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May 2010 1
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Contents
Vol.23, No.5; May 2010
SILICON
CHIP
www.siliconchip.com.au
Features
12 Slash Your Factory/Office Lighting Bill
Want to save up to 50% on your shop/factory/office lighting power bill and get
even more light into the bargain? Here’s how – by Leo Simpson
20 A Look At The TDA7377 Quad 12V Amplifier IC
This versatile amplifier IC can provide four single-ended channels, two bridged
channels or two single-ended channels and one bridged channel. Here’s a
look at how it works – by Nicholas Vinen
How To Slash Your Factory/Office
Lighting Bill – Page 12.
12.
79 Review: Tektronix DMM4050 6½-Digit Multimeter
Full-featured instrument boasts 6½-digit readings, a graphic LCD readout plus
trend plot, histogram, logging and dual measurement mode. Its short-term and
1-year accuracy figures are outstanding – by Nicholas Vinen
Pro jects To Build
26 A Solar-Powered Lighting System
Easy-to-build system combines a 5W solar panel, a 12V SLA battery and a
smart controller with 3-stage charging. It runs the solar panel at maximum
efficiency and is ideal for use in garden sheds, at a camp site or to power
garden lights – by John Clarke
54 Build A Compact 12V 20W Stereo Amplifier
Amplifiers that run from 12V DC generally don’t put out too much power. Not
so with this unit. With a 14.4V supply, it delivers up to 20W per channel into
4-ohm loads at very low distortion – by Nicholas Vinen
Solar-Powered Lighting System
For Gardens & Sheds – Page 26.
66 Low-Power Car/Bike USB Charger
It charges USB devices from a 12V battery and consumes just 160µA on
standby, so it won’t flatten the battery if left connected – by Nicholas Vinen
74 Digital Audio Signal Generator, Pt.3
Final article on this versatile new test instrument has the driving instructions
plus other useful information – by Nicholas Vinen
Special Columns
35 Circuit Notebook
(1) Momentary Switch Teamed With Latching Relay; (2) Digitally-Controlled
Tone Filter; (3) People Counter Uses Light Beam Sensors; (4) Level Translator
For A PIC Programmer; (5) Switching Balanced Microphones Using A Foot
Switch; (6) PICAXE Traffic Light Controller
40 Serviceman’s Log
Build A Compact
12V 20W Stereo
Amplifier – Page 54.
The perils of salvaged computer parts – by the Serviceman
84 Vintage Radio
How AGC works and why it’s necessary – by Rodney Champness
Departments
2
4
53
89
Publisher’s Letter
Mailbag
Product Showcase
Order Form
siliconchip.com.au
90 Ask Silicon Chip
93 Notes & Errata
94 Market Centre
Low-Power Car/Bike
USB Charger – Page 66.
May 2010 1
SILICON
SILIC
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
Mauro Grassi, B.Sc. (Hons), Ph.D
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
Mike Sheriff, B.Sc, VK2YFK
Stan Swan
SILICON CHIP is published 12 times
a year by Silicon Chip Publications
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2 Silicon Chip
Publisher’s Letter
Saving energy is not the issue
Back in the April 2007 issue we ridiculed the Federal Government’s proposed ban on incandescent lamps
(introduced by the then Liberal Environment minister
Malcolm Turnbull). In fact, we had a fairly detailed
article on why the whole proposal was impractical.
None of what we said has ever been refuted (nor can
it be) and the amount of energy subsequently saved
in typical households due to the edict is vanishingly
small. Most householders would not be able to identify
any reduction at all from their electricity bills. In fact,
I will wager that most households would now be using more electricity, even if
they have substituted all their incandescent lights, because lighting is a quite
small component of domestic electricity bills.
In the commercial area, in offices, shops and factories, lighting is a bigger
component of energy use, typically around 30%, so it is worth looking for savings. However, most offices and factories use very few incandescent lamps; they
mostly use fluorescent tubes or even more efficient forms of gas discharge lighting. But fluorescent lighting has become more efficient in recent years and this
is the reason for the feature article on slashing lighting energy costs in this issue.
In the first instance, this exercise came about because all the lighting at the
SILICON CHIP offices was looking decidedly dingy. The tubes were overdue for
replacement and all the prismatic diffusers needed cleaning.
The outcome was that we got more light in the office and cut the energy use
by half. But that only means that our total annual electricity use will drop by
about 15%, since we estimate that lighting was about 30% of our total. By the
way, I don’t think the reduction in fluorescent light consumption will have much
effect on our air-conditioning energy. It might reduce slightly in summer but
there would be an equivalent increase in winter and would probably balance
out over the year.
Ultimately, the estimated saving of about $400 a year is hardly worth worrying
about, considering that our annual electricity bill is such a small proportion of
our overall costs. So was it worth doing? Yes, but I would not advocate that all
businesses do it unless they need to change fluoro tubes anyway. And while our
payback period is quite short, it could be quite different in other establishments.
All of which serves to demonstrate that reducing lighting electricity use is only
fiddling in the margins as far as overall energy use is concerned. If Australians
really want to make a large difference in energy use, we would all need to make
very big investments in public transport, drive smaller cars and so on. And while
smaller cars are selling well, there has also been a big increase in sales of SUVs,
so it suggests many consumers are not worried about fuel bills or energy use.
Unfortunately, it seems as though the only way that most consumers, and
the country as a whole, will ever make a significant reduction in energy use is
by governments taking action. But any action will need to be far more credible
than the ban on incandescent lamps, subsidised installation of roof insulation,
free energy audits, subsidised replacement of hot water systems with solar and
heat pump systems and so on.
As far as electricity consumption is concerned, current Australian government
edicts seem to be driven more by “carbon-pollution” reduction mantras than any
sensible strategy. Those same governments seem to be unconcerned about the
increasing number of coal mines, coal seam gas, natural gas and other schemes
to exploit fossil fuels.
If governments were really concerned about carbon dioxide emissions they
would go to nuclear power. Then nobody would worry about reducing electricity consumption, apart from the question of cost.
Leo Simpson
siliconchip.com.au
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siliconchip.com.au
May 2010 3
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”.
Australia should
recycle e-waste
I wish to comment on the March
issue Publisher’s Letter on the topic
of e-waste.
Being a prosperous country also
means we could afford to recycle.
Dumping a few million tons of waste
into landfill is equally expensive and
as our population grows so will the
waste. The inference that our prosperity is built on the throughput of
goods from factory (foreign) to landfill
encapsulates much of what is suspect
in our current economic models.
I wonder how many people in
Sydney realise that their garbage is
now compacted into containers and
trained, everyday, to a little town
called Tarago, not far from Canberra.
From the specially-built rail depot it is
then trucked to an old open-cut mine
called Woodlawn.
This solution to Sydney’s garbage
problem has quietly developed over
the last decade and has been promoted
locally as a clean solution: with meth-
Free Insulation
and Green Loans
I have just read your April 2010
Publisher’s Letter on the insulation scheme and I totally agree.
Unfortunately, the Green Loans
program seems to have been even
more mismanaged. There is a Senate
Inquiry and there are horror stories
appearing about how assessors have
been treated. But that is not the real
story. The real story is how bad the
assessments were.
The assessment for my own house
is an example. Total use for my
house was 60,000 litres of water per
year but the report lists 33,000l. It
suggests electric-boosted solar hot
water rather than off-peak and subtly
suggests solar uses zero electricity.
In addition, Victorian kWh to CO2
figures were used for NSW. Victorian
4 Silicon Chip
ane capture to produce power, and a
series of wind turbines around the
area. As it happens Sydney’s water
deficit developed in parallel and the
turbines took on another reason for
their existence.
There is a common theme here with
SILICON CHIP editorials over the last
few years: commentary on obvious
problems thrown up by an unfettered
economic model coupled with rapid
population growth. The commentary
offered, essentially business as usual
and ramp it up, is quite unimaginative.
This uncritical acceptance of the
status quo illustrates the paradox
which climate science presents to the
Editor; accepting the science questions
the status quo. Let’s be quite clear that
the fundamental science, ie, whether a
gas absorbs and re-radiates particular
wavelengths, is as sound as the science that enables the electronic and
material wonder world that ends up
in our spent mines.
I wonder which other aspects of
science the Editor finds questionable.
figures are in fact 30% higher than
NSW.
If I implemented all the water
savings I would be left with 3000l
of water per year to use for drinking
and washing. Replacing my washing machine would cost $1/year in
electricity and 8kg of CO2 with no
water savings listed but they recommended that I replace it anyway.
The raw data they used contained
the following errors: under-floor
insulation was ignored; 13 external
doors were listed for my house (I
have 6); they listed my alarm as
using 100W continuous whereas it
is closer to 10W; my rechargeable
Philips shaver is listed as using
400W for 15 minutes a day (the
power supply is 6W).
Darryl Smith, VK2TDS,
Ingleburn, NSW.
I suspect only those that might jeopardise our ability to fill up holes in
the ground.
Rory Shannon,
Goongerah, Vic.
Comment: it is true that a great deal
of Sydney’s rubbish does end up at
Woodlawn. It is also true that Australia does quite a lot more recycling
than some other western countries.
However, much of what is collected
for paper and plastic bottle recycling
also ends up in landfill simply because
there is no market for it. We suspect
that recycling of e-waste may be similarly non-viable.
As far as science is concerned, certain gases do absorb and re-radiate
particular wavelengths. However,
science has yet to come up with the
answer to the riddle: why has the
large increase in atmospheric carbon
dioxide over the last 15 years not been
accompanied by a corresponding large
increase in global temperatures?
DAB+ sampling rates
not too low
Readers of SILICON CHIP may not
be aware that Poul Kirk entered the
radio broadcasting industry some 38
years ago as a technician at Perth radio
station 6PR. He founded Poul Kirk
Electronics (PKE) in 1975 where he
continued to design and build broadcast studios as well as some recording studio equipment for other radio
stations and recording studio clients.
PKE later concentrated exclusively
on radio station studio equipment
and made and sold a large range of
practical, reliable and durable equipment to government and commercial
broadcasters here in Australia and to
overseas customers.
Many PKE designs became “Broadcast Industry Standards” which set
layout and operational trends, still
current today. He started Elan Audio
in 1995 which still provides quality
audio products to the broadcasting
siliconchip.com.au
industry. I have known Poul at an
industry level for some 20 odd years
and consider him a doyen in the design
and manufacture of quality broadcast
audio equipment. He is extremely
qualified to talk about audio quality.
Whilst I do not disagree that the
audio quality from our DAB Radio
System is “not necessarily beautiful”,
I would like to challenge some statements made in Poul’s letter in the
March issue and provide your readers
with some more information.
Firstly, Australia has adopted the
DAB+ standard for its Digital Audio
Broadcasting service. DAB+ uses AAC
HE V2 (Advanced Audio Coding High
Efficiency Version 2 or AAC+) as the
audio compression system for Digital
Audio Broadcasting (DAB). AAC+
was never designed for high fidelity;
it was designed for high efficiency. In
other words, it has the ability to fit
more audio services, at an acceptable
audio quality, into any given piece
of Band 3 or L Band radio frequency
spectrum, utilising the DAB standard
as a transport mechanism.
DAB+ bit rates of 48 kilobits per
second and higher, with light audio
processing applied, can sound very
good indeed! To talk about the old UK
DAB standard, MPEG 1 Layer 2, in his
article is irrelevant here in Australia.
We just don’t and never will transmit
it. It is an old technology.
Poul claims “DAB+ is better than
DAB but not twice as good”. Unfortunately, in this case, he is simply
Simpler solution
for solar boosting
I write in reply to your suggestion
regarding solar hot water boosting
on page 100 of the April 2010 issue,
whereby you suggested the use of a
timer to switch on the booster element after 4PM. There is an even
simpler approach. Rather than install a timer, all that needs to be done
is to connect the booster element
to the normal tariff supply. When
needed, the existing switch is closed
for a period of only 15 minutes.
Thirty years ago my wife and I
designed and built our house with
energy and water conservation in
mind. We have been using the above
system since then without any trouble whatsoever.
Very rarely, if ever, is the total
capacity of any hot water service
required. If the total water volume is
incorrect. Blind listening tests carried
out under scientifically controlled
conditions by the EBU in Europe and
by the ABC here in Australia show
that 64kb/s DAB+ is perceived to be
the same quality or better than 128kb/s
DAB.
Poul also claims that many listeners
in the UK complain about bit rates.
This is not true – a few very vociferous
listeners complain repeatedly on the
internet, however market research carried out with listeners shows 80% are
satisfied or more than satisfied with the
brought up to the thermostat cut-off
then this is a waste of energy when
not all of the hot water is required.
Less electrical energy is used
and the cost at the normal tariff is
less than the cost of heating a larger
quantity of water than needed at the
off-peak rate. Our solar system has a
capacity of 300 litres.
When we leave on holidays the
household electrical system is
switch
ed off. On returning from
holidays, if the day has been overcast
and the hot water is too cool, it is
only a matter of 15 minutes before
we can have a hot shower.
The only disadvantage is the necessity to remember to switch the
booster off. Perhaps a 15-minute
timed switch could be used in place
of a normal switch.
Col Hodgson,
Wyoming, NSW.
audio quality. Radio is a mass market
medium and the truth is that the mass
market would prefer 20 services at a
quality they are happy with rather
than the four services they would get
if the most demanding (256kb/s) bit
rate discussed by Poul was deployed.
Broadcasters would be irresponsibly
squandering the valuable public resource of radio frequency spectrum if
they did this.
Radio is about broadcasting to
the masses and giving the consumer
what they want. Time and time again
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May 2010 5
Mailbag: continued
Is our government
totally inept?
Just a quick comment on the hot
water heater fiasco. Correct me if I
am wrong, our coal-fired power stations run 24-7 and one of the most
efficient ways to store the unused
electricity generated in the early
hours of the morning is with offpeak hot water services. These are
the very ones that have been ripped
out under the Labour governmentfunded scheme and replaced with
mechanical heat pump hot water
services which run 24-7, need more
maintenance, will not last as long
and are least efficient in the cold of
night. Am I wrong or is our government just totally inept?
Stephen Dyer,
Swan Hill, Vic.
Comment: while we are tempted
to agree that our governments are
inept, the picture is a little more
complicated. Possibly our base-load
power stations are using significantly more coal at night to maintain offpeak hot water than they otherwise
would if this “optional” load was
the consumer has demonstrated they
value choice and convenience over
quality. You only have to look at the
massive uptake of MP3 players around
the world to realise this. Commercial
radio, in particular, has to give the
audience what they want in order to
survive and thrive. In Australia, commercial radio stations are broadcasting
with bit rates as low as 32kb/s and as
high as 96kb/s.
The 64kb/s used by most Australian commercial broadcasters has been
proven to be equal to or better than
the 128kb/s used by UK broadcasters,
which has been shown to be perfectly
acceptable to the vast majority of UK
listeners. It should also be noted that
the national broadcasters, ABC and
SBS, transmit at bit rates of between 48
and 80kb/s depending on the service.
