LED Vehicle Lights
• High brightness,
long life LED
• IP65 rated
• Rechargeable
SL-2809
• Spot or flood beam patterns available
• Stainless steel mounting hardware
• Compact size 70(H) x 40(W) x 55(D)mm
• Sold individually
Suitable for illuminating a
warehouse, automotive
workshops etc.
• Requires 3 x AAA batteries
• Size: 165(L) x 30(D) x 16(W)mm
ST-3466
$
8A Heavy Duty Battery Charger
Suitable for both 6 and 12 volt car,
boat, motorcycle and lawnmower
batteries up to 6 amps. Switched
between trickle
or heavy duty
$
95
charge rates.
59
• 4-stage LED
charge indicators
• Overload and reverse polarity
protection
• Complies with Australian
Electrical Safety Regulations
MB-3522
50 Silicon Chip
2295
$
The rigid bracket holds your
iPhone 5® or iPod touch 5® and
charges the device through the
lightning connector for
handsfree functionality.
Slim Ballast HID Light Kits
H7 Cree® Module
• 1800 Lumens per LED bulb
SL-3499 WAS $169.00 NOW $149 SAVE $20
NEW!
12/24VDC FM
Transmitter/Charger
12VDC Mounting LED Headlamp Modules
Extremely bright drop-in replacement LED headlights for your car. Each kit
contains 2 x 25W per LED bulbs, 2 x controller assemblies, and all the wiring
is pre-terminated to appropriate connectors
to make installation as quick and easy as possible.
2
Easily monitor your battery
voltage, or the voltage in
any DC powered system.
Supplied with a panel
mount and a surface
mount "hood".
In-Car FM Transmitter
with Charger
Replacement for an original GPS charger, but
with 2 x 2.1A high power USB outputs, for
charging both a GPS and a Smartphone
or other USB gadgets at
the same time. Includes
1.2m USB cable with 6
replaceable connectors
to suit most GPS models.
• Input: 12-24VDC
• Output: 5VDC, 4.2A max total
• Size: 100(L) x 42(W) x 25(H)mm
MP-3676
Self Powered LED Voltmeter
High quality USB charger with
1.0A and 2.1A ports.
Compatible with 12V and 24V
battery systems and can be
mounted in various options.
• Connects via 6.3mm spade terminals
• Includes under dash bracket
(PS-2020 only)
Single (shown) PS-2020 $14.95
Dual
PS-2022 $19.95
Single with LED
Voltmeter
PS-2024 $27.95
Single with 2 x USB Ports
(1A + 2.1A)
PS-2026 $29.95
2 Port USB Charger
To order call 1800 022 888
74
95
Amazingly bright. Shock and waterproof alloy housing.
Equivalent to a 35W halogen. All-round
solution for many different applications.
Operated from 10-36VDC.
Flood
Spot
SL-3915 $49.95 ea
SL-3916 $49.95 ea
4995ea
$
Buy 2 for $89.90 SAVE $10
"Condura" Style DC Rocker Switches
Superb looking rocker switches that you see in 70-100ft luxury motor
cruisers. Basic switch comes with double-LED illumination, a standard
rocker cover and a standard range of decals to customise the switch to
your application. For more professional finish, special laser-etched covers
are available to match the basic switches.
NEW!
• Rated 12V 20A, 24V 10A
1295
Typical decals include: windscreen wipers, horn, heater & $
many more.
LASER-ETCHED COVERS
BASIC SWITCHES
"12V Power"
SK-0920 $2.95
White SK-0910 $12.95 "Fridge"
SK-0921 $2.95
Red
SK-0912 $12.95 "Aux Battery"
SK-0922 $2.95
Blue
SK-0914 $12.95 "Interior Light"
SK-0923 $2.95
Amber SK-0916 $12.95 "Spot Lights"
SK-0924 $2.95
SK-0910
"Horn"
"Rear View Camera"
"Inverter"
"Driving Lights"
"Thermofan"
SK-0920
SK-0925 $2.95
SK-0926 $2.95
SK-0927 $2.95
SK-0928 $2.95
SK-0929 $2.95
siliconchip.com.au
www.jaycar.com.au
Savings off original RRP. Limited stock on sale items
OUTDOOR DAD
Slide Drawer for Portable Fridge/Freezers
Portable Fridge/Freezers
Keep your food and drinks fresh and cold! Equipped with renowned
Danfoss® compressor and control module, these portable fridges
features digital display control panel, internal LED light, and 3-stage
battery protection.
If you're planning to install your Powertech
fridge/freezer in the back of your 4WD,
installing with one of these
slide drawers is a very secure
& convenient way to go.
ide
Compressor Ins
• Superb energy efficiency and reliability.
• Powered by either 12/24VDC or 240VAC
• Uses just 0.7A per hour
• Locks in 3 positions
• Handles up to
100kg load
GH-1609
DUE EARLY SEPTEMBER
Four models available:
30L Fridge/Freezer GH-1600 $695
40L Fridge/Freezer GH-1602 $749
50L Fridge/Freezer GH-1604 $825
GH-1601
Accessories available:
30L Insulated Bag GH-1601 $59.95
40L Insulated Bag GH-1603 $69.95
50L Insulated Bag GH-1605 $74.95
FROM
GH-1600
$
695
Semi-flexible Solar Panels
REGISTER
ONLINE
TODAY!
REWARD
YOU
Suitable for a variety of mobile and permanent power installations. Provides standard
protection (overload, high temperature, over/under input voltage and output short
circuit) as well as host of additional features to
FROM
improved performance and reliability under
adverse conditions. Range from 180 to 2000W.
$
199
• USB port
• 12VDC input, 230VAC output
9995
$
399
100W
• Short circuit current: 5.69A
• Weight: 2.8kg
ZM-9116
LET US
299
Pure Sine Wave Inverters
These 12V flexible solar panels offer
performance at an affordable price. No
heavy rigid frame makes them light and
portable. Both units have a fully sealed
terminal box with approx 1.2m of power
cable with PVC outer sheath.
20W
• Short circuit current: 1.24A
• Weight: 0.78kg
ZM-9112
NEW!
$
$
180W
360W
800W
1100W
1500W
2000W
ZM-9112
MI-5700
MI-5700 $199
MI-5702 $239
MI-5704 $449
MI-5706 $649
MI-5708 $899
MI-5710 $1,149
MI-5710
See online for Modified Sine Wave Inverters
Deep-Cycle Gel Batteries
9 Step Switchmode Battery Charger
• 12VDC
Fully automatic 25A high current charger with maintenance charging of all types
of lead-acid batteries (SLA, Gel and AGM) as well as lead-calcium batteries from
50 - 500Ah, either 12V or 24V. Microprocessor controlled and protected against
user error, so is totally safe to leave connected for
months at a time. Perfect for caravan and boat
users. See our website to download full product
info sheet.
These are genuine deep-cycle batteries that can be operated and charged in
any position. Leakproof and completely sealed. Ideal for
solar power, 4WD, camping, etc.
FROM
129
$
26Ah SB-1698 $129
38Ah SB-1699 $189
100Ah SB-1695 $379
SB-1698
DEAL!
*FREE Battery Conditioner
(NA-1420) valued at $7.75
*Valid with purchase of
SB-1698, SB-1699 & SB-1695
SB-1699
SB-1695
SLA Battery Boxes
Snap On Battery
Terminals
Designed to suit larger SLA
batteries or your standard car
battery. Perfect for mounting in
your boat, trailer or caravan.
Includes mounting clamps and
lid strap to secure the box
properly in place.
FROM
1995
$
To suit 40Ah SLA Batteries
HB-8100 WAS $24.95
NOW $19.95 SAVE $5
SAVE $5
To suit 100Ah SLA Batteries
HB-8102 WAS $29.95 NOW $24.95 SAVE $5
• Rated at 500A
• Red and black supplied
HM-3087
Battery not included
The pulse width modulation (PWM) used in this controller allows you to vary
intensity of a 12V device from 0 to 100% with high efficiency. Operating on
any 12V system at up to 8 amps, the circuitry is
fully potted and the control potentiometer is
splash proof.
27
$
siliconchip.com.au
95
To order call 1800 022 888
349
$
SAVE $50
Universal Programmable
Battery Charger
Used for protecting the
exposed positive/negative
battery connections from
dust, grime or other build
up. Ideal for automotive,
marine, or industrial use.
12V 8A Dimmer/Motor Speed Controller
• Suitable for harsh or wet conditions
• Size: 95(L) x 47(W) x
26(H)mm
MP-3209
• IP44 rated
• Input: 170 - 260VAC, output: 12/24VDC
• Current: 4A max
• Size: 260(L) x 135(W) x 70(H)mm
MB-3608 WAS $399.00
Charges, discharges and balances Li-ion, Li-Po, Ni-Cd,
Ni-MH and lead acid batteries. Particularly suited to radio
control hobbies. It can be powered with a mains plugpack
or directly from a 12V battery or any other DC
source from 10 - 18 volts.
1495
$
• Microprocessor controlled
• Delta V charging detection
• 2, 3, 4, 5 and 6 cell
balanced charging
$
outputs
MB-3632
7995
Flexible LED Strip Light
Over 1,000 lumens of brilliant white light to light up under your awning, inside a
tent, or anywhere else around the campsite. Fitted with hook and loop backing
for quick and easy hanging.
• IP67 waterproof
• 12VDC, 1.0A
• 1.2m long light
• 5m long cord
ST-3950
8995
$
September 2014 51
www.jaycar.com.au
3
DIY DAD
IP67 Sealed Waterproof Connectors
XLR
2.1mm DC Power
A matching IP67
waterproof
plug and
socket suitable
for harsh
environments.
Great for use with PA
gear and cabling that
are used in outdoor
conditions.
995
Snap Fit ABS Enclosures
NEW!
FROM
1295
395
$
• 96% tin, 4% silver, cadmium free
• Includes 14g solder with
14g of flux
NS-3045
129
This liquid can be used instead of
insulation tape. Simply brush it on and
it will insulate and seal out moisture.
1295
1995
$
595
HB-6431
2995
Reinforced Plastic
Tool Set
Handy tool set that won't rust!
Supplied as a one-piece mould simply snap out the tools you need.
• Includes scraper, tweezers,
spanners (M1.6/M2/M2.6/M3/M4),
grip (driver) with many
common heads
NEW!
TD-2116
DUE EARLY SEPTEMBER
34
To order call 1800 022 888
495
Used religiously in marine, aircraft and other
fabrication industries as an essential corrosion
inhibiting material to seal joints between
dissimilar metals of all types, including
magnesium and alloys.
3295
$
• 115ml tube
NA-1026
SIGN UP NOW & BE REWARDED
Quality tinned hook-up wire on plastic spools.
8 rolls included, each roll a different colour.
95
$
"DURALAC" Anti-Corrosive
Jointing Compound
Hook-up Wire Pack
52 Silicon Chip
FROM
$
$
• Size: 300(W) x 310(H) x
145(D)mm
HB-6301
5 times stronger that regular solder
and 100% lead free. Will join all
metals excluding aluminium. Use
with a soldering iron, torch.
Liquid Electrical Tape
4
NEW!
DUE EARLY SEPTEMBER
$
$
HB-6431 $5.95
HB-6433 $5.95
HB-6432 $7.95
HB-6434 $7.95
Perfect storage solution for fasteners and other
small parts. Unique "double lock" design on each
storage box keeps contents in their bins when
shut. Commercial grade.
NEW!
• 12 storage compartments
149
Buy TS-1318, get 50% off NS-3045
• 25m on roll
WH-3009
FROM
1495
Portable Storage Cabinet
"Silver" Solder
$
$
Grey, 1-Way Cable Entry
Black, 1-Way Cable Entry
Grey, 2-Way Cable Entry
Black, 2-Way Cable Entry
FROM
$
This kit contains a
Portasol Pro Piezo Gas
Soldering Iron, cleaning
sponge and tray, 2.4mm
double flat tip, hot air blow,
hot knife tip, hot air
deflector and flame tip.
Black NM-2836 $12.95
Red NM-2838 $12.95
RJ45 Socket PS-1450 $27.95
RJ45 Plug
PP-1452 $14.95
Cap to Suit PP-1454 $8.95
Available in 2 sizes, either light grey or black.
HB-6431 & HB-6433 - 91(L) x 79(W) x 45(H)mm
HB-6432 & HB-6434 - 91(L) x 122(W) x 69(H)mm
NEW!
Pro Gas Soldering
Tool Kit
• Acid & salt resistant
• 28g tube
• 15/16”-20 UNEF thread locking
Made of high impact resistant ABS plastic, these enclosures can withstand
wide range of temperature and humidity fluctuations. Snap-in design for easy
opening and closing without using any tools.
Features a generous 2.5L 304-grade stainless steel bowl,
controllable heating element and digital controls. Stylish
cabinet design and very well built.
DEAL!
This set of connectors makes it safe
to use RJ45 connectors in harsh
environments.
ABS Enclosures with Snap-in Hinged Lid
Digital 2.5L 170W Ultrasonic Cleaner
• Quality storage case
• 15-75 Watts (adjustable)
TS-1318
RJ45
• Four internal moulded standoffs to mount PCB horizontally
• Includes 2 x wall mount holes (4.5mm Dia.)
and 4 x internal holes (2.0mm Dia.)
• 4 sizes available
• Tank Capacity: 2500ml
(Max 2100ml, Min 600ml)
• 5 selection time settings
• Weight: 2.5kg
• Size: 290(W) x 223(D) x 185(H)mm
YH-5412
$
95
HB-6006
Range of black ABS cases with side flanges
allowing wall, or ceiling mount. Snap fit design
that locks together to enclose the circuit board or
project inside.
HB-6006 $3.95
HB-6007 $4.95
HB-6008 $5.45
HB-6009 $5.45
Panel Mount Socket
PS-0789 $14.95
Line Plug with 1m Cable
PP-0787 $12.95
7
$
• 3A max at 12VDC
PS-0785
XLR Line Plug
PP-1013 $9.95
XLR Line Socket PS-1017 $9.95
70(L) x 50(W) x 27(H)mm
90(L) x 50(W) x 42(H)mm
100(L) x 80(W) x 43(H)mm
127(L) x 70(W) x 50(H)mm
Available in panel mount socket and
line plug models.
Features a standard 2.1(ID) x 5.5(OD)mm
DC connector set. Pre-fitted with a 100mm
pigtail lead, allowing you to make up your
own lead set. Very handy!
NEW!
• Cables are 20AWG
NEW!
$
2.5mm Stereo
*Conditions apply.
See website for T&Cs
REGISTER
ONLINE
TODAY!
Earn a point for every dollar spent
at any Jaycar Company store* & be
rewarded with a $25 Rewards Cash
Card once you reach 500 points!
Register online today by visiting
www.jaycar.com.au/rewards
siliconchip.com.au
www.jaycar.com.au
Savings off original RRP. Limited stock on sale items
Dad’s Workbench
13.8VDC Regulated Switchmode
Power Supplies
120W Stepdown Transformer
Quality fully-enclosed stepdown
transformer with fold up metal
carry handles, approved
3-wire power cord &
US style 2 pin
110 - 115V socket.
High current general workshop
power supply for
equipment, component
testing etc.
• Input voltage:
190 - 240VAC
• Banana socket style
binding posts
• LED power on indication
• Rear mounted M205 fuse
FROM
69
$
12A MP-3079 $69.95
40A MP-3089 $199.00
• 120W 240V 115V Isolated
• 120VA, 1.0A rated
MF-1080
95
Test & Measurement
Plug-In USB Datalogger
Power Point and
Leakage Tester
• Temp range: -40˚C to 70˚C
• 32,000 memory samples
QP-6013
USB / LCD Readout Type
also available QP-6014 $149
1995
Cat III True RMS DMM
with Temperature
119
$
Non-Contact Thermometer
with Dual Laser Targeting
Measure the temperature of any surface
from a safe distance with this compact
sized non-contact thermometer. With a
wide temperature range and laser
targeting, this portable instrument is easy
to use for quick and accurate
temperature checking of any surface.
A powerful true RMS multimeter that
includes non-contact voltage testing,
backlit LCD, and a carrying pouch.
• 4000 count, 600V
• Temp range: 20°C to 760°C
• Voltage, current, resistance,
capacitance, frequency
and more
• Powered by 1 x 9V battery
(included)
QM-1551
$
95
• Temp range: -50˚C to +650˚C /
-58˚F to +1202˚F (±1%)
• Size: 146(L) x 104(W) x
$
43(D)mm
QM-7221
99
59
300mm Copper Cable Shears
NEW!
1595
• Base size: 115(W) x 94(D)mm
TH-1769
1995
$
To order call 1800 022 888
• Adjustable head strap
• Built-in LED work light
• 1.5x, 3x, 8.5x or 10x
magnification
• Requires 2 x AAA batteries
(SB-2426 $1.95)
QM-3511
2995
$
Desktop LED
Magnifying Lamp
Sixty LEDs provide ample illumination,
perfectly even light and the 3x and 12x
magnifying lenses will show all the detail
needed. Being LED, there's no delay in
startup and they'll never need replacing. Ideal
for hobbies, modelmaking or jewellery etc.
• Size: 320(H) x
95(Dia.)mm
QM-3544
6P6C RJ11/12
8P8C RJ45
Insulated Terminals
BNC/TNC RG58/59/62
F Connectors CATV RG6/59
Non-Insulated Terminals 26-18AWG
Non-Insulated Terminals 20-10AWG
SMA/Fibre Optic 1.09-6.48mm
SMA/Fibre Optic 1.07-4.52mm
Strip wire sizes from 0.6mm to 2.6mm. Spring-loaded
with locking jaws. Soft rubber handles
for added comfort.
The base will clamp to any bench
or table up to 55mm thick and the
40mm jaws will take a job up to
58mm in size. Once in position,
the head is easily fixed in position
with a quick release lever.
229
Leaves both hands free and can be worn over
prescription or safety glasses. Ideal
for jewellery, radio electronics,
& camera repair etc.
$
4995
Quick interchangeable dies available:
Stainless Steel Wire Stripper and Cutter
270˚ Rotation
Clamp Vice
$
Heavy duty and ergonomic
crimper that uses quick
interchangeable dies, no
screwdriver needed. Has
Ratchet mechanism for max
power and quick release.
TH-2000
24
$
• Rated power handling: 500 VA
(fused)
• Input voltage: 240VAC <at>50Hz
• Output Voltage: 0 - 260VAC <at>50Hz
• Size: 165(D) x 120(W) x 160(H)mm
MP-3080
Heavy Duty Crimp Tool
Features a precision cutting head forged from carbon steel attached
to drop forged steel handles for extra leverage. Cuts copper
cable up to 35mm2 and any
cable up to 2GA.
NEW!
• 310mm long
$
95
TH-1900
• Strips stranded wire from 12-24 AWG
and solid wire from 10-22 AWG
• Will also cut steel wires up to 3.0mm
• 164mm long
TH-1841
Controls AC votage and of voltage-dependent
parameters such as current, power,
temperature, light intensity, motor speed
etc. It enables the AC input to a
mains powered appliance to be
easily varied from 0 to full line
voltage (or greater). Encased in
heavy-duty steel housing.
LED Headband Magnifier
Log temperature and
humidity readings.
Download to PC via
USB.
Test your power points using
this versatile tester. It checks
most types of power points
within 110V to 240V for correct
wiring and earth
leakage circuit
$
breaker trip levels.
QP-2000
siliconchip.com.au
99
$
Also available:
250W 240V - 115V Isolated
MF-1082 $129
0-260VAC Variable Laboratory
Autotransformer (Variac)
Pocket Size Gas Blowtorch
Fully self-contained butane 1300˚C
portable blow torch. Simple press button
Piezo ignition, flame control and safety
lock. Refillable with butane gas (NA-1020).
Ideal for hobby use, low
temp silver soldering,
NEW!
heat shrinking etc.
1695
$
• Size: 95(H) x
55(L) x 26(W)mm
TH-1610
For suitable Butane Gas use
For Silver Solder use
NA-1020 $5.95
NS-3045 $19.95
TH-2001
TH-2002
TH-2003
TH-2004
TH-2005
TH-2006
TH-2007
TH-2008
TH-2009
$17.95
$17.95
$17.95
$17.95
$17.95
$17.95
$17.95
$17.95
$17.95
NEW!
$
4995
100 Piece Driver Bit Set
The ultimate driver bit set. It has a
magnetic bit holder, square to hex
socket drivers, & square to
hex bit adaptor. See
website for full list of bits.
• Snap lock case
TD-2038
$
1995
September 2014 53
www.jaycar.com.au
5
AV DAD
4 Input HDMI Switcher
4 Input HDMI Switcher
with Audio Return
Switches between up to 4
HDMI sources. Supports
resolution up to UHD
4K x 2K and also
features 3D capability
as well as TOSLINK
audio output.
Switch between four HDMI sources to one HDMI
equipped display. Features Audio Return Channel
(ARC) to allow audio
signals to be returned
from the TV display
to sound system.
NEW!
• Inputs: 4 x HDMI
• Output: 1 x HDMI
$
95
• Resolutions: All
resolutions up to 4K x 2K
• Audio formats: Dolby TrueHD, DTS-HD
Master Audio 7.1CH
• Compliant with HDMI 1.4a, CTS 1.4a, DVI
1.0, and VESA
• Size: 146(L) x 70(W) x 24(H)mm
AC-1707
• Inputs: 4 x HDMI
• Outputs: HDMI, TOSLINK, 3.5mm stereo
• Supported resolution: Up to 4k
x 2k / 3D TV support / 1080p /
NEW!
1080i / 720p / 720i
$
• Digital Audio Support
• Dolby TrueHD
• DTS-HD Master Audio 7.1CH
• Size: 191(L) x 83(W) x 25(H)mm
AC-1709
94
119
3G SDI & HDMI Converter
Allows HDMI equipped
TVs and PC monitors
to playback
uncompressed
2.970Gbps digital
footage from cameras
supporting this format over long
distances.
3G SDI to HDMI Converter AC-1727 $99.95
HDMI to 3G SDI Converter AC-1729 $99.95
• Size: 170(H) x 110(W) x 89(D)mm
CS-2463
1m WQ-7301 $14.95
3m WQ-7302 $24.95
5m WQ-7303 $39.95
$
3995
6495
399
SAVE $100
FATHER’S DAY
GIFT IDEA!
Concord RCA Leads
Economy HDMI Leads
• 2 x RCA plugs to
2 x RCA plugs
1.5m WV-7915 $19.95
3.0m WV-7916 $24.95
5.0m WV-7917 $39.95
Cost-effective solution without compromising
quality or performance. Gold plated
connectors. HDMI 1.4 standard
with Ethernet classification.
0.5m
1.5m
3.0m
5.0m
WQ-7227 $16.95
WQ-7226 $18.95
WQ-7228 $24.95
WQ-7230 $29.95
FROM
CW-2822
Suits Panels 23" to 37" Up to 45kg
CW-2826 $39.95
Ceiling-Mount
Projector Bracket
Designed to fit most of the projector models
on the market, this bracket can be rotated
through a full 360˚ and extends up to 370mm.
Mounting hardware and instructions included.
• Rigid extruded aluminium construction
• Supports up to 15kgs
• Size: 182(W) x 235 - 310(H) x 182(D)mm
CW-2827
Suits Panels 32" to 60" Up to 80kg
CW-2822 $89.95
Suits Panels 23" to 37" Up to 45kg
(Rotation and Tilt)
CW-2829 $109.00
6
$
95
Mount your TV on the wall for a better view. Features solid steel construction, safety lock for security
(CW-2822 and CW-2826 only) and are VESA standard compliant. Mounting hardware and instructions
included
FROM
1995
16
$
Plasma, LCD & LED TV Wall Brackets
54 Silicon Chip
99
$
Stereo parallel cables utilising
99.96% pure OFC and 24 carat
hard gold
plated contacts.
FROM
Suits Panels 32" to 60" Up to 80kg
(Rotation and Tilt)
CW-2825 $149.00
$
NEW!
• Class D amplifier
• Mains powered
• Size: 320(L) x 320(W) x 475(H)mm
CS-2549 WAS $499
LIMITED STOCK
NEW!
1495
$
A clever device that allows you to hide your HDMI
audio/video sources in cabinets or
behind walls but still be able to
NEW!
control them.
Lightweight PA system which includes 2 x 100W speakers,
7-channel mixer and a microphone. Features built-in DSP
effects, peak indicator and a variety of controls to fine-tune
the audio frequency range. It can also play
$
MP3s from an SD card or a USB flash drive.
Fibre Optic Audio Leads
A range of fibre optic TOSLINK
cables with superb build
quality. Suitable for
achieving excellent
audio reproduction in
home cinemas that
support Dolby Digital 5.1
(AC-3) surround sound,
DTS, and more.
HDMI Repeater with IR Extender
10" Portable PA System with 7 Channel Mixer
Centre Speaker with Bracket
2 x 2.5" full range speakers rated at
15WRMS, housed inside a
rectangular shaped
speaker box to suit most
existing systems.