Time spent listening and listener
ratings figures will tell if the audiences
value the higher bit rate services in
Australia and tune into these stations
for longer. If it is demonstrated that
6 Silicon Chip
not being applied. We don’t know
if this is the case or not. Nor do we
know what is the coal consumption
when a power station is simply on
“spinning reserve”.
The best form of electricity storage is already being applied by the
Snowy Mountains Hydro Electric
Commission whereby it buys cheap
electricity at night to pump water
for generation of electricity at peak
demand times.
We should point out that offpeak hot water systems can also
be powered for substantial times
during the day, so if heat pumps are
being substituted, there may be an
overall reduction in energy usage.
Having said that, we think that all
the subsidies which are available to
people to convert their off-peak hot
water systems to solar, heat pump
or gas-fired systems have very little
overall energy benefit compared to
their high cost to the taxpayer.
In other words, as with many government carbon-pollution reduction
initiatives, no cost/benefit analysis
has been done or published.
consumers value the high bit rate services, then other broadcasters would
be foolish not to follow this lead.
However, listeners value content
more than quality, a fact clearly demonstrated by the fact that the most
popular stations in Australian cities
are usually AM services.
A DAB+ multiplex system here
in Australia can fit 18 DAB+ audio
services at 64 kilobits per second at
equal to or better audio quality than the
maximum number of nine DAB audio
services at 128kb/s that could fit into
the same system in the UK.
Try listening to FM or AM radio
whilst driving a car in and around the
CBD of Melbourne and other mainland
capital cities. The multipath distortion
on FM is atrocious and the man-made
interference on AM makes listening virtually impossible. Recently, I
successfully installed a DAB+ radio
receiver in my own vehicle and integrated it into the existing audio system
and antenna system on the car. The
results driving around Melbourne and
its suburbs are excellent!
It should be noted that the big
three vehicle manufacturers here in
Australia are looking to line fit DAB+
receivers into their vehicles within
the next few years, so DAB+ listening
in cars will become more prevalent.
I can now listen to any AM radio station simulcast on DAB+ in crystal clear
digital sound. It is so good that one can
even hear the announcers breathing in
between words. It is like being in the
studio with them. All this is achieved
at a bit rate of somewhere between 32
and 64kb/s depending on the station
you’re listening to at the time. If you
listen to talk-back, sport or news radio
on AM, then DAB+ is for you.
FM stations simulcast on DAB+ are
free from multipath distortion and
man-made interference. Personally, I
find the lighter audio processing used
on DAB+ much easier to listen to than
the heavier audio processing used on
FM. Again, the majority of FM stations
transmit their DAB+ audio at 64kb/s.
The audio quality is very good.
Add to this, a plethora of new radio
services only available on DAB+ for
the listener to consume for free and I
believe Australia is on a winner!
Steve Adler
Woodforde, SA.
GPS car computer
enhancements
I love the GPS Module (GPS Car
Computer, January & February 2010)
and will be building one as soon as I
can source the components.
I would suggest the spare inputs
could be used with piezo gyroscopes
to integrate pitch and roll and an accelerometer to measure G forces. This
way it might be possible to download
a log of an aerobatic sequence and see
how you went; much like the Red Bull
Air Race coverage.
Mark Bolton,
Perth, WA.
NMR spectrometers now use
Fourier Transforms
In reading The Serviceman article
of March 2010, I was reminded of my
early experiences with NMR spectrometers, when I was a PhD student
in Boston, MA, in the early 70s. Fortunately, we were allowed to service
siliconchip.com.au
our own equipment (if we dared) and
I learnt a lot working with a Varian
T-60, whose manuals were well laid
out with plenty of waveforms. NMR
spectrometers are particularly useful
to synthetic chemists and detect atoms
(nuclei) with magnetic spin, a property
which means that they can exist in low
and high energy states in the presence
of a magnetic field.
Fortunately, hydrogen is one such
nucleus and we can deduce a lot about
chemical structure from just where the
signal occurs and how it is split. The
position in the spectrum indicates the
sort of structure in which the hydrogen
may be found and the splitting tells
us about its near neighbours in the
structure.
The need for signal integration
derives from the observation that the
signal intensity is proportional to the
number of hydrogen atoms producing
the signal. To do this you need a very
homogeneous magnetic field as a hydrogen spectrum is only about 10ppm
wide and so several 10-turn pots are
used to adjust the field homogeneity.
Substitute transistor for the
Hacker radio
I have just read the Serviceman’s
March 2010 article in which he discusses repairing a Hacker Sovereign
RP18 radio. He mentions having
problems with the ubiquitous (for
the era) AF117/AF117N transistors.
There were manufacturing issues
with this and other AF*** transistors which has resulted in the failure
of nearly all of them, including “new
old stock” replacements.
A direct replacement transistor
Sample spinning is then used to average out the remaining inhomogeneities. As a result, even with these early
machines, we could resolve spectral
lines 1/1000th of the spectrum width
or better. We soon became adept at
tuning the machine, changing transmitters and receivers so we could use
it to detect fluorine atoms and effecting
repairs, which were greatly aided by
the manuals, although the integrated
circuits probably only contained a
is the NTE160, which is available
reasonably easily from suppliers
here in Australia, one of them being
RS Spares. This transistor does not
suffer from the same manufacturing
problems as the AF117.
I would recommend replacing
all the AF117s with the NTE160 to
prevent seeing this radio back on
the repair bench for the same fault.
Best regards and congratulations
on an enjoyably diverse magazine.
Ron Pond,
Maddington, W.A.
few transistors. However, I did finally
solve one problem which puzzled us
for some time.
In normal use, a recording pen
moves across a chart, drawing out the
signals. Its movement is linked to the
magnetic field so that each signal is
recorded according to its position in
the spectrum. On this occasion, the
pen would be as quiet as long as there
was no signal but as it approached any
signal and passed through it, it became
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siliconchip.com.au
May 2010 7
Mailbag: continued
Frothing at
the mouth
The March issue certainly had
some interesting letters and articles.
I feel that there are some letters in
particular that need replying to.
Your comment to Graham Hunt,
referring to wind generators and
desalination plants, was that there
is in fact nowhere on Earth where
the wind blows continuously, 365
days a year. Those places on Earth
that have the most wind do not have
it at sufficiently high enough speeds
all of the time to generate consistent
power. As for the “roaring forties”,
anyone who has sailed across Bass
Strait knows that the wind does not
blow all the time.
I hope Paul Garson was being
sarcastic and not as silly as the
electricity authority appears to be.
Blackouts are not caused by people
using air-conditioners or plasma
televisions. How dare people in
40°C plus temperatures even think
of cooling themselves down – they
should obviously die from heat
stroke. The real reason for blackouts
is the failure of the power companies
and the Government to adequately
resource the infrastructure required
for the growing population, regardless of how much power is being
used.
Unless people are rich and/or
increasingly noisy. We could find no
fault with the drive mechanism and
its interface and it took me some time
to deduce that one of the 10-turn trim
pots had developed a noisy wiper
contact. This caused small fluctuations
in the magnetic field but as long as no
signal was being detected it made no
difference. As the pen approached a
signal, the field would drift in and out
with the pot noise and this produced
the noise on the chart.
Such machines are now obsolete
and we have moved to superconducting magnets to increase the field
strength, because the signal intensity
increases with the magnetic field and
so less sample is needed. The machines tend to be designated by the
8 Silicon Chip
stupid, they are not and can’t be
wasting power at the extortionate
and increasing charges that are being
levied on them, not because of cost
but greed. This means bigger profits and more money in CEOs’ and
shareholders’ pockets, at everyone
else’s expense.
Commenting on the letter by Rob
Holmes on global warming sceptics,
there has not been a shred of concrete indisputable evidence to show
that what we are experiencing is not
natural. Just because there are higher
or lower (not global warming) temperatures than we have experienced
in the infinitesimally short time we
have been on this planet, does not
offer proof of anything.
Weather patterns, and I say
weather patterns as the term “climate change” is grossly misused by
people who apparently don’t even
understand its definition, have many
external influences, like the Sun and
the effects of axis shift. Not to mention the amount of seismic activity
we have been experiencing over the
last six or so years.
The Earth is releasing pressure
build-up which is normal. This is
responsible for the changes in ocean
levels, not global warming.
However the climate change idiots
do not take any of this into account.
Now we have those clowns in the
hydrogen resonant frequency in MHz,
so the T-60 operated at 60MHz. Even
simple scanning methods, such as I
used, are obsolete and spectra are produced by applying an excitation pulse
and generating the spectrum from a
Fourier Transform of the decay signal.
This has the advantage that many
spectra can be acquired and averaged
before the transform to increase the
signal to noise level.
The T-60 had a button marked CAT
(Computer of Average Transients, if
I remember correctly) but I’ve never
seen one in practice and the time
needed to acquire data would be
prohibitive.
Dr Graham P. Jackman,
Oakleigh East, Vic.
UN and Copenhagen fudging figures
because they are more interested in
covering up their incompetence than
admitting they are wrong.
Nothing we do in this world is
without some risk. If we were afraid
of taking some calculated risk,
we would still be living in caves.
Nuclear power is a safe and clean
energy and it is pretty much the
only answer.
Concerning the article on Digital
TV by Alan Hughes, Australian
television networks, especially the
commercial ones, are anything but
short of funds. They can easily find
hundreds of millions of dollars to
throw at the football alone. However,
they constantly cry poor when people want more Australian programs
or more funding for them. The lack of
imagination in Australian television
programs and movies is an absolute
disgrace.
New Zealand has surpassed us
and no doubt earns much more
through their television shows and
movies than we do. If New Zealand
can make films like Lord of the
Rings, King Kong and District 9,
there is no excuse or reason why
we can’t make films of this calibre
in Australia. Digital television is a
joke. The networks will not pick up
their game unless forced to and we
probably will not see MPEG4 in this
country unless they pushed.
Tony Joyce,
Macquarie Fields, NSW.
Valve & transistor
radio commentary
I always enjoy reading the ‘Serviceman’s Log’ and found his foray
into early valve and transistor radios,
(March 2010), made interesting reading.
The trap of connecting the first
electrolytic capacitor directly to earth
instead of the transformer centre tap
(when back bias is employed) is one
that many restorers have fallen into
and is made easier when a set has
been “fiddled with” or a circuit is not
available. The advice given to him
that the value of the first electrolytic
is important is in fact correct. Valve
manufacturers typically specify a
maximum peak cathode current for
siliconchip.com.au
their rectifiers and their data sheets quote a maximum value
for the first electrolytic in combination with a minimum
value of anode supply impedance to keep this current
within safe limits. The anode supply figure is usually the
impedance of each half of the secondary winding of the
power transformer.
The difference between 16µF and 22µF is of no consequence and is probably overlapped by the tolerances of
the two values. Where trouble starts is when a repairer
decides that “bigger must be better” and fits 47µF or 100µF
units and this can certainly result in a shortened life for
the rectifier valve.
Valve output transformers have a fairly high mortality
rate, often as a result of electrolysis. The laminations are
usually connected to the chassis, at earth potential while
the primary winding has in the order or 250V applied.
Add a little moisture and a leakage path between the two
is soon completed, resulting in failure of the fine wire
used for the winding.
This was a particular problem in some battery sets
where the on/off switch only disconnected the filament
voltage and left the HT permanently connected. One way
to overcome this problem was to remove the potential
difference between the laminations and the winding. The
first method used to achieve this was to mount the whole
output transformer on a panel insulated from earth and
connect the laminations to B+. Some filter chokes were
also mounted in this way for the same reason.
In later years, the transformer manufacturers produced
a range of ‘Isocore’ transformers where the complete
transformer was sealed in pitch and housed in an isolated
metal case with the core internally connected to B+. This
also reduced the number of “nasty surprises” for repairers!
I have not seen a set where the complete loudspeaker is
connected to B+ and maybe the Philips set mentioned in
the article also had some other modifications made to it.
The AF116/7 series of transistors, as used in the Hacker
Sovereign and many other sets of the era, were notorious
for developing shorts between the case shield and the
other electrodes. This appears to have been some form of
metal migration and I am not sure if the problem was ever
solved with these types. The good news is that cutting
off the shield lead can often restore normal operation. A
number of manufacturers who used this series of transis-
tors did not use the shield connection and removed the
lead before assembly. I have not seen an instance on a
radio where removal of the shield connection caused any
stability problems. Since these alloy diffused types are
not plentiful these days, any trick that can extend their
life is worth a try.
By 1968, Philips had re-packaged these transistors in
the smaller TO-72 case as the AF126/7 series. I have not
heard of similar shorts occurring in these types.
Regarding the ongoing failure of the IF amplifier in the
Hacker, the AF117 has a collector-emitter voltage rating
(VCER) of 32V so it seems unlikely that a variation on
Are all oscilloscopes
created equal?
"Cleverscope is still the best out there,
keep up the good work !!!!!" Karl, USA
Signal:
Video color burst,
as presented to an
ADC.
Task: check DC
Ours: We have proper DC offset and 10, 12 or
levels, noise, and Ours
spectral leakage. 14 bit resolution. We digitize over the range 1.2
www.cleverscope.com
siliconchip.com.au
to 1.5V. With the 10 bit ADC the resolution is
0.3/1000 = 300 uV - with 14 bit ADC it’s 18uV!
You see all the detail. The spectral response has
good SNR.
Theirs: They don’t have DC offset, and only 8
bits. They have to digitize over -2V to +2V to
capture this signal. The resolution is
4000/256 = 16 mV - 52x worse than ours.
You don’t see all the detail, and the spectral
response has poor SNR.
May 2010 9
Mailbag: continued
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10 Silicon Chip
the 7V rail could cause the problem.
Perhaps there is another “gremlin”
and maybe we can look forward to a
follow-up article?
Warwick Woods,
Glen Iris, Vic.
More spelling errors
I know that these are not your spelling errors but on the page opposite
Alex Danilov’s letter (SILICON CHIP,
March 2010, page 4) is an advertisement for solar panels which feature
“3.2mm TAMPERED GLASS”. One
would hope that the product’s quality
control is better than that applied by
the copy writer.
Rob Holmes’ letter that follows Alex
Danilov’s one has “global warming
deniers”. No-one is concerned with
the size of these people but there is
a group of “Global Warming DENYERS”. By the way; all three errors will
cheerfully pass a mindless computer
spell checker.
Brian Wilson,
Curtin, ACT.
Most people don’t care
about the latest technology
So Alan Hughes is already bored
with MPEG-2 DVB-T and thinks the
standards should be changed; just
what those of us who’ve already accumulated MPEG-2 digital boxes for
umpteen TVs and VCRs want to hear!
And just how long are digital boxes
producing a 625-line composite video
output going to be available anyway?
When we’re up to MPEG-10? I think
not.
Like most technology pushers, I
think Alan is oblivious to the fact that
most of the population is not only not
interested but find it inconvenient having to constantly change and replace
equipment to suit the whims of these
people. I know it’s a hard concept to
grasp but life actually does go along
just fine with TV channels sharing
the FM band, listening to our AM and
FM radios, watching VHF low-band
transmissions on our analog TV sets
and whatever else the technology
pushers dislike.