Supplied with an
adjustable swivel mount
bracket for wall installations.
119
• 1080p signals up to 45m
AC-1641
• HDMI 1.3b and
HDCP1.1 / DVI1.1 compliant
• 1080p signals up to 30m
• Size: 100(L) x 65(W) x 25(H)mm
AC-1730
9995
• Inputs: 4 x
HDMI
• Outputs: 2 x HDMI
• DTS digital, Dolby Digital, DTS-HD and
Dolby TRUE HD
• Size: 85(W) x 192(D) x 26(H)mm
AC-1714
$
Transmits HDMI and IR
signals across
distances up to 30m
over two common
Cat6 cables.
$
• Size: 80(L) x 43(W) x 23(D)mm
Distribute up to four HDMI sources to 2
displays simultaneously. Supports resolution
up to UHD 4K x 2K
as well as 3D
and EDID.
NEW!
HDMI Over 2 x Cat5e/6 - 30m
with IR Extender
NEW!
HDMI 4 x 2 Switcher/Splitter
with UHD 4K Support
$
FROM
3995
To order call 1800 022 888
CW-2825
7995
$
siliconchip.com.au
www.jaycar.com.au
Savings off original RRP. Limited stock on sale items
SECURIT Y DAD
Low Cost Home Automation
Don't spend tens of thousands of dollars to create a smart home. With our new
low cost range of Wireless Home Automation, you can create a fully automated
system and only spend a few hundred dollars.
Simple and easy to use, all sensors, controllers and swicth modules are
operating wirelessly on 433MHz frequency at a max range of 100m (line of sight).
Home Automation Main Controller
A powerful controller with built-in 16 wireless alarm zones and 16 wireless
home automation control. Easily interfaces with a wide range of wireless
security devices such as a PIR motion detectors (LA-5157), magnetic reed
switches (LA-5158), light sensors (LA-5598)
and remote key fobs (LA-5155) to protect
your home and property.
• Timer schedule programming
• Group programming
• Matrix (Scenes) programming
• 100 Alarm event memory
• 12VDC
• 240VAC power adaptor included
LA-5592
Accessories to suit:
Key FOB Remote
PIR to suit
Wireless reed switch to suit
• Voltage input: 12VDC
• Wireless Range: 100m line of sight
• Wireless Frequency: 433MHz
• Size: 340(L) x 200(W) x 75(D)mm
LA-5579
• Adjustable light setting
• Voltage Input: 12VDC
• Wireless Range: 100m line of sight
• Wireless Frequency: 433MHz
LA-5598
NEW!
119
$
• Up to 150m2 size of operation
• Voltage input: 12VDC
• Wireless Range: 100m line of sight
• Wireless Frequency: 433MHz
LA-5597
High Resolution Cameras
with IR Illumination
Feature a high quality colour CMOS
sensor and IR LEDs for night time
illumination. Supplied with power
supply and 18m combined
video/power lead.
• 420TV Lines
• 12VDC
• 600 TV Lines
• Up to 10m range
• 12VDC
QC-8632
Outdoor Bullet Camera (IP66)†
QC-8632 $99
$
Dome Camera†
ea
QC-8633 $99
49 ea
95
99
Peephole Viewer with Image Capture
Displays video from the other side of your door on a clear 3" LCD screen.
MicroSD card required for image capture (sold separately XC-4992 $47.95)
triggered by adding either the knock or PIR sensors (sold separately).
• Requires 2 x AA batteries
• Peephole tube diameter: 12mm
• Peephole tube length: 33 to 45mm
• Viewer size: 158(H) x 87(W) x 32(D)mm
QC-3735 WAS $225.00
$
199
SAVE $26
Optional sensor modules:
PIR Motion Sensor
QC-3736 WAS $84.95 NOW $69.95 SAVE $15
Vibration Knocking Sensor
QC-3737 WAS $44.95 NOW $39.95 SAVE $5
8 Zone Wireless Alarm Kit
Everything you need to get a basic wireless
system set up in your home! Includes key fob
remote control, backlit LCD control panel, PIR
sensor and two reed switches.
$
149
See online for our full range of spare accessories.
To order call 1800 022 888
3995
$
Mount on the roof to directly control your household appliances. Will learn
your appliances infrared remote command and repeat them
when matched with a home automation input device.
109
Quality SHARP colour CCD cameras,
featuring adjustable focus lens
and composite video
output to feed into DVR or
TV for security and
monitoring purposes.
Ramp not included
siliconchip.com.au
3995
Wireless Infrared Controller
$
Mini Colour CCTV Cameras
• Back-up battery
• Size: 210(L) x 113(W) x 127(H)mm
LA-5145
$
Interfaces with the home Automation System to
turn an output device on or off.
LA-5155 $19.95
LA-5157 $49.95
LA-5158 $39.95
$
• Voltage input: 240VAC
• Wireless Range: 100m line of sight
• Wireless Frequency: 433MHz
LA-5594
Also available:
12VDC Switch Controller Module
LA-5595 $59.95
240VAC Mains Light Dimmer Module LA-5596 $39.95
Wireless Light Sensor Module
Works as an audible and visual deterrent, the siren produces a
wailing 94dB of output and a powerful strobe when alarm is
activated. Supplied with 240VAC mains power adaptor.
Colour CCD with IR†
QC-3694 $49.95
Designed to be hard wired to your GPO, wall switches
or other mains device, it enable you to remotely
activate any mains appliances.
*Note: A licensed electrician is highly recommended to
hard wire this device into 240V mains wiring.
Wireless Bell Box
Colour Pinhole† (shown)
QC-3692 $49.95
240VAC Mains Switch Controller Module
7995
$
(L
†
A- Fre
51 e C
01 C
) v TV
alu S
Access your CCTV system via the Internet or
ed tic
your local intranet. Access the camera through a
k
web interface by hitting the IP address of the device at $ er
3.9
and logging in. The web interface allows you to adjust
5
Vandal Proof Mini
Dome Camera
visual settings, record, take snapshots and setup
scheduled recording.
• H.264/MJPEG video compression
• CMOS camera sensor
• 12VDC, PoE
$
• Size: 110(Dia.)
x 54(H)mm
QC-8626†
†Valid with purchase of any of these CCTV cameras.
299
Wireless 7" Colour Video Doorphone
Monitor the front door of your home or office without the
need to run wires. The weatherproof
outdoor camera can be powered from the
included power supply or from 6 x AA
batteries (not included). The AV signal
transmits wirelessly to the 7" colour
monitor. It also records any visitors you had
while you were out, saving the footage to
an SD card (available separately).
• 2.4GHz for transmission up to 100m
• Weatherproof (IP55) camera with rain shield
QC-3621
299
$
Indoor Commercial Grade Doorway Beam
An entry buzzer designed for use in shops, restaurants, doctors and dentist
surgeries, workshops etc to alert you to the entry of customers and visitors.
• Mains adaptor included
$
• Up to 6m range
• Adjustable alarm time & volume
LA-5193
Accessories to suit:
Infrared Beam
LA-5179 $99.00
Door Counter
LA-5197 $34.95
Door Extension Buzzer LA-5188 $34.95
79
September 2014 55
www.jaycar.com.au
7
BUILD IT DAD
ICSP Programmer for Arduino
24
Program new applications into a
$
95
wide range of microcontrollers
using this ICSP programmer with a
USB interface. Compatible with a wide range of
microcontrollers, including all Arduino boards.
• Supplied with a USB cable and
ISP programming cable
XC-4237
Add an interactive
touch screen to your
existing Arduino
project. Includes a
3.2" LCD colour
display with resistive
touch and multiple
input/outputs, a 4D
Arduino shield and 5
way interface cable.
XC-4280
$
119
This large, bright 512 LED matrix panel has onboard
controller circuitry designed to make it easy to use
straight from your board.
• 32 x 16 high brightness blue LEDs
(512 LEDs total) on a 10mm pitch
• Viewable over 12 metres away
XC-4251
NOTE: Can for
comparison only
Also available:
Red Large Dot Matrix
LED Display Panel
XC-4250 $39.95
EtherTen
Connect this to your board and point it at a
surface or heat source to remotely
measure its temperature. This is our
special version of the industrial
infrared remote thermometer
units with an onboard power
supply, communication
support and a software
library with examples
supplied.
3495
$
• 3.3 to 5V operation
• -33 to +220˚C measurement
range, 1 second response time
XC-4260
$
8995
Eleven
Includes onboard Ethernet, a
USB-serial converter, a microSD
card slot for storing
gigabytes of web server
content or data, and even
Power-over-Ethernet support.
• ATmega328P MCU
running at 16MHz
• 10/100base-T Ethernet built-in
XC-4216
Also available: Mega Prototyping
Shield to suit XC-4257 $17.95
6995
$
The "Eleven" is just like an Arduino Uno - but better!
It's a microcontroller board based on the
ATmega328 with 14 digital input/output pins
(of which 6 can be used as PWM
outputs), 6 analogue inputs, a
16MHz crystal oscillator, a
USB connection, a power
jack, an ICSP header, and
a reset button.
XC-4210
See instore or online for more
RFID Door Lock
Shield Kit
3995
$
Terminal Shield
Breaks out all the Arduino
headers to handy screw
terminals, making it easy to
connect external wires without
using a soldering iron. Ideal for
quick experiments or for robust
connections!
This shield enables your
Arduino to control a door lock
using an electric strike plate and
one of a number of commonly
available RFID modules.
4 Channel PoE Midspan
Injector for Arduino
• 4 channels of input/output
jacks
XC-4254
Blue Dot Matrix LED Display Panel
ARDUINO COMPATIBLE BOARDS
IR Temperature Sensor Module
Power up to 4 EtherTen's
(XC-4216) or
EtherMega's (XC4256) with DC from a
low cost plugpack
across your home or
office network cables. It
isolates and powers the
correct wires automatically.
4D Systems Intelligent
Module with Touch
• Supported readers include
ID12, ID20, RDM630,
RDM880, and HF MultiTag
XC-4215
29
$
95
• Gold-plated surface
• Large prototyping area
XC-4224
1695
$
SIGN UP NOW & BE REWARDED
2695
$
Earn a point for every dollar spent at any Jaycar
Company store* & be rewarded with $25 Rewards
Cash Card once you reach 500 points!
Register online at www.jaycar.com.au/rewards
*Conditions apply. See website for full T&Cs
YOUR LOCAL JAYCAR STORE - Free Call Orders: 1800 022 888
AUSTRALIAN CAPITAL TERRITORY
Belconnen
Fyshwick
Ph (02) 6253 5700
Ph (02) 6239 1801
NEW SOUTH WALES
Penrith
Port Macquarie
Rydalmere
Smithfield
Sydney City
Taren Point
Tuggerah
Tweed Heads
Wagga Wagga
Warners Bay
Wollongong
NEW
Ph (02) 4721 8337
Ph (02) 6581 4476
Ph (02) 8832 3120
Ph (02) 9604 7411
Ph (02) 9267 1614
Ph (02) 9531 7033
Ph (02) 4353 5016
Ph (07) 5524 6566
Ph (02) 6931 9333
Ph (02) 4954 8100
Ph (02) 4226 7089
Mackay
Maroochydore
Mermaid Beach
Nth Rockhampton
Townsville
Strathpine
Underwood
Woolloongabba
Ph (07) 4953 0611
Ph (07) 5479 3511
Ph (07) 5526 6722
Ph (07) 4926 4155
Ph (07) 4772 5022
Ph (07) 3889 6910
Ph (07) 3841 4888
Ph (07) 3393 0777
Albury
Ph (02) 6021 6788
Alexandria
Ph (02) 9699 4699
Bankstown
Ph (02) 9709 2822
Blacktown
Ph (02) 9678 9669
Bondi Junction
Ph (02) 9369 3899
SOUTH AUSTRALIA
Brookvale
Ph (02) 9905 4130
Adelaide
Ph (08) 8231 7355
Campbelltown
Ph (02) 4625 0775
Clovelly Park
Ph (08) 8276 6901
NORTHERN TERRITORY
Castle Hill
Ph (02) 9634 4470
Elizabeth
Ph (08) 8255 6999
Darwin
Ph (08) 8948 4043
Coffs Harbour
Ph (02) 6651 5238
Gepps Cross
Ph (08) 8262 3200
Croydon
Ph (02) 9799 0402
Modbury
Ph (08) 8265 7611
QUEENSLAND
NEW Ph (02) 6881 8778
Dubbo
Aspley
Ph (07) 3863 0099
Reynella
Ph (08) 8387 3847
Erina
Ph (02) 4365 3433
Browns Plains
Ph (07) 3800 0877
TASMANIA
Fairy Meadow
NEW Ph (02) 4225 0969
Caboolture
Ph (07) 5432 3152
Hobart
Ph (03) 6272 9955
Gore Hill
Ph (02) 9439 4799
Cairns
Ph (07) 4041 6747
Launceston
Ph (03) 6334 2777
Hornsby
Ph (02) 9476 6221
Caloundra
Ph (07) 5491 1000
VICTORIA
Liverpool
Ph (02) 9821 3100
Capalaba
Ph (07) 3245 2014
Cheltenham
Ph (03) 9585 5011
Maitland
Ph (02) 4934 4911
Ipswich
Ph (07) 3282 5800
WE HAVE
Newcastle
Ph (02) 4968 4722
Labrador
Ph (07) 5537 4295
Coburg
Ph (03) 9384 1811
MOVED
Arrival dates of new products in this flyer were confirmed at the
HEAD OFFICE
ONLINE ORDERS
time of print but delays sometimes occur. Please ring your local
320 Victoria Road, Rydalmere NSW 2116
Website: www.jaycar.com.au
store to check stock details. Savings off Original RRP.
Prices valid from 24th August 2014 to 23rd September 2014.
Ph: (02) 8832 3100 Fax: (02) 8832 3169
Ferntree Gully
Frankston
Geelong
Hallam
Kew East
Melbourne
Mornington
Ringwood
Roxburgh Park
Shepparton
Springvale
Sunshine
Thomastown
Werribee
WE HAVE
MOVED!
Ph (03) 9758 5500
Ph (03) 9781 4100
Ph (03) 5221 5800
Ph (03) 9796 4577
Ph (03) 9859 6188
Ph (03) 9663 2030
Ph (03) 5976 1311
Ph (03) 9870 9053
Ph (03) 8339 2042
Ph (03) 5822 4037
Ph (03) 9547 1022
Ph (03) 9310 8066
Ph (03) 9465 3333
Ph (03) 9741 8951
WESTERN AUSTRALIA
Joondalup
Maddington
Mandurah
Midland
Northbridge
Osborne Park
Rockingham
OPENING
SOON!
Ph (08) 9301 0916
Ph (08) 9493 4300
Ph (08) 9586 3827
Ph (08) 9250 8200
Ph (08) 9328 8252
Ph 1800 022 888
Ph (08) 9592 8000
Email: techstore<at>jaycar.com.au
Occasionally
there are C
discontinued
items advertised on a special / lower price in this promotional flyer that has limited to nil stock in
56 Silicon
hip
certain stores, including Jaycar Authorised Stockist. These stores may not have stock of these items and can not order or transfer stock.
siliconchip.com.au
electronics design & assembly expo
Design, Develop, Manufacture
with the Latest Solutions!
In the fast paced world of electronics you need to see,
test and compare the latest equipment, products and solutions
for manufacture and systems development.
electronics
& assembly expo
Showcasing
new and design
future technologies
in electronics
Register Online Now
www.electronex.com.au
Knowledge is Power
Make New Connections
SMCBA CONFERENCE
The Electronics Design and Manufacture Conference
delivers the latest information on a host of topics.
• Australian & NZ based suppliers with the
latest ideas and innovations
• New product, system & component technology
releases at the show
• Australia’s largest dedicated electronics
industry event
Mono Version
• NEW technologies to improve design and
manufacturing performance
• Meet all the experts with local supply solutions
electronics design & assembly expo
The last conference in Sydney attracted over
200 delegates and featured an impressive list of
international presenters.
For conference details please visit
www.smcba.asn.au
Australian Technology Park - Sydney 10-11 September 2014
www.electronex.com.au
B
C
P
F
E
R
This year the
U exhibition returns to Sydney
T
E A (Australian Technology Park,
Eveleigh, September 10-11).
While the exhibition covers all aspects
of electronics from components and
design through to assembly, the concurrent
SMCBA conference means there is a focus
on PCBs and surface mount technology.
SILICON CHIP (also exhibiting at
– stand A32) is pleased to
support
and showcase many
of the organisations also at this month’s
Now in its 5th year, Electronex – The Electronics Design &
Assembly Expo – is regarded as the definitive event for the
electronics industry. The expo alternates annually between
Sydney and Melbourne and the last event in Sydney in 2012
attracted over 1200 engineers and decision makers from the
electronics sector.
Improvements in design, system development and manufacturing assembly can be more easily achieved by keeping up to
date with the latest technologies, products, development tools
and industry knowledge base. The competitive future of practically every Australian industry sector is increasingly dependent
on the utilis ation and integration of the latest electronics into
all aspects of production, assembly, systems development,
maintenance and service.
Design, electronic and electrical engineers, OEM, scientific,
IT and communications professionals are invited to attend the
event where they will find the latest technology driving future
product and system developments. This specialised trade
event continues to enjoy strong growth and is the pre-eminent
electronics technology showcase and conference in Australasia.
Electronex comprises a major trade show, with more than 90
companies represented, that will showcase and demonstrate
the latest new product releases for industry, scientific and commercial applications.
The SMCBA – Electronics Design & Manufacture Conference
is being held in conjunction with the exhibition. This year’s conference will feature several acclaimed international presenters
and deliver a wealth of information on electronics design and
manufacture as well as new streams on Embedded Systems
and New Product Development.
New Rigol MSO1000Z Mixed
Signal Oscilloscopes at Electronex
Emona Instruments will launch the new Rigol MSO1000Z
series mixed signal oscilloscopes at the Emona Instruments
stand, B1, at Electronex 2014.
The MSO1000Z series are the latest in Rigol’s popular
range of oscilloscopes. Rigol have built a solid reputation
for quality and excellent performance, with thousands of
units in use in educational institutions and industry around
Australia. The new MSO1000Z series continue this tradition of quality and performance by providing advanced
features at an affordable price.
The MSO1000Z series offer four channels, the choice
of 70MHz and 100MHz bandwidth, as well as 16 digital
channels. Sampling rate is 1GS/s and units come with
12Mpts standard memory with optional 24Mpts. Typical
of Rigol oscilloscopes, the MSO1000Z series provide a fast
30,000wfms/s waveform capture rate and a unique optional
60,000 frames real-time waveform record and play-back, as
well as UltraVision technology that provides multi-level
intensity grading display.
While offering Australia’s best value in mixed signal
oscilloscopes, the MSO1000Z series also offer a variety
58 Silicon Chip
of trigger and serial bus decoding functions (RS232, I2C
and SPI), wider vertical range (1mV/div~10V/div), lower
noise floor, better for small signal capturing and optional
in-built 25MHz dual channel Function/Arbitrary waveform
generator. All units offer a wide range of interfaces USB
Host, USB Device, LAN (LXI), AUX and include a large 7inch TFT (800x480) WVGA display with multi-intensity
waveform display.
If you can’t get to Electronex 2014, contact Emona Instruments at 78 Parramatta Rd, Camperdown NSW 2050, Tel:
(02) 9519 3933 or via their website, www.emona.com.au
siliconchip.com.au
siliconchip.com.au
Pb
September 2014 59
B
C
P
F
T
A
E
E
Brand new
R
U Raspberry Pi B+ board
The new Raspberry Pi B+, now available from element14,
is the first major update to the popular credit-card sized
computer. It adds connectivity and power features to enable bigger and better projects.
The new board, which marks the first significant change
to the multi-million selling credit card-sized computer, is
priced at just $38. The new board offers more sensors and
accessories than before, enabling users to build bigger and
better projects.
Advanced power management and enhanced connectivity make it possible to power four USB accessories, such
as 2.5 inch hard drive, through the device. Up to 1.2A can
be delivered to the USB ports to connect power-hungry
devices and accessories without needing mains power or
an external USB hub.
Featuring a 40-pin extended GPIO interface, even more
sensors, connectors and expansion boards can be added to
the board, allowing users to increase the complexity of their
Raspberry Pi projects. The first 26 pins remain identical
to the original Raspberry Pi Model B for 100% backward
compatibility.
The Raspberry Pi B+ is based on the same Broadcom
BCM2835 Chipset and 512MB of RAM as the previous
model. It is powered by micro USB with AV connections
through either HDMI or a new four-pole connector replacing the existing analog audio and composite video ports.
The SD card slot has been replaced with a micro-SD
slot, tidying up the board design and helping to protect
the card from damage.
The B+ board also now uses less power (600mA) than
the Model B Board (750mA) when running.
Since its launch in February 2012 over three million
Raspberry Pi boards have been sold and the element14
Community has become one of the leading websites for
discussion and collaboration around Raspberry Pi projects
and developments.
With over 250,000 registered users the element14 Community is the largest online community for design engineers
to share ideas, knowledge and solve challenges.
For more information on the new board or the Raspberry
Pi phenomenon in general, call into stand B11 at Electronex
2014 or visit the element14 Raspberry Pi Community website at http://www.element14.com/raspberrypi
60 Silicon Chip
Prototype and low volume PCBs
and PCB Assembly
Brisbane based Iconic
PCB locally manufactures
and assembles printed
circuit boards, whether
for prototypes or for small
production runs.
Iconic PCB has the ability
to rapidly deliver electrically tested PCBs. Iconic
PCB also manufactures
multilayer boards.
The PCBs are supplied
as brass boards or fully
finished in green solder
mask, white overlay and
immersion silver.
Recent introduction of a
very competitively-priced
low volume rapid in-house stencil and SMT assembly
process augments the overall capability. Obtaining prototype PCB/PCBA product from Iconic PCB ensures your IP
remains within the Australian legal framework.
Iconic PCB also offers quality imported bare boards.
With Iconic PCB you will have good communication,
accessibility and flexibility.
Please visit our web site www.iconicpcb.com e-mail
sales<at>iconicpcb.com or call 07 32033637 for further information.
Brisbane based PCB/PCBA manufacturer
Prototype and low volume
Quick turnaround
Single / double and multilayer PCBs
PCB assembly SMT and PTH
Source of overseas PCBs
www.iconicpcb.com
sales<at>iconicpcb.com
07 32033637
siliconchip.com.au
PCB Designing and
Manufacturing Tips –
straight from the horse’s mouth!
Most decent electronics engineers can design a half-decent Printed Circuit
Board. But few understand what happens when they send their PCB file
off to the manufacturer. There are many traps that most wouldn’t know
about, let alone consider. We asked Tejas Shah, the Business Development
Manager of major Australian/New Zealand PCB supplier QualiEco Circuits,
to give us some tips (with examples) from the manufacturing side.
P
CB designers are often confused as to
what manufacturers need to turn their
masterpiece into reality. Without knowing the requirements of the manufacturer,
mistakes are often made – and mistakes are
always costly.
The manufacturer has great skill in interpreting what the designer actually wants
but sometimes, they are left scratching their
heads.
The adage “impossibilities done immediately, miracles take a little longer” springs
to mind!
This article explains some basic PCB
design/manufacturing concepts and ideas
which will help expand your knowledge in
not only PCB design but how your choices
affect cost of efficiently manufacturing PCBs.
Shielding or open tracks
raised if the gap is smaller.
If you use shielding tracks or open tracks
for antennas, please mention this clearly.
CAM engineers normally catch such tracks
and may result in a query.
Tracks too close to cut lines
If any of your copper area or tracks are
close to cut lines, the CAM engineer might
ask your permission to shave copper to avoid
cutting into it during routing or v-cut.
If you allow 0.3mm gap for routing and 0.4-0.5mm gap for v-cut, it
would be considered a safe distance.
How to design a
manufacturer-friendly PCB
Every manufacturer has a CAD/CAM department, where your PCB design is checked
thoroughly before it goes in final production.
An EQ (Engineering Query) may be raised
if the CAM engineer has any doubts. This
process not only increases manufacturing
lead time but can create confusion if there
are many queries to resolve.
To-and-fro communication may also annoy you if queries are not handled professionally by the CAM engineer.
The million dollar question is – Is it really
possible to design query-free PCBs?
Yes, it is possible, if some simple rules are
followed throughout the design phase. A few
examples that I am going to discuss here will
certainly help you achieve this.
siliconchip.com.au
Multilayer PCB design
Inter-track gaps
If you are designing a multilayer
PCB, please provide a detailed layer
stack-up, if you have any special requirements . Remember – there is more than
You should
have at least 2
to 3mil (0.05
to 0.076mm)
gap between
two adjacent
solder mask
openings. A
query would
most likely be
September 2014 61
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one way to build a
structure and every
manufacturer can prepare the layer stack up
differently, based on the stock
they carry for prepreg and core.
Plated holes
If your design file requires any holes to be
plated, please provide copper pads on both
sides. If the CAM engineer leaves the design
unchanged, there could be plating issues, so
you will most likely be asked for permission
to add copper pad or, if you change your
mind to non-plated hole, to isolate copper.
Surface finish considerations
You need to choose the surface finish
very carefully. HASL is a default finish for
most PCB manufacturers. If your product
requires RoHS compliance, you can choose
either lead-free HASL or immersion silver/
gold/tin finish.
As a rule of thumb, if the minimum pitch
of your SMD components is 0.5mm or lower,
it is strongly advisable to choose immersion
silver/gold/tin finish.
A word of caution: immersion silver finish
PCBs need to be used within 2.5 to 3 months
of the date of manufacturing. Silver finish
demands great care in packing and storage.
Some interesting facts –
Did you know this?
1. Rigid PCBs can be made as
thin as 0.25mm. It means you can
use it like a flexible PCB in certain
cases. It is not a perfect replacement
but if your aim is only to achieve little
bit of flexibility, this is not a bad idea!
Technical specifications
Mating PCBs
If your project requires one PCB to be
inserted in another PCB (ie, mating PCBs),
always consider both laminate thickness
tolerance (±10%) and routing tolerance
(±0.1 to 0.2mm) before designing slots
It is best practice to provide basic technical specifications in one of your layers.
Some manufacturers do not send a detailed
technical confirmation report and assume
lot of technical parameters to their own
standard, which may not be same as your
expectations.
Communication is extremely critical for
PCB manufacturing and one little misunderstanding could cost a fortune.
What makes a PCB expensive?
If you know what specifications are standard, you can make the maximum out of your
design. Unfortunately, specifications differ
from manufacturer to manufacturer – there
is no “standard” specification.
The table below shows what QualiEco
Circuits considers standard/non-standard
features. Standard features result in the
lowest cost PCBs. Non-standard features
can of course be achieved but will result in
a more expensive board.
2. If you are designing a panel (ie
array) of PCBs for pick and place
assembly, you can get away with
panel strip on only two longer sides
of the panel by wisely placing break
off tabs. Tab and hole sizes and
positions are extremely important.
You can save up to 20% of unit
price by intelligently designing your
panel structure. For high volume
manufacturing, it is indeed a huge
saving!
A smart PCB manufacturer can
study your component reference to
judge required mechanical strength
of the panel before suggesting an
optimum panel structure.
PCB Specifications
QualiEco - Standard
QualiEco - Non-Standard
Laminate thickness
Copper thickness
Via hole size
Track width/spacing
Solder mask colour
Overlay colour
Surface finish
High Tg laminate
Peelable solder mask
Impedance control
Blind/Buried via
No “X” out panels
Via tenting
Via plugging
Gold finger
Edge connector
Edge bevelling
Plated rout/PTH cut out
Countersunk hole
Jump scoring
0.8mm to 1.6mm
1oz (35µ)
0.25mm and above
5mil (0.127mm) and above
Green, Red, Blue, White, Black
White, Yellow
Leaded or Lead-free HASL
Tg 130°-135°C
No
No
No
No
Using solder resist (not guaranteed 100%)
Using HASL (not guaranteed 100%)
No
No
No
No
No
No
0.4mm, 2.0mm & above
2oz and above
>0.1mm & <0.2mm
>3mil (0.076mm) & <5mil (0.127mm)
Red, Blue, White, Black (for high volume)
Yellow (for high volume)
Immersion silver/gold/tin, OSP
Tg 150°-180°C
Yes
Yes
Yes
Yes
100% guaranteed
100% guaranteed (silicon plugging)
Yes
Yes
Yes
Yes
Yes
Yes
62 Silicon Chip
siliconchip.com.au
Lintek has 27 years experience in
Manufacturing PCBs in Australia
T
he PCB manufacturing industry has
certainly changed over Lintek’s 27
year involvement. To survive in this
industry is not easy; your customer service,
quality and knowhow must be second to
none – local clients know that they are
paying a premium and they don’t need too
many excuses to move offshore.
The ‘heavyweights’ of the 1980s and 90s
have all but disappeared – or have moved
higher up the food chain where they can
value-add by providing turnkey solutions.
For Lintek, a 100% Australian manufacturer, the trick has been to try to stay
nimble, dynamic and quick to respond.
Developing good customer relationships
and educating designers about the process
complexities we encounter is paramount to
our survival. They find that the best clients
‘Design for manufacture’ and are willing to
modify their designs if it improves quality,
consistency and price.
There is always a compromise between
price and performance as higher quality dielectrics cost more, can be more difficult to
process and manufacturing times are longer
due to tighter process controls. Having an
in-depth understanding of material behaviour
over many years of processing exotic laminates gives their engineers the confidence
to take on the most complicated projects,
many of which their clients find difficult to
source anywhere else. Knowing your ‘sweet
spot’ is extremely important when taking on
the rest of the world – having a technological
advantage certainly helps.
R&D is extremely important to Lintek as it
helps the company stay in touch with industry
trends. The continuous miniaturisation of
parts can leave you falling behind the pack
very quickly and new opportunities become
more difficult to find.
Driven by industry demands, Lintek is
currently developing a number of new capabilities. One of these is to develop ‘via-in-pad’
technology around vacuum metalisation. This
will enable the formation of copper-filled
‘microvias’ laser-drilled down to copper
capture pads on multilayer PCB stacks. The
copper-filled vias will simplify the assembly
of BGA devices down to 0.4mm pitch and will
be a first for Australia.
LINTEK
To help develop these capabilities,
Lintek has been successful in receiving
funding for this project through DMO under the PICIP (Priority Industry Capability
Innovation Program).
The successful application for funding
is testament to the critical role they play
in supporting key defence suppliers. They
are also working with the team from DIIC
(Defence Industry Innovation Centre) to
take business to the next level. Their understanding of business and government
assistance available, along with training
and awareness programs, has been a
great help. Since their involvement with
DIIC Lintek have joined SCIP (Sustainable Continuous Improvement Program
or SC21), have become more active in
the GSC (Global Supply Chain) and are
working on implementing ‘lean management’ practices.
Finally, Lintek would also like to thank
Andrew Pollock and his team at the
SMCBA, they do a great job and offer
an invaluable service to the Australian
electronics industry.
PRINTED CIRCUITS
TOMORROWS PRINTED CIRCUITS TODAY
Incorporated in 1986, Lintek is a quality Australian
manufacturer of Microwave printed circuit boards. Lintek’s
patented High Vacuum Deposition process enables the
production of extremely accurate microwave circuit features
on a wide variety of conventional and exotic substrates including precision milled metal backed carriers. High bond
strength to PTFE and minimal side wall undercut are two
key features synonymous to Lintek’s process. This innovative
process allows Lintek to provide PCB’s for the latest high
frequency commercial or military designs as well as the
standard FR4 Single sided, DSPTH and Multilayer circuit
boards.
Unrivalled Accuracy
i) Lintek’s process requires significantly less etching to
remove a very thin 1-2 micron vacuum deposited copper
seed layer instead of the standard 18 microns copper base
layer used on Electroless copper processes, thus eliminating
undercut and ensuring the repeatability of:a. very fine track and spaces.
b. accurate copper features and filters.
c. near perfect side wall resolution.
d. superb impedance control.
Repeatability of
Fine track and spaces.
e. High bond strength to exotic substrates
ii) Plated through holes are stronger and more reliable due to
the same amount of copper being deposited in the hole barrel
as on the surface. This is particularly important on PTFE
materials, which have a large thermal expansion in the Z
direction.
iii) The elimination of Sodium etching that is normally used
on PTFE materials, this saves time, cost and our environment.
Testing and Verification
Quality System AS/NZS ISO 9001:2008 compliant.
Underwriters Laboratories (UL) Approval File Number
EI24884. IPC-A-600 Trainer on staff, all Inspectors are
IPC-A-600 Certified Specialists. Compliance certification is
available on request.
Please visit our website to see our latest stock list.
www.lintek.com.au
Lintek Pty Ltd, 18-20 Bayldon Road, Queanbeyan NSW 2620. Australia Tel: +61 2 6299 1988 Fax: +61 2 6297 6958 sales<at>lintek.com.au
siliconchip.com.au
Near perfect side wall
resolution and minimal
undercut.
Strong plated through
holes, Copper on the surface and through the hole
is the same thickness.
ISO9001:2008
UL Approval
September 2014 63
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Understanding CO
How, When, Where and Why they’re used
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You may not realise it but many, if not most, PCBs these days have a
conformal coating. But what is that – and what is its purpose?
C
onformal coatings are thin
polymeric films which cover and
protect solder joints, the leads of
electronic components, exposed tracks
and other metallized areas on PCBs
from corrosion.
Humidity, condensation, salt-spray,
corrosive gases or a combination of all of
these activate the start of the corrosion
process, which can be accelerated by
residues from soldering and other assembly processes prior to coating.
There are many conformal coating
chemistries available and each have their
own benefits and drawbacks. Conformal
Coatings are available in solvent-based,
water-based and 100% active materials
(nearly everything that is applied in liquid
form is converted into solid protective
coating), as well as vapour deposited
coatings.In these, gases are mixed in a
vacuum, where they are polymerized and
deposited onto the surface of the PCB
as a protective film.
The primary benefits and disadvantages of the different chemistries available
can be summarised as follows:
Coating Standards
Most conformal coatings are either
qualified to MIL-I-46058C or meet the
Coating Type
Solvent-Based Acrylic
Solvent-Based Urethane
requirements of the closely related
IPC-CC-830B specifications. In addition
they may be recognised by Underwriters
Laboratories, either as a permanent coating, in which case the flammability of the
coating is assessed to UL94V0, or as a
conformal coating, where the electrical
properties will be assessed as part of
the UL746E standard.
The actual protective capability of the
coating in the end use environment is of
greatest concern to the user.
Corrosion
Corrosion is a complicated electrochemical process with a variety of
potential mechanisms and causes, well
beyond the scope of this article. However,
in the vast majority of cases, there are
three requirements that must be fulfilled
in order for corrosion to proceed, as
shown above right.
In order to prevent the possibility of
corrosion, it is necessary to remove one
of the pre-requisite conditions.
The choice of metals is limited to
those used in the solder and solder finish
chemistries (which are often dissimilar)
and there will always be areas of potential
difference in an operating circuit. Cleaning can help remove ionic species, but
In order to obtain the maximum levels
of protection available from the particular chemistry, two key criteria must be
fulfilled:
1. The coating must display excellent
adhesion to the substrate in question
under both dry and highly humid or damp
conditions to prevent delamination.
2. The coating must fully cover the
exposed metal surfaces in order to be
effective as a moisture barrier.
Thus, selecting the ‘correct’ conformal
coating is merely the first stage in the
protective process. Perhaps of greater
importance is the preparation prior to
coating (eg cleaning) and the actual ap-
Primary Disadvantage(s)
Ease of use
Fast Drying
Good general purpose protection
Easy rework
Poor solvent-resistance
High Volatile Organic Compound emissions
Adhesion unpredictable
Ease of use
Better chemical resistance
High Volatile Organic Compound emissions
Harder to rework
Excellent High and Low Temperature performance
Excellent protection against liquid water
Low odour, easy to use
64 Silicon Chip
Application Process
Primary Advantage(s)
Silicone Chemistry
UV curable
cannot prevent the re-deposition of ionic
species from the operating environment.
Conformal Coatings help prevent the
formation of electrolytic solutions by acting as moisture barriers. The coating must
have good adhesion to the substrate to
prevent delamination. Once the coating
is delaminated, moisture can eventually collect in this ‘pocket’ and form an
electrolytic solution with any pre-existing
ionic contamination. This is the reason
that cleaning prior to conformal coating
is recommended.
Low VOC emissions
Fast-curing
Reduced Work In Process (WIP)
Porous to moisture vapour
Less protection against corrosive gases
Silicone cross-contamination
Can have high VOC emissions
More sophisticated process
Harder to rework
siliconchip.com.au
ONFORMAL COATINGS:
by Phil Kinner
Technical Director, Electrolube
plication process itself. Conformal coating materials are not intelligent; they go
where they are placed.
Most materials will tend to slump away
from sharp component edges, leads
and solder joints due to gravity, and this
behaviour can be made worse by longer
drying times and also by baking, if the
initial viscosity drop is greater than the
increase due to solvent evaporation. It is
also extremely difficult to achieve good
coating coverage on the backsides of
leads. Understanding and controlling this
behaviour, and its effect on the conformal
coating coverage, will be key to the performance of coated assemblies operating
in harsh environments.
Therefore, the process by which the
conformal coatings are applied, and the
workmanship and control within that
process, will have the greatest influence
on the success or failure of that particular
coated assembly.
Conclusion
Understanding that the conformal
coating can only protect the surfaces to
which it is applied with perfect coverage,
and that voids, bubbles and cracks in
the coating are likely to present a highprobability corrosion initiation site, is a
major step towards developing a reliable
product.
Choosing a suitable conformal coating
chemistry that can withstand the expected environmental challenges whilst still
Fig.1 – required conditions for
corrosion of a printed circuit board.
yielding acceptable performance levels
is the next step.
But ensuring that the material can be
combined with an application process
that gives a suitable level of defect-free
coverage, is consistent, repeatable and
yields the required levels of performance
is the ultimate step towards ensuring a
high-reliability product.
10
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75
25
5
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siliconchip.com.au
EL_AU_181x120mm_Conformal Coatings_07204_prepress
September 2014 65
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R
U Pushbutton
Crazyflie – DIY Nano Quadcopter
for harsh
environments
APEM have released the IA series
of pushbutton switches designed for
harsh environments. The pushbuttons are
highly resistant to salt spray, frost, sand
and hydrocarbons and are rated at IP67 above panel. The
polyurethane membrane is UV resistant and is press fitted onto the bushing, ensuring high resistance to ingress.
The actuator provides a positive tactile feedback even if
the operator is wearing gloves.
The maximum current and voltage rating into a resistive
load is 2A and 24VDC with an electrical life at full load
tested to 1 million operations. The total travel of the actuator is 1.5mm with a typical operating force of 7N. Electrical functions are N/O or change over and flying leads are
supplied as standard. The case is supplied only in black
but the actuator colours can be blue, black, green, yellow,
red, white or orange.
For further information contact Control Devices on stand
D29 at Electronex 2014, or via www.controldevices.net
Tel 1800 266 876.
Ever wanted a development kit that flies? Well
now you can! The
Crazyflie is an open
source nano quadcopter kit designed
for flexible development and hacking. It’s
among the smallest in the world, weighing only 19 grams
and measuring 90mm motor to motor.
There is a 2.4GHz radio chip onboard which is used for
receiving commands and sending telemetry data back
to the USB RF Module (included) on the host computer.
All you need is a PC compatible joystick and micro-USB
cable for charging (both sold separately).
This nano quadcopter was designed with development
in mind and has an expansion header and backed with
good software support. The platform is open source, which
means schematics, firmware and source code are available
for customisation, or even just to check out how it ticks.
This kit requires partial assembly, some soldering skills
and is not for absolute beginners.
Contact: Core Electronics Pty Ltd Website:
www.core-electronics.com.au
Taking the burden out of prototyping
Embedded Logic Solutions Pty Ltd has been a supplier
of quality tools for embedded system development and
prototype assembly for over ten years.
Teaming up with leading names like LPKF and Number
One Systems, the company provides cost effective in-house
PCB production and SMT board assembly solutions for
prototype applications.
Understanding the fast turnaround importance for PCB
prototyping and the challenges faced with outsourcing or
in-house manual component placement, Embedded Logic
Solutions now distributes the complete range of SMT assembly solutions, from German manufacturer, Mechatronic
Systems, offering customers an end-to-end, cost effective
prototyping line, in-house.
Going beyond boxed solutions, the company is considering a PCB routing and assembly service for proof-of-concept
and prototype boards.
The service, soon to start as a pilot project, will target
companies, professional designers and amateurs and will
include component sourcing if required. For further information on this service and other prototyping solutions,
please contact us by phone or via website.
Embedded Logic Solutions Pty Ltd are on stand D12 at
Electronex 2014; otherwise you’ll find them Suite 2, Level
3 144 Marsden St, Parramatta NSW 2150 Tel: (02) 9687
1880 Web: www.emlogic.com.au
NUMBER ONE SYSTEMS
THE WORLD BEATING PCB DESIGN SOFTWARE
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even more remarkable
value for money and
sets the new benchmark
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PCB CAD.
Easy-PC features
• Hierarchical SCM Design
• Star/Delta points
• Layout patterns and groups
• Design calculators
• Electrical rules check (ERC)
• Panel Editor
• Full and Split Powerplanes
• Design analyser feature
• Plus many more exciting features...
You can also download a trial version from www.NumberOne.com
Call us today... +61 2 9687 1880
530
$
FROM O
NLY
+GST
Embedded Logic Solutions Pty Ltd Email | sales<at>emlogic.com.au | www.emlogic.com.au
66 Silicon Chip
siliconchip.com.au
“Rigol Offer Australia’s Best
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Power Supply
Spectrum Analyser
RIGOL DP-832
RIGOL DM-3058E
9kHz to 1.5GHz
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Triple Output 30V/3A & 5V/3A
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USB Device, USB Host, LAN & RS232
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Buy on-line at www.emona.com.au/rigol
Sydney
Tel 02 9519 3933
Fax 02 9550 1378
Melbourne
Tel 03 9889 0427
Fax 03 9889 0715
email testinst<at>emona.com.au
siliconchip.com.au
Brisbane
Tel 07 3275 2183
Fax 07 3275 2196
Adelaide
Tel 08 8363 5733
Fax 08 83635799
Perth
Tel 08 9361 4200
Fax 08 9361 4300
EMONA
web www.emona.com.au
September 2014 67
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Need solder paste stencils?
Mastercut Technologies now
manufactures DEK Stencils in Australia
Mastercut Technologies is now
licensed by DEK Singapore to manufacture DEK VectorGuard stencils, as
well as supply new frames.
The DEK VectorGuard Framing System is an automatic tensioning system
for solder paste stencils. It eliminates
the need for complex alignment procedures and is independent of traditional
pneumatic assistance processes.
The stencils feature an extruded
aluminium guard, which is securely
attached to the edge of the foil using
interlocking plastic corners. Providing
accurate and automatic tensioning, it
takes only seconds to mount a foil into
the VectorGuard frame.
Mastercut will be launching the
DEK VectorGuard Framing System in
Australia, at Electronex in September
this year. This comes after the launch
of the LPKF ZelFlex System in 2013,
also by Mastercut.
68 Silicon Chip
With over 20 years experience,
Mastercut is the only solder
paste stencil manufacturer
in Australasia and pride
themselves on providing
the highest quality stencils
and fast turnaround.
Mastercut Technologies Managing Director,
Mr Jim Cove, explained,
“All of our stencil customers demand guaranteed high precision and fast delivery, in order to meet
their forever tight deadlines”.
“We use German laser cutting technology which has been specifically
designed to manufacture stainless
steel SMD solder paste and adhesive
stencils, for a consistent high quality
cut and excellent paste release”, Mr
Cove Said.
Both VectorGuard and ZelFlex systems provide superior tensioning and
result in a reduction of stencil storage
space by up to 75% compared to traditional mesh mounted stencils, as well
as being more cost effective to freight.
Visit Mastercut at stand A15 at Electronex in Sydney, 10-11th September
to see both the VectorGuard and ZelFlex frames first hand.
Alternatively, you can contact Mastercut Technologies at 22 Leda Drive,
Burleigh Heads QLD 4220, Tel. (07)
5576 1900; website www.mastercut.
com.au
siliconchip.com.au
Juicy fruit... get more
Raspberry for your money
with the NEW Model B+
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Order code: 2431426
Get yours today at element14
au.element14.com
1300 361 005
nz.element14.com
0800 90 80 80
® Raspberry Pi is a trademark of the Raspberry Pi Foundation
siliconchip.com.au
Visit us at ElectroneX 2014!
10-11 September 2014
Australian Technology Park, Sydney
STAND B11
September 2014 69
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Introducing
Soltronico
Soltronico is a new Australian company
providing a unique blend of high quality, small
volume manufacturing and custom jobs that larger
manufacturing plants ignore. Being local (their plant is
located near Newcastle, NSW), customer service is their
top priority.
Their work includes prototyping, small production runs,
electronic repair and custom re-design of older equipment.
Soltronico are open to discuss any need that you have
requiring an electronic solution.
Give Jose a call at (02) 4911 1124, or check them at
www.soltronico.com.au
FE
SOLTRONICO
Electronic Manufacturing Services
******** Australian owned ********
Customized solutions for your electronic
manufacturing needs !!
Turnkey manufacturing solutions:
* PCB assembly from prototype to production runs
* Custom design
* SMT and through hole to IPC-A-610 requirements
* Wire harness and cable assembly to IPC requirements
* Component parts kitting and supply
* Mechanical chassis assembly
* Test, repair service solutions
Contact Jose Lopez | Operations Manager
e: jose.lopez<at>soltronico.com.au or m: 0422 7000 48
Need prototype PC boards in a hurry?
Mill them yourself!
Satcam’s range of Quick Circuit machines will take your computer
PCB design and turn it into a finished prototype faster than it takes
a courier to deliver one from a bureau!
Gone are the days of messy (and dangerous!) chemicals, film
negatives or positives, a light source and then the clean-up – not
to mention the tedious task of drilling all those holes.
The Quick Circuit takes a blank piece of PCB material, reads the
design (from the vast majority of PCB layout packages) and then
goes to work milling, or if you like grinding, off the areas where
you don’t want copper – the inter-track spaces and even the holes.
Change the bit and even those holes are drilled for you. It’s fascinating to watch the QuickCircuit move over the blank board – but
you don’t even have to stick around watching because the process
is largely automatic. And it can even produce double-sided boards.
The result is a finished PCB ready for component placement
and soldering – it really is that easy.
What about strange shaped boards, cutouts, notches and fitted
shapes for components? No worries – again, with a suitable bit,
the QuickCut will cut any shape required. It will even tell you when
the bit needs changing to achieve these.
And how long?
A typical 300 x 300mm single-sided board will take about an
hour to produce. Compare that with traditional (photo) methods
which don’t have the flexibility of the Quick Circuit Mill.
If you need prototype boards in a hurry, there is only one way
to make them: mill them, with a Quick Circuit from Satcam.
Visit Satcam on www.satcam.com.au or call (02) 9807 7081.
QUICK
Prototype PCBs
With
Quick Circuit
you can
make your
own prototype
circuit boards
and accurately
machined panels
in next to no time
Why isn't
there one on your bench?
SOLTRONICO PTY LTD
Unit 8/9 GEORGE ROAD
Salamander Bay NSW 2317
Phone: +61 2 4911 1124
www.soltronico.com.au
70 Silicon Chip
Web: satcam.com.au
email: satcam<at>satcam.com.au
siliconchip.com.au
Rohde & Schwarz:
German engineered
quality at an
unexpected price.
Established more than 80 years ago, Rohde & Schwarz is a leading
global supplier in the fields of test and measurement, broadcasting, secure
communications, and radiomonitoring and radiolocation.
We help you develop the technologies of the future. Here are our
latest innovations in the field of oscilloscopes and power supplies.
Want to know more?
Visit: www.rohde-schwarz.com/value
NEW
¸HMO1002 Signal Oscilloscope
NEW
¸HMC8041/2/3 Power Supply
sales.australia<at>rohde-schwarz.com
siliconchip.com.au
September 2014 71
B
C
P
F
T
A
E
E
R
U
Keysight Technologies’
New U5855A Handheld
Thermal Imager
With the shift toward predictive maintenance, the
U5855A TrueIR thermal imager allows engineers to
safely and efficiently identify potential faults without
shutting down the systems or disrupting the productivity
of an industrial plant.
The U5855A comes with Fine Resolution capability,
which enhances the quality of thermal images by reconstructing the image based on multiple continuously captured infrared frames. This allows the U5855A to achieve
an effective image resolution of 320 x 240 pixels from a
160 x 120 pixel detector.
With this feature, the U5855A provides four times more
resolution than typical 160 x 120 thermal imagers. Together
with a 4x digital zoom, the U5855A reveals finer details,
especially when inspecting small cracks on industrial
pipelines even from a distance.
The U5855A’s light and ergonomic design allows engineers to comfortably use the thermal imager for longer
periods of time and operate it single-handedly in tight
HAMEG Instruments now carry the
Rohde & Schwarz name
Test and Measurement products from Rohde & Schwarz
subsidiary HAMEG Instruments are now marketed under
the Rohde & Schwarz logo.
The well-known brand name will help improve the
international position of the economical, general-purpose
T&M instruments from HAMEG, which are part of the joint
Value Instruments portfolio.
Previously, all HAMEG products had a dual logo that included the company names Rohde & Schwarz and HAMEG.