Let me ask this question to the technology addicts: is the real quality of
your life really better surrounded by all
these mass-produced, short-lived fads
(or is it more appropriate to call them
“electronic fashion accessories”)? Are
such items a cure for unhappiness or
any other lack of well-being one could
name? Put technology into medicine
where it really can make a difference,
not so people can be shut indoors all
day watching mind-numbing TV and
adding to the obesity epidemic.
The fact is, we already have the
best TV system in the world with
the 625-line PAL transmissions and I
do not know anyone personally who
felt it lacking in quality to the point
of thinking something “better” was
required. In fact, from my experience
installing television aerials, it’s often
hard to convince the customer to go
with a good ghost-rejecting design
rather than one of the cheaper aerials.
Ghost-cancelling and definitionenhancing signals were actually developed for analog TV in the 1980s
but little was heard of them, because
again the consumers weren’t interested. Stereo sound was also a short
lived fad with few actually wanting it.
However, all these add-ons, including
colour, were compatible and viewers
could keep using their existing sets. As
a result, I still can (and do) watch sets
produced in the 1950s, with the additional signals simply being ignored.
My experience in dealing with the
average non-technical consumer is
that the only thing making most people
get digital TV is the fear of the analog
transmissions being turned off. This, of
course, is purely political when in actual fact both systems can operate side
by side indefinitely and keep everyone
happy. Alan and Co can have 1000s
of lines, 3D, IP-addressable brain implants (no need for any display then)
or whatever else is in vogue at the time,
replacing their gear every few months
if that’s what they want, whilst leaving
the decades-old proven and reliable
system for those happy with it.
A case in point: having installed
digital boxes for an elderly neighbour
for this very reason, changing channels is no longer the simple process of
turning the turret tuner to the required
channel or pressing the button labelled
siliconchip.com.au
MacBook review
is too enthusiastic
I am not sure how to phrase this.
As a fairly regular buyer of SILICON
CHIP I have assumed it to be reasonably unbiased and very informative.
The March 2010 review on the MacBook has disturbed my confidence.
This email is from a MacBook Pro
OS 10.5 (ie, Leopard) using Mozilla.
We have various other computers
and systems in the house with IBM
W98, XP, Win7 etc and Linux –
Ubuntu and Debian plus a Puppy
too. So all sorts with various pros
and cons.
This Mac is using a Logitech wheel
mouse because of the inadequacy of
the Mac. We use Mozilla because of
the inadequacy of the Mail program.
We still (after two years) have problems with the Mac printing emails
in super small font (I am over 50)
and we still have problems with
the one corner window expansion
and “dumb” windows compared to
Linux on a Mac and so on.
The worst part was the lack of
help when we first got the Mac, with
horrible phone support and shop
tutorials (my view). We only had
dial-up when we got it although we
do now have broadband.
We found “The Missing Manual”
(by David Pogue from O’Reilly Press)
to be 800 pages of excellent advice
on how to use the secret commands.
The title says all you need to know
about this excellent piece of hardware and design and the “more
excellent” marketing.
I do, however, suggest YOU take
with the channel number. Now, the
only way to do so is via a complicated
remote control which is a hindrance
rather than a convenience.
Initially, my neighbour was under
the impression her sets were too old
and wouldn’t be usable with the DVBT service. This made me wonder how
many sets have been thrown out simply because their owners didn’t know
that a digital box (with external VHF
modulator if necessary) will work on
any set; even one made in 1956!
On a completely different topic,
regarding the Serviceman and his curiosity about the valve radio speaker
siliconchip.com.au
the Mac home (disconnected from
the internet) and try to use it. Read
the Preface of Pogue’s book. It’s not
just me.
Bob Barrett,
via email.
Kevin Poulter replies: I have four
Macs and my wife uses a “vintage”
Mac 9600 on OS 8.5, all used daily.
Until last year I also used a PC daily.
The MacBook got me excited, as
everything works so well. I would
not have written such a glowing test
of any previous Mac.
I’m not sure why you use a wheel
mouse. I like them too but have
not used mine for months, since
mastering the track pad. Mac’s mail
system has suited me for years and
if it displays text too small, this can
be enlarged to huge text in Mail ->
Preferences -> “Fonts and colours”.
I totally understand less than 20:20
vision and there are many ways of
assisting readability, from the new
super-bright screen, to the easy mag
nification of anything by moving
fingers on the track pad, to a choice
in preferences for the computer to
permanently enlarge file names.
Some of your issues are not fully
explained so I cannot comment,
however my Mac’s mail on ADSL2
works well.
With every computer brand
there will be lemons and “learning
curves”. I agree with your complaint
about lack of instructions. That’s
why I chose a long-respected supplier who accepts calls for assistance. I
also read many magazines and am
a member of a Mac club.
transformer laminations being connected to the B+ supply, that is actually
common practice. The reason this is
done is to prevent the primary winding
going open circuit due to electrolysis
caused by the minute leakage currents
flowing between the winding and the
laminations. However, in most such
sets the laminations are insulated from
the mounting clamp. Where the clamp
is live, one could reduce the shock
hazard by connecting the transformer
laminations to B+ through a high value
resistor, eg, 220kΩ, instead of directly.
John Hunter,
SC
Hazelbrook, NSW.
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May 2010 11
Slash your FA
OFFICE LIGHTIN
Most offices, factories and shops waste a lot of money in power
for lighting. How would you like to save up to 50% of your lighting
power bill . . . and get even more light into the bargain? We show
you how – and have the measurements to back it up!
I
n a typical commercial building, lighting accounts for
about 30% of total energy consumption.
Air-conditioning amounts to about 50%, while the
remainder is taken up by office equipment such as computers, copiers, printers and so on. So how can we reduce
overall power consumption?
Over the next few years this question will become far
more pressing as electricity tariffs increase dramatically.
Since air-conditioning is the main energy user, it behoves
the building or office manager to ensure that everything has
been done to minimise energy use. In particular, attention
must be paid to anything which generates heat in summer,
which means the air conditioner has to work even harder
– and use even more energy – to overcome.
Regular servicing of the air-conditioning system (especially cleaning the filters, which you can usually do
yourself), monitoring of temperature settings in winter
and summer, ensuring that doors are kept closed to stop
drafts and so on are all important. Ultimately, measures
like window tinting and double-glazing can provide further
energy savings but the initial investment will be a lot higher.
But cutting lighting energy use is the focus of this article.
This came about for the very practical reason that all the
fluoro tubes in the SILICON CHIP offices obviously needed
replacing.
In most offices, the approach would be to have all the
tubes and starters replaced, together with cleaning the
diffusers. That should be done every few years as a matter
of course but this simple approach will not provide any
energy savings. We were looking for significant savings.
Our first step was to measure the light levels around
the office and it must be stated that they ranged from just
adequate to poor. In an office of about 12 x 8 metres, the
levels ranged from under 150 lux to about 280 lux, at best.
The average level was about 210 lux. The whole area is lit
by 12 twin-36W fittings, more correctly referred to as recessed luminaires (or in the trade as “troffers”) which have
prismatic diffusers.
In our case, as we moved into this building in 2004, the
tubes were probably at least six years, or around 16000
hours old – well overdue for replacement. Not only were
the tubes noticeably down in emission but the prismatic
diffusers were quite dirty.
The second step was to replace the old tubes in two of the
luminaires in my office area with new GE Cool White tubes
which have a colour temperature of 5000°K. These tubes
Inside a traditional (iron ballast) fluorescent fitting, as found in hundreds of thousands of offices, factories and shops
around the country. The two ballasts are in the middle, the power factor correction capacitor is on the right, while the
starters are mounted on the ends. Note the blackening of the tube ends – a sure sign these tubes are on the way out.
12 Silicon Chip
siliconchip.com.au
ACTORY/
NG bill!
are significantly whiter than the old tubes which have the
distinct greenish hue (or “cast”) of conventional fluorescent
tubes. With the new tubes fitted, the light measurement
went from 210 lux to 320 lux. This was much brighter but
then we decided to try some Mirabella Tri-Phosphor tubes,
again with a colour temperature of 5000°K.
These were much brighter again; too bright in fact. So
we opted to have just one Mirabella Tri-phosphor in each
fitting. This gave a light reading of 270 lux, well above what
we had started with.
But we also wanted to try NEC quad-phosphor tubes
which are claimed to be 15% brighter than tri-phosphor
tubes. While slowly becoming more popular, they’re not
the easiest things in the world to buy (as yet, they’re not
in your local supermarket), nor are they cheap.
But we found them in a Bunnings Hardware store and
purchased a couple to try out.
Incidentally, we also found out while shopping around
that it is getting almost impossible to buy older, singlephosphor tubes any more. The vast majority of tubes on the
shelves of both supermarkets and hardware stores were in
fact tri-phosphor. So at least that’s a good start!
We’re getting a bit ahead of ourselves here but we were
so happy with our tests we bit the bullet and purchased a
box of 25 NEC quad phosphor 37W tubes from our local
electrical wholesalers, John R Turk, here in Brookvale. The
cost was $316.25 including GST, or $12.65 per tube. This
might seem expensive for 25 fluoro tubes but it is much
cheaper than buying them retail.
With a single NEC quad-phosphor tube in each luminaire, the light was up dramatically to around 310 lux.
This was great so we then did the same for six twin-36W
By LEO SIMPSON
luminaires – fitting one quad-phosphor tubes for the old
tubes and cleaning all the prismatic diffusers and whitepainted surfaces of the light fitting. This brought about a
dramatic change. The final light reading on my desk was
now 330 lux.
By contrast, here’s a modern fluorescent luminaire fitted with a single electronic ballast (centre-right). Note the absence
of a power factor correction capacitor and starters – they’re not needed with the electronic ballast. The downside of this
particular fitting is that it cannot drive a single tube – you must have two fitted. But they should last longer.
siliconchip.com.au
May 2010 13
Fig.1: The operation of a conventional ballasted fluorescent
light. The yellow trace is the incoming 230VAC waveform
while the blue trace shows the waveform across the
fluorescent tube. The pink waveform is the tube current
while the purple waveform is the product of the tube
voltage and current (power is 36W).
Fig.2: These scope waveforms are taken from a twin36W electronic ballast luminaire. The green trace is the
incoming 230VAC waveform while the yellow trace shows
the overall current. The purple waveform is the product of
the voltage and current (power is 77W).
That’s towards the low end of the relevant Australian
standard for office lighting (see separate panel: “What is the
correct office light level”) but I found that it was more than
enough for normal work. In fact, I found anything much
greater than about 300 lux started to become a problem,
especially when trying to read glossy or even semi-gloss
(ie, coated) magazine pages.
250VAC power factor correction capacitor in the luminaires.
This has been selected to correct the power factor of two
ballasts in the luminaire and it over-compensates when
just one ballast (ie, one tube) is in use.
So in practical terms, we were able to reduce the power
consumption of a twin 36W luminaire from around 90W
to about 48W. The extra wattage compared with the power
rating of the fluorescent tubes themselves (37W) is the
amount of power wasted in the ferromagnetic ballasts.
Pull out a tube!
All of the tests so far had involved twin-36W luminaires
using conventional ferromagnetic ballasts and starters.
And by removing one lamp from each fitting, we obtained
a reduction in power of just under 50%.
Why not exactly 50%? The discrepancy is due to the 8F
BALLAST
ACTIVE
230V AC
NEUTRAL
PFC
TUBE
FILAMENT
Traditional fluorescent
light connection
STARTER
STARTUP
ACTIVE
230V AC
FILAMENT
~350V DC
NEUTRAL
Electronic ballast
fluorescent light connection
OSCILLATOR
AC
CAPACITOR
INDUCTOR
TUBE
RESONANT
CAPACITOR
Compare the traditional fluoro lighting circuit to one with
an electronic ballast. While the electronic ballast looks
much more complicated, there is no starter nor power
factor correction capacitor. Most electronic ballasts power
two 36W tubes (not one as shown here for simplicity). The
tube filaments in an electronic ballast circuit are essentially
ignored – there is certainly no need to heat them.
14 Silicon Chip
Small office tests
In order to do a more controlled test, we decided to repeat
the procedure in a separate office measuring 3.2 metres
square (10.24 square metres), occupied by one Ross Tester.
It was lit by two twin-36W luminaires, although one tube
in one fitting was missing. The initial light measurement
was 270 lux and that rose to 340 lux, with four tubes fitted.
Removing the rather dusty prismatic diffusers increased
the reading to 350 lux.
Cutting to the chase, we removed the tubes from both
fittings and fitted two NEC 37W quad phosphor 5000°K
tubes to the luminaire immediately above the centrally
placed desk. Now, with the lux meter sitting on the desk
(as it was for the previous measurements), the reading
jumped to 380 lux and then increased again to 420 lux with
the prismatic diffuser cleaned and replaced. (Obviously
the diffuser concentrates the light downward, hence the
increase in brightness with it fitted).
Pretty good eh?
So, we have reduced lighting energy use in that small
office from around 180W (with four tubes fitted) to 90 watts.
But wait, there’s more!
Electronic ballasts
While simply replacing tubes with the new quad phosphor units makes a lot of sense, it is not without problems.
First, starters, starter sockets and tombstones (the sockets
in which the tubes sit) can become quite brittle with age and
siliconchip.com.au
Fig.3: by contrast, these waveforms are taken from a twin36W conventional ballast luminaire. Notice that the purple
power waveform is 87.85W, substantially higher than for
the electronic ballast fitting.
Fig.4: the high frequency operation of a single tube in a
twin-36W electronic ballasted fitting. It is being driven at
32kHz and gives about 9 or 10% more light output.
the mere act of changing tubes or starters can fracture them.
Then what do you do? If you’re doing the changeover
yourself in a small office, you might consider replacing
dud sockets but it is a time-consuming and dirty job. It
would certainly not be practical to have the job done by an
electrician, as the labour costs would be high. In any case,
suitable tombstone sockets may not be readily available
(most fittings these days have snap-in sockets made to fit
a specific punch-out).
In this case, you would simply replace the entire luminaire with one using an electronic ballast. These are now
readily available at lighting wholesalers and are actually
cheaper than the identical fittings with conventional ballasts.
The catch is that typical twin-36W luminaires usually
have one electronic ballast driving two tubes; you cannot
operate them with a single tube. And while it is possible
to purchase luminaires with a ballast driving a single tube,
they will not necessarily fit into the same space occupied
by the twin-36W fitting.
But depending on the spacing of the twin-36W luminaires, it may be possible to fit electronic ballast versions
and leave some fittings without any tubes. And that is what
we did in the small office just discussed. We substituted
a twin 36W luminaire with electronic ballast for the two
conventional luminaires.
This leads to two further benefits. First, electronic
ballast luminaires are far more efficient than those with
conventional ballasts. Compared with the 90 or so watts
drawn by a twin-36W conventional ballast version, the
electronic version only draws 77 watts, a power saving
of 15%. Better still, the light output can be expected to
increase by about 9%.
Now why is that?