According to Roland Steffen, Executive Vice President and
Head of the Test and Measurement Division, “In recent
years, HAMEG has grown rapidly in Europe. Now we want
to expand this growth to other regions. The best way for
this to succeed is with the Rohde & Schwarz brand, which
enjoys an outstanding reputation worldwide. This strategy
clearly sets us apart from other suppliers.”
Using the Rohde & Schwarz logo is also the logical continuation of the Value Instruments initiative, where the two
companies’ portfolios of reliable precision instruments in
the entry-level price segment are marketed together under
the Value Instruments label.
André Vander Stichelen, Managing Director of HAMEG
Instruments, elaborates, “By changing the logo, we want
to underscore the common bond between the two companies. The strategic focus of HAMEG will not change. We
will continue to offer affordable, optimum performance
T&M equipment.”
The company HAMEG Instruments GmbH will continue
to operate as an independent company under the umbrella
of the Rohde & Schwarz group of companies. The two sites
in Mainhausen and Chemnitz will be expanded.
For more information on Value Instruments, visit http://
value.rohde-schwarz.com or call into the Rohde & Schwarz
stand (D2) at Electronex 2014.
72 Silicon Chip
locations. Users can also easily change settings or access
frequently used functions such as torch light and laser
pointer, auto scaling or trigger with quick access buttons.
Keysight Technologies are on stand C11 at Electronex
2014. If the name Keysight Technologies doesn’t ring any
bells, you probably remember them by their old name,
Agilent Technologies. Keysight Technologies Australia is
on stand C11 at Electronex 2014; you can also contact them
via their website, www.keysight.com or call 1800 629 485.
Address is 679 Springvale Rd, Mulgrave, Vic 3170.
Altronics at Electronex
As well as releasing their all-new
2014/2015 product catalog at Electronex 2014 Altronic Distributros
will also be showcasing a selection of their products, including
the ‘latest thing’ – a 3D printer
from Velleman.
Did you ever wanted to create
your own prototype products in
3D? Did you dream that your 3D
creations become real products?
This is your chance to make
it happen with Velleman K8200
printer. It’s a build-your-own
3D printer kit which can print objects up to 200x200x200mm
using PLA or ABS filament 3mm plastic wire.
It’s extremely fast, precise and reliable printer even
when printing at higher speed. The K8200 is compatible
with all free ‘Rep Rap’ software and firmware. It is made
out of aluminium profiles and is easy to assemble; it leaves
room for the user to freely alter the machine and modify it
to their liking. The print bed is heated.
You can convert the Velleman K8200 to be used as a CNC
machine or a Computerised
PCB drilling machine. Create
your own custom designed
one-off PCBs, cut Acrylic
shapes and do much more.
Check the Velleman K8200
out at Electronex, or for further
information and assistance
please call Altronic Distributors on 1300 780 999 or send an
email to: sydwsale<at>altronics.
com.au or refer to their web
site, www.altronics.com.au
siliconchip.com.au
Agilent’s Electronic Measurement Group,
including its 9,500 employees and 12,000
products, is now Keysight Technologies.
Learn more at www.keysight.com
siliconchip.com.au
September 2014 73
Mini-D Stereo
10W/Channel
Class-D Audio
Amplifier
This little chip can deliver
a whopping 30 watts! With
no heatsink!
Main Features
•
•
•
•
•
•
•
•
•
•
•
•
•
•
•
•
•
•
Stereo or mono Class-D amplifier
on a single, small PCB
No heatsink required
Low EMI
DC power supply, wide operating
voltage range
Drives one or two 4-8Ω speakers
Selectable gain
On-board volume control
RCA input sockets
Shutdown mode
Output short-circuit protection
DC offset protection
Over-temperature shutdown with
auto resume
Selectable output power limit with
soft clipping
Low quiescent current
Reversed supply polarity protection
Input signal overload protection
Power and fault indicator LEDs
Under-voltage and over-voltage
lock-out
74 Silicon Chip
This tiny Class-D amplifier module can
work in two modes. In stereo it can deliver
more than 10W per channel or you can
connect its output channels in parallel
to deliver more than 25W into a single
speaker. It is up to 91% efficient, with
selectable gain, volume control and other
features such as a low-power shutdown
mode and over-temperature, over-current,
short circuit and speaker protection.
By NICHOLAS VINEN
H
OW CAN A CHIP this small deliver so much power? And how can it
deliver so much power without needing a big heatsink? The answer to both
questions is Class-D operation. It’s a
switching amplifier and its efficiency
can be over 90%. High efficiency is
also good if you want to run it from a
battery since it will last longer. And if
running from mains, you don’t need
a bulky power supply; a 1A plugpack
should be more than adequate.
We published our first switching
amplifier design, the CLASSiC-D,
in November & December 2012. It’s
a powerful beast, able to deliver up
to 250W into a 4-ohm load or 500W
into an 8-ohm load (bridged) with low
distortion. Lots have been built since
its publication.
But while you may want the high
efficiency of Class-D, the CLASSiC-D is
simply too big and expensive for many
applications where you only need a
few watts of audio, perhaps running
off a small battery – for busking, for
siliconchip.com.au
GVDD
PVCCL
BSPL
PVCCL
PBTL Select
OUTPL FB
Gate
Drive
OUTPL
OUTPL FB
LINP
Gain
Control
PGND
PWM
Logic
PLIMIT
GVDD
LINN
PVCCL
BSNL
PVCCL
OUTNL FB
OUTNL FB
FAULT
Gate
Drive
OUTNL
SD
GAIN0
TTL
Buffer
SC Detect
Gain
Control
GAIN1
PLIMIT
Reference
PLIMIT
Ramp
Generator
Biases and
References
Startup Protection
Logic
AVDD
AVCC
PGND
DC Detect
Thermal
Detect
GVDD
PVCCL
BSNR
UVLO/OVLO
LDO
Regulator
PVCCL
GVDD
Gate
Drive
GVDD
OUTNR
OUTNN FB
OUTNR FB
RINN
Gain
Control
PLIMIT
PGND
PWM
Logic
GVDD
RINP
PVCCL
BSPR
OUTNP FB
PVCCL
Gate
Drive
PBTL
TTL
Buffer
OUTPR
PBTL Select
OUTPR FB
AGND
PGND
Fig.1: block diagram of the TPA3113D2 Class-D audio amplifier IC. The left & right channel differential inputs are
buffered and fed to Schmitt trigger stages where they are compared against a ramp (triangle) signal. The resulting
PWM signals are then fed to PWM logic blocks which then drive two bridge-mode stereo switching amplifiers.
example. Or say you want to build a
pair of self-powered computer speakers. Whatever the reason, a few watts
can go a long way.
That’s where Mini-D amplifier
module comes into its own. It’s based
on the Texas Instruments TPA3113D2
which contains two complete bridgemode stereo switching amplifiers. It’s
so efficient that it doesn’t need a heatsink for normal program material; the
PCB itself dissipates the heat.
Only a simple output filter is required to minimise the amount of RF
interference generated by its switchmode operation. This consists of just
four ferrite beads and four ceramic
capacitors, or eight components for
the two channels. All the components
are surface-mount types, selected
so that they are straightforward to
solder.
Because the Mini-D module’s outputs are bridged, it has good power
delivery even with moderate supply
siliconchip.com.au
rails. With a 12V supply, it can deliver
at least 5W per channel into 8-ohm
speakers or 2 x 10W into 4-ohm loads.
More power is available with higher
supply voltages.
Unusually, the Mini-D can also operate in mono mode, with the outputs
paralleled. This doubles its current
capability, allowing more power into
low-impedance loads, eg, 25W or more
into 4Ω.
By the way, we’ve said this in the
past but it bears repeating: while the
output transistors in Class-D amplifiers spend most of their time either
on or off, they aren’t really ‘digital’
amplifiers. While there may be some
digital circuitry involved, they still
work on the principle of analog negative feedback to generate the correct
output waveform for a given input
signal.
Class-D amplifier operation
We won’t go into the full theory of
how a Class-D amplifier works but let’s
look at the functional block diagram
of the TPA3113D2 IC (Fig.1) which is
the heart of the circuit.
The two inputs are differential.
Looking at the left channel, the signals
are fed to LINP (in-phase) and LINN
(ground/out-of-phase) at top left. The
feedbacks from the switching outputs,
OUTPL FB (positive) and OUTNL
FB (negative), pass through low-pass
RC filters internal to the IC and these
four signals all go into a differential
amplifier which performs this analog
computation:
(LINP - LINN) x GAIN - (OUTPL - OUTNL)
The GAIN setting is determined by
the state of two digital inputs, GAIN0
and GAIN1, which control the resistances in this part of the circuit to select
an effective gain of 20dB, 26dB, 32dB
or 36dB. The output of this differential
amplifier then passes through another
RC low-pass filter, to further attenuate
September 2014 75
Parts List
1 double-sided PCB, code
01110141, 46 x 85mm
4 HI1812V101R-10 ferrite beads,
SMD 4532/1812 (FB1-FB4)
(element14 2292377)
2 PCB-mount switched RCA
sockets, white & red (CON1CON2) OR
2 2-way pin headers plus shielded
cable, header plugs and
chassis-mount RCA sockets
3 2-way mini terminal blocks,
5.08mm spacing (CON3-CON5)
1 3-way pin header, 2.54mm pitch
(CON6)
3 shorting blocks
1 10kΩ dual gang 9mm log
potentiometer (VR1) OR
2 10kΩ mini horizontal trimpots
(VR2-VR3) OR
1 20mm length tinned copper wire
or two component lead off-cuts
3 2-way pin headers, 2.54mm pitch
(LK4-LK6)
3 tapped spacers with M3 x 6mm
machine screws (optional, for
mounting)
Semiconductors
1 TPA3113D2PWP Class-D Audio
Amplifier IC, HTSSOP-28
(element14 1762987)
1 IRFML8244 N-channel Mosfet,
SOT-23 (Q1) (element14
1857298)
1 BSS84 P-channel Mosfet, SOT23 (Q2) (element14 1431318)
the switching artefacts in the signals,
and then into a differential buffer.
During normal operation, with the
output correctly tracking the input
(after gain is taken into consideration),
the output of these amplifiers will be
virtually nil, ie, the two differential
lines will be at the same potential.
Any deviation from this state means
that the amplifier output must swing
one way or the other.
The buffered signal passes through
the PLIMIT block which allows an
external voltage to limit the maximum
output swing, for speaker overload
protection. The signals then pass into
a pair of Schmitt-trigger comparators
where they are compared against a
ramp (triangle) signal, generated by
an internal oscillator.
This is a common method for pro76 Silicon Chip
5 5.6V zener diodes, SOT-23 (ZD1ZD5) (element14 1431238)
2 BAT54A dual Schottky diodes,
SOT-23 (D1,D2) (element14
2114869)
1 high-brightness green LED, SMD
3216/1206 (LED1) (element14
2217905)*
1 high-brightness red LED, SMD
3216/1206 (LED2) (element14
1226389)*
Capacitors (all SMD 3216/1206**
unless stated)
2 100µF 25V low-ESR radial
electrolytics
7 4.7µF 25V X7R ceramic
(element14 1828835)
6 220nF 50V X7R ceramic
(element14 1327724)
8 1nF 50V NP0/C0G ceramic
(element14 2280692)
4 330pF 50V NP0/C0G ceramic
(element14 3606090)
Resistors (all SMD 3216/1206** 1%)
9 100kΩ (element14 1811974)
2 10kΩ (element14 1811973)
2 100Ω (element14 1632521)
5 10Ω (element14 1591420)
2 4.7Ω (element14 2142059)
2 0Ω (element14 1632520) (LK1-3)
* or use 2 x 2-pin headers with offboard LEDs
** SMD 2012/0805 size parts can
also be used
ducing PWM (pulse width modulation), typically used in motor control
circuits. The main difference here is
that the operating frequency is much
higher; around 310kHz. This is necessary to allow accurate reproduction of
audio signals up to 20kHz.
PWM output
These signals then pass through the
PWM logic to the Mosfet gate drivers
and then the totem-pole output stages,
consisting of N-channel Mosfet pairs.
This chip uses a ‘centre-aligned’ or
‘dual-ramp’ PWM, a different modulation scheme to that used in many
other Class-D amplifiers. This is shown
in Fig.2 and is possible because the
TPA3113D2 always operates in bridged
mode. In the quiescent condition, both
outputs are driven in-phase with a 50%
duty cycle (top of Fig.2) and this results
in no current flowing in the speaker(s)
or filter at all.
To drive the output positive, the
duty cycle of the positive output is
increased while the negative output duty cycle decreases (middle of
Fig.2). This is done by shifting both
the leading and trailing edges of both
waveforms. Since none of these edges
line up, this spreads RF emissions out,
making them easier to filter. To drive
the output negative, the reverse condition occurs (bottom of Fig.2).
Since the output transistors are Nchannel Mosfets, a supply above the
positive rail is required for the upper
gate drive. This is generated by four
220nF capacitors between the OUTPL
& BSPL terminals, OUTNL & BSNL etc.
When the respective output is low, its
capacitor charges through an internal
diode from GVDD (~7V) and when the
output goes high, the capacitor charge
maintains the associated boost pin 7V
above that output, sufficient to keep
the upper Mosfet conducting.
The block diagram also shows the
protection circuitry, including shortcircuit detection, output DC offset
detection, high temperature detection and under/over-voltage lock-out.
Should any of these fault conditions
occur, the output drivers are all
switched off. The over-temperature
cut-out kicks in when the die temperature hits 150°C and operation resumes
once it has dropped by around 15°C.
When the chip is running in mono
mode, as set by the PBTL input pin, the
PWM logic is modified slightly so that
OUTPL and OUTNL carry an identical
signal. At the same time, OUTPR and
OUTNR are both driven with the same
out-of-phase PWM signal, allowing the
pairs of outputs to be paralleled.
Speaker wires
Because ‘centre-aligned’ PWM is
used in this chip, only a very simple
output filter is required to minimise
the amount of RF interference generated. This consists of just four ferrite
beads and four ceramic capacitors. The
data sheet states that the ferrite bead
output filter is sufficient for twisted
speaker wires up to 1.2m long. We
imagine that standard figure-8 speaker
wires should also be OK, given that
the conductors are in close proximity.
If you want to use longer speaker
leads or are particularly concerned
about radio interference, you can add
siliconchip.com.au
No output (quiescent)
33µH
OUTP
OUTP
L1
OUTN
33µH
OUTP-OUTN
Speaker
Current
C1
1µF
OUTN
L2
0V
Positive Output
OUTP
C2
1µF
Cutoff Frequency = 27kHz, Speaker Impedance = 8Ω
OUTN
15µH
OUTP
OUTP-OUTN
Speaker
Current
L1
C1
2.2µF
0V
15µH
Negative Output
OUTN
OUTP
L2
C2
2.2µF
OUTN
Cutoff Frequency = 27kHz, Speaker Impedance = 4Ω
OUTP-OUTN
Speaker
Current
0V
Fig.2: the quiescent (top), positive output (middle) and
negative output (bottom) signal waveforms for the TPA
3113D2 Class-D audio amplifier IC.
an external LC output filter. This could
be wired externally to the board, ie,
between the output terminals and
speakers. Note that you would need to
keep the components relatively close
and run some connections to a PCB
ground point.
One disadvantage of this approach
is that the filter component values
must be selected based on the speaker
impedance. Also, the inductors must
handle the peak load current (up to
4A in some cases) without saturating.
The recommended filters for 8-ohm
and 4-ohm loads are shown in Fig.3.
Note that an LC filter may also give
improved efficiency.
Speaker impedance
For supply voltages up to 15V, the
unit can drive speakers with nominal
impedances from 4-8Ω. Above 15V,
however, it isn’t recommended to
drive 4Ω speakers. Plenty of power for
4Ω loads is already available at supply
voltages below 15V anyway.
To drive 4Ω speakers from a supply above 15V, it’s necessary to run
the Mini-D in mono mode; more on
that later. To drive two speakers in
this mode, you will need to build two
boards but in exchange for that, you
siliconchip.com.au
Fig.3: an external LC filter can be added if long speaker
leads are to be used, with the filter component values
selected according to the speaker impedance. These two
diagrams show the recommended values for 8-ohm and
4-ohm loads.
get more power and higher efficiency.
Circuit description
The full circuit is shown in Fig.4.
All the real work is done by IC1. The
left & right channel input signals are
applied to RCA connectors CON1 and
CON2. Alternatively, pin headers may
be fitted in their place for connection
to chassis sockets or another board.
From this point on, we shall refer to
the operation of one channel only.
The signal first passes through a
low-pass RF-rejecting filter, comprising a 100Ω series resistor and 1nF
ceramic capacitor. Both the signal
and ground pins are then AC-coupled
to the volume control potentiometer
(VR1) via 4.7µF ceramic capacitors.
The signal ground is also connected to
power supply ground via a 4.7Ω resistor, taking advantage of the differential
inputs provided by the IC.
This 4.7Ω resistor reduces the
chance of hum being injected into
the signal due to the common input
grounds.
The volume control potentiometer is
either a dual-gang log pot (VR1) or two
horizontal trimpots (VR2 & VR3), the
latter used for a pre-set volume level.
If you don’t need volume control at all,
simply link out VR2 and VR3. Regardless, the wiper of each pot goes to the
non-inverting input for each channel
(pins 3 & 12) while the bottom (ACgrounded) end goes to the inverting
inputs (pins 4 & 11).
The TPA3113D2 can handle a
strictly limited voltage range at each
input pin of -0.3V to 6.3V so we have
added protection components to limit
these voltages when the power is off or
in case a high level signal is applied
(which is common when plugging and
unplugging RCA leads).
These parts consist of 5.6V zener diodes (ZD1-ZD4) and parallel Schottky
diodes (D1 & D2) between each input
and ground. The zener diodes take
care of clamping positive signal swings
while the Schottky diodes clamp negative excursions more effectively.
The outputs of IC1 pass through the
recommended output filter, consisting
of four large ferrite beads (FB1-FB4;
HI1812V101R-10) and four 1nF C0G
ceramic capacitors. C0G capacitors
have a very low temperature coefficient (±30ppm) but also low ESR
(equivalent series resistance) and
ESL (equivalent series inductance);
just what we need to suppress sharp
voltage spikes.
September 2014 77
Speaker impedance: 6-8Ω; 4-8Ω in mono mode or in stereo with up to 16V supply
Power LED1 (green) can either be an
on-board SMD LED or it can be mounted off-board via pin header CON7.
Supply current for LED1 and LED2
is around 1-2mA, so high-brightness
types should be used.
Continuous output power: 2 x 5W or 1 x 10W (12V, 8Ω)
Power supply
Specifications
Supply voltage: 8-25V DC
Quiescent current: typically <40mA active, <2mA shutdown
Peak output power: 2 x >15W or 1 x >30W (thermally limited)
THD+N: typically <0.1%; see Figs.6 & 7
Signal-to-noise ratio: 100dB
Frequency response: 20Hz-20kHz ±1dB; see Fig.9
Efficiency: up to 82% (stereo), 91% (mono)
Gain: 20dB, 26dB, 32dB or 36dB
Under-voltage lockout: ~7.5V
Output offset voltage: typically within ±1.5mV
Power supply rejection ratio: typically -70dB
Switching frequency: ~310kHz
We have also added snubbers, consisting of 330pF C0G ceramic capacitors in series with 10Ω resistors, from
each output to ground. They are actually wired to the boost supply pins but
these are AC-coupled to the outputs
via much larger 220nF capacitors so
the effect is the same. These reduce
radiated EMI further by limiting the
output voltage slew rates.
We have used a 1:1 voltage divider
between GVDD (pin 9; ~7V) and
ground, with a 4.7µF filter capacitor,
to set PLIMIT (pin 10) at 3.5V. This
limits the output amplitude to about
±11V (22V peak-to-peak). Thus it will
only limit the output power with a DC
supply over 20V.
If you are trying to get the maximum
possible power from the chip at 24V,
you could reduce the upper divider
resistor to 47kΩ but in most cases it
won’t make much difference; the ‘soft
clipping’ provided by this limiter may
have some benefits in reduced treble
artefacts if you are going to drive the
amplifier that hard anyway.
Other features
100kΩ pull-ups on GAIN0 and
GAIN1 allow links LK4 and LK5 to
define these input states. A table in
the circuit diagram shows the possible
settings. With a gain of 20dB (10x),
input sensitivity is 425mV RMS for
a 12V supply and 850mV RMS for a
24V supply. With the gain set to 36dB
(63x), input sensitivity is 67mV RMS
for a 12V supply and 135mV RMS for
a 24V supply.
The unit can handle signals up to
78 Silicon Chip
at least 3V RMS. For line-level signal
sources such as CD players, 20dB of
gain should be plenty, so most constructors should stick with that.
The FAULT output (pin 2) is connected to pin 1 on CON6, which can
go to a microcontroller pin (but with
some provisos, see below). It goes
low if the IC detects that an output is
short-circuited or there is a DC offset
fault. The FAULT signal also switches
P-channel Mosfet Q2 via a resistive
divider (which ensures that Q2’s gate
is not over-driven). If there is a fault,
Q2 switches LED2 (red) on. This can
either be an SMD LED mounted on the
board or an external LED wired up via
pin header CON8.
The shut-down input (pin 1) is also
connected to CON6 (at pin 2) and is
pulled up by a 100kΩ resistor so that
the amplifier will power up automatically. If pulled to ground, the amplifier
shuts down and only draws about
250µA. However, that doesn’t include
the current for LED1 and the various
pull-ups, which increase total shutdown current to around 2mA.
If a shorting block is placed on LK6
and an output short circuit is detected,
once the short has cleared, the amplifier will automatically resume operation. Otherwise, short circuit faults are
‘latched’ and the unit remains off (with
LED2 lit) until the power is turned off
and back on again.
Over-temperature faults are automatically cleared and LED2 will not
light if IC1 overheats; rather, output
will simply cease and then resume
once it has cooled.
The 8-25V DC supply (from a battery, plugpack or power ‘brick’) comes
in via terminal block CON3, with
Mosfet Q1 providing reverse polarity
protection. If the supply polarity is
correct, Q1’s gate is pulled positive
via the 100kΩ resistor. This switches
Q1 on, so current from the circuit can
flow back to the supply ground.
However, if the supply polarity is
wrong, Q1’s gate will be pulled negative relative to its source and Q1 will
remain off, so no ground current can
flow and the circuit is protected. Q1’s
drain-source voltage is rated at 25V, so
as long as the DC supply is within the
specified range, this will be sufficient
to block the supply voltage.
Zener diode ZD5 limits Q1’s gate
voltage to a safe level when the supply
voltage is above 20V.
There’s little else to the power supply other than the bypass capacitors,
which consist of one 100µF electrolytic, one 220nF X7R ceramic and
one 1nF C0G ceramic for each pair of
power VCC pins, ie, PVccL (pins 27
& 28) and PVccR (pins 15 & 16). The
analog supply, AVcc, is at pin 7 of IC1
and has a 10Ω/4.7µF RC low-pass filter
to remove switching noise.
IC1’s internal Mosfet gate supply
regulator has a 4.7µF output filter
capacitor at pin 9 (GVDD).
Mono (parallel) mode
To operate in mono mode, LK1 and
LK2 are fitted and LK3 is left out. The
speaker in then connected between
CON4 and CON5 as shown on the
circuit diagram. LK1, LK2 & LK3 are
0Ω surface-mount resistors.
In this case, you can also omit
FB2, FB3 and the two associated 1nF
capacitors. Plus you can omit CON1
and its associated components as the
mono signal is fed into the right input
(CON2).
Note though that you will only
get more power in mono mode (also
known as PBTL or Parallel Bridge-Tied
Load mode) with a low-impedance
speaker, eg, 4Ω. This is because with
higher speaker impedances, you will
run into clipping before the maximum
siliconchip.com.au
siliconchip.com.au
September 2014 79
2
2
1
10k
LOG
32dB
36dB
26dB
K1
VR1a
10k
D2
BAT54A
VR3
10k
K1
A
A
G
5.6V
5.6V
ZD3 A
K
ZD1 A
K
5.6V
5.6V
ZD4 A
K
ZD2 A
K
X7R
4.7 µF
GAIN
0
LK4
100k
10Ω
GAIN
1
LK5
100k
LK6
AUTO RESET
IN
IN
MONO
LK2
OUT
LK1
OUT
MODE
STEREO
OUT
IN
LK3
STEREO/MONO MODE LINKING
K2
K2
100k
100k
‘MINI–D’ 10W X 2 CLASS D AMPLIFIER
OUT
LOG
VR1b
10k
K
λ
A
D1
BAT54A
VR2
10k
10k
FAULT
LED2
D
S
Vcc
GND
X7R
4.7 µF
100k
X7R
4.7 µF
100k
X7R
A
ZD1- ZD4
K
100k
10
11
12
9
6
5
4
3
14
7
1
2
C0G
1nF
A
CATHODE
BAND
220nF
* EITHER DUAL LOG POT VR1 OR
TRIMPOTS VR2 & VR3 ARE FITTED;
THE LATTER FOR PRESET VOLUME
STEREO
LK3
100k
FAULT LOW ESR
100 µF
25V
SHUTDOWN
CON6
DIAG
27
15
BSPL
16
BSNR
OUTNR
OUTPR
BSPR
BSNL
OUTNL
OUTPL
PVccR
IC1
TPA3113D2
28
LEDS
K
8
0
K1
24
K2
BAT54A
19
AGND PAD PGND PGND
PLIMIT
RINN
RINP
GVDD
GAIN1
GAIN0
LINN
LINP
PBTL
AVcc
SD
FAULT
PVccL
A
21
20
18
17
22
23
25
26
X7R
330pF C0G
FB4
FB3
330pF C0G
330pF C0G
FB2
FB1
330pF C0G
LOW ESR
100 µF
25V
A
K
10Ω
1nF C0G
1nF C0G
10Ω
10Ω
1nF C0G
1nF C0G
10Ω
ZD5
5.6V
G
100k
G
S
D
IRFML8244, BSS84
PAD
UNDER
28
S
D
1
–
–
+
1
CON5
–
+
RIGHT
SPEAKER
2
DC
14
SPEAKER
CONNECTION
IN MONO
MODE
CON4
2
1
LEFT
SPEAKER
Q1
IRFML8244
CON3
1
POWER IN
2
+ 8–25V
TPA3113D2
NOTE: FB1–FB4 ARE HI1812V101R-10 SMD
FERRITE ‘BEADS’ (1812 SIZE, 8A RATED)
X7R
220nF
LK2
MONO
X7R
220nF
X7R
220nF
LK1
MONO
X7R
220nF
220nF
C0G
1nF
Vcc
Fig.4: the complete circuit diagram of the Mini-D 10W x 2 Class-D Amplifier. The audio input signals are fed in via CON1 & CON2, filtered and fed to the LINP
(pin 3) and RINP (pin 12) inputs of IC1 via dual-gang volume control VR1. The amplified outputs appear at pins 25 & 23 (left channel) and pins 18 & 20 (right
channel) of IC1 and these drive the left and right speakers via ferrite bead/capacitor filter networks. Links LK1-LK3 select either mono or stereo operation (see
table), while links LK4 & LK5 set the gain. Mosfet Q1 provides reverse polarity protection, while Mosfet Q2 drives the fault indicator LED (LED2).
SC
20 1 4
IN
OUT
OUT
IN
LK5
IN
OUT
4.7 µF X7R
4.7 µF X7R
4.7 µF X7R
4.7 µF X7R
K
Q2
BSS84
GAIN
20dB
POWER
λ LED1
LK4
IN
4.7Ω
C0G
1nF
(MONO INPUT)
RIGHT INPUT
CON2
100Ω
C0G
1nF
100Ω
4.7Ω
CON1
LEFT INPUT
CON8
K
A
(LED2 WHEN
OFF PCB)
CON7
A
K
1
(LED1 WHEN
OFF PCB)
A
100k 220nF
4.7 µF
0
+
LK3
STEREO
100 µF
(LK1)
10Ω
FB2
FB3
220nF 220nF
1nF 1nF
330pF
1nF
220nF
Lout
CON4
1nF
330pF
10Ω
FB1
1nF
CON5
4.7 µF
100k
330pF
10Ω
(LK2)
D2
ZD4
100k
IC1
TPA3113D2
LK5
LED1
LK4
LED2
1nF
4.7 µF
10Ω
Q1
10Ω 330pF
FB4
+
VR1
220nF
220nF
100k
100k
(VR3)
ZD5
–
100 µF
LK6
+
CON2
100Ω 4.7 µF
10kΩ + 10kΩ LOG
POWER
CON3 100k
G
CON6
S
100k
A 4.7 µF A
1nF
F
ZD2
ZD1
1nF
100Ω 4.7 µF
10k
10k
4.7Ω
Rin
100k
(VR2)
–
Right in
100k
–
CON1
ZD3
Lin
D1
4.7Ω 4.7 µF
Q2
Left in
Rout
INSTALL DOTTED LINKS AT VR2 & VR3
FOR FIXED VOLUME ONLY – SEE TEXT
NOTE: INSTALL LK3 (0 Ω) FOR STEREO. OMIT LK3 & INSTALL LK1 & LK2 FOR MONO
Fig.5: follow this parts layout diagram to build the Mini-D amplifier. You can either install
potentiometer VR1 or trimpots VR2 & VR3 for volume control (see text). Alternatively, leave
all these parts out if no volume control is required and link out VR2 & VR3 as indicated.
output current becomes the limiting
factor. With a 4Ω speaker at 15V in
mono mode, output power is up to
30W, which is pretty good! Even if
you don’t need the extra power, it’s
preferable to use the module in mono
mode as it improves efficiency.
24V battery operation
Since the maximum recommended
operating supply voltage for IC1 is 26V
and there are a number of 25V-rated
components in the circuit, we don’t
recommend running directly from a
24V battery. In theory, if you increased
the voltage ratings of the 25V capacitors and Mosfet Q1, you might get away
with it as the absolute maximum specified for IC1 is 30V. But it’s outside the
recommended operating voltage range
so we don’t suggest doing that.
A better option is to use a 24V lowdropout pre-regulator, eg, by placing
a 12V zener diode in series with the
ground pin of an LM2940CT-12 regulator to ‘jack it up’ to 24V. You will need
appropriate input and output filter
capacitors. The LM2940 is only rated
at 1A but is unlikely to run into current
limiting during normal operation. It
may need a small heatsink though, as
it could dissipate up to 5W.
PCB layout
Being a switching amplifier, instantaneous currents can be high and the
voltage rise/fall times are very short,
so the the design of the PCB has been
quite rigorous. We also wanted to keep
switching noise away from the analog
circuitry. Bypass capacitors need to
be near IC pins and the output filter
must be kept tight for maximum EMI
suppression. There are also thermal
considerations, given that the amplifier
80 Silicon Chip
IC uses the board as a heatsink.
We’ve placed ground planes on both
the top and bottom of the board immediately under IC1 and fanned them out
to the full width of the board. There are
15 vias placed directly under the IC,
on and around its thermal pad, both
to reduce ground impedance for better performance and to help conduct
heat from the IC to the bottom side of
the board where it can be effectively
radiated away.
The 1nF and 220nF bypass capacitors are immediately adjacent to the
IC, with the 1nF C0G types the closest,
as they have the best high-frequency
performance. The placement of the
100µF electrolytics is less critical. Note
that there is provision to use 22µF 25V
SMD multi-layer ceramic capacitors
(1812 size) instead but the cheaper
electros do the job well.
The IC’s pin layout is well-optimised, with the main power supply
and all output related pins on one side,
which we have orientated towards the
right side of the PCB. Thus the filter
components are placed immediately
between the IC and CON4/CON5 at
right. The analog ground pin (pin 8) is
on the left side of the IC and this is the
only point at which the power ground
meets the signal (analog) ground.
Construction
Fig.5 shows the assembly details.
Apart from some of the components
being relatively close together, the only
tricky thing about building this board
is soldering IC1 (a magnifying lamp
will come in handy here).
We used hot-air reflow as this (or
oven reflow) is best for ICs with thermal pads (like the TPA3113D2). The
equipment is surprisingly cheap; we
paid around $60 for an Atten 858D+
hot-air soldering station while hot-air
reflow wands can be had for as little as
$25. But you can do it with a regular
soldering iron too.
For hot-air, the trick is to use a very
thin layer of fresh solder paste (kept
in the fridge!). Spread this sparingly
on the pads, drop the IC on top, heat it
(gently at first) until all the pins reflow
and then for a few seconds longer and
Bob’s your uncle.
If all you have is a regular iron, apply
some no-clean flux paste to the thermal
pad on the board and also the pad on
the bottom of the IC. Then melt a small
amount of solder to both; just enough
to tin them. Start with the PCB pad
so you can get an idea of the correct
amount. If you add too much, add a bit
more flux and then remove the excess
with some solder wick (harder to do
with the IC!).
Having tinned both, place some
fresh flux paste on all the IC pads
on the PCB, including the thermal
pad, then pop the IC down in place,
checking its orientation. Next, move it
slightly out of the way, tin one small
corner pad and then slide the IC into
place while heating that pad.
Now check that the IC lines up with
all its pads. If it’s misaligned, reheat
and gently nudge it into place. Try to
avoid getting solder on any other pads
Use a magnifying glass (or magnifying lamp) to check carefully that all
the pins are sitting properly over their
pads, then tack down the diagonally
opposite pin. Re-check the alignment,
then solder the rest of the pins, making
sure not to disturb either of those first
two solder joints.
Having soldered the pins, it will
then be necessary to flip the board over
siliconchip.com.au
and apply enough solder to the pad
on the bottom to transfer heat through
the vias. Heat this solder until the flux
between the IC and board vapourises,
indicating that the thermal pad has
reflowed. This will take a good few
seconds but don’t overdo it as you
could cook the chip.
Regardless of which method you
used to solder the IC, check carefully
for bridged pins (again, use a magnifying glass) and clean up any that look
dodgy up with some flux paste and a
clean piece of solder wick. The bridges
should clear easily; press the wick
down onto the board but not over the
IC pins as they are small and easily
damaged.
As a final measure, it’s a good idea
to clean the flux residue off the board
using a specialised flux cleaner (or in
a pinch, an alcohol or acetone) and
then carefully check all the soldering,
again with a magnifying glass. Check
that all the bridges are gone and that
the solder has flowed cleanly onto all
the pins and pads.
Remaining parts
There are nine SOT-23 package
transistors, diodes and zener diodes to
solder. These are quite easy as the pins
are well spaced but don’t get the various device types mixed up. Start with
Q1 and Q2, then solder D1 and D2 and
finally the five identical zener diodes.
The easiest method is to put a bit of
solder on the central pad and slide the
device into place while heating that
pad. Then solder the other two pads (a
dab of flux paste makes it easier) and
refresh the first.
Now move onto the SMD passives,
starting with the resistors and then
the capacitors and ferrite beads. Use
siliconchip.com.au
Mini-D THD+N vs Power
08/12/14 13:27:27
Filter: AP AUX-0025 + 20Hz-80kHz bandpass
Total Harmonic Distortion + Noise (%)
5
2
1
0.5
4Ω+47µH <at> 15V
0.2
0.1
8Ω+47µH <at> 18V
4Ω+47µH <at> 12V
0.05
8Ω+47µH <at> 12V
0.02
0.01
0.1
8Ω+47µH <at> 14.4V
Solid = Stereo mode
Dashed = Mono mode
0.2
0.5
1
2
5
10
20
Power ( W atts)
Fig.6: distortion versus power for a range of load impedances and supply
voltages. Performance is generally better for 8Ω loads but power delivery is
higher into 4Ω. Note the test load series inductance, to simulate loudspeakers.
10
Mini-D THD+N vs Frequency
08/12/14 13:28:51
Filter: AP AUX-0025 + 20Hz-80kHz bandpass
5
Total Harmonic Distortion + Noise (%)
Left: the completed
PCB assembly. Don’t
be intimidated by the
SMD parts; they’re
quite easy to install
if you follow the
instructions in the
text but you do need
a good magnifying
glass (or magnifing
lamp), tweezers and a
soldering iron with a
small chisel tip.
10
2
1
0.5
0.2
4Ω+47µH <at> 12V, 1W
0.1
0.05
8Ω+47µH <at> 12V, 1W
0.02
0.01
20
50
100
200
500
1k
2k
5k
10k
20k
Frequency (Hz)
Fig.7: distortion versus frequency at 1W. As usual, the distortion rises with
frequency but it also rises at the low end due to coupling capacitor-induced
distortion. It’s below 0.1% between 40Hz and about 1.5kHz.
a similar method as for the SOT-23s.
The main thing to check for with these
parts is that the solder has flowed onto
the pad and not just the end of the
component. As before, adding flux
smoothes solder flow.
Note that the resistors will have
printed values on them but the capacitors and ferrite beads will not,
so check the packaging before fitting
them. Remember to fit either 0Ω resistor LK3 only (stereo mode) or LK1 and
LK2 only (mono mode).
If using the SMD LEDs, they can
September 2014 81
V+
VCC
CON3
+
S1
K
K
A
A
−
(OPTIONAL CLAMP DIODES)
MICROCONTROLLER
1
1k
2
470nF
1
FAULT
POWER
10Ω
SHUTDOWN
2
100 µF
25V
MINI-D
3
MINI-D
FAULT
SHUTDOWN
3
GND
CON6
GND
CON6
B: START-UP DELAY & SHUTDOWN WITH A SWITCH
A: CONNECTING A MICROCONTROLLER TO THE MINI-D
Fig.8(a): the shutdown pin (pin 2) of CON6 can be pulled low under no-signal conditions (eg, using a microcontroller)
to reduce power consumption. The RC filter shown provides slew rate limiting, while external clamp diodes may also
be required with some micros (see text). Fig.8(b) at right shows how to add a capacitor (eg, 100μF) to give a switch-on
delay, while a DPDT power switch (S1) can be used to eliminate switch-off clicks or pops.
go in next but first you will have to
check their polarity. Unfortunately,
markings are inconsistent so use a
DMM in diode test mode and try connecting the probes both ways around.
When the LED lights, the red probe is
to the anode and this goes towards the
bottom of the PCB (marked with “A”).
We used a green LED for LED1 and a
red LED for LED2.
Through-hole components
That’s it for the SMDs so once
you’re confident that they’ve all been
+3
soldered correctly, there are just a few
through-hole parts left. If you aren’t using an on-board volume control, solder
wire links in place of VR2 and VR3
where shown. Also, if using off-board
LEDs, fit 2-way pin headers CON7 and
CON8 in place of the LEDs.
Next, move on to links LK4-LK6,
CON6 and the inputs (if you aren’t fitting RCA sockets). That done, dovetail
two screw terminal blocks together
and solder them in place for CON4
& CON5 (wire entry holes facing outwards). CON3 can then go in.
Mini-D Frequency Response
08/12/14 12:39:04
Filter: AP AUX-0025 + 80kHz lowpass
+2.5
+2
Amplitude Variation (dBr)
+1.5
+1
+0.5
+0.0
-0.5
-1
-1.5
Set-up & testing
Initially, fit LK4 and LK5 (note that
they go in vertically) and LK6. Turn
the volume pot(s) to minimum, then
apply DC power to CON3 (say, 12V)
and measure the current. It should
be just under 40mA (but possibly as
high as 55mA) and LED1 should be on
while LED2 should be off. If anything
is wrong, switch off immediately and
check for faults. Also double-check
that you have connected the supply
wires with the correct polarity.
Assuming that all is OK, switch off
and connect a signal source such as a
CD player, MP3 player, oscillator or
mobile phone. Connect the speaker(s),
then switch back on and slowly turn
the volume up. It’s now just a matter
of making sure it sounds right. If you
get to maximum volume and it’s still
too quiet, switch off and increase the
gain by changing LK4 and/or LK5 but
remember to turn the volume down
before re-applying power.
Shutdown control
-2
-2.5
-3
If you are using onboard volume
control pot VR1, fit it now (or trimpots
VR2 & VR3). RCA sockets CON1 &
CON2 can then go in, followed by the
electrolytic capacitors (take care with
their orientation).
20
50
100
200
500
1k
2k
5k
10k
20k
Frequency (Hz)
Fig.9: the amplifier’s response is effectively flat in the audible frequency range.
There is a low-frequency roll-off due to the high-pass filter formed by the
input coupling capacitors and volume pot, while the rise at the high end can
be attributed at least partially to the inductance of our test load.
82 Silicon Chip
To reduce power consumption
when power is applied but no signal
is present, you can pull the shutdown
input (pin 2 of CON6, pin 1 of IC1) low
to enter a power-saving state. However,
there are a couple of provisos.
First, the data sheet specifies that
this pin should be slew rate limited to
10V/ms unless the source impedance
siliconchip.com.au
SIGNAL HOUND
USB-based spectrum analyzers
and RF recorders.
The TPA3113D2 IC (circled) should be installed first, following the procedure
described in the text. The photo above right shows the corresponding heatsink
area for this IC on the back of the PCB. It’s connected to a thermal pad on the
top of the board by 15 vias.
This larger-thanlife-size view shows
the heatsink pad on
the underside of the
TPA3113D2 Class-D
audio amplifier IC.
is at least 100kΩ but it doesn’t say why.
Confusingly, they also show sample
circuits where a “control system” (eg, a
microcontroller) drives the shutdown
pin via just a 1kΩ series resistor, which
is unlikely to limit the slew rate to their
specification.
We would be tempted to try that but
not knowing the reason for the limitation, a safer approach would be to
add an RC filter, as shown in Fig.8(a).
The same comments apply if you’re
going to use a switch, relay, transistor
or something else to pull down the
shutdown pin.
If connecting a micro in this manner,
note that the on-board pull-up resistor
could pull its control pin above the
micro’s supply voltage. Normally, the
microcontroller pin will have a clamp
diode to its positive supply rail to limit
the voltage on that pin to a safe level.
However, some micros lack a positive
clamp diode (eg, 5V-tolerant pins on a
3.3V micro) and in that case, you will
need to add an external clamp diode
(or a low-voltage zener to ground) to
protect the micro – see Fig.8(a). The
situation is the same if connecting the
FAULT signal to a micro.
Powering up & down
We didn’t hear any clicks or pops
or run into other issues when powering the Mini-D up or down normally
but there are a couple of issues noted
in the data sheet which constructors
should be aware of.
If the signal source is powered up
at the same time as the Mini-D and
there are large initial transients on
those signals, that could trigger the
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Thermometer for
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AM/FM/SSB/CW demod
USB 2.0 interface
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Another view of the completed PCB
assembly. Links LK1-LK3 have been
configured for stereo operation; ie,
LK1 (0Ω) in, LK2 & LK3 out.
DC offset protection in the Mini-D
and once that’s activated, its outputs
will remain disabled until the power
is switched off and on again. So in that
case you need to hold shutdown low
until the audio signals stabilise. This
can be achieved with a capacitor between the shutdown pin and ground.
A 22µF capacitor will give a switch-on
delay of around 100-200ms, a 100µF
500-1000ms and so on. Or if a micro
is connected to shutdown, it can do
the same job.
The data sheet also states that
pulling shutdown low before power
is removed will minimise clicks or
pops. While not strictly necessary, this
can be achieved using a DPDT power
switch; see Fig.8(b). This will bring
shutdown low almost immediately
while the supply capacitors take some
SC
time to discharge.
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The BB60C also adds new
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configurable I/Q.
Streaming bandwidths
which will be retroactively
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also available.
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Wagga Wagga NSW 2650
Ph: (02) 6931 8252
contact<at>silvertone.com.au
September 2014 83
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.
REG1 LM3940 -3.3
+3.3V
OUT
GND
47 µF
TANT
28
+
IN
5V DC
INPUT
–
100nF
+5V
A
1
13
SSR3
20
47 µF
TANT
A
MICROMITE
N
SSR2
19
A
N
SSR1
LIGHTS 2
λ
14
8
LIGHTS 3
λ
2
5.6M
AC
INPUT
λ
16
15
100nF
N
A
LIGHTS 1
N
SSR1–3: FSS1-1022
LM3940IT
Micromite-based controller for
230VAC LED downlights
I have recently added a couple of
LED downlights to my living area to
improve the lighting when someone
wants to read or work. Unfortunately
though, these are far too dazzling
for those for us who want to watch
television. I did not want to go to
the effort or expense of wiring in
additional switches for each light
but wanted to be able switch on any
combination of lights.
This circuit is based on the Micro
mite (see May-August 2014 issues)
and allows you to set any combination of lights using a single light
switch which feeds power to the
Micromite. The Micromite controls
three solid-state relays (SSRs) and
these provide the 230VAC switching
of the downlights.
Power to the Micromite is supplied by a 5V mobile phone charger.
They are readily available but avoid
using cheap ones from China which
do not have the required shrouding
GND
IN
GND
OUT
and sleeving of the two 230VAC
pins. An LM3940 3-terminal regulator provides 3.3V for the Micromite.
When you apply power, only
the lights that were last on will be
switched on. If you turn the switch
off, wait for around one second,
then switch it back on again, it goes
into program mode, which will then
cycle through each combination,
with a 3-second pause between
each change. If you then turn it off,
it will save the current setting in
the Micromite’s EEPROM and then
use that setting whenever you turn
it back on. It’s necessary to wait for
three seconds before turning it back
on immediately after saving the
new setting, to avoid triggering the
program mode again.
Most of the hard work is done by
the Micromite controller with a short
BASIC program. The circuit includes
a resistor/capacitor combination at
pin 2 which is used to determine if
Issues Getting Dog-Eared?
the lights should come on normally
or if the device starts in program
mode.
When the program starts, it reads
the voltage on the capacitor and if
the voltage is 0.8V or higher (set in
line 22), it goes into program mode.
Once the voltage is read, it outputs
3.3V on pin 2 to charge the capacitor.
When the power is switched off, the
capacitor is discharged through the
5.6MΩ resistor.
The solid-state relays are switched
by 5V-tolerant open-collector outputs on the Micromite. You can add
more lights to the system by using
other 5V-tolerant pins or using an
external transistor on a normal digital output.
You can set the sequences for all
the lights by entering values in the
Data statements in lines 5-7 of the
program and setting Num (line 4) to
the number of values plus 1. Make
sure the last values of each sequence
are 0. This is used by the program
to turn off all the loads when the
EEPROM is written to. This minimises the load from the power supply, ensuring the program has plenty
of time to write to EEPROM.
Suitable solid-state relays can be
purchased from Jaycar (Cat. SY-4080)
or Altronics (Cat. S-4410). Note that
the load current to be switched must
be less than the rating of the SSR.
Note also that all mains wiring must
be done to Australian/NZ standards.
Testing revealed a problem when
using CFL lamps with the solid state
relays, as they would flash occasionally. This can apparently occur with
solid state relays but is not a problem
with other types of lamps and can be
fixed by having a normal incandescent lamp in parallel with the CFL.
The software, LEDSwitch.bas, is
available on the SILICON CHIP website.
Dan Amos,
Macquarie Fields, NSW. ($50)
Keep your copies safe with our handy binders
Order online from www.siliconchip.com.au or fill in and mail the handy order form in this issue or ring (02)
9939 3295 and quote your credit card number.
84 Silicon Chip
siliconchip.com.au
Measuring the frequency output of the
Induction Motor Speed Controller
9V OR 12V
AC PLUGPACK
TO INDUCTION
MOTOR SPEED
CONTROLLER
OUTPUT SOCKET
10k
230V
9 – 12V
100nF
TO FREQUENCY
METER OR
OSCILLOSCOPE
Above: this simple circuit allows the frequency output of the
Induction Motor Speed Controller to be safely measured.
A number of readers have requested a simple method of reading
the output frequency of the Induction Motor Speed Controller (SILICON CHIP, April, May and December
2012). This is needed as part of the
initial set-up procedure. As it happens, there are two simple ways of
doing this.
The first requires that the lid is
removed so that you can access the
ICSP socket adjacent to the microcontroller. Pin 15 of the microcontroller
runs at half the output frequency,
so that when the Speed Controller’s
output frequency is 50Hz, there is
a 25Hz square wave at pin 15, with
an amplitude of just slightly less
than 3.3V.
This can easily be measured with
an oscilloscope, frequency meter (or
DMM with frequency capability) between pins 5 & 3 of the ICSP socket.
However, there is some hazard to
using this method as the lid must be
off and this exposes the high-voltage
circuitry which could be a lethal
hazard for an uninformed observer.
A somewhat easier and much safer
method, which does not necessitate
access inside the Induction Motor
Speed Controller case, involves the
use of a 9VAC or 12VAC plugpack
Right: this scope grab
shows a 22Hz output
waveform from the Speed
Controller, as measured
using the above circuit.
plugged into the 230VAC output
socket. Some digital multimeters will
be able read the output frequency
directly from the output of the AC
plugpack while others may be unable
to resolve the low-frequency signal,
due to the high-amplitude, highfrequency PWM switching signal at
around 16kHz and above, although
this will be partially filtered by the
AC plugpack.
In that case, a simple RC filter comprising a 10kΩ resistor and 100nF
capacitor will will attenuate signals
above 1kHz to enable an oscilloscope,
frequency meter or DMM (with frequency capability) to easily measure
the signal.
The accompanying scope grab
shows the result when the Speed
Controller is set for an output of
22Hz. This would give slightly less
than half nominal speed for a induction motor, eg, around 720 RPM for a
motor with a name-plate speed rating
of 1440 RPM.
SILICON CHIP.
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If you want the ultimate in high-power
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PCBs & special components available from PartShop
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MAY THE BEST MAN WIN!
As you can see, we pay $$$ for contributions to Circuit Notebook.
Each month the BEST contribution (at the sole discretion of the editor)
receives a $150 gift voucher from Hare&Forbes Machineryhouse.