It’s not magic. In a conventional ballasted fluorescent light
fitting, the light output from the tube varies more or less
sinusoidally at 100Hz, ie, double the 50Hz mains supply
siliconchip.com.au
These two graphs show the spectra of warm white (3000°K)
versus “natural” 5000°K tubes. Notice that there is far more
output at the “blue” end of the spectrum for the 5000°K
tubes. (Courtesy Nelson Lamps Australia, distributors of
NEC fluorescent tubes.)
May 2010 15
Fig.5: this is the same test set-up as in Fig.4 but the
scope is set to display the power waveform (purple
trace) and shows a result of 34W. Depending on how this
measurement is taken, it can vary from around 40W to less
than 25W but the averaged long-term value is around 34W.
Fig.6: this waveform shows the light output from a
ballasted fluorescent tube, measured with a phototransistor.
Notice that the light output is modulated at 100Hz, ie, with
peaks corresponding to twice the 50Hz mains supply
frequency. In effect, the lamp is extinguished 100 times a
second but the persistence of the tube phosphor smooths
this out so that flicker is normally not noticeable.
By contrast, electronic ballasts run the tubes at much
higher frequencies. In the case of the units we purchased,
the drive frequency is around 32kHz.
In effect, there is less variation in the UV radiation from
the mercury vapour in the tube and the phosphors provide
further smoothing. We have included some scope grabs of
the typical light variation from a conventional ballast fitting
and one fitted with electronic ballast.
Interestingly, the light from the electronic luminaire still
exhibits 100Hz modulation, overlaid with a much smaller
modulation at 32kHz. However, the 100Hz modulation is
about half that from the conventional ballast fitting.
So what happened is that when we changed to an electronic ballast luminaire in Ross Tester’s office, the light
reading increased to around 460 lux. By this stage Ross was
asking whether he should be issued with sunglasses and
skin cream for protection from UV exposure. It certainly
is quite bright . . . but he got short shrift!
Electronic ballasts have other side benefits as well. First,
there is no apparent light flicker.
Second, there is no audible hum or buzz which can
be a problem with conventional ballasts. Third, there is
none of that flick, flick, flickity flick when the lights are
first turned on.
Finally, because no starters are involved, they don’t
need to be replaced when they fail (another saving!) and
the ends of the tubes do not blacken so much as they age.
However, there are two minor drawbacks with using electronic ballasts. The first is that if the ambient temperature
is less than 5°C, the tubes may not start reliably. This is a
problem with all fluorescent lights but apparently it is more
pronounced in those fittings which have electronic ballasts.
We have not tested this aspect – not only was it a balmy
autumn (albeit damp) when we did our tests but the last
time it regularly got to less than 5° here on the northern
beaches of Sydney, dinosaurs were dropping dead.
Secondly, the twin-36W electronic ballast luminaire we
tested produced significantly more interference to AM radio
reception than a conventional ballasted fitting. We have
included some scope grabs of the interference waveform
from each type.
Even in this un-retouched photo of a twin fluoro fitting (which really doesn’t do it justice!) you can readily see the light
level difference between a 4200°K tri-phosphor (the tube on the bottom) and 5000°K quad-phosphor (on top). While the
“warmer” colour temperature of the tri-phosphor accounts for some of this difference, the quad phosphor is much brighter.
16 Silicon Chip
siliconchip.com.au
Fig.7: this shows the light output from a fluorescent tube
driven by an electronic ballast. Notice that the light output
is actually higher but still modulated at 100Hz and by about
50% less. It also shows very slight modulation at 32kHz.
This could be a problem if you live in an area where
AM reception is weak. But you’d probably already know
this from interference from all your switchmode supplies!
Colour temperature
All our tests involved fluorescent tubes with a 5000°K
colour temperature. They are noticeably brighter than
Cool White 4200°K or other colour ratings. Their colour
rendering is also quite reasonable with a Colour Rendering
Index (CRI) of 84.
In practice, we found the NEC quad-phosphor Natural
5000°K tubes to be far superior to all other tubes, especially
those labelled Warm White (3000°K).
Total power savings
In all, we replaced the two old tubes in each of 17
twin-36W luminaires with 17 NEC quad phosphor tubes.
The total power saving (including the changeover to one
electronic ballast twin-36W fitting) is around 730 watts.
Considering that these lights are typically on for 10 hours
a day or around 2500 hours per annum, that means a saving
of 1825kWh per annum. At the current tariff of 22c/kWh,
that is a saving of over $400.
Neglecting labour cost for the exercise (because we
would have had to replace many tubes anyway), that means
the payback is less than one year. And the whole office is
considerably brighter into the bargain.
By the way, we have been told by a distributor that the
wholesale cost of NEC quad-phosphor fluorescent tubes is
now actually less than their equivalent tri-phosphor tubes.
So retail prices of quad-phosphor tubes should be coming
down quite soon.
T8 versus T5 tubes
In none of this discussion have we mentioned T5 fluorescent tubes. Hmm, what’s this about T8 and T5 tubes?
Simply put, this nomenclature refers to the diameter of the
tubes in eighths of an inch.
siliconchip.com.au
Fig.8: this is the same waveform as in Fig.7 but with
the scope settings changed to highlight the slight 32kHz
modulation in the light output.
What is the correct office light level?
Insufficient light level in the workplace can cause eye
strain, headaches and possibly induces migraine. And accidents occur more often when workers have difficulty seeing
at less than optimum levels.
By the same token, excess light levels are also not good for
the health and safety of workers. Again, headaches, fatigue,
stress and possibly migraines have been blamed on excessive
light levels in the office. Try reading a newspaper in direct
sunlight, for example and you will agree it’s not comfortable!
Even if there were no ill-effects from excess light levels in
the office, they of course waste a lot of energy. And that’s becoming even more important as electricity costs keep rising.
As you might expect, there is an Australian standard
covering the amount of light required in an office.
AS1680.2.2 suggests that for ordinary office tasks, the
lighting level should be in the range of 300-400 lux at desk
(task) level and 160 lux as a background.
The simple action of moving a desk (to accommodate
other furniture or fittings, for example) may mean that what
was acceptable light level is no longer enough. Or vice versa
of course.
Some applications will require stronger lighting – intensive
manual graphic arts (ie, not on computer screen) such as
drafting, illustrating, etc, may require illumination of up to
750 lux. Tasks involving constant reading, especially from
small type, working with material that is not sharp (eg,
poor photocopies) and similar has a suggested minimum
of 600 lux.
Older workers, too, usually require stronger lighting (ie
more illumination) than younger workers.
And speaking of computer monitors, every graphic artist
will attest that too much illumination (whether from lighting
or natural sources) on a monitor can drastically alter results,
especially where colour rendition and lightness/darkness in
image manipulation is concerned.
May 2010 17
Making the measurements
Quite a few different measurements were made in preparing this
article. First, we measured the light output in the offices with a Digitech
light meter available from Jaycar (Cat QM-1587). This will measure
in lux or foot-candles. In parallel with that, we used Digitech (Jaycar
QM-1580) digital multimeter which includes ranges for measuring lux.
The various oscilloscope measurements posed a number of problems. First, most oscilloscopes can only handle limited input voltages
and we wanted to measure the 230VAC mains voltage waveforms.
These will overload any normal scope with a maximum input range
of 5V/div when used with a 10:1 divider probe. Our solution is to use
our 100:1 divider probe which is a PMK PHV621, made in Germany.
When plugged into an
oscilloscope with probe
sensing, the maximum input range becomes 500V/div. For current and most of the scope
measurements in this article we used a setting of 100V/div. It was used to monitor the
incoming 230VAC 50Hz sine waveform.
We also wanted to monitor the voltage across the fluorescent tubes themselves in both
the conventional ballast and electronic ballast luminaires. This presents several problems.
First, we need to measure the current in the Active-Neutral circuit and this really needs to
be done with an active current probe which can be isolated from the mains circuit. To that
end, we used an Agilent 1147A current probe which has a bandwidth from DC to 50MHz
and a continuous current rating of 15A (50A peak). Conventional current probes for oscilloscopes simply do not have sufficient bandwidth to measure the fluorescent tube operating
frequencies which can range well above 35kHz in luminaires which have electronic ballasts.
The Agilent 1147A current probe is a hybrid unit combining a Hall Effect sensor for
DC measurements and a current transformer for AC measurements. Its output is 0.1V/A
and if connected to an oscilloscope such as the Agilent 5000/6000/7000 series, it will be
automatically sensed and the trace will show amps/div rather than volts/div.
A further complication arose because we wanted to measure and display the voltage
waveform directly across the fluorescent tubes. This is difficult
enough in a conventional ballasted fitting but is more complicated in
fittings with electronic ballasts which operate two tubes from the one
ballast. The solution is to use an active differential probe and in this
case we used a Pintek DP-25. This can handle a maximum voltage
of 1000V RMS on its differential inputs while the maximum voltage
between each input and ground is 600V RMS, ie, more than adequate
to handle the voltages involved when making scope measurements
on the 230VAC mains supply. It has three ranges: x 20, x50 and x200.
For further information on the three items described above, the
high voltage probe, current probe and active differential probe can
be obtained from Trio-Smartcal, 3 Byfield Street, North Ryde, NSW
2113. Phone 1300 134 091. www.triosmartcal.com.au
Other measurements
We also measured power consumption of the various luminaire fittings and this was done with our own Appliance Energy Meter which
was featured as a constructional project in the July & August 2004
issues. In addition, we compared the level and modulation of the light
output of the conventional ballast and electronic ballast fittings. This
was done using a standard phototransistor with a 10kΩ collector load
resistor. These scope waveforms (Figs. 6, 7 & 8) are measured with
the same reference level. We confirmed that not only is the light output
from the electronic ballast fitting higher than the conventional ballast
fitting but that the 100Hz modulation was about half.
Finally, as a crude measurement of electromagnetic interference
from the two types of luminaire, we used a standard portable AM radio
while the interference waveforms were taken from a small coil of wire
in close proximity to the respective fluorescent tubes.
18 Silicon Chip
siliconchip.com.au
Fig.9: the 50Hz interference signal radiated from a
fluorescent tube with conventional ballast. It will be heard
as a characteristic loud buzz in an AM radio.
Hence, a T8 tube is nominally eight eighths or one inch
in diameter and a T5 tube is 5/8-inch. The newer T5 tubes
are claimed to be more efficient than T8 tubes and can only
be run with electronic ballasts. However, if T8 tubes are
similarly run with electronic ballasts, there is no difference
in efficiency in terms of lumens/watt.
In any case, T5 luminaires and T5 tubes are currently a
great deal more expensive than T8s. There is no point in
changing over.
And why not LED replacements?
Some readers may wonder why we have not considered
LED replacements for fluorescent tubes. After all, they are
available overseas, even in a “drop-in” package; that is,
the same size and shape as a conventional fluoro tube and
capable of being driven in the same fittings.
The simple answer is that while the very best of them
can only just match the efficiency of NEC quad-phosphor
tubes (around 100lm/W), they are extremely expensive.
In the next few years that is bound to change.
The next step?
The next step in the power saving saga is to eliminate
those wasteful halogen downlights in our office. We will
bring you more in due course.
SC
Here’s what to look
for on the fluorescent
tubes themselves. Top
is the 3000°K NEC
tri-phosphor, while
below is the brighter
5000°K NEC quadphosphor. Both are
rated at 37W and
both are “T8”, or oneinch diameter, tubes.
Note the absence of
the “HG” (mercury)
marking on the quad
phosphor.
siliconchip.com.au
Fig.10: the 50Hz interference signal radiated from a
fluorescent tube with electronic ballast. It will produce
a lot more interference to AM radio reception.
Simple steps to start saving
(1) At the very least, remove and wash the diffuser
and while it is out, wipe over both the fluorescent
tubes and the inside of the fitting with a damp cloth.
This won’t save you any power but you won’t be
wasting any of the light output from what you’ve got.
(2) Better still, do No.1 but at the same time, replace
the old tubes with tri-phosphor tubes. Again, you’ll
get even more light output for the same power.
(3) Much better again, replace the old tubes with
quad-phosphor tubes. You may well find (as we
did) that you only need one quad-phosphor in
each fitting. That’s an immediate power saving of
50% or more AND more light output than the pair
of old tubes.
(4) Best, replace the whole light fitting (usually
called a “troffer” in the trade) with one fitted with
an electronic ballast AND a quad-phosphor tube.
You can normally do this quite legally yourself because these days, the vast majority of commercial/
industrial fluorescent lighting fixtures are fitted with
a standard 3-pin power plug which mates with a
3-pin socket on the lighting circuit inside the false
ceiling.
You might well ask “why not keep the existing fitting but simply replace the ballast with an
electronic type?” We asked the same question
of our wholesalers and found that the electronic
ballast cost almost as much as a complete fitting
(within a couple of dollars!) . . . and then you have
to pay an electrician to replace it because that’s
something you cannot legally do yourself! So it is
economically unviable.
May 2010 19
A look at the TDA7377
quad 12V amplifier IC
The TDA7377 IC from ST Microelectronics is the main component
of this month’s 12V Mini Stereo Amplifier. It’s not a new chip –
they’ve been making them since at least 1998 – but it is the first
time we’ve used it so it deserves some elaboration. It comes in a
15-pin “Multiwatt” package similar to TO-218 and is available in
both horizontal and vertical mounting packages.
By NICHOLAS VINEN
T
HIS IC is designed for use in car
stereo systems and can provide
four single-ended channels, two
bridged channels or a combination
of two single-ended and one bridged
channel. Maximum power depends
on speaker impedance, supply voltage and channel configuration but
the most useful figures are 4 x 10W
into 2Ω, 4 x 6W into 4Ω and 2 x 20W
into 4Ω.
Noise performance and channel
separation are also quite good. The
S/N ratio is typically close to -100dB
and channel separation is generally at
least 60dB at 10kHz. This is surprisingly good when you consider that all
four power amplifiers share the same
package and power supply pins.
The best features of this IC are its
low distortion (down to 0.02% or less)
and high power. The most basic circuit
for driving two speakers requires just
the IC, five small capacitors, one large
capacitor (for supply bypassing) and
one resistor. It doesn’t get much easier
than that!
The TDA7377 quad amplifier
comes in a 15-pin Multiwatt
package.
Because there are no external gainsetting resistors, this means that the
gain is internally fixed. This is both
a blessing and a drawback – while it
reduces the component count, we can’t
adjust the gain to our liking. However,
their choice of 20dB gain per circuit
is reasonable.
This actually results in 26dB of gain
in bridge mode. The reason is that
in bridge mode, twice the voltage is
placed across the speaker as in singleended mode. This equates to +6dB of
additional gain.
As is typical for integrated amplifiers, there is a standby pin which
allows the amplifiers to be electronically shut down when not in use. In
this condition, the quiescent current
is around 1µA. The standby pin also
prevents clicks and pops during turnon and turn-off, because it either mutes
or un-mutes the signal paths when it
is switched.
Protection
The maximum supply voltage for
the IC is 18V but it can withstand up
to 28V when it is not operating and
spikes of up to 50V for no longer than
50ms. Each channel can deliver up to
3.5A continuously (4.5A peak) and the
maximum dissipation is 36W.