That’s yours to spend at Hare&Forbes Machineryhouse as you see fit
- buy some tools you’ve always wanted, or put it towards that big
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editor<at>siliconchip.com.au
or post to PO Box 139, Collaroy NSW
September 2014 85
An improved tweeter
horn for the Majestic
loudspeaker system
When we published the Majestic loudspeaker system in the
June 2014 issue, it created a great deal of interest; more than
even we had hoped for. We thought that readers might think
it a huge throwback to the 1950s but evidently it has been a
hit. So much so that the originally specified Etone tweeter
horn has now become unavailable. Fortunately though, we
have been able to source a Celestion horn which looks and
sounds even better.
By Allan Linton-Smith & Leo Simpson
This photo shows the
front and rear views of the
Celestion T5134 diecast
aluminium horn, together
with the mating Celestion
CDX1-1730 compression
driver. Note the two rubber
inserts in the horn on its
longer axis. These evidently
are for damping as the horn
itself is quite ‘dead’. Note
also that only two mounting
holes are provided for
attaching the horn to the
compression driver.
86 Silicon Chip
siliconchip.com.au
This photo shows two views of the assembled compression driver with the
diecast aluminium horn. The horn has four holes for attaching it to the baffle
and pan head screws should be used.
Majestic Speaker Frequency Response
Etone vs Celestion Horn <at>1 watt / 1 metre
07/04/14 19:19:16
+50
+40
W
siliconchip.com.au
+30
+20
+10
dBr A
E WERE PEEVED, to say the
least, when the Etone tweeter
horn used in the Majestic speaker system became unavailable shortly after
the June issue went on sale. The news
was even worse when Etone advised
us that the Asian manufacturer of the
horn had gone out of business.
We had to do some frantic searching
to find a substitute horn which would
perform at least as well as the Etone
horn. Ultimately, we found that Celestion themselves had a suitable diecast
aluminium horn which looked to be
even better than the larger Celestion
H1-9040P composite/plastic horn
which we originally tried before rejecting it in favour of the Etone.
We then had to source the horns
from Celestion in the UK and had to
wait weeks before they arrived. Then
they had to be fitted to the Majestic
enclosures, and listening comparisons made between the Celestion and
Etone horns. Our initial impressions
were that the Celestion horns gave a
smoother overall response and their
vertical dispersion was somewhat better than the Etone unit. Then the whole
system had to be precisely measured
with a calibrated microphone etc.
Fortunately, our listening impressions were confirmed and the Celestion compression driver and horn com-
0
-10
-20
-30
-40
-50
20
50
100
200
500
1k
2k
5k
10k
20k
Frequency (Hz)
Sweep
Trace
Colour
Line Style
Thick
Data
Axis
Comment
2
3
4
5
1
1
1
1
Red
Mauve
Blue
Cyan
Solid
Solid
Solid
Solid
15
15
15
15
Anlr.Level A
Anlr.Level A
Anlr.Level A
Anlr.Level A
Left
Left
Left
Left
Etone Horn
Etone Horn Treble Boost
Celestion Horn
Celestion Horn Boosted
Fig.1: these four sweeps show the frequency response of the Etone and
Celestion horns when fitted to the Celestion CDX1-1730 compression driver.
As can be seen, the sweeps with the Celestion horn are smoother overall.
bination is clearly superior. It would
have been great if we had known about
this horn right from the start!
Frequency & distortion
The Audio Precision graph in Fig.1
gives a comparison between the Majestic fitted with the now defunct Etone
horn and the new Celestion horn. There
are four frequency sweeps, numbered
2, 3, 4 & 5. Sweeps 2 & 3 are for the
Etone horn, with sweep 3 showing the
effect of the treble boost above 10kHz,
produced by the peaking circuit in the
crossover network.
Both sweeps produced a pronounc
ed dip at 2.5kHz which is not audible
but was caused by a standing wave
September 2014 87
We made this adaptor plate out of 4.8mm thick Masonite to cover the large
hole in the baffle for the Etone horn. We made the slightly elliptical cutout with
a circle cutter set for a diameter of 130mm and then used a rasp to slightly
chamfer both sides to suit the wider axes of the Celestion horn. It was finished
with a matt epoxy-based paint to match the finish of the diecast horn.
from the floor reflecting into the test
microphone. However, using exactly
the same measuring set-up with the
Celestion compression driver and aluminium horn gave no trough at this frequency. In this case, sweep 5 includes
the boost above 10kHz while sweep
4 is without the boost. Overall, the
Celestion horn had a much smoother
response which was a confirmation
of our initial listening tests.
More importantly, the harmonic dis-
Etone vs Celestion Horn THD+N 1 Watt (500kHz bandwidth)
07/04/14 19:42:56
100
50
20
10
5
2
1
THD + N (%)
0.5
0.2
0.1
0.05
0.02
0.01
0.005
0.002
0.001
0.0005
0.0002
0.0001
1k
2k
3k
4k
5k
6k
7k
8k
9k 10k
20k
Frequency (Hz)
Sweep
Trace
Colour
Line Style
Thick
Data
Axis
Comment
2
3
4
5
1
1
1
1
Red
Mauve
Blue
Cyan
Solid
Solid
Solid
Solid
15
15
15
15
Anlr.Level A
Anlr.Level A
Anlr.Level A
Anlr.Level A
Left
Left
Left
Left
Etone Horn
Etone Horn Treble Boost
Celestion Horn
Celestion Horn Boosted
Fig.2: these four sweeps show the THD performance of the Etone and Celestion
horns when fitted to the Celestion driver. These figures have been taken with a
500kHz measurement bandwidth, resulting in higher overall figures than those
shown in the June 2014 issue. Overall, the Celestion horn is the better performer.
88 Silicon Chip
tortion was also reduced, as shown in
Fig.2. This shows harmonic distortion
taken with a measurement bandwidth
of 500kHz for both horns, over the
range from 1kHz to 20kHz. Again,
sweep 2 is for the Etone without treble
boost and sweep 3 is with the boost.
Sweep 4 is for the Celestion without
treble boost and sweep 5 is with boost.
Overall, the Celestion compression driver/horn combination seldom
exceeded 0.6% THD+N, even when
boosted, whereas with the Etone horn
it often exceeded 1%. Note that these
THD figures are significantly higher
than our original published sweeps
which used an 80kHz measurement
bandwidth. This tends to include a lot
more harmonics and high-frequency
noise, but of course anything above
20kHz is simply not audible.
Incidentally, some readers have
noted that the CDX1-1730 driver is
only rated at 45 watts on the Celestion
website but we have the actual printed
specification sheet which clearly states
that it is rated at 75 watts RMS (AES
standard) which we believe is the
correct rating.
Physical dimensions
As can be seen from the photos, the
Celestion diecast aluminium horn has
a smooth hyperbolic flare and an elliptical mouth, somewhat wider than
it is higher, to give better horizontal
dispersion. Even so, it also turns out
to have improved vertical dispersion
than the Etone horn and that means
that the “sweet spot” for listening is
somewhat higher – you don’t have
to be seated to get the best treble response; it is more widely dispersed.
The horn also has rubber inserts
along its wider axis and we assume
that these have been included to
damp any resonances. Certainly the
horn itself is quite “dead”, with no
tendency to ring.
The horn is attached to the Celestion
CDX1-1730 compression driver using
two M6 x 20mm bolts, with a washer
under each bolt head. These bolts are
quite tricky to fit as they are little too
long to be easily poked through the
two mounting holes of the horn. To fit
them, you need to slightly distort the
rubber inserts, to temporarily provide
clearance for the bolt heads. The bolts
should not be over-tightened.
The new Celestion diecast aluminium horn is more compact than
the Etone horn and will require a
siliconchip.com.au
Fig.3: this diagram of the Majestic cabinet
has been modified to show the smaller
baffle cutout for the Celestion horn. If you
have already made the larger cutout for
the now unavailable Etone horn, you will
need to make an adaptor plate (see text).
Note: the original article stated that the 1.5mm gap
between the angled panel and rear baffle resulted
in a 63cm2 port whereas the correct size is actually
6.3cm2. Also, the acoustic wadding used (from
Jaycar) is made from acrylic rather than bondedacetate fibre (BAF).
smaller cutout in the front baffle of
the enclosure. The cutout can be in the
form of a rectangle measuring 140mm
wide by 100mm high. Fig.3 shows the
dimensional diagram of the Majestic
cabinet, amended with the smaller baffle hole for the Celestion horn. If you
have already made the larger cutout
for the Etone horn, you will need to
make an adaptor plate because the new
tweeter horn will not cover the larger
hole. We made our adaptor plate from
4.8mm thick Masonite.
siliconchip.com.au
We made two Masonite adaptor
plates, one for each enclosure. These
plates each measure 255 x 205mm.
Instead of cutting a rectangular hole
in each for the horns we used a circle
cutter set for a diameter of 130mm. We
then used a circular rasp to chamfer
both sides of the hole to allow the elliptical tweeter horn to sit squarely on it.
After lightly sanding it with very
fine emery paper, we painted it with
a matt-finish black epoxy-based paint
which resulted in a finish quite similar
to that on the Celestion horn. The horn
requires four mounting screws and we
used 8G x 25mm pan head stainless
steel screws for this task although we
would have preferred screws with a
black oxide coating, to make them
less obtrusive.
Finally, the Celestion T5134 “NoBell” horn is available from Elfa (www.
elfa.com.au) for $35 plus p&p (order
code 28/H1-7050). The Celestion
CDX1-1730 compression driver is also
SC
available from Elfa for $189.00.
September 2014 89
Australia’s Largest
The Canberra
by KEVIN POULTER
E
very few years, the Historical Radio Society of Australia (HRSA)
displays a multitude of vintage radios and accessories, in a
central location, for Australia’s largest Radio Exhibition.
After a very successful event in Melbourne during 2012, Canberra
is the host city for RadioFest 2014. If you’d like an unparalleled opportunity to view and purchase most radio-related items, then the
HRSA RadioFest is for you. The venue is University House, in the
ANU grounds, during the weekend of September 19 to 21.
A highlight this year is the members-only auction of the Rare, Early
and Unusual, featuring masterpieces from the dawn of broadcast
radio in the early 1920s. Superior to any previous Vintage Radio
auction, there’s never been anything quite like it.
Expect everything “top shelf”: antique and unusual crystal sets,
very early valve radios, spark gap transmitting coils, spectacular
horn speakers. Full listings with photographs will be displayed on
the HRSA website from mid-August: www.hrsa.asn.au
Saturday night’s members dinner is an amazing opportunity to
mix and chat with enthusiastic radio collectors and restorers from
all around Australia and even some from overseas.
Great food and company is supported with the leading speaker,
David Kilby from the ABC. Well-known for his Rare Collections program (Sunday nights 9.30pm) on Radio National, hear him at his
funniest, most informal best.
Workshops are always popular too, demonstrating skills and
techniques employed to resurrect silent, poor condition radios to
make them look and work like new again.
Workshops include: Restoration with Stan Snyders (see SILICON
CHIP, Feb. 2014, for a fine example of Stan’s restoration), Mike Osborne showing a clever fix for dud early triodes in his session titled
“1920s valves in the 21st century”, plus “Safe Practice in Restoring
A huge d
ispla
microph y of early teleph
ones we
ones. R
telephon re often similar adio
the
e mouthp
ieces.
A rare ivory
“marble” AWA Empire State radio.
An extre
mely rar
e examp
first com
le of AW
merc
the 1925 ial tunable radio A’s
Radiola
4 model. s,
maculate
est: An im radio,
F
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on at
board
For aucti ater Kent Bread A-K horn,
l
tw
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A
in
4
ig
2
r
9
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1
with the
man-buil
complete nd superb crafts e.
a
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ilicon
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hip
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literatur s display enclos
glas
ose
ical of th
siliconchip.com.au
items typ RadioFest.
o
n
o
h
p
e
nd
Radios a and for sale at th
y
la
p
is
d
n
o
Vintage Radio Event:
RadioFest
September 19-21,
ANU University House,
Canberra, ACT
Mains Radios”, with experienced technician John Carr.
The Saturday afternoon is free to be a tourist and the best opportunity for members, wives and families to see Canberra’s highlights
on the free bus tour, or in your car. Spring in Canberra is beautiful
featuring the Floriade flower display. Other often-visited attractions
include the National Film and Sound Archive and the War Memorial.
The free bus will also be available on Saturday night to ferry members
from the preferred accommodation venues to the dinner and return.
Sunday’s RadioFest sale and exhibition is open to all, with displays
and a huge market of every conceivable radio, parts, books and
ephemera. Collections on display include the magnificent output of
Philips Radio at the height of its golden period, old telephones, early
and intriguing transistor radios, plus much more. Society members
will have access to the main trading hall early on the Sunday, from
8.30am. The hall is then open to the public from 9am to 3pm.
ing
s, includ
rophone used by
ic
m
ly
r
of ea
one
A range a of the microph er first
h
in
a
lb
a replic
e
llie M
Dame Ne broadcast.
No doubt you’ve noticed there are members-only privileges
throughout the weekend; however it’s easy to become a member.
The HRSA encourages people with an interest in vintage radio to
join. At just $35 a year, including the quarterly colour magazine,
access to circuits and 50,000 valves plus parts and so much more,
like monthly meetings and regular auctions, the HRSA has to be the
best value. Details on the HRSA website.
After the major display and sale, in the evening the HRSA’s AGM
will be held. The HRSA again acknowledges the contribution SILICON
CHIP magazine makes toward the conservation and promotion of
Vintage Radio and their sponsorship of the event.
Further information on the Auction, Accommodation and Bookings
is on the HRSA website www.hrsa.asn.au and the special event site:
www.ozradios.com, or contact Richard Elliott, telephone (02) 4846
1096 for dinner and seller-stall bookings.
SC
The winner of the
best restored radio
at the last RadioFest,
an AWA C54.
Early an
d orn
At the tim ate loudspeaker
s.
e spe
external
to the ra akers were
dio, not
built-in.
coloured
n
s love
nditio
siliconchip.com.au
Collector Astor in fine co st.
n
e
e
e
F
d this gr
st Radio
radios an r $4,500 at the la
fo
sold
A display of batteries, essential for
early valve radios.
SSeptember
eptember 2014 91
2014 91
Vintage Radio
By Ian Batty
Welcome To The Jet Age: Pye’s Excellent
C-2 Jetliner Transistor Radio
Pye’s C-2 “Jetliner” meets all the obvious criteria for a successful
portable radio. It’s good-looking, has loads of audio output, picks
up distant stations with ease, runs on almost-flat batteries and
offers a tuning meter to precisely locate the “sweet spot”. But it’s
what’s under the hood that’s really interesting.
A
N ADDENDUM to the landmark
1960 “Mullard Reference Manual
of Transistor Circuits” described a
portable radio using the (then) new
family of alloy-diffused transistors, the
OC169/170. This design had a sensitivity of 20µV/m and considering that a
ferrite rod antenna has a “loss” of some
10:1 (20dB in voltage terms), this implied a basic sensitivity of about 2µV.
At the time, the Mullard circuit
demonstrated that transistor portables
had developed to a point where they
could compete with valve sets and
win the contest. Very few valve radios
could get anywhere near this figure
without an RF amplifier stage.
Both the Bush TR82C Mk.2 and the
Kriesler 41/47 (described in this column in September & December 2013)
adopted the basic Mullard design. The
TR82C, in particular, achieved out92 Silicon Chip
standing sensitivity but suffered from
excessive noise on its broadcast band.
As with the above two sets, Pye’s
Jetliner follows the iconic “Mullard Design”. And like the 41-47, the Jetliner
uses a PCB (the TR82C used a metal
chassis and point-to-point wiring).
PCB construction often means restricted access to the circuit for servicing. Most sets, including the Jetliner,
mount the board “component side” up,
leaving the connecting tracks on the
“inside” of the case. The Pye service
data helpfully includes a component
layout diagram. You can download the
circuit and service details from Kevin
Chant’s excellent website at www.
kevinchant.com
Circuit Description
Fig.1 shows the circuit details of
the Pye Jetliner. Like the TR82C and
41-47, it follows the design that had
become standard for the time: a selfoscillating mixer (TR1), two IF stages
(TR2 & TR3), a diode demodulator and
a transformer-coupled audio driver
(TR4) feeding a push-pull transformercoupled output stage (TR5 & TR6).
It uses six transistors (seven really),
so it’s the standard “trannie” that we
all know. The transistors used in mine
are Philips/Mullard germanium PNP
types – alloy-diffused in the RF/IF section and alloyed-junction in the audio.
Bottom-coupled IF coils
Whoever put this circuit together
threw away the conventional handbook when it came to designing the
455kHz IF strip. That’s because it uses
separate bottom-coupled IF coils in
each stage (rather than conventional
IF transformers).
siliconchip.com.au
Fig.1: the Pye Jetliner’s circuit uses a self-oscillator mixer (TR1), two IF stages (TR2 & TR3), a diode demodulator (D2), a transformer-coupled audio driver (TR4)
and a push-pull transformer-coupled output stage (TR5 & TR6). D1 is connected to the mixer’s output and provides AGC.
siliconchip.com.au
FROM
CONVERTER
IF
TRANSFORMER
TO IF
C3
SECONDARY
TUNING
C1
PRIMARY
TUNING
PRIMARY
CURRENT
C2
BOTTOM
COUPLING
SECONDARY
CURRENT
Fig.2: a bottom-coupled IF circuit. It uses
two single-winding IF coils in separate cans
and C2 couples the energy from the primary
coil to the secondary coil.
Basically, a conventional IF transformer uses
primary and secondary windings, both tuned to the
IF (intermediate frequency). They are placed close
enough so that their magnetic fields interact and
couple energy from the primary to the secondary.
Their exact characteristics depend on the inductance of each winding and the spacing between
them. It’s possible to calculate the mutual inductance between them (ie, the degree of coupling),
along with the primary-to-secondary voltage ratio
and the total bandwidth.
However, while this method works well, calculations are laborious and transistor circuits require
a low-impedance tapping on the tuned secondary
for maximum power transfer.
A less intuitive (but simpler) connection uses
bottom coupling. In this case, the two coils can
be in separate metal cans and the calculations
are greatly simplified. This design works just as
well as the traditional “primary-plus-secondary”
version but it does require two separate coil (and
can) assemblies.
If you’re familiar with valve circuits, top and
bottom coupling may seem commonplace but this
is the first time I’ve seen the technique used in a
transistor set. It’s a clever technique for several
reasons. First, although it involves an extra coil
can, each IF transformer has only a single slug
that’s adjusted from the top. So there’s no need to
get to both sides of the PCB for alignment adjustments, as would be the case with the conventional
IF transformers.
Second, getting the exact degree of inductive
coupling needed between two coils in the one
can is an exacting piece of electrical and physical
design. With bottom (or top) coupling, the coils
are simply wound individually. The degree of
coupling is then determined by a simple formula
that specifies the coupling capacitor’s value.
Finally, there’s no confusion over correct slug
positions: either of the two peaks is correct.
Coupling circuits
Before going further, let’s digress and take a
generalised look at coupling circuits, so that
we can better understand how the Pye Jetliner’s
circuit works.
September 2014 93
L
SMOOTHED
DC OUT
FROM
RECTIFIER
C1
C2
(a) ‘PI’ FILTER AS USED IN MAINS POWER SUPPLY
FROM
POWER
AMPLIFIER
L
C1
TO
ANTENNA
C2
(b) ‘PI’ FILTER AS USED IN TRANSMITTER OUTPUT
FROM
POWER
AMPLIFIER
C1
TO
ANTENNA
L
C2
(c) CAPACITIVE DIVIDER AS USED IN TRANSMITTER OUTPUT
Fig.3: (a) shows the conventional Pi filter configuration, (b) shows how
it’s used for RF impedance matching (C2 many times larger than C1)
and (c) shows a reconfigured version with a capacitive voltage divider
as used in the Pye Jetliner (again C2 is much larger than C1).
Basically, we need to match a highimpedance tuned circuit to a transistor’s low input impedance. Transmitter
circuits also need to match into lowimpedance antenna feedlines, usually
50 ohms. As well, load impedances
may be less than the feedline, requiring a step-up in impedance matching.
Although tapped coils can be used,
it’s easier to use some kind of capacitive voltage divider. This removes the
“cut and try” method often needed at
very high frequencies, where a coil
may be only two or three turns and
the exact tap location can be difficult
to determine.
Most of us are familiar with the
Pi-filter configuration that’s used in
mains-derived power supplies to
smooth pulsating DC. What’s not so
obvious is that it can also be used in
a tuned circuit to match impedances.
Fig.3(a) shows the conventional
Pi-filter configuration, while Fig.3(b)
shows how it can be for RF impedance
matching. Finally, Fig.3(c) shows a reworked version with a capacitive voltage divider, as used in the Pye Jetliner.
In a conventional power supply
94 Silicon Chip
Pi-filter, C1 and C2 are often of equal
values, eg, 8µF in vintage radio sets.
However, in the RF version (Fig.3(b)),
C2 is usually several times larger than
C1, so that C2’s lower circuit impedance matches the antenna impedance.
C1, on the other hand, provides a highimpedance load as required by the
power amplifier’s output stage.
Similarly, in the capacitive divider
(Fig.3(c)), C2 is much larger in value
than C1. The design calculations are
simple and any desired impedance
step-down is easily achieved.
The capacitive voltage divider has
an additional bonus: in the Jetliner, the
mixer’s collector voltage is blocked by
the “top” capacitor. As a result, the bias
network can apply bias directly to the
first IF stage, as this point is also isolated from DC ground by the “bottom”
capacitor. So we achieve resonance,
impedance matching and DC blocking
with just three components and no
coil tappings.
Back to the Jetliner circuit
Unlike most ‘broadcast-only’ transistor sets, the Jetliner uses a tuning
gang with identical aerial and oscillator sections. In fact, it’s quite unusual
to see this in a Japanese-manufactured
‘polyvaricon’ that uses a sheet plastic
dielectric rather than air-spacing.
As in its valve predecessors with
identical tuning-gang sections, this
means a that padder capacitor must be
added to the oscillator provide tracking. This is the 315pF capacitor (C5)
coupling the tuning gang to the top of
the tuned oscillator coil (ie, just to the
right of the 2N374/AF116n transistor
– see Fig.1).
The mixer uses collector-emitter
feedback, thereby reducing the amount
of local oscillator radiation that’s fed
back out through the antenna rod. This
design also includes an OA91 damping
diode between the DC collector load of
the first IF amplifier (2N373/AF117n)
and the mixer’s collector circuit. This
diode considerably improves the performance of the AGC (automatic gain
control) on strong signals.
The mixer’s output (ie, from TR1’s
collector) feeds the untapped primary of the first IF transformer and
it’s here that some thoughtful design
work becomes apparent. Conventional broadcast-band IF amplifiers
use tappings on the IF transformers to
match impedances, especially on the
secondary winding. This is necessary
to match the low base impedances of
the IF amplifier transistors and the low
impedance of the demodulator diode.
By contrast, in this circuit, the first
IF transformer’s secondary is tuned by
C9 (330pF) and C10 (5.6n) connected
in series (giving 310pF). Importantly,
C10’s low reactance provides a good
match for the first IF transistor’s base
impedance.
But it’s even more complicated than
that! The original Pye circuit drawing
depicts the first IF transformer as the
usual “two coils in the one can” configuration, coupled by their mutual
magnetic fields. In reality, L3 and L4
are individual inductors in separate
coil cans. They are bottom-coupled via
the 33nF capacitor (C8) that appears to
be a simple bypass.
In reality, the IF signal circulating
in L3’s resonant circuit is fed through
capacitor C8, raising one end above
signal ground. The signal at this end is
in turn coupled through to L4 to create
a signal current in its resonant circuit.
The use of bottom coupling also
explains the unusual connection of
L4’s ‘cold’ end. Why not just connect
siliconchip.com.au
it straight to ground? Because there
would be no signal introduced into
L4’s tuned circuit; that’s why.
Second IF stage
The second IF stage is simplicity
itself. The signal from the first IF amplifier (2N373) is fed to a single tuned IF
coil and then coupled via a capacitive
divider into the base of the second IF
transistor (also a 2N373). This divider
circuit uses the same component count
as a tapped-inductor version but is
easier to manufacture because there are
no coil tappings. There’s also no need
for a separate, low-impedance secondary winding on the IF coil to match into
the second IF transistor’s base.
The final IF transformer uses a
tuned primary but also includes a
low-impedance, untuned secondary to
drive demodulator diode D2 (OA90).
The two IF amplifier transistors
operate in a similar manner to the IF
amplifiers used in most other sets.
The first IF stage (TR2) operates with a
collector current of about 0.5mA. This
allows the AGC to reduce its collector
current effectively, to lower the gain
as required.
TR2’s emitter is connected to ground
via an 820Ω resistor and a small meter
labelled “Radicator”. This is a 500µA
meter with a righthand zero and it
functions as a signal-strength indicator.
With the set is turned off, the needle
rests at the righthand end of its travel.