In fact, not only can the IC handle
voltage spikes but it is virtually indestructible if kept within its limits.
Output shorts, excessive current, overheating, inductive and capacitative
loads, short-term open-circuit ground
wiring, reversed battery – none of these
will destroy it, thanks to internal protection circuitry.
The thermal limiting isn’t just a
simple cut-out which disables the
amplifier either. The current limiting
gradually increases with die temperature, so that at first it creates only mild
output distortion while reducing the
dissipation in an attempt to prevent
further temperature increases.
If driven hard enough it will eventually lead to heavy clipping but this is a
nice feature. The amplifier can still be
used if it is approaching its junction
limits and if the overload is temporary
or marginal, the listener may not even
notice.
Implementation
While implementing an amplifier
with this IC is simple, there are a few
tricks. Firstly, because it is optimised
for bridge configurations, two of the
amplifier circuits are inverting and two
are not. This means that if you want
20 Silicon Chip
siliconchip.com.au
Vcc
B
Vcc
C
Q1
DRIVER
E (NPN)
B
B
+
Vbias
B
C
Q3
POWER
E (NPN)
+
Q1
DRIVER
E (NPN)
Q3
POWER
C (PNP)
Vbias
–
–
IN
OUT
IN
OUT
+
+
Vbias
Vbias
B
–
E
B
C
E
Q4
POWER
C (PNP)
–
Q2
DRIVER
(PNP)
B
Fig.1: the traditional amplifier output stage consists
of two complementary Darlington transistor pairs in
emitter-follower configuration.
to use them as four separate channels,
you need to reverse the speaker wires
for the two which are being driven
from the inverting amplifiers. That
way, all four outputs are kept in phase.
Care must also be exercised to keep
the power ground and signal ground
lines separate, except where they meet
at the star-earth point.
The purpose of the “SVR” capacitor is not explained in the data sheet
but “SVR” stands for “Supply Voltage
Rejection”. This capacitor filters the
internal half supply in the IC, so that
supply variations do not couple into
the signal paths. This is why it must
be connected to the signal ground. If
connected correctly, the supply voltage rejection figure is in excess of 50dB
at 300Hz.
One feature that we did not use in
our 12V Minis Stereo Amplifier design
is the diagnostic pin. It is an open
collector output which is turned on
during clipping, thermal limiting or
an output short circuit. It can be used
to light an indicator lamp or drive
some kind of fault display. Alternatively, a circuit can be added to engage
dynamic range compression if high
volume is causing the outputs to clip.
Clipping can be distinguished from
other faults by noting the duration of
the diagnostic output pulses or by
measuring the average current sunk
E
B
C
Q2
DRIVER
(PNP)
DARLINGTON OUTPUT STAGE
siliconchip.com.au
C
E
C
Q4
POWER
E (NPN)
COMPOUND OUTPUT STAGE
Fig.2: the compound pair output stage configuration.
It’s advantage is that is has a greater voltage swing
than the Darlington arrangement shown in Fig.1.
by that pin. Shorter pulses indicate
clipping, longer pulses are caused by
short circuits or thermal limiting.
Output stage
The most interesting feature of the
IC is its output stage. It achieves a
true rail-to-rail swing (minus transistor saturation at high currents) with
no possibility of oscillation and yet
doesn’t introduce high levels of distortion. Let’s see how they did it.
Integrated amplifiers like the TDA
7377 are sometimes referred to as
“power op amps”. The main difference
between an amplifier IC and an op
amp is the amount of current they can
deliver. The TDA7377 can be likened
to a high power rail-to-rail op amp.
There are two different types of railto-rail op amps. The first is usually
referred to as just “rail-to-rail” or “RR”
and this means that the output voltage
swing goes very close to both the positive and negative supply. How close
depends on the load – at light loads
(ie, high impedances) it will swing
very close indeed, often to within a
few millivolts. At heavier loads (ie,
low impedances) it may only go within
a half a volt or so, due to resistance
effects in the output transistors.
The second type is usually more
expensive and is called “rail-to-rail
input/output” or “RRIO”. This means
that not only can the output voltage
go close to both supply rails but the
input common mode voltage range
also extends to, or beyond, both rails.
Since in this case we are dealing
with a power amplifier that has a large
fixed voltage gain, the inputs do not
need to extend to the rails. With a gain
of 20dB (a factor of 10), a 1.2V peakto-peak sinewave input signal (424mV
RMS) is enough to drive the outputs to
a full 12V swing. So RRIO is not really
necessary for an AC signal when there
is enough voltage gain.
Traditional output
architectures
A traditional amplifier output stage
consists of two complementary Darlington transistor pairs in an emitterfollower configuration – see Fig.1. This
is very simplified but shows the most
important components. This output
stage can only swing to within about
1.4V of each supply rail, because of
the two base-emitter drops in each
transistor pair. In other words, if VCC
is 12V and the base of Q1 is at 12V, the
emitter of Q3 will be around 10.6V.
If we used this architecture for a 12V
amplifier, the maximum output swing
would be 9.2V peak-to-peak, resulting
in a poor maximum power figure.
Fig.2 shows a similar but arguably
superior configuration. The Darlington
May 2010 21
Vcc
B
B
D1
C
Q1
DRIVER
E (NPN)
+
B
Vbias
–
A
K
B
C
Q3
POWER
E (NPN)
+
C boost
C
Q1
DRIVER
(NPN)
E
E
Q3
POWER
C (PNP)
Vbias
–
IN
OUT
IN
+
R2
R1
OUT
+
Vbias
Vbias
–
Vcc
Vcc/2
B
–
E
Q2
DRIVER
C (PNP)
B
C
C
Q4
POWER
E (NPN)
Fig.3: the boosted “quasi-complementary” arrangement
uses a “boost” capacitor to generate a voltage above
VCC. This is used to drive the upper half of the output
stage and allows the output to swing all the way up to
the positive rail, minus the collector-emitter drop of Q3.
Charge pump
The circuit works by using the
output of the amplifier as a charge
pump. When the output swings low,
the boost capacitor (Cboost) is charged
up to nearly the full VCC voltage via
diode D1 – let’s say to 10V. Then when
the output swings high again, D1 pre22 Silicon Chip
Q2
DRIVER
(PNP)
B
BOOSTED 12V OUTPUT STAGE
pairs have been replaced by compound
pairs, also known as “Sziklai” pairs.
Compound pairs only have a single
base-emitter drop (in the drivers), so
this improves the output swing to more
like 10.6V peak-to-peak.
Some integrated amplifiers use both
these concepts. By using a Darlington
upper stage and a compound lower
stage, both of the high current output
devices are NPN transistors. Silicon
NPN transistors are traditionally better
than their PNP equivalents, although
this is less true now than it once was.
Fig.3 illustrates this arrangement,
which is known as a “quasi-complementary” output stage. It also adds a
“boost” capacitor to generate a voltage
above VCC, which is used to drive the
upper half of the output stage. This
allows the output to swing all the
way up to the positive rail, minus the
collector-emitter drop of Q3, which
depends on the transistor size and
output current.
E
B
C
Q4
POWER
E (NPN)
TDA7377 OUTPUT STAGE
Fig.4: the output stage configuration of the TDA7377.
It’s similar to the compound pair arrangement of Fig.2
but includes local gain. Because the emitters of the
driver transistors are no longer tied to the output, their
base-emitter voltage no longer affects the output swing.
vents the capacitor from immediately
discharging.
Because the voltage across the
capacitor stays the same, when the
output swings up, Q1’s collector does
too. It goes well above VCC if the output
swing is large enough – in this example, nearly 22V. This higher voltage
means that both Q1 and Q3 can be
turned fully on, even when the output
is near VCC.
During the time when the output is
above about 9.5V, the boost capacitor
discharges through Q1 and then Q3’s
base. It must be large enough so that
at 20Hz it won’t discharge below 1.4V
before the output swings back below
9.5V and it is recharged.
This design has an output swing of
11.3V – just one diode drop away from
being rail-to-rail. It’s possible to add
a second boost capacitor for the negative rail but there are other techniques
which provide a full rail-to-rail swing
with a single boost capacitor. They
usually involve making the lower
output pair into an NPN Darlington
and adding a more complex driving
arrangement.
How the TDA7377 does it
Fig.4 is derived from the diagram
in the ST Microelectronics data sheet
and shows the output architecture
used. It’s basically identical to Fig.2
(the compound pair stage) except that
it also includes local gain. The main
advantage is that because the emitters
of the driver transistors are no longer
tied to the output, their base-emitter
voltages no longer affect the output
swing.
Consider the case where the gain set
by the resistors is 10 (as in the IC) and
the output is at +11V. The junction of
R1 and R2 will be at 6 + (11-6)/10 or
6.5V. Thus, it’s only necessary to drive
the base of Q1 up to 6.5V + 0.7V or
around 7.2V in order to turn on Q1
and thus also turn on Q3.
So with this arrangement there is no
problem turning on Q3 until the point
where the output rises to VCC.
Now we can take account of the output transistor saturation and calculate
just how large the output swing will
be. All the previously described output
stages will suffer from transistor saturation, as this depends almost entirely
on the output transistors themselves.
According to the data sheet, the
equivalent resistance in the collectoremitter junctions of Q3 and Q4 is 0.3Ω.
We can calculate that with a 4Ω resistive load and a 14.4V supply, there will
be a maximum of 14.4 / 2 / 4 = 1.8A
flowing through the power transistor.
This will result in a collector-emitter
siliconchip.com.au
drop of 0.3 x 1.8 = 0.54V, meaning that
the output swing under such conditions will be 13.32V peak-to-peak – not
bad at all.
Amplifier stability
Another area where the TDA7377
has improved on previous designs is
with its stability. Virtually all amplifiers with feedback systems – and this
includes op amps – can suffer from
instability. This is because there is
always a signal delay within the amplifier. A change in the input signal does
not immediately result in a change in
the output.
The signal is delayed by various
capacitance effects inside the amplifier, mainly within its transistors.
This delay, in combination with the
negative feedback used to set the gain
and eliminate distortion, can result
in oscillation. The amplifier behaves
a bit like a fish-tailing vehicle – each
corrective input has a delayed effect
and leads to wild over-correction.
As a result, the corrections need to
be damped in order to prevent this
problem.
In an op amp, this is usually done
with an internal compensation ca-
pacitor, although some (such as the
NE5534) require external compensation. If an IC lacks compensation pins,
a small capacitor between the inverting input and output, or between the
two inputs, can do the job.
However they are attached, these
capacitors are configured to reduce
the gain at high frequencies, where
the signal delay is large compared to
the waveform period. As long as the
gain is below unity before the phase
shift exceeds 180°, the amplifier is
usually stable. The difference between
the phase shift at unity gain and 180°
is known as the “phase margin” and
indicates how much extra phase shift
can be added before oscillation will
occur.
For power amplifiers, stability is
achieved differently. A Zobel network
(also known as a “Boucherot cell”) is
typically added to the output. This
consists of a resistor and capacitor in
series connected between the output
and ground. Sometimes an RLC filter
is also added, to isolate the amplifier
from the capacitance of the circuitry
it is driving.
The Zobel network has the effect
of being a frequency-dependent load.
At low frequencies, the capacitor’s
impedance is high, so it has no effect.
However, as frequency climbs, the
impedance drops to a value limited
by the resistor and the loading starts
to become significant.
As a result, the output stage needs
more current to create the same magnitude of voltage swing, reducing the
gain. Thus, high-frequency oscillations are damped.
We’ve already seen how the TDA
7377 avoids the need for an external
boost capacitor or for gain-setting
resistors. In addition, the boffins at
ST Microelectronics have found a way
to avoid the requirement for a Zobel
network.
How did they achieve unconditional
stability? According to the data sheet,
it is partially due to the way the gain
is incorporated in the output stage,
and partly by way of careful control
over the HFE (ie, current gain) of the
output transistors. They have adjusted
this gain (by changing the transistor
geometry) so that it is high enough to
provide sufficient open loop gain for
decent sound quality but low enough
that runs out of steam at high frequenSC
cies before oscillation begins.
Radio, Television & Hobbies: the COMPLETE archive on DVD
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And speaking of the war years, R & H had some of the best propaganda imaginable!
Even if you’re just an electronics dabbler, there’s something here to interest you.
• Every issue individually archived, by month and year
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• A must-have for everyone interested in electronics
Please note: this archive is in PDF format on DVD for PC.
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SILICON
CHIP
If you are seeing a blank page here, it is
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which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Please feel free to visit the advertiser’s website:
dicksmith.com.au
High efficiency solar lighting system with MPPT and
Solar-Powered
Lighting System
Need lighting away from a power source? Try this one: it’s ideal for your
garden, shed or even a camp site. With a 5W solar panel, a 12V SLA
battery and a smart controller, it has 3-stage charging for the battery and
Maximum Power Point Tracking (MPPT) for the solar panel.
Part 1 – By JOHN CLARKE
26 Silicon Chip
siliconchip.com.au
Features
3-stage charging. . .
1[ 12V SLA battery operation
1[ Ideal for LED lighting
1[ Constant current LED
N
o, it’s not the old Irish joke about the bloke who
invented the solar-powered torch!
Solar-powered lighting is ideal where it is impractical or unsafe to install mains-powered lighting. It can
be installed just about anywhere and best of all, running
costs are zero because it uses energy from the sun.
In its simplest form, solar powered lighting comprises a
solar panel, a battery and a lamp that can be switched on
and off. But you do need to ensure that the battery is not
over-charged during the day or over-discharged at night;
so you need some sort of charge and discharge controller.
Fig.1 shows the arrangement of our Solar Lighting Controller. The solar panel, the battery and the lamps connect
to the Controller, allowing full management of charging and
lighting. Additional inputs to the Controller include a light
sensor to monitor the ambient light, a Passive Infra- Red
(PIR) detector and a timer.
For use in garden lighting, the light sensor allows the
lights to switch on at dusk and they can remain lit for a
preset period of up to eight hours, as set by the timer. Alternatively, you may wish to have the lights lit for the entire
night and to switch off automatically at sunrise (subject,
of course, to sufficient battery charge).
For security or pathway lighting, the lights can be set to
switch on after dusk but only when someone approaches
the area.
In this case, a PIR movement detector switches on the
lights while the timer switches off the lights after a predetermined period, typically about one to two minutes but
settable up to the 8-hour timer limit.
For shed lighting, you may opt to switch the lights on
and off using a remote pushbutton switch. They can remain
on until they are switched off again or they can switch
automatically after a preset period, or at sunrise.
Normally the Controller would be set so that the lights
can only come on when it is dark. However, you might want
the lights on during day in a shed and this is also possible.
Table 1 shows a summary of all the lighting options
12V/5W SOLAR PANEL
TEMP SENSING
(NTC1)
LIGHT SENSING
(LDR1)
PIR DETECTOR
12V LAMP
OR LEDS
SOLAR
LIGHTING
CONTROLLER
12V SLA
BATTERY
REMOTE
SWITCH
TIMER
Fig.1: this shows the arrangement of our Solar Lighting
Controller. The solar panel, SLA battery and the
lamps connect to the Controller. Optional inputs to the
controller include a light sensor to monitor the ambient
light, a PIR detector and a timer.
siliconchip.com.au
driver option
PIR, switch or ambient
light turn-on
[ Lamp timer included
[ 5W solar panel with
3-stage battery
charging
1[
1
1
which are selected using jumper links. We’ll look at these
various options later.
Types of lighting
The Solar Lighting Controller can power 12V compact
fluorescent lamps (CFL), halogen lamps and 12V LED lighting. In addition, the Controller can directly drive LEDs
using a constant current driver. Best efficiency is obtained
with three 1W or 3W white LEDs in series.
The actual total wattage of the lights depends on the application. We recommend that the Solar Lighting Controller
be used with up to 10W of lighting when the lights are used
for a maximum of 2.5 hours each day.
Lower wattage lighting can give longer lighting periods.
For example, 3W of lighting can be used for around seven
hours per day.
The restriction on the lighting wattage and usage depends
mainly upon the solar panels and their ability to recharge
the battery each day. The specified 5W solar panel is ideally
suited for recharging a partially discharged 3.3AH battery
during the day, assuming at least six hours of winter sunlight is available.
Summer time will obviously provide more hours of
sunlight for charging but then there will usually be less
need to use the lights because of the reduced night period.
Lead-acid batteries (including SLAs, despite popular
belief to the contrary) will be seriously damaged or rendered inoperative if they are fully discharged and/or left
in a discharged state. Hence, we have included low battery
detection. Should the battery become discharged below
11V, the lights will switch off.
Low standby current
Standby current drain of the Solar Lighting Controller is
low to conserve battery power and this has been achieved
without using special components, apart from the PIR sensor. This sensor is designed for use with battery equipment
where current drain is a major consideration, and is available from Altronics (Cat SX5306). We measured current
drain on our sample unit at 73A from a 12V supply. This
May
ay 2010 27
BATTERY
VOLTAGE
ing will be indicated by a short flash of the charge LED
every four seconds.
CUTOFF VOLTAGE
CUTOFF
POINT
BULK
ABSORPTION
FLOAT VOLTAGE
FLOAT
TIME
CHARGE
CURRENT
TIME
Fig.2: this shows the three charge stages. First is the initial
bulk charge until the battery reaches the cutoff voltage.
Then the absorption stage to fully charge the battery and
then the float charge at a lower voltage to maintain charge.
rises to 1.3mA with movement detection, due to lighting
of the internal detection indicator LED. Overall quiescent
current for the Controller is 2.8mA.
3-stage charging
The Controller charges the SLA battery from the solar
panel in three stages, as shown in Fig.2. First is the “bulk
charge”, applied when the battery voltage drops below
12.45V. This charge cycle applies maximum power from
the solar panel until the battery voltage reaches cut-off at
14.4V, <at> 20°C.
Next is the “absorption” phase where the battery is
maintained at the cut-off voltage for one hour, to ensure
the battery becomes fully charged. After that, the battery
is maintained on “float” charge at 13.5V.
The cut-off voltage for the bulk charge and the float voltage is reduced for temperatures above 20°C, in accordance
with the battery manufacturers’ charging specifications.
Typically, this is 19mV per °C for a 12V battery. So at 30°C,
the voltages are reduced by 190mV, ie, 14.21V and 13.31V
respectively.
Ambient temperature is measured using a NTC (negative temperature coefficient) thermistor located within the
Controller. The monitored ambient temperature should
be similar to that of the battery, provided it is located in
the same area as the Controller. The thermistor can also
be located adjacent to the battery, if required for a more
accurate temperature measurement of the battery.
No charging will occur if the thermistor is shorted or if
it is not connected. This feature is useful when the thermistor is remotely located where the wiring could become
shorted or broken. A LED indicator flashes momentarily
once every two seconds when the thermistor is open circuit
and momentarily once every one second when shorted.
Charging is also indicated using the same LED indicator.
Bulk charge is indicated when the LED is on continuously
while it flashes on for 0.5s and 0.5s off for the absorption
and one second on, one second off during float.
A battery that has been discharged below 10.5V will be
charged using short burst of current until it reaches 10.5V
whereupon the main charge will begin. This initial charg28 Silicon Chip
MPPT & charge optimisation
The Controller optimises the available charge from the
solar panel. As shown in Fig.3, a typical solar panel provides
an output that follows the curve that ranges from maximum
current when the output is shorted (ISC) to maximum voltage when the output is open circuit (VOC).
For the Altronics N0005 panel featured in this article,
ISC is 320mA and VOC is 21.6V. Maximum power is 5.05W
at 290mA and 17.4V.
When we consider the power delivered to the battery,
the story becomes more interesting. If we were to connect
the solar panel directly to the battery, the charge current
would be about 320mA at 12V (3.84W) and about 300mA
at 14.4V (4.32W). Both these values are less than the 5.05W
available from the solar panel at 17.4V.
The solar panel operates at peak efficiency when it is
delivering maximum power. And that is where the Maximum Power Point Tracking (MPPT) aspect of the controller
comes into play.
It is essentially a switchmode step-down power converter,
which couples the available power from the solar panel to
the battery with minimal power loss. At the same time, it
provides 3-stage charging to the battery.
Fig.4. shows how this takes place. Current from the
solar panel flows through diode D1 via Q1. When Q1 is
on, current (i1) flows through inductor L1 into the 470F
capacitor and the battery. The inductor charges (ie, current
rises to its maximum value) and after a short period, Q1 is
switched off and the stored charge in L1 maintains current
flow (i2) via diode D2.
The ratio of the on to off period (duty cycle) for Q1 is
controlled so that the solar panel delivers its maximum
power. The solar panel is not required to supply the peak
current into the inductor as this is drawn from the 470F
reservoir capacitor, C1. Similarly, capacitor C2 acts as a
reservoir to charge the battery when current is not flowing
through the inductor. Incidentally, these capacitors are
low ESR (effective series resistance) types, suited to the
switching frequency of 31.24kHz.
The voltage from the solar panel is monitored by op
amp IC2a while the current is monitored by measuring the
voltage across a 0.1Ω resistor. This voltage is multiplied
by –50 in op amp IC2b. Both op amps feed their signals
I(mA)
290mA
Isc = 320mA
300
MAXIMUM
POWER
200
100
Voc = 21.6V
0
0
2
4
6
8
10
12
14
16 18
17.4V
20
22
24
V
Fig.3: the solar panel provides an output that follows this
curve, ranging from maximum current when the output is
shorted (Isc) to maximum voltage when the output is open
circuit (Voc). For best efficiency it is necessary to operate
the solar panel at its maximum power point.
siliconchip.com.au
Here’s the controller mounted
inside its box. It snaps into place on the
integral PC board supports. The cable glands
on the left side make it fairly water-resistant
but this box is definitely not waterproof!
to microcontroller IC1 which controls the whole circuit.
it cannot provide much current before the voltage drops
significantly. Hence, the input loading for this sensor signal
is 10MΩ .
Note that resistor R2 is not used with the SX5306 PIR
sensor. R2 is included if a standard PIR detector is used.
Many standard PIR detectors include a relay with normallyclosed contact that opens when movement is detected.
With R2 included this provides a pull-up to 5V when the
contact opens.
A 12V power supply for either type of PIR detector is
included.
A pushbutton switch (S1) is monitored by the RB1
Circuit details
The full circuit for the Solar Lighting Controller is shown
in Fig.5 and is based around a PIC16F88 microcontroller,
IC1. It monitors IC2, the PIR sensor, switch S1, light dependent resistor LDR1 (for day/night sensing), the NTC
thermistor and also controls lamp operation via Mosfet Q4.
For PIR operation using the Altronics SX5306 PIR detector, output from the PIR is normally at 0V but when it
detects movement, the trigger output goes high to 4.5V.
Output impedance of this PIR is high, at about 700kΩ, so
A
i1
Q1
D1
L1
K
FUSE
F1
K
+
BUFFER
SOLAR
PANEL
A=1
(IC2a)
C1
470 F
V
BUFFER
I
0.1
siliconchip.com.au
A = –50
(IC2b)
MICROCONTROLLER
(IC1)
D2
A
i2
+
12V
SLA BATTERY
–
C2
470 F
Fig.4: charging the battery from the solar panel uses a switchmode
circuit. Current from the solar panel flows through reversepolarity protection diode D1 via Q1. (D1 also prevents the battery
discharging into the solar panel at night via the internal diode in
Q1). When Q1 is on, current (i1) flows through inductor L1 into
the 470F capacitor and the battery. The inductor charges (ie,
current rises to its maximum value) and after a short period, Q1
is switched off and the stored charge in L1 maintains current flow
(i2) via diode D2.
May 2010 29
input, normally held high at 5V with a 10kΩ pull-up resistor. Pressing the switch pulls the RB1 input low. S1 is
included on the Controller PC board for test purposes but
an external on/off (pushbutton) switch can be connected
as well. The 100nF capacitor at RB1 prevents interference
when long leads are used to an external switch.
Ambient light is monitored using the light dependent
resistor (LDR1) at the AN5 analog input of IC1. The LDR
forms a voltage divider with the series-connected 100kΩ
resistor and VR5 connecting to the 5V supply. In normal
daylight the LDR is a low resistance (about 10kΩ) but this
rises to over 1MΩ in darkness. Therefore the voltage at
the AN5 input will be relative to the ambient light. If the
voltage across LDR1 is below 2.5V IC1 determines it is
daylight; above 2.5V it reads it as dark.
This measurement is made when Mosfet Q6 is switched
on, tying the lower end of the LDR close to 0V. VR5 allows
threshold adjustment of the LDR sensitivity.
pendent on ambient light, according to the LK1 selection.
If PIR operation is selected with LK2 but the PIR detector is not connected to the circuit, then the lamp can only
be switched on with S1.
If LK2 is set to the LDR position, the PIR does not switch
on the lamp – the lamp is switched on at the change of
ambient light, day to night or night to day (again, dependent on LK1).
Link Options
Lamp driver
There are three options available for turning on the LED/
light: (1) only at night, (2) only in daylight or (3) either. The
position of link LK1 selects the first two options, while the
third option operates with the link in the “night” position
but has the LDR left out of circuit.
The lamp can be switched on using the pushbutton
switch S1 (internal or external), provided the ambient light
level is correct according to the selection made with LK1.
When link LK2 is in the PIR position, the lamp can also
be switched on when the PIR detects movement; again de-
Built-in timer
The lamp can also be switched off with a timer or ambient light. The various options are summarised in Table 1.
The lamp “on” period is adjustable using trimpot VR4,
which connects between 5V and the drain of Q6. When
Q6 is switched on, the trimpot is effectively connected
across the 5V supply. The wiper voltage is monitored at
the AN0 input of IC1.
We’ll cover the procedure to set VR4 later.
The Controller includes a constant current lamp driver
which can power LEDs or standard 12V incandescent
lamps. Current control is important for LEDs because with
voltage control, small variations in the supply voltage can
result in large changes in the current flow.
Mosfet Q4 and its associated components form an active
current sink. Q4’s transconductance is varied in response
to the voltage developed across R1, which is proportional
to the lamp current.
IC1’s RB0 output switches on the lamp by applying
Specifications
Lamp driver................................... Constant current LED drive
Lamp current................................. Typically less than 350mA for 1W LEDs or less than 1A for 3W LEDs, or at
2A for 12V halogen and 12V LED lamps
Lamp timer.................................... 2s to 8h. See table 3.
LED driver..................................... Up to 3 white LEDs in series. 1W or 3W types.
Lamp switch on............................. Via ambient light change, PIR sensor and switch
Lamp Switch off ........................... Via ambient light change, timer or switch
Low battery lamp off voltage........ 11V
Quiescent current ......................... 2.8mA
Charging voltage........................... 14.4V at 20°C for main bulk charge and absorption cut-off voltage.
Float is 13.5V <at> 20°C
Compensation............................... Adjustable from 0 to 50mV per °C, reducing charge voltage above 20°C and
increasing below 20°C. No increase below 0°C.
Thermistor warning....................... Open or short circuit (Charge LED flashes 262ms every 2s for open circuit
and 262ms every 1s for short circuit)
Low battery charge....................... At less than 10.5V charging via a 6.25% duty cycle charge burst
(Charge indicator flashes 260ms each 4.2s)
Bulk charge initiation.................... When battery drops below 12.45V or the equivalent of 75% charge
Charge LED indicator ................... Bulk charge: Continuously lit.
Absorption: flashing at 0.5s on 0.5s off.
Float: 1s on and 1s off
Charger.......................................... Charging can start when solar panel is >12V
Charger operation......................... Switch mode power converter at 31.24kHz maintains solar panel operation
at maximum power output.
30 Silicon Chip
siliconchip.com.au
+
100nF
0.1
5W
10k
8
100nF
4
IC2b
100k
1nF
IC2a
100nF
5
6
2
3
ZD2
30V
1W
7
1
IC2: LM358
A
K
10k
100k
R2 -SEE TEXT
2.2k
2.2k
10 F
35V
LK1
+5V
LDR
PIR
LK2
B
10
DAY
E
C
K
A
10k
NIGHT
Q3
470 F
35V
LOW ESR
SOLAR LIGHTING CONTROLLER
S1
10M
+12V
1k
1k
12V/5W
SOLAR
PANEL
100nF
100
K
4.7k
100nF
D3
B
2
9
7
8
15
3
4
1k
A
K
14
AN2
1
10
LED1
RB4
Vdd
G
TP1
TP2
K
CHARGE
A
ZD1
18V
1W
(mV/°C)
+5V
470
100nF
A
K
5
Vss
A
AN6
AN0
AN1
RB5
AN5
K
1N5822
RB1
RB2
RA6
AN4
11
12
13
17
18
TP4
TP3
+5V
K
A
K
ZD1,ZD2
A
D3: 1N4148
VR4
10k
TIMER
VR3
10k
10nF
+5V
100 F
+5V
10
LDR
1
NTC
1
10k
22k
G
1nF
470
2
LED1
VR5
500k
K
A
8
+12V
10nF
100k
VR2
20k
4.7k
SET 5V
VR1
20k
470 F
35V
LOW ESR
L1 100 H 3A
D2
1N5822
IC1
PIC16F88
6 COMPENSATION
-I/P RB0
RA7
AN3
PWM
MCLR
10
Q2
16
E
C
D
Q1 IRF9540
S
Fig.5: the circuit is based around a PIC16F88 microcontroller, IC1. It monitors IC2, the PIR sensor, switch S1, light
dependent resistor LDR1 (for day/night sensing), the NTC thermistor and also controls lamp operation via Mosfet Q4.