Conversely, when the set is on and
there is full emitter current through
TR2 (ie, no station tuned), the needle swings fully left, indicating “no
signal”.
When a station is being tuned, TR2’s
emitter current falls due to AGC action
and the meter swings to the right, towards the “maximum signal” position.
In practice, it’s just a matter of tuning
the station for a maximum reading on
the meter.
This signal-strength meter circuit is
a common design and works equally
well with both valve and transistor
IF amplifier stages. Both types draw
maximum current with no signal and
minimum current with maximum
signal. This is why these meters
commonly indicate maximum signal
strength when the power is off.
All the RF/IF transistors are AF116/117 (or 2N374/2N373) alloydiffused types. Their feedback capacitance is low enough that no neutralisation is needed at 455kHz.
siliconchip.com.au
This photo shows the component side of the PCB but note that the heatsinks
for the output transistors and the bias diode (at right) have yet to be riveted
together again following transistor replacement.
The demodulator (D2) is a conventional OA90 diode. The demodulated
audio is fed via a voltage divider to the
volume control, while the AGC voltage
is derived via R14 and C21 and fed
back to the bias network for the first IF
amplifier (TR2). The diode’s output is
positive-going, so it “bucks” the negative bias applied to TR2’s base, thereby
reducing the transistor’s collector current and lowering its gain. The stronger
the signal, the greater the reduction in
TR2’s collector current and the greater
the reduction in gain.
As with all AGC systems, the net
effect is to keep the audio signal
fairly constant with varying RF signal
strengths. However, the amount of control we can apply to a single IF stage is
limited; eventually the transistor will
be almost completely cut off and there
will be no further gain reduction.
It’s not practical to control a selfoscillating mixer’s collector current
for AGC, as this would force the local
oscillator off frequency. However, it
is possible to apply damping to the
primary of the first IF coil and thus
reduce the converter’s overall gain.
In the Pye Jetliner, that’s done using
the auxiliary AGC diode (D1). As shown
in Fig.1, this diode (OA91/1N60-A) has
its cathode connected to the DC supply
for the first IF amplifier, while its anode
connects directly to the mixer’s output
(ie, as fed to the first IF coil’s primary).
With no AGC action (ie, little or no
signal), the TR2’s collector current
pulls D1’s cathode down to about 2.5V.
This is about 2V more positive than its
anode, so the diode is reverse biased
and does not conduct. Conversely, as
the AGC takes effect (and TR2 draws
less current), the D1’s cathode voltage
rises, eventually becoming less posi-
tive than its anode. When that happens,
D1 begins to conduct and this damps
(or reduces) the signal at the converter’s
collector.
As a result, the mixer’s output is effectively reduced and this significantly
improves the overall AGC action.
According to Mullard, the AGC
range improves from about 35dB (ie,
input signal increase for a 6dB audio
output increase) without the diode to
over 55dB with the diode in circuit.
Audio stages
The audio driver stage (TR4) is
biased in a similar manner to the IF
amplifiers and works identically. However, it uses a larger emitter bypass capacitor and this is necessary to ensure
that it is effective at audio frequencies.
TR4 drives the primary of transformer T1 which operates as a phase splitter.
Its centre-tapped secondary drives a
Class-B push-pull output stage based
on transistors TR5 & TR6 and these in
turn drive the centre-tapped primary
winding of speaker transformer T2.
T2’s secondary then drives either two
parallel-connected loudspeakers or a
set of headphones via a headphone
socket. Resistor R24 provides feedback
from the output of transformer T2 to
TR4’s emitter to minimise distortion.
Note that the output stage dispenses
with the usual voltage divider or voltage divider-plus-thermistor arrangement for thermal stability. Instead, a
series resistor feeds a diode-connected
transistor (TR7) and this reduces the
bias applied to the output stage as the
temperature rises. But that’s not all it
does, as we shall see.
A diode for bias?
Unfortunately, both the Bush TR82C
September 2014 95
tors. This gives tight thermal coupling
so that the transistor-connected diode
will respond to output transistor
temperature variations. Even the best
thermistors, separately mounted flat
on a circuit board, cannot match this
degree of bias voltage response.
Transistor manufacturing tolerances
mean that some form of bias adjustment is needed. As a result, the Jetliner
provides a jumper to select one of two
bias values. This jumper either places
resistor R28 in parallel with R29 or a
series combination of R28 & R27 in
parallel with R29.
Finally, emitter resistors R25 & R26
provide some local feedback and help
balance differing gains in the two output transistors.
Getting it going
The PCB has been lifted free of the case here, revealing the two loudspeakers
and the dial-drive mechanism. Note that the two dial pointers must be aligned
with the case slots during reassembly.
and the Kriesler 41/47 suffer from increasing distortion with falling battery
supply voltage, due to decreasing output stage bias. This is a common fault
in many transistor radios, especially
those using germanium transistors.
It’s common to see a thermistor used
in the output stage bias circuit but, in
many cases, this only compensates for
ambient temperature changes and cannot counteract falling bias with falling
battery voltage. Worse, thermistors are
often mounted on the circuit board and
cannot compensate for overheating in
an output stage that’s being run at high
volume. The Ferris M134 portable car
radio was notorious for blown OC72
output transistors caused by just this
problem.
In many sets, increasing crossover
distortion as the batteries age can be
so bad that owners will discard batteries before they are truly “flat”. As
a result, I’ve actually modified some
of these sets for family and friends to
improve performance.
Unlike the TR82C and the 41/47, the
Jetliner uses a semiconductor “diode”
in the bias network. Well, it’s not really
a diode. Instead, it’s a diode-connected
transistor (TR7), which has its base
directly connected to its collector.
The reason for doing this is straightforward. In operation, a simple germanium diode begins to conduct at
around 0.2V but its forward voltage
rises quite rapidly with current. This
96 Silicon Chip
means that a varying battery voltage
would pass a varying current through
a resistor in series with the diode and
the diode’s forward voltage would
change accordingly.
Connecting TR7’s base to its collector brings in transistor action. As soon
as base current begins to flow, it will
cause a larger collector current. This
means that even a small increase in
base voltage will cause a significant
rise in total current, so the device acts
as a diode with a sharper ‘knee’ than
using the base-emitter junction alone.
This device not only delivers the
required bias voltage but also has the
same voltage-vs-temperature coefficient as the output transistors. As
the temperature increases, the voltage
across it reduces slightly to ensure that
the correct bias is applied to the output
transistors to ensure thermal stability.
As a result, the Jetliner (and sets
with the same bias circuit design)
delivers good audio performance until
the batteries are almost dead flat. On
test, the set easily delivered 50mW
at under 10% distortion with “flat”
batteries supplying just 3V, ie, half
the nominated 6V supply voltage (4
x 1.5V cells).
The actual circuit specifies either of
two bias transistors (AV-2 or OA675),
depending on the actual output transistors used. The transistor is fitted
with a “flag” heatsink that’s riveted to
those used for the two output transis-
As it came to me, the set was almost
dead. A common problem with old
transistor sets is no output at all due
to corroded/tarnished contacts on
headphone jacks and power switches.
By contrast, this set worked but its
performance was extremely weak.
What was strange was that the signal
meter indicated a “strong signal”, with
the pointer stuck at the righthand end
of its travel. That just had to be wrong
but it was also a clue as to the fault.
It didn’t take long to find the cause –
a bad solder joint between resistor R7
and the meter. And since R7 is transistor TR2’s emitter resistor, this upset the
operation of the first IF amplifier stage.
Once this joint had been resoldered,
the set leapt into action. However, I
was unhappy with the performance
of the output transistors, so I raided
my junkbox and replaced them. I then
tested the set and found that I was able
to tune stations from one end of the
broadcast band to the other. Considering my country location, it was a good
result and the Pye Jetliner seemed to
be a pretty sensitive set.
A note on circuit board removal and
replacement: the two dial pointers sit
in a channel moulding behind the dial
inserts and cannot be removed unless
they are set to the top end of the band,
so that they align with a couple of slots
in the case. Similarly, on replacement,
the two pointers must be lined up
with these slots, as shown on one of
the photos.
A bit about noise figures
It was time to pop the set onto the
test bench to find out just how sensisiliconchip.com.au
This photo shows the needle positions
on the ‘Radicator’ for various signal
strengths at 1400kHz & 600kHz.
tive it really was and take a few noise
measurements. Before doing that
though, I applied contact cleaner to
the switches and volume pot, and then
gave it a quick alignment check.
I measure sensitivity for a 20dB
signal-to-noise ratio at 50mW output
and at 30% modulation. To meet this
20dB requirement, I first set the input
signal for 50mW output. I then turn
the modulation off and (hopefully) get
only 0.5mW of output. This gives me
a S/N power ratio of 20dB.
If the noise-only signal is above
0.5mW, the volume control is turned
down until the output reaches this
level. I then turn the modulation back
on and increase the input signal to get
the 50mW standard output. In practice, it’s common to juggle the volume
control and signal generator output to
get 50mW output at 20dB S/N ratio.
You may wonder why I don’t simply
detune the signal generator or turn it
off, as this would give less noise. The
reason is that the 20dB figure must be
the “on signal” ratio, ie, the ratio of
the audio output to the noise in the
received signal.
How good is it?
The frequency response of this set
from the volume control to the loudspeaker is 140Hz to 25kHz ±3 dB. So
the high end is pretty “snappy” but a
few more henries in the transformer
windings would have given a better
bottom end. Unfortunately, the IF
channel (as in most broadcast-band
AM radios) is the bottleneck. From
antenna to speaker, the frequency
response is 140Hz to about 2.8kHz,
confirmed by an IF selectivity of -3dB
at ±2.8 kHz. At 60dB down, the selectivity is about ±15kHz.
The audio performance is pretty
siliconchip.com.au
good, with a total harmonic distortion
of just 3.5% for a 1kHz signal at 10mW
output. At 50mW output, the distortion is still just 4%. It rises to around
7% just as the amplifier begins to clip
at 250mW output.
The transistor-diode’s biasing superiority shows up with a low battery.
At 3V (only 0.75V per cell), distortion
is still only around 4.2% for 10mW
output and is still under 5% at 50mW.
Sets with resistor-biased output stages
simply can’t match this performance.
The Jetliner’s RF sensitivity is out
standing and is under 3µV (ie, at the
antenna terminal) for an output of
50mW. However, at this level, the
signal-to-noise ratio is only 13dB
at 1400kHz. The sensitivity falls to
about 5.5µV if the gain is reduced to
give the standard 20dB S/N ratio at
this frequency. It’s about the same at
600kHz, ie, 5µV for 50mW output at
20dB S/N ratio.
In operation, this set produces a
50mW output at a field strength of
20µV/m at 1400kHz and 55µV/m at
600kHz (both at full gain). The required field strength rises to 50µV/m
at 1400kHz to deliver a 20dB S/N ratio
though.
Where the Jetliner shines is in the IF
channel. In fact, its sensitivity is four
times better than the Kriesler 41/47’s
when taken at the input to the first
IF stage – about 50µV compared to
200µV. Since both sets use the same
transistors, it seems that the Jetliner’s
IF transformers and its improved coupling circuits are the secret.
AGC checks
Checking the AGC system revealed
that the AGC control held the output
to a 6dB rise for a signal increase of
some 33dB. However, Mullard quoted
55dB with the specified AGC diode
(D1), so what was going on?
Further checks showed that transistor TR2’s collector voltage was only
going to about 4V on full signal, during which the output was becoming
distorted. Suspecting a fault in this
stage, I tried shorting TR2’s base to
ground. This should have turned the
transistor off and allowed its collector
voltage to rise to at least 4.5V but this
didn’t happen.
Even with the set turned off, there
was still some measurable resistance
between TR2’s collector and ground
and the logical suspect was the .047μF
(47nF) bypass capacitor (C12). This
was one of those “red-tipped” highvalue ceramics that’s been notorious
for leakage. On removal, it gave a
resistance reading of about 10kΩ so it
was effectively forming a voltage divider with the 3.9kΩ collector resistor
(R8). And that in turn was preventing
the AGC diode’s cathode from rising
high enough to obtain forward bias.
A new “greencap” capacitor fixed
the problem. Shorting TR2’s base to
ground now resulted in its collector
voltage rising to about 4.6V, as expected. More importantly, the AGC circuit
was now working correctly with the set
now handling a 60dB signal increase
for an output power increase of just
over 6dB (well in line with the original
Mullard specification).
So leaky ceramic capacitors are a
cause of trouble in low-voltage transistor radios. It’s not just the electrolytic
types that can cause problems.
Summary
The Jetliner is not a pocket set; instead its size and dual-speaker design
make it a “picnic portable”. Its sensitivity is one of its main features and
the signal-strength indicator makes it
possible to accurately tune stations.
It’s a simpler set than the Bush
TR82C and although the circuit is
similar to that used in the Kriesler
41/47, its performance is much better.
In fact, its performance is excellent.
It meets the manufacturer’s impressive specifications for sensitivity and
low-battery performance and my only
reservation is the quoted output of
500mW, which I was unable to obtain.
Some manufacturers do indicate up to
750mW output (with a 6V supply) for
an OC74 push-pull output stage but the
alternative 2N217 transistors appear
to be lower-rated than the OC74s. It’s
possible that the 500mW figure quoted
is for an OC74-equipped model.
Finally, note that the original circuit
diagram for the Pye Jetliner shows
TR7’s base connected to its emitter.
The base should in fact go to the collector (so that it correctly functions as a
bias diode) and the circuit reproduced
here has been corrected.
Further reading
If you’ve not already done so, take a
look at Kevin Chant’s excellent website
at www.kevinchant.com It’s a free resource for (mainly) Australian vintage
radios, and includes circuits, photos
SC
and parts information.
September 2014 97
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
Battery power
for GPS Tracker
I am interested in building the GPS
Tracker featured in the November
2013 issue of SILICON CHIP. We will
be travelling to the UK later this year
and hiring a car for part of our trip.
At other times, we will be on taxis/
buses/trains or walking, and we will
not have access to a cigarette lighter
socket. Is it possible to power the GPS
Tracker from batteries (rechargeable or
otherwise)?
Alternatively, could the unit run
on 6V batteries and do away with the
cigarette lighter socket totally? (D. W.,
via email).
• Yes, it would be possible to power
it from nine AA cells but that is not
very portable and the current drain
of about 50mA would quickly flatten
the battery. Because of how the power
supply works you need at least 9V to
power the device and it will not work
properly with a 6V source.
GPS master
clock wanted
Being a person with multiple clocks
around the house I never really know
the correct time as their drifts differ.
Have you or would you design a master
clock with a GPS module, that sends
a signal to one or more slave clocks
around the house, each slave clock
having its own alarm setting function?
The alarm for each of the clocks
could also have the ability to use an
MP3 file or such. To expand on the
slave clocks’ ability to play an MP3
file, said clock could be set to play a
file not only to wake you up but one
also to send you to sleep, such as a
slowly increasing sound of waves or
white noise. (P. R., Bribie Island, Qld.)
• That sounds like a complicated
project indeed. In fact, it would be
simpler just to build one of our GPS
clocks for each room where you really
need an accurate time indication.
Of course, any mobile phone will
also give you accurate time and if it
is a smart phone it can provide white
noise or whatever ambient sounds you
want to send you to sleep.
CLASSiC-D amplifier
transformer query
I have previously written to you regarding the modification of the ClassicD DC-DC Converter (SILICON CHIP, May
2013), to make it have an output of
±20V rather than the designed ±35V,
so that I could use it to power the
“Tiny Tim” stereo amplifier from the
October 2013 issue. You advised that
the secondary bifilar winding of T1
should have 15 turns rather than the
originally specified 21 turns.
However, I foresee a problem in that,
with the 21 turns, the bobbin well ac-
commodates 7 turns across from S1
and S2, 7 turns back, and then 7 turns
across again to terminate at pins F1
and F2. However, with 15 turns, there
are only 5 turns on each pass, which
doesn’t fully cover the bobbin, there
being gaps between the windings and
therefore not a neat, compact three layers of windings. Would this affect the
efficiency of the transformer?
I had thought that instead of having
three layers of 5 turns, I could have
one layer of 7 and one layer of 8 turns.
This would bring the terminating
wires back to the S1 and S2 position,
but would it be then OK, after the
primary winding of 7 turns is added
on top of the secondary, to bring the
end wires of the secondary winding
straight over the top to the primary to
terminate them on pins F1 and F2? (C.
B., via email).
• Either way would be OK. The efficiency is not critical since you are
not intending to draw the full power
rating from the transformer.
For the first winding option, the
gaps between windings are not important. With the second winding option
with two layers, the final wire connection should run at right angles to the
windings to terminate to F1 and F2.
Solar panels
for hot water
With the dramatic drop in the price
Problem With MPPT Charge Controller
I have built the MPPT Charge Controller from the March 2012 issue but
I am having difficulty in implementing this project. My input is 18V <at>
4A, while the output is 13V <at> 4A.
So the input power is 72W while the
output power is 52W.
Can you please help me to trace
out the problem with this unit? (S.
Y., via email).
• The voltage values you have for
the MPPT charger input and output
show that it is working as it is step98 Silicon Chip
ping down the voltage from 18V to
13V with the solar panel operating
at its most efficient point which is
usually around 18V for a 12V panel.
How the input power versus output power is measured and calculated is important for accurate results.
Note that current is not continuous
but with a switching component
that is a significant proportion of the
overall current. We suspect that the
true output current from your MPPT
Charge Controller is over 4A.
Your current measurement will
need to be an RMS reading rather
than an average current. A true RMS
reading current meter will be required that is accurate for high crest
factors and able to measure RMS
values at 32kHz. There is no digital
multimeter that will do this job.
You really need to use a digital
oscilloscope which can provide
RMS values for the current being
monitored through low resistance
shunts.
siliconchip.com.au
24V Speed Controller Needs Fast Recovery Diodes
I have an enquiry regarding the
24V/20A Speed Controller described
in the June 1997 issue. Over the last
15 or so years, I have purchased
three of these kits. Two have ultimately failed but overall they have
performed quite well considering the
conditions they operate under, ie, on
a portable sawmill which is normally
left out in the bush all the time.
Regarding diodes D1 & D2, it
would appear as if I have replaced
these with a 35A bridge rectifier at
some stage. How I worked this out I
do not know. But is this modification
OK or is it better to stick to the original design? The motor load is 11A.
I would like to be able to find
exactly what has failed on the other
two boards. The first is obvious, as
the two Mosfets are well cooked.
On the second board, I fitted large
of solar panels, it is now becoming
feasible to use power directly from a
bank of solar panels to heat water using
an electric hot-water service. Certainly,
such a system overcomes many of the
problems of traditional solar hot-water
systems – running water pipes to the
roof, freezing and boiling of the water,
supporting the weight etc.
However, the element in a standard
electric hot-water service is designed
to run on 230VAC and so is not a good
match to the variable output from a
bank of solar panels. This is a long
shot but would it be possible to adapt
the MPPT Solar Charge Controller to
efficiently couple the output from a
solar panel bank into the resistive element in an electric hot-water service?
(D. S., via email).
• We have touched on this topic previously and the idea does have some
serious drawbacks.
A typical hot-water heating element
requires far more current and voltage
than the MPPT Solar Charger could
deliver. It requires several kilowatts
at 230VAC compared with 120W at
18V from the MPPT solar charger. In
addition, providing DC to the heating
element could accelerate corrosion.
If you were to use solar panels,
the better option would be to series
sufficient panels so that each panel
provides 18V (assuming a 12V panel)
at full sun for a total of 230V. The
siliconchip.com.au
heatsinks to the Mosfets and I cannot
see any obvious failure. The voltage
readings are not to specification but
the “Testing” section of the text does
not explain what to do if the readings
are incorrect.
How would I test the Mosfets? I
am getting quite a collection of them
and I would like to know which
are serviceable. By the way, I think
that “C2” on page 30, second last
paragraph should read “C3”. (B. W.,
via email).
• The diode across the motor (D2)
should not be a standard bridge rectifier. You need a fast rectifier such
as an MUR1515 or MBR20100CT
(Jaycar ZR1054). That substitution
could be the cause of the Mosfets
being damaged.
Note that better Mosfets have become available since we published
panels would need to be chosen to
match the heater element current. A
suitable DPDT heavy-duty relay could
be used to switch element polarity
each day or so.
433MHz sniffer project
has no signal indication
I built the 433MHz sniffer described
in the January 2011 issue but I have
found that the ZW-3102 module supplied by Jaycar Electronics differs from
the one in the article, as it now uses
the Spirit-on Enterprises PT-4302 chip
rather than the RX-3400.
While the modules seem to be
otherwise similar, the PT-4302 chip
lacks a peak signal output (RSSI tap
in the article) so that a signal strength
indication is not obviously possible.
Can you suggest a workaround for this
problem? (I. M., Mt Waverley, Vic).
• Unfortunately, the newer 433MHz
modules do not have the ‘hidden’
Received Signal Strength Indication
(RSSI) due to use of a different circuit.
There’s no easy solution to this so that
while the piezo will still function, the
LED signal indicator will not work.
Battery Lifesaver
design query
I was interested in the Battery
Lifesaver circuit as published in the
the June 1997 controller. The IRF
1405N (Jaycar ZT2468) is higher
rated than the original BUK456-60A
and is rated for automotive use.
The Mosfets can be tested for a
short circuit (low ohms) between
drain and source with the power
off. This resistance as measured on
a multimeter should be high (megohms) rather than close to 0Ω.
C2 is the 10µF soft-start capacitor at pin 4 of IC1. C3 is the 220nF
(0.22µF) capacitor across the motor.
If the voltages are not correct when
measuring as detailed in the testing
section, IC1 is possibly faulty or you
have a faulty resistor.
Finally, note that an improved
version of this 12/24V Motor Speed
Controller was published in the June
2011 issue and is sold as a kit by
Jaycar (Cat. KC5502).
September 2013 issue. On page 66
about half way down the third column,
it is stated that “. . . The other half of
D1/D2 clamps input pin 3 of IC1 to
the 5V supply if the battery voltage is
particularly high”.
The cathode of the double diode
(BAT54c) is connected to the input of
the 5V LDO regulator which would
be at the battery voltage or the battery
voltage minus ZD1 if fitted and not to
5V as in the above statement. Is it a
mistake in the schematic or an oversight in the design? (L. S., via email).
• That was a mistake in the design
but the series resistor from the battery
positive to pin 3 of IC1 limits the current flowing through its clamp diode in
that situation anyway, so it shouldn’t
be a problem.
We tested the circuit to the maximum specified battery voltage and we
haven’t had any reports of failures.
CLASSiC-D amplifier
module overheats
I recently built two CLASSiC-D
Amplifier kits (SILICON CHIP, November & December 2012), which I purchased from Jaycar. While one unit
works perfectly the other one has a
strange fault in which Q1 and Q2 both
get very hot without any input signal or
with the input shorted to ground. Q1
and Q2 will cool down immediately
September 2014 99
Ultrasonic Cleaner Not Causing Cavitation
I purchased an Ultrasonic Cleaner
kit from an Altronics store in Clayton, Melbourne. After constructing
the kit I have not been able to achieve
cavitation from the transducer.
Everything seems to work fine; it
seems to be able to do both sweeping
frequencies and higher frequency
functions, both LEDs light up accordingly and it sounds like it should
judging from the video on YouTube
etc. It just doesn’t seem to be getting
enough power.
There is a staff member at Altronics who has had experience with
this particular kit and he told me to
solder the 10kΩ resistors over the
zener diodes (which I missed) and
to use a proper potting compound
for setting the transducer in the pipe
(as previously it was set in silicone
caulk as per the instructions).
I’ve made those adjustments howwhen the Protect link is shorted.
I have replaced Q1 and Q2 but
it made no difference. All checks
and balances test OK. I’m currently
stumped as to what it could be since
the unit will still operate with this
condition, with the only problem being that it will shut down after about
10 minutes due to over-temperature.
Any advice? (B. W., via email).
• Check the 15V supply (Vcc), measured with respect to B-, and the VB to
VS voltage (also 15V). This may be the
problem if the gate drive voltage is well
below 15V. If it is low, check resistor
R9 and zener diode ZD1.
Alternatively, the dead time resistors may have incorrect values. Check
the 5.6kΩ and 4.7kΩ resistors at pin
9 of IC1.
Tiny Tim is
smoking resistors
I have built the Tin Tim amplifier
(SILICON CHIP, October & December
2013, January 2014) and the two 47Ω
resistors are smoking and burnt out.
Do you know what the cause could
be? (Y. H., via email).
• You possibly have a short from the
-20V lines to the early stages of the
amplifier. The most likely cause is
either a short between tracks on the
PCB or diodes D12 & D14 have been
100 Silicon Chip
ever I just can’t get cavitation. I’ve
included videos of both frequency
modes and a picture of the circuit.
What could possibly be wrong? (J.
F., via email).
• Correct operation of the Ultrasonic Cleaner is reliant on the power
supply being able to deliver sufficient current. You need a supply that
can deliver at least 2.5A at 12V. The
4700µF capacitors deliver much of
the peak current to the transformer
but the supply needs to be able to
deliver current to maintain charge
on the capacitors.