2010
SC
EXT
ON/OFF
PIR
SENSOR
–
+
4.7k
22k
A
D1 1N5822
siliconchip.com.au
May 2010 31
IC3
Q5
1k
4
5
5
S
G
S
2N7000
Q6
2N7000
D
D
2
1 4N28
4
IC4
TL499A
+12V
E
C
1
E
B
C
G
–
G
10nF
S
D
S
Q4
IRF540
EXT
LDR
D
COMMON
EXT
NTC
R1
(SEE TEXT)
D
Q1, Q4
VR6 20k
CURRENT
ADJUST
–
Q2,Q3,Q5:
BC337
82k
B
+
12V
12V LAMP
SLA
OR LEDS
BATTERY (SEE TEXT)
+
FUSE
F1
3A
Table 1: Lamp Operation
PIR
(LK1)
LDR
(LK2)
Lamp
ON
Lamp
OFF
In
Night
PIR movement
detection or
with S1 during
night time only
Timer timeout,
S1 or at dawn
In
Day
PIR movement
detection or
with S1 during
day time only
Timer timeout,
S1 or at dusk
In
Night
(LDR1
disconnected)
PIR movement
detection or
with S1 during
day and night
Timer timeout
or S1
Out
Night
Day to night
transition
or with S1,
night only
Timer timeout,
S1 or
automatically at
dawn
Out
Day
Night to day
transition or
with S1,
day only
Timer timeout,
S1 or
automatically at
dusk
Out
Night
(LDR1
disconnected)
S1 during
day or night
Timer timeout
or S1
5V to Q4’s gate, allowing current to flow from its drain
to source. If the current through R1 rises enough for the
voltage across it to exceed 0.6V, transistor Q5 turns on and
reduces Q4’s gate voltage. This reduces the current flow.
A steady state arises so that the voltage across R1 is kept
at approximately 0.6V.
If R1 is 2.2Ω, about 270mA will flow through Q4 and
the lamp. VR6, in combination with the 82kΩ resistor,
acts as a voltage divider, allowing the current flow to be
adjusted upwards. If VR6 is set for maximum resistance
than the voltage across R1 will be 0.76V before Q5 turns
on, allowing up to 345mA through the lamp.
2.2Ω for R1 is suitable for a lamp consisting of three 1W
white LEDs in series. Their combined forward voltage is
about 10.5V. With 0.76V across R1, this means that there
will be 0.74V across Q4 (its minimum drop is around 0.1V
in this case). With this setup, the lamp driver consumes
some 0.51W (1.5V x 340mA) and the LEDs consume a
total of 3.57W. Thus efficiency is about 87%.
If the 270-340mA range is inadequate then R1’s value can
be changed. For 3W star LEDs, use 0.68Ω, which results
in a range of 0.9-1.1A. For standard 12V lamps, the current regulator serves as short circuit protection – a 0.33Ω
resistor allow up to 2A before limiting occurs.
Charging
For charging, we use the switchmode step-down circuit
previously described in Fig.3. Mosfet Q1 is a P-channel
type that switches on with a gate voltage that is negative
with respect to the source. The voltage at Q1’s source (from
the solar panel and diode D1) can range up to about 21V
when the solar panel is not delivering current.
The gate is pulled negative with respect to the source
via transistor Q3, a 10Ω resistor and diode D3. Transistor
Q3 is pulse-width-modulated by the RB3 output of IC1
via a 4.7kΩ resistor.
32 Silicon Chip
When RB3 goes to 5V, Q3 is switched on and pulls the
gate of Q1 low. The Mosfet is therefore switched on.
Transistor Q2 is held off due to its base being held lower
than the emitter via the forward-biased diode D3.
The 10Ω resistor at the collector of Q3 limits initial
zener diode current through ZD1 in the event that the
gate voltage exceeds 18V. This zener protects the gate
from breakdown with excess gate voltage. With extreme
over voltage, transistor Q3 will come out of saturation,
preventing little more than about 20mA current through
the 18V zener diode.
When the output of RB3 is taken to 0V, transistor Q3
switches off and the base of Q2 is pulled to the Q1 source
voltage via a 10kΩ resistor. Transistor Q2 switches on and
pulls the gate of Q1 to the source and so switches off Q1.
The switch-on and switch-off action for Q1 as controlled
by the RB3 output of IC1 is at 31.24kHz.
Battery voltage is monitored at IC1’s AN2 input via
optocoupler IC3 and a resistive divider comprising a 22kΩ
resistor and 20kΩ trimpot, VR2. This divider, or more
properly the trimpot, is adjusted to so that the voltage appearing at AN2 is actually 0.3125 times the battery voltage.
The reason for this is so that the 5V limit of analog input
AN2 is not exceeded – for example, a 15V battery voltage
will be converted to just 4.69V. We’ll cover this procedure
in the setup later.
The resistive divider is not directly connected to the battery but via the transistor within optocoupler IC3, which
connects the battery voltage to the divider whenever the
LED within IC3 is on. The voltage between the collector
and emitter of the transistor has a minimal effect on the
battery voltage measurement, as it is only around 200V.
The divided voltage is converted to a digital value by
the IC’s firmware.
The optocoupler LED is driven from the 5V supply
through a 470Ω resistor and to 0V when Mosfet Q6 is
switched on. The thermistor (NTC1) forms a voltage divider with a 10kΩ resistor across the supply when Q6 is
switched on. The AN6 input to IC1 monitors this voltage
and converts it to a value in degrees Celsius.
At the same time, IC1’s AN1 input monitors the setting
of trimpot VR3, which is also effectively connected across
the 5V supply when Q6 is switched on. The AN6 and AN1
inputs are converted to a mV/°C value, which can range
from 0mV/°C when VR3 is set to 0V to 50mV/°C when
VR3 is set for 5V.
Power saving
As we just mentioned, Mosfet Q6 connects trimpotsVR3
and VR4, the LDR and the NTC to 0V and also powers the
optocoupler LED. Q6 is powered on with a 5V signal from
the RB5 output of IC1. The Mosfet then momentarily connects these sensors to 0V so the IC1 microcontroller can
measure the values. When Q6 is off, these trimpots, sensors
and battery divider are disconnected from the supply to
conserve the power drain from the battery.
One problem with using Q6 to make the 0V connection
for the trimpots, battery and sensors is that these sampled
voltages cannot be measured easily with a multimeter. This
is because a multimeter will not be fast enough to capture
the voltage as Q6 switches on momentarily. And we do
need to measure some of these voltages for setting up.
For example, we need to be able to set VR2 so that the
siliconchip.com.au
Parts List – Solar Powered Lighting Controller
1 PC board coded 16105101, 133 x 86mm
1 UB1 box 157 x 95 x 53mm
4 3-way PC mount screw terminals 5.08mm pin spacing (CON1,CON2)
1 2-way PC mount screw terminals 5.08mm pin spacing (CON1)
1 100H 3A Choke (Altronics L6522, Jaycar LF1272 or equivalent)
1 SPST PC mount tactile membrane switch with 3.5 or 4.3mm actuator (S1) (Altronics S1120, Jaycar SP0602)
1 10kΩ NTC thermistor (Altronics R4290, Jaycar RN3440 or equivalent)
1 LDR with 10kΩ light resistance, 1MΩ dark resistance (Altronics Z1621 or Jaycar RD3480 or equivalent)
4 IP68 cable glands for 6mm cable
2 4.8mm female spade crimp connectors
1 DIP18 IC socket
2 M205 PC mount fuse clips
1 3A M205 fast blow fuse
1 TO-220 U shaped heatsink 19 x 19 x 10mm
1 M3 x 10mm screw, nut and washer
2 PC stakes (TP1,TP2)
1 2-way pin header with 2.54mm pin spacing (TP3,TP4)
2 3-way pin headers with 2.54mm pin spacings (LK1, LK2)
2 jumper shunts for pin headers
1 100mm cable tie
1 100mm length of 0.7mm tinned copper wire or 4 0Ω links
Semiconductors
1 PIC16F88-I/P microcontroller programmed with 1610510A.hex (IC1)
1 LM358 dual op amp (IC2)
1 4N28 optocoupler (IC3)
1 TL499A regulator (IC4)
1 IRF9540 P-channel Mosfet (Q1)
3 BC337 NPN transistors (Q2,Q3,Q5)
1 2N7000 N-channel Mosfet (Q6)
1 IRF540 N-channel Mosfet (Q4)
2 1N5822 3A Schottky diodes (D1,D2)
1 1N4148 switching diode (D3)
1 18V 1W zener diode (ZD1)
1 30V 1W zener diode (ZD2)
1 3mm high intensity red LED (LED1)
Additional Parts (as required)
Capacitors
2 470F 35V (or 50V) low ESR
1 100F 16V
1 10F 35V
6 100nF MKT polyester
3 10nF MKT polyester
2 1nF MKT polyester
Resistors (0.25W 1%)
1 10MΩ 5% 2 100kΩ
4 10kΩ
3 4.7kΩ
2 470Ω
1 100Ω
1 82kΩ
2 2.2kΩ
3 10Ω
1 Altronics low current PIR movement detector
(IR-TEC IR-530LC) (Altronics SX5306)
or
1 PIR movement detector with NC relay contacts
(preferably with 1mA or less standby current
– will also need R2, an extra 100kΩ resistor)
2 22kΩ
4 1kΩ
Resistors (5W)
1 0.1Ω
1 0.33Ω – 3.3Ω (value selected from Table 1)
LEDs
1W white LEDs (Jaycar ZD0424, ZD0426,
ZD0508, ZD0510) (Altronics Z0251, Z0252A)
3W white LEDs (Jaycar ZD0532, ZD0534,
ZD0442, ZD0-0444) (Altronics Z0258A,
0259A
Mini horizontal trimpots (5.08mm pin spacings)
2 10kΩ (103) (VR3,VR4)
3 20kΩ (203) (VR1,VR2,VR6)
1 500kΩ (504) (VR5)
LED drivers (see text; Controller has a LED driver built in)
Jaycar AA0592, Altronics M3310 for 1-6 LEDs
at 1W
Jaycar AA0594 for 1-6 LEDs at 3W (Altronics
M3320 for 1-3 LEDs at 3W)
Miscellaneous
1 12V 3.3AH SLA battery
1 12V 5W solar panel array (Altronics N0005 or N0704,
Jaycar ZM9091 or ZM9026 or equivalent)
Figure-8 wire, solder, 4-way alarm cable.
12V lamps
IP67 3-LED modules (eg Jaycar ZD0490)
MR16 lamps (eg Jaycar ZD-0346-ZD0349)
10W Halogen (eg Altronics Z2400)
12V DC LED Globes (eg Altronics X2150)
siliconchip.com.au
May 2010 33
Internal (above) and external shots of our 3-LED light
which is perfect for this controller. You can just see the
blurry LEDs through the translucent lid in the photo below.
Construction details will follow next month.
battery divider is correct and to measure the timer and
mV/°C values set with VR4 and VR3. In order make these
measurements; Q6 is switched while ever S1 is pressed.
Other power saving methods includes how the charge
LED (LED1) is driven. It is only used to show charging when
there is supply available from the solar panel. Current to
drive the LED is therefore provided from the solar panel
instead of the battery. The only time this LED will light
using battery power is if the thermistor is open or short
circuit. In these cases, the LED flashes these indications
at a low duty cycle, again conserving power.
Op amp IC2 is also powered from the solar panel itself.
This arrangement is suitable because we only want to
measure the solar panel voltage and its current whenever
34 Silicon Chip
the solar panels are generating power.
Power for IC2 is derived from the solar panel via a 100Ω
series resistor. A 30V zener diode limits transient voltages
that could occur in long wiring that connects between the
Solar Lighting Controller and the solar panel. Diode D1
prevents the battery from powering IC2 via Q1’s internal
diode and L1.
Solar panel voltage is monitored using a 22kΩ and 4.7kΩ
voltage divider. A 100nF capacitor filters any transient
voltages or noise that could be induced through long leads
from the solar panel. Voltage is buffered by IC2a and the
output is applied to the AN3 input of IC1. The voltage
divider ratio allows for measurement of up to about 28V
from the solar panel. Should IC2a’s output go above 5V,
the 2.2kΩ resistor limits current into IC1.
Current through the solar panel is measured by voltage
developed across a 0.1Ω resistor. The voltage is only around
30mV with 300mA flowing. Voltage at the negative terminal
of the panel does go (slightly) negative with respect to 0V
when there is solar panel current flow.
This voltage is inverted and amplified by IC2b, which
has a gain of -50. Therefore IC2b’s output will be around
1V per 200mA of current flow from the solar panel. This
output is applied to the AN4 input of IC1 via a current
limiting 2.2kΩ resistor.
Note that the actual calibration of voltage and current
is not overly important. Software within IC1 multiplies
the voltage and current readings obtained at the AN3 and
AN4 inputs to find where the maximum power point is for
the solar panel. This calculation is not after any particular
value but just the maximum in a series of power calculations. It does this calculation periodically once every 20
seconds and varies the on and off duty cycle of mosfet Q1
to find the duty cycle that provides the maximum power
from the solar panels.
Power for the remainder of the Solar Lighting Controller
circuit is from the 12V SLA battery via a TL499A regulator, IC4, a low quiescent current type that can run as a
linear step-down regulator and as a switch mode step-up
regulator.
We have used it as a 12V to 5V linear regulator, with the
output voltage trimmed using VR1. Setting the output to
5V calibrates the analog-to-digital conversion within IC1,
ensuring correct charging voltages for the battery.
Protection against reverse polarity connection of both
the 12V battery and solar panel are included. If the solar
panel is connected with reverse polarity, IC2 is protected
because zener diode ZD2 will conduct in its forward
direction, preventing more than 0.6V reverse voltage
applied across its pin 4 and pin 8 supply rails. Diode D1
prevents reverse voltage being applied to the remainder
of the circuit.
Should the battery be connected back to front, diode D2
will conduct via inductor L1 and the fuse, F1. The fuse
will blow breaking the connection.
Construction next month
That’s a fair amount to digest in one bite but broken
down into functional parts, it’s not that difficult!
Next month, we’ll cover full constructional details and
even show how we made some LED lights to go with the
project.
SC
siliconchip.com.au
CIRCUIT NOTEBOOK
Interesting circuit ideas which we have checked but not built and tested. Contributions from
readers are welcome and will be paid for at standard rates.
This circuit allows an SPST moMer
mentary pushbutton to act as a pushis th v Thom
as
is
on push-off switch, using a DPDT
wi mont
latching (bi-stable) relay. It was
Pea nner of h’s
kA
a
originally intended to allow a single
Inst tlas Tes
r
u
pushbutton switch on the dash of a
men t
t
vintage car to provide a latched function. The relay only draws current when
it is being switched. At other times, the only current
drain on the 12V supply is the leakage current of one
22µF capacitor, which is very low. It works as follows.
Assume that initially the latching relay is in the
reset state, with pins 4 and 6 connected together. In
this state, C2 charges up to +12V via 2.2kΩ resistor
R2 while capacitor C1 remains discharged as it is not
connected to the 12V supply.
If S1 is pressed, C2 discharges via the relay’s “set”
coil, diode D2 and S1. This switches the relay into its
set position, connecting pins 4 and 8. C1 then begins
to charge via R1.
While S1 is being held down, the relay does not
return to the reset position because the current supplied via R1 is insufficient for the coil to latch the
armature. As soon as S1 is released, current no longer
flows though the coil so C1 can finish charging, ready
for the next button press.