One common problem with constructors of this kit is with the fuse
clips. Check that the end stops on the
clips are positioned on the outside
so that they don’t prevent the fuse
from being inserted correctly. Make
sure also that the clips grip the fuse
tightly to ensure good contact.
installed the wrong way around. If
the diodes have been reversed, install
them correctly and replace the 47Ω
resistors. The chances are that it will
then work OK.
Balance control needed
for old amplifier
I recently encountered problems
with the volume and balance pots
while trying to resurrect my Studio
Twin-50 Stereo Amplifier (SILICON
CHIP, March & April 1992) that I built
some years ago. A replacement volume
control was obtained from Jaycar but
the balance pot has proven difficult
to obtain.
Are these 10kΩ MN pots still available or is there a workaround for this
potentiometer? (D. W., via email).
• If you do a Google search for “MN
dual gang potentiometer” you will find
that there are a number of overseas
sources for this type of potentiometer.
However, getting an exact match for
the dual-gang 10kΩ pot in your amplifier may be quite difficult.
Have you tried a squirt of Servisol
contact cleaner (Jaycar NA1012) into
the pot? Alternatively, you could try
replacing it with a dual-gang linear
10kΩ pot. It will not be quite as good
as the MN pot and it might not be
mechanically centred to obtain equal
gain in both channels but it will work.
However, the simplest way is to
just bypass it, since you will probably
never use it anyway. We have not included a balance control in any stereo
amplifier or preamplifier we have
published since the Twin-50 design.
Speed control for a
shunt-wound motor
Regarding your ‘Speed Controller
For Universal Motors’ in the February
& March 2014 issues, I am considering
purchasing one of these kits to power
a DC shunt motor (not a universal
motor).
At present, this motor is driving a
metal lathe and the present speed control causes an unsatisfactory cutting
tool feed, particularly at low speeds.
This of course does not lead to a good
surface finish. I think that much improved control could be obtained by
connecting rectified and smoothed DC
to the motor field and connecting your
speed controller only to the armature.
I would consider that with a constant
DC field and your PWM control, the
motor would run much more smoothly
with a narrow pulse width. I would
appreciate your thoughts on this application . (G. M., via email).
• A shunt motor with constant DC to
the field winding can be regarded as
being similar to a permanent magnet
motor. So to connect it for speed control, you should have a constant DC
supply fed to the field windings while
a PWM supply varies the voltage fed
to the armature connections (via the
brushes and commutator). It should
work very smoothly.
The DC supply can be obtained
using a suitably-rated bridge rectifier
(same as BR1 in the PWM circuit) but
no filtering is required and nor should
it be used as it would result in a DC
supply of over 320V – too high for the
field windings. With a rectified but
unsmoothed supply, the field current
should be close to the value normally
applied to the field.
Simple projects
needed
I think that some of the recent SILICON CHIP projects have been a little too
elaborate and expensive. More simple
projects are needed. I have ideas for
two projects:
Firstly, how about a video pattern
siliconchip.com.au
Massive Battery Charger For Camper Van
I am a grey nomad who prefers
being off-grid and as green as possible. I abhor those campers who run
a generator 15 hours or more a day
to charge their house batteries. The
incessant drone is enough to drive
one to drink excessively or worse.
Most generator battery charger circuits are 11A DC at most, so running
a 3kVA generator to use less than
10% of its capacity, at an insufficient
charge rate to restore full charge,
means it is an exercise in futility.
Their $20/day+ generator running
costs means it would be better all
round if they stayed connected to
the grid.
Barring ‘nuking’ them, which
may also damage my equipment, a
high-power laser or electromagnetic
pulse gun would be on my wish list
of SILICON CHIP ‘must have’ projects.
In the meantime, my wish to remain
off-grid was recently thwarted by
more than a week of inclement
weather.
Being ‘plugged in’ at Cann River
Caravan Park provided my 2 x
generator that will generate a series
of test patterns and blank coloured
screens? While this type of project
has featured previously, with the new
video standards lately, it might be time
for a new version. In order to be versatile, the pattern generator would need
to have outputs for AV, VGA, DVI and
HDMI and be capable of generating 4:3,
16:10 and 16:9 patterns. This might
be a big ask but this device could be
used for testing just about every video
device ever invented.
200Ah, deep cycle, flooded cell, 12V
lead-acid, normally solar-charged
house batteries, a much needed recharge at a maximum of 35A.
However, the ability to employ my
unused 3kVA generator to quickly
bulk charge my batteries means a
rugged battery charger would be
nice (see article in SILICON CHIP,
April 2013).
eBay had 50 matching 11.5V 4A
iron-core halogen downlight transformers with 45°C thermal cut-out
at $1 each. However, the pickup in
Melbourne only yielded 21 for $20.
So I now have questions regarding
my proposed 14.4V 100A rugged
battery charger.
Is my proposed charger specification achievable? With one of the
transformers connected as an autotransformer to increase the primary
voltage to the other 20 transformers
as per page 91 of May 2013 issue?
With four 35A 400V bridge rectifiers
all paralleled and heatsinked and
with fan cooling?
If I build a second charger and
The other thing I would like to see
is a reasonably simple PCB layout
without the use of microscopic, multilegged SMDs. Keeping the construction simple would make the project
more suitable for a wider range of
readers with varying skills.
The second project I’m thinking of
would be a sine/square wave generator with varying frequency outputs.
There have been several projects of
this nature over the years but many
had very limited ranges. Such a device
connect both in parallel, would the
charge rate be the sum of both or
would one charger take the bulk of
the load as might an individual mismatched transformer? What would
be the maximum current I could
safely pump into such batteries? (T.
H., via email).
• We have some misgivings about
your proposed charger, using so
many halogen lamp transformers
in parallel. It will be a brute to wire
up, will be very bulky and heavy
and will get quite hot, since these
transformers are not very efficient.
You will need to use heavy-duty
wiring and battery cables to suit the
high current output. And you will
definitely need a fan for cooling.
You will need to monitor the batteries quite closely because there is a
major risk of over-charging if the setup is left unattended for more than
a couple of hours. You will need to
check with the battery manufacturer
to determine the maximum recommended charging rate.
would have a wide variety of uses,
from testing audio circuits to testing
CRTs. (B. P., via email).
• Neither of those projects could
be regarded as simple, particularly
not the video pattern generator with
your stipulation of HDMI, DVI, VGA
etc. Commercial equivalents are very
expensive. Apart from that, there is really not much need for such a device.
After all, any PC can do the same job.
Similarly, you can easily obtain a
continued page 103
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.
siliconchip.com.au
September 2014 101
ONLINESHOP
SILICON
CHIP
PCBs and other hard-to-get components available now direct from the S
ILICON CHIP ONLINESHOP
NOTE: PCBs from past ~12 months projects only shown here but there are boards going back to 2001 and beyond.
For a complete list of available PCBs, back issues, etc, go to siliconchip.com.au/shop
REVISED 10 CHANNEL REMOTE CONTROL RECEIVER
JUL 2013
15106133
$15.00
INFRARED TO UHF CONVERTER
JUL 2013
15107131
$5.00
UHF TO INFRARED CONVERTER
JUL 2013
15107132
$10.00
IPOD CHARGER
AUG 2013
14108131
$5.00
PC BIRDIES
AUG 2013
08104131
$10.00
RF DETECTOR PROBE FOR DMMs
AUG 2013
04107131
$10.00
BATTERY LIFESAVER
SEP 2013
11108131
$5.00
SPEEDO CORRECTOR
SEP 2013
05109131
$10.00
SiDRADIO (INTEGRATED SDR) Main PCB
OCT 2013
06109131
$35.00
SiDRADIO (INTEGRATED SDR) Front & Rear Panels
OCT 2013
06109132/3 $25.00/pr
TINY TIM AMPLIFIER (same PCB as Headphone Amp [Sept11])OCT 2013 01309111
$20.00
TINY TIM POWER SUPPLY
DEC 2013
18110131
$10.00
AUTO CAR HEADLIGHT CONTROLLER
OCT 2013
03111131
$10.00
GPS TRACKER
NOV 2013
05112131
$15.00
STEREO AUDIO DELAY/DSP + REVERB UNIT (Feb 2014)
NOV 2013
01110131
$15.00
BELLBIRD
DEC 2013
08112131
$10.00
PORTAPAL-D MAIN BOARDS
DEC 2013
01111131-3 $35.00/set
(for CLASSiC-D Amp board and CLASSiC-D DC/DC Converter board see Nov 2012/May 2013)
LED PARTY STROBE (also suits Hot Wire Cutter [Dec 2010]) JAN 2014
16101141
$7.50
BASS EXTENDER Mk2
JAN 2014
01112131
$15.00
LI’L PULSER Mk2 Revised
JAN 2014
09107134
$15.00
10A 230VAC MOTOR SPEED CONTROLLER
FEB 2014
10102141
$12.50
NICAD/NIMH BURP CHARGER
RUBIDIUM FREQ. STANDARD BREAKOUT BOARD
USB/RS232C ADAPTOR
MAINS FAN SPEED CONTROLLER
RGB LED STRIP DRIVER
HYBRID BENCH SUPPLY
2-WAY PASSIVE LOUDSPEAKER CROSSOVER
TOUCHSCREEN AUDIO RECORDER
THRESHOLD VOLTAGE SWITCH
MICROMITE ASCII VIDEO TERMINAL
FREQUENCY COUNTER ADD-ON
VALVE SOUND SIMULATOR PCB
VALVE SOUND SIMULATOR FRONT PANEL (BLUE)
TEMPMASTER MK3
44-PIN MICROMITE
NEW THIS MONTH:
OPTO-THEREMIN MAIN BOARD
OPTO-THEREMIN PROXIMITY SENSOR BOARD
ACTIVE DIFFERENTIAL PROBE BOARDS
MINI-D AMPLIFIER
MAR 2014
APR 2014
APR 2014
MAY 2014
MAY 2014
MAY 2014
JUN 2014
JUL 2014
JUL 2014
JUL 2014
JUL 2014
AUG 2014
AUG 2014
AUG 2014
AUG 2014
SEP 2014
SEP 2014
SEP 2014
SEP 2014
14103141
04105141
07103141
10104141
16105141
18104141
01205141
01105141
99106141
24107141
04105141a/b
01106141
01106142
21108141
24108141
$15.00
$10.00
$5.00
$10.00
$10.00
$20.00
$20.00
$12.50
$10.00
$7.50
$15.00
$15.00
$10.00
$15.00
$5.00
23108141
$15.00
23108142
$5.00
04107141/2 $10/SET
01110141
$5.00
Prices above are for the Printed Circuit Board ONLY – NO COMPONENTS OR INSTRUCTIONS ETC ARE INCLUDED! P&P for PCBS (within Australia): $10 per order (ie, any number)
PRE-PROGRAMMED MICROS
Price for any of these micros is just $15.00 each + $10 p&p per order#
As a service to readers, SILICON CHIP ONLINESHOP stocks microcontrollers and microprocessors used in new projects (from 2012 on)
and some selected older projects – pre-programmed and ready to fly!
Some micros from copyrighted and/or contributed projects may not be available.
PIC12F675-I/P
PIC16F1507-I/P
PIC16F88-E/P
PIC16F88-I/P
PIC16LF88-I/P
PIC16LF88-I/SO
PIC16F877A-I/P
PIC18F2550-I/SP
PIC18F45K80
PIC18F4550-I/P
PIC18F14K50
UHF Remote Switch (Jan09), Ultrasonic Cleaner (Aug10),
Ultrasonic Anti-fouling (Sep10), Cricket/Frog (Jun12) Do Not Disturb (May13)
IR-to-UHF Converter (Jul13), UHF-to-IR Converter (Jul13)
PC Birdies *2 chips – $15 pair* (Aug13)
Wideband Oxygen Sensor (Jun-Jul12)
Hi Energy Ignition (Nov/Dec12), Speedo Corrector (Sept13),
Auto Headlight Controller (Oct13) 10A 230V Motor Speed Controller (Feb14)
Projector Speed (Apr11), Vox (Jun11), Ultrasonic Water Tank Level (Sep11),
Quizzical (Oct11) Ultra LD Preamp (Nov11), 10-Channel Remote Control
Receiver (Jun13), Revised 10-Channel Remote Control Receiver (Jul13),
Nicad/NiMH Burp Charger (Mar14)
Garbage Reminder (Jan13), Bellbird (Dec13)
LED Ladybird (Apr13)
6-Digit GPS Clock (May-Jun09), Lab Digital Pot (Jul10)
Semtest (Feb-May12)
Batt Capacity Meter (Jun09), Intelligent Fan Controller (Jul10)
USB Power Monitor (Dec12)
GPS Car Computer (Jan10), GPS Boat Computer (Oct10)
USB MIDIMate (Oct11)
USB Data Logger (Dec10-Feb11)
Digital Spirit Level (Aug11), G-Force Meter (Nov11)
Intelligent Dimmer (Apr09)
Maximite (Mar11), miniMaximite (Nov11), Colour Maximite (Sept/Oct12),
Touchscreen Audio Recorder (Jun/Jul 14)
PIC32MX150F128D-501P/T 44-pin Micromite (Aug14) (NEW!)
PIC32MX250F128B-50I/SP Micromite (May14) – also includes FREE 47F tantalum capacitor
PIC32MX250F128B-I/SP
GPS Tracker (Nov13) Micromite ASCII Video Terminal (Jul14)
PIC32MX470F512H-I/PT
Stereo Audio Delay/DSP (Nov13), Stereo Echo/Reverb (Feb 14)
dsPIC33FJ128GP802-I/SP Digital Audio Signal Generator (Mar-May10), Digital Lighting Controller
(Oct-Dec10), SportSync (May11), Digital Audio Delay (Dec11) Level (Sep11)
Quizzical (Oct11), Ultra-LD Preamp (Nov11), LED Musicolor (Nov12)
dsPIC33FJ64MC802-E/P
Induction Motor Speed Controller (revised) (Aug13)
dsPIC33FJ128GP306-I/PT CLASSiC DAC (Feb-May 13)
ATTiny861
VVA Thermometer/Thermostat (Mar10), Rudder Position Indicator (Jul11)
ATTiny2313
Remote-Controlled Timer (Aug10)
ATMega48-20AU
RGB LED Strip Driver (May14)
ATMega48
Stereo DAC (Sep-Nov09)
PIC18F27J53-I/SP
PIC18LF14K22
PIC18F1320-I/SO
PIC32MX795F512H-80I/PT
When ordering, be sure to nominate BOTH the micro required AND the project for which it must be programmed.
SPECIALISED COMPONENTS, SHORT-FORM KITS, ETC
NEW: AD8038ARZ Video Amplifier ICs (SMD)
For Active Differential Probe (Pack of 3)
44-PIN MICROMITE Complete kit inc PCB, micro etc
P&P: FLAT RATE $10.00 PER ORDER#
PCBs, COMPONENTS ETC MAY BE COMBINED (in one order) FOR $10-PER-ORDER P&P RATE
“LUMP IN COAX” MINI MIXER SMD parts kit:
(Jun13)
$20.00
Includes: 2 x OPA4348AID, 1 x BQ2057CSN, 2 x DMP2215L, 1 x BAT54S, 1 x 0.22Ω shunt
LF-HF UP-CONVERTER SMD parts kit:
(Jun13)
$15.00
Includes: FXO-HC536R-125 and SA602AD and all SMD passive components
CLASSiC DAC Semi kit – Includes three hard-to-get SMD ICs:
(Feb-May13)
$45.00
CS8416-CZZ, CS4398-CZZ and PLL1708DBQ plus an accurate 27MHz crystal and ten 3mm blue LEDs
with diffused lenses
ISL9V5036P3 IGBT Used in high energy ignition and Jacob’s Ladder(Nov/Dec12, Feb13) $10.00
2.5GHz Frequency Counter
(Dec12/Jan13)
LED Kit: 3 x 4-digit blue LED displays
$15.00
MMC & Choke Kit: ERA-2SM+ Wideband MMC and ADCH-80+ Wideband Choke
$15.00
(Sept 2014)
(Aug14)
$12.50
$35.00
MAINS FAN SPEED CONTROLLER - AOT11N60L 600V Mosfet
RGB LED STRIP DRIVER - all SMD parts and BSO150N03 Mosfets,
(May14)
$5.00
does not include micro (see above) nor parts listed as “optional”
(May14)
$20.00
HYBRID BENCH SUPPLY- all SMD parts, 3 x BCM856DS & L2/L3
(May 14)
$45.00
USB/RS232C ADAPTOR MCP2200 USB/Serial converter IC
NICAD/NIMH BURP CHARGER
(Apr14)
$7.50
(Mar14)
1 SPD15P10 P-channel logic Mosfet & 1 IPP230N06L3 N-channel logic Mosfet
$7.50
10A 230V AC MOTOR SPEED CONTROLLER
(Feb14)
$45.00
ZXCT1009 Current Shunt Monitor IC
STEREO AUDIO DELAY WM8731 DAC IC and SMD capacitors.
GPS Tracker MCP16301 SMD regulator IC and 15H inductor
SMD parts for SiDRADIO
RF Probe All SMD parts
(Nov13)
$20.00
(Nov13)
$5.00
G-FORCE METER/ACCELEROMETER OR
DIGITAL SPIRIT LEVEL Short form kit (Aug11/Nov11) $44.50
(Oct13)
$20.00
(Aug13)
Same as LF-UF Upconverter parts but includes 5V relay and BF998 dual-gate Mosfet.
LF-HF Up-converter Omron G5V-1 5V SPDT 5V relay
(Jun13)
$5.00
40A IGBT, 30A Fast Recovery Diode, IR2125 Driver and NTC Thermistor
$2.00
(Oct12)
As used in DCC Reverse Loop Controller/Block Switch (Pack of 2)
$5.00
$40.00
(contains PCB (04108111), programmed PIC micro, MMA8451Q accelerometer chip and 4 Mosfets)
IPP230N06L3 N-Channel logic level Mosfets
As used in a variety of SILICON CHIP Projects (Pack of 2)
$7.50
JST CONNECTOR LEAD (Jan12) 2-WAY $3.45 3-WAY $4.50
*All items subect to availability. Prices valid for month of magazine issue only. All prices in Australian dollars and included GST where applicable. # P&P prices are within Australia. O’seas? Please email for a quote
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NIXIE CLOCK KITS
SILICON CHIP July-Aug 2007
Full kits & spare tubes
still available
(For a limited time only)
Phone 0403 055 374; Email glesstron<at>msn.com
KIT ASSEMBLY & REPAIR
VINTAGE RADIO REPAIRS: electrical
mechanical fitter with 36 years experience and extensive knowledge of valve
and transistor radios. Professional and
reliable repairs. All workmanship guaranteed. $10 inspection fee plus charges for
parts and labour as required. Labour fees
$35 p/h. Pensioner discounts available
on application. Contact Alan on 0425
122 415 or email bigalradioshack<at>
gmail.com
KEITH RIPPON KIT ASSEMBLY &
REPAIR:
* Australia & New Zealand;
* Small production runs.
Phone Keith 0409 662 794.
keith.rippon<at>gmail.com
DOWNLOAD OUR CATALOG at
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Ph: (08) 9307 7305 Fax: (08) 9307 7309
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Ask SILICON CHIP
. . . continued from page 101
sinewave generator which will work
with your computer’s sound card. Just
do a Google search.
Ultra-low-power
LED driver wanted
I need to drive a LED from a very low
power source (1-1.2V with 200µA).
siliconchip.com.au
I’m less than a beginner at this stage
and have built a ‘Joule Thief’ which
won’t run that low. I have read about
a Mosfet-based one that may do it and
charge pumps etc (but they are such
small chips and it looks very difficult
to solder them without a microscope).
Do you know of any circuits you could
point me towards? (G. A., via email).
• It depends on what you want from
the LED. If you are saying that you only
have a 1.2V supply and only want to
draw 200µA, then the LED will not
show much past a very dim glow.
That is after the voltage is stepped up
to sufficient voltage to drive the LED.
Typically, indicator LEDs are barely
visible at currents below 1mA. A Joule
Thief will not be able to supply any
more power than is available from
the supply.
If you want the LED to flash, then
that might be achievable since the
overall current will be low but LED
current will be higher during the flash
continued page 104
September 2014 103
LED Causes Car Computer False Alarm
I’m hoping you can help me with
a small problem I have. I recently
had installed an after-market radio
in my BMW X5 and this included
a rear-view camera. The camera
replaces one of the number-plate
lights and has a LED for lighting the
number plate.
The problem is that because of
the lower power consumption of
the LED, the car computer thinks
the number-plate light is blown and
constantly brings up a warning of
“check number plate light” on the
dashboard.
I’m guessing I would need to put
a resistor either in series or parallel
with the LED to get the car computer
to stop nagging me. Can you suggest
a suitable resistor value and should
it be wired in series or parallel? (B.
A., Margate, Tas).
• A 100Ω 5W resistor should be
suitable and should be wired across
the original number plate light connection (not across the camera LED).
Presumably this would also be the
power connection for the camera.
What’s probably happening is that
the current drawn by the camera that
includes the LED is insufficient for
the car computer to accept that the
bulb is not blown.
If a 100Ω 5W resistor doesn’t solve
the problem, use a 47Ω 10W resistor. The resistor should be mounted
so that its heat can be dissipated
without burning any plastic parts.
Mounting it in a small diecast box
would be best and you should ensure
that the leads are insulated from
the case.
The resistor should be secured
against the box to heatsink it. Some
heat resistant epoxy such as JB Weld
can be used to affix it to the case or
you could attach it using suitable
brackets.
Advertising Index
Altronics......................................... 3
Aust. Exhibitions & Events............ 57
Blamey & Saunders Hearing.......... 5
Core Electronics........................... 33
element14.................................... 69
Embedded Logic Solutions.......... 66
Emona Instruments...................... 67
Front Panel Express....................... 9
Futurlec.......................................... 6
Gless Audio................................ 103
Hammond Manufacturing............... 9
Hare & Forbes.......................... OBC
HK Wentworth (Electrolube)......... 65
Icom Australia.............................. 11
Iconic PCB................................... 60
Jaycar .............................. IFC,49-56
Keith Rippon .............................. 103
Keysight Technologies.................. 73
period. An LM3909 can flash a LED
while drawing low current. You can
purchase the IC and get a data sheet
from www.futurlec.com/Linear/LM3909Npr.shtml
BFO wanted for
shortwave listening
Did SILICON CHIP or “Electronics
Australia” ever do a project for an
external BFO to use with a shortwave
receiver? This would resolve amateur
SSB transmissions for listeners.
A useful addition to your web page
would be the ability to search for
projects, using supplied keywords. Of
course, someone has to index the lot.
(D. H., via email).
• We have a very comprehensive
search facility on our website. Just
go to the home page, hover over “Articles” and you will get a choice of
searches: contents, word etc.
If you type “BFO” into the word
search you will get nine results at
www.siliconchip.com.au/Articles/
WordSearch and the relevant one is at
November 2010 at www.siliconchip.
com.au/Issue/2010/November/Highperformance+shortwave+converter
This takes you to a preview of the
November 2010 issue. The relevant
item is in the Circuit Notebook pages
of that issue under the title “High Performance Shortwave Converter”. This
is suitable for AM and SSB reception
from 6MHz to 17MHz.
Note that to access this article, you
SC
need to buy the full issue.
KitStop............................................ 6
LD Electronics............................ 103
LEDsales.................................... 103
Lintek Pty Ltd............................... 63
Master Instruments.................... 103
Mastercut Technologies................ 68
Microchip Technology................... 19
Mikroelektronika......................... IBC
Ocean Controls.............................. 8
QualiEco Circuits Pty Ltd............. 59
Quest Electronics....................... 103
Rohde & Schwarz........................ 71
Satcam......................................... 70
Sesame Electronics................... 103
Silicon Chip Binders..................... 84
Notes & Errata
Playing USB-Stick & SD/MMC Card
Music Without a PC, January 2012:
on page 86, the article states that
the Tenda TD896 requires two 2-pin
JST leads for the audio outputs and
a 3-pin JST lead for the earphone/
speaker outputs. However, the two
2-pin JST headers/leads are for the
earphone/speaker outputs while the
104 Silicon Chip
3-pin header/lead is for the audio
(line level) outputs.
40V Switchmode/Linear Bench Supply, April-June 2014: the parts list
swaps the part numbers for Q6 and
Q7. Q6 is the BC327 and Q7 is the
BC337. This is shown correctly on
the circuit and parts layout diagrams
and on the PCBs we supply.
Silicon Chip Online Shop........... 102
Silicon Chip Subscriptions........... 31
Silvertone Electronics.................. 83
Soltronico Pty Ltd......................... 70
Tronixlabs Pty Ltd....................... 103
Virtins Technology.......................... 7
Wiltronics...................................... 10
Worldwide Elect. Components... 103
siliconchip.com.au
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