Once the relay has switched and C1 has finished
charging, pressing S1 again causes the relay to switch
CON1
+12V
R1
2.2k
RLY1*
6 4 8
R2
2.2k
11
13
9
Momentary switch teamed
with latching relay
2
1
RESET
C1
22 µF
25V
A
15
A
16
SET
C2
22 µF
25V
D2
D1
K
K
S1
* DPDT LATCHING RELAY
(JAYCAR SY-4060 OR SIMILAR)
D1, D2: 1N4004
A
K
back to the reset state via the same process.
The unused set of relay contacts can be used as an
SPST or SPDT switch.
The circuit as shown has been tested with the Jaycar
SY4060 relay. It will work with other DPDT twin-coil
latching relays but the resistor and capacitor values
may need to be adjusted to suit. Relays with lower
resistance coils will need larger value capacitors and
smaller value resistors.
Merv Thomas,
Mutarnee, Qld.
Contribute And Choose Your Prize
As you can see, we
pay good money for
each of the “Circuit
Notebook” items published in SILICON CHIP.
But now there are four
more reasons to
send in your circuit
idea. Each month,
the best contribution published will
entitle the author to
choose the prize: an LCR40 LCR meter,
a DCA55 Semiconductor Component
Analyser, an ESR60 Equivalent Series
Resistance Analyser or an SCR100
siliconchip.com.au
Thyristor & Triac Analyser, with the
compliments of Peak Electronic Design
Ltd www.peakelec.co.uk
So now you have even more reasons
to send that brilliant circuit in. Send it to
SILICON CHIP and you could be a winner.
You can either email your idea to
silicon<at>siliconchip.com.au or post it
to PO Box 139, Collaroy, NSW 2097.
May 2010 35
4
IC3c
13
SO
SCK
1k
2
Vss
4
RS
SI
11
SHDN
CS
3
1
IC2
MCP42010
12
560pF
5 PB1
8 PA0
10 PB0
7 PA1
Vdd
14
1k
1k
2.2k
36 Silicon Chip
K
A
D1-D4: 1N4148
A
D2
NP
2
IC3a
3
LEFT
INPUT
SI
SCK
CS TREBLE
CS BASS
TO MICROCONTROLLER
6
RIGHT
INPUT
5
IC3b
1
7
NP
2.2 µF
K
A
D1
K
+5V
A
D4
K
A
2.2 µF
K
D3
+5V
2.2k
470nF
2.2k
470nF
1k
2.2k
PW1 6
PW0 9
13
SO
SCK
2
3
Vss
4
RS
SI
11
SHDN
CS
12
1
560pF
100nF
22k
9
10
–15V
8
11
13
12
22k
5 PB1
IC1
MCP42010
PW1 6
PW0 9
10 PB0
7 PA1
8 PA0
22k
LEFT
OUTPUT
–15V
100nF
+15V
IC3d
IC3: TL074
14
100 µF
Vcc/2
100nF
14
Vdd
Digitally-controlled
tone filter
2.2 µF
NP
22k
2.2 µF
NP
22k
22k
RIGHT
OUTPUT
+5V
Circuit Notebook – Continued
This circuit is a Baxandall active
tone control filter which can be
driven by a microcontroller. The
micro could also be fitted with an
infrared receiver so that you have
remote control of the treble and bass
levels of a stereo audio signal.
Some of the component values,
such as the 470nF MKT capacitors,
have been changed from a typical Baxandall circuit to better suit
digital potentiometers. Normally we
would use 25kΩ -100kΩ pots for the
bass and treble adjustment but 10kΩ
digital pots perform better than the
higher resistance types.
Digital pots typically run off much
lower voltages than most op amps, in
this case +5V. Hence, a dual supply
is required, with balanced rails for
the op amps and +5V for the digital
potentiometer ICs. Virtually any
audio op amps can be used as long
as the supply rails are suitable.
Op amps IC3a & IC3b buffer the
input signal which is assumed to
be ground referenced. Their outputs
are coupled via 2.2µF non-polarised
capacitors to the Baxandall tone
control network comprising the two
MC42010 digital dual-gang potentiometers and the associated resistors
and capacitors. Diodes D1-D4 protect the digital potentiometers from
excessive signals input, clipping any
signal above about 1.77V RMS (5V
peak-to-peak).
Note that the entire Baxandall
circuit is effectively based around
op amps IC3c & IC3d. These two op
amps are biased to +2.5V, as provided by a voltage divider consisting
of two 22kΩ resistors and bypassed
with a 100µF capacitor.
The bass and treble levels are
controlled via the 4-line digital bus.
Normally, both CS-bar lines are held
at +5V. IC1’s CS-bar line is pulled
low to adjust the bass, while IC2’s
CS-bar line is pulled low to adjust
the treble. The new cut/boost value
is then sent via SPI, with MOSI driving the SI line. A value of 128 gives
a flat response. Higher values (up to
255) provide boost and lower values
(down to 0) cut.
The MCP42010 data sheet documents the SPI commands necessary
siliconchip.com.au
OUT
270Ω
1M
470k
12k
1
2
14
13
12
220nF
6
Dis
8.2k
LDR1
A
IC2a Out
Thr 556
Trg
IC1f
λ
14
Vcc
470nF
2
Rst
4
CV
5
IC1d
9
λ
8
LDR2
220nF
8.2k
12V AC
INPUT
470 µF
25V
LED
6
4
Vcc
PL
CPd
MR
TCu
P3
Q3
P2
Q2
IC3
74192
P1
Q1
K
CLEAR
S1
470Ω
16
11
14
12
A
D1-D4
7 A
K
6 A
K
2 A
K
RLY1
K
D6
Dis
10
Rst
10
9
IC2b Out
12
Thr 556
11
2 CV
8
A
POWER
λ LED1
10nF
1M
13
GND
100nF
9
12k
IN
+5V
5
470k
K
K
3
IC1c
IC1: 7404
D5
REG1 7805
+5V
Trg
1
470nF
15
IC1a
Gnd
7
1
10nF
2
5
P0
Q0
CPu
GND
8
7
TCd
3 A
A
NC
COM
2.2k
K
Q1
2N2222
B
E
13
7805
2N2222
People counter
uses light beams
This circuit keeps track of the
number of people entering and leaving a room or building. The entrance is fitted with two photoelectric beams so that people passing
through will break one beam before
the other. The order differs depending on whether the person is entering
or leaving and a counter is incremented or decremented in response.
If the counter value is non-zero,
a relay is energised. This could, for
example, turn lights on as the first
person enters the room and turn
them off when the last person leaves.
A manual reset button is provided to
correct any miscounts which could
occur if two people pass when breaking the beams.
to set the pot “wiper” position. After
the command has been sent, CS-bar
should be brought high again.
The advantage of the MCP42010
(from www.futurlec.com) is that it
comes in DIP packages and has two
pots in a single IC, with low noise
and crosstalk. It has 256 positions,
which is plenty for this application.
Nicholas Vinen,
SILICON CHIP.
siliconchip.com.au
D1-D4: 1N4148
A
K
D5, D6: 1N4004
A
K
The circuit is based on a 7404 hex
inverter (IC1) with only four sections
used, a 556 dual timer (IC2) and
a 74192 up/down decade counter
(IC3). It works as follows.
LDR1 and LDR2 are positioned
so that when a person enters the
area, the beam to LDR1 is broken
first. Since both sensors will be
in close proximity, a single light
emitter (mounted on the opposite
side of the entrance) can be used to
illuminate both.
When LDR1’s beam is broken, its
resistance increases, bringing inverter IC1f’s input high and generating
a negative pulse at the trigger pin
of IC2a. IC2a is configured as a oneshot timer in order to provide a fixed
pulse duration each time the beam
is broken. When IC2a’s output goes
high, IC3’s counter is incremented.
LDR2 and IC2b form an identical
circuit which decrements the counter when LDR2’s beam is broken.
Since both circuits are triggered
each time a person enters or leaves,
whichever circuit is triggered first
must inhibit the other for a short
period. This is achieved by connecting the inverted output from each
half of IC2 to the opposite reset pin.
NO
C
B
E
GND
IN
C
GND
OUT
As a result, if LDR1’s beam is
broken first, pin 10 of IC2b is temporarily brought low so that when
LDR2’s beam is broken shortly after,
the counter will not be immediately
decremented. The same happens in
reverse if LDR2’s beam is broken
first.
Diodes D1-D4 provide a simple
zero comparator at the output of
IC3. If IC3’s count is non-zero, at
least one of the Q0-Q3 outputs from
IC3 will be held high. In this case,
transistor Q1 is turned on and the
relay is energised. When the counter
returns to zero, IC3’s Q0-Q3 outputs
will be low and so transistor Q1 will
switch off.
Because IC3 is a decade counter,
if more than nine people enter the
area being monitored, the counter
will overflow. If needed, additional
74192 decade counters can be daisychained in order to increase the
maximum number to 99, 999, etc.
Note that it is possible to substitute the more common (and cheaper)
74HC04 and 74HC192 devices for
IC1 and IC3. 74LS04 and 74LS192
are also acceptable substitutes.
Craig Kendrick Sellen,
Carbondale, PA, USA. ($50)
May 2010 37
Circuit Notebook – Continued
Vpp IN
+13V
100k
27k
B
E
C
120k
Vpp
OUT
Q2
BC558
Q3
BC558
100k
E
B
27k
C
47k
4.7k
1k
D1 1N4148
B
C
E
K
Q1
BC548
A
C
Q4
BC548
K
E
ZD1
5.6V
4.7k
10k
B
22k
A
BC548, BC558
ZD1
38 Silicon Chip
2
OUTPUT
TO PREAMP
MIC
INPUT 1
XLR PLUG
(REAR
VIEW)
3
2
XLR
SOCKET
(REAR
VIEW)
1
A foot switch can be used to select
one of two balanced microphones by
controlling a 12V DPDT relay. When
the relay is off (ie, not energised), Mic1
is connected to the output XLR plug
via the normally-closed (NC) contacts.
When the relay is on, Mic2 is connected via the normally-open (NO)
contacts. A 12V DC plugpack drives
LED1 via the 400Ω coil of the relay and
the 2.2kΩ resistor. When the relay is
on, LED1 is off and LED2 is on.
The Jaycar SY4061 DPDT relay
or similar can be used. The 12V DC
plugpack should be rated at greater
than 40mA. Note that the 12V supply
negative connection must not connect
to the pin 1 earth for the XLR sockets
and plug. This is to prevent noise from
being injected into the microphone
lines when switching.
John Clarke,
SILICON CHIP.
C
grammer (bought via eBay) which
would only drive the Vpp line to
11.9V, making reliable programming
difficult.
If the Vpp IN line of the circuit is
driven at normal logic voltages (eg,
3.3V or 5V), its output, Vpp OUT,
will swing between 0V and 5V.
3
Switching balanced
microphones using a
foot switch
E
1
Some PICs require 12.75-13.25V
on the Vpp line to be programmed
correctly. This level translator
circuit was designed to overcome
a shortcoming of a cheap PIC pro-
K
XLR
SOCKET
(REAR
VIEW)
2
Level translator for a
PIC programmer
A
MIC
INPUT 2
3
K
1
A
B
1N4148
However, if the input is brought
above 8V then the output rises to
13V. This way, the IC’s Vpp pin is
not taken above 5V unless it is being
programmed.
When Vpp IN is above 2V, transistor Q4’s base rises above 0.6V, turning it on. Q4 turns on Q3, allowing
current to flow through a 1kΩ resistor and 5.6V zener diode, ZD1. This
forward-biases diode D1 so that its
cathode (and thus the Vpp output)
will be at 5V.
If Vpp IN exceeds 8V, transistor Q1
is turned on. Q1 pulls the base of Q2
low, turning it on and this pulls the
output up to 12.9V. In this condition,
D1 is reverse biased and the 5V level
shifter has no effect on the output.
When Vpp IN is below 2V, all four
transistors are off and the output is
pulled to ground via a 4.7kΩ resistor.
The supply voltage should be
between 12.9V and 13.2V to ensure
that most PICs can be programmed
properly. This can be achieved with
an LM317-based adjustable linear
regulator.
Andrew Partridge,
Toowoomba East, Qld. ($40)
12V
RELAY
COIL
(400 )
12V DC
INPUT
+
2.2k
A
LED2
K
–
FOOT
SWITCH
(PUSH ON/
PUSH OFF)
2.2k
LEDS
A
LED1
K
K
A
Use this simple circuit to select between two balanced microphones
using a foot switch. When the foot switch is open, Mic Input 1 is selected.
Conversely, when the switch is pushed closed, Mic Input 2 is selected.
siliconchip.com.au
REG1 78L05
IN
–
OUT
GND
S1
4
5x
1.2V
RECHRG
100nF
SERIAL
1
22k
G
D
2
3
7
22k
10k
1
Vdd
P3
P1
IC1
P0 PICAXE P2
220
6
P4
Q1
ZTX653
C
B
E
220
3
LAMP2
+
–
C
E
220
5
-08
2 SER
IN
B
Vss
8
LAMP1
+
LAMP3
+
Q2
ZTX653
B
–
C
E
Q3
ZTX653
S
Q4 2N7000
2N7000
PICAXE traffic
light controller
This traffic light controller was
built as part of a fancy dress costume. Three different people wore
a traffic light array (ie, red, amber
and green lamps) based on torches
which used a cluster of white LEDs
with suitable current-limiting resistors and drawing 400mA at 6V.
Cellophane paper was used to
obtain the red, amber and green tint.
A PICAXE chip controls the light
sequencing. Power comes from five
1.2V rechargeable cells, resulting in
a supply voltage of 4.2-7.5V. The
78L05 regulator ensures that the
PICAXE’s 5.5V maximum supply
limit is not exceeded.
As the battery discharges, the IC’s
supply will drop below 5V due to
the 78L05’s dropout voltage but
since it can operate down to 2.7V
this is not an issue.
ZTX653
NOTE: LAMPS INCLUDE MULTIPLE
LEDS AND CURRENT LIMITING
78L05
GND
B
D
G
S
The 2N7000 Mosfet provides reverse supply protection without the voltage drop
of a diode. ZTX653 transistors were chosen for Q1-Q3
because they have a low Vce
saturation voltage (0.25V
at 600mA), maximising the
voltage available for driving
the LEDs.
Depending on how long S1
is held down, four different
functions are available:
(1) < 2 seconds: manually
cycles through colours;
(2) 2-4 seconds: automatically cycle – 10 seconds green,
2 seconds yellow, 10 seconds red;
(3) 4-6 seconds: randomise light
colour and timing;
(4) > 6 seconds: standby – all lights
out, current draw is 2mA.
C
E
IN
OUT
Photo credit: Bernard Golder
The software (TrafficLights.bas)
can be downloaded from the SILICON
CHIP website.
Paul Vaughan,
Christchurch, NZ. ($45)
Looking for real performance?
We explain the why as well as the how-to . . .
160 PAGES
23 CHAPTE
RS
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•
•
•
•
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pub lish ers
of
Intelligen
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turbo timer
I SBN 0958
5229 4 -
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5
8 5229
4
$19.80 (inc GST)
4
TURBO B
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& nit
rous fuel co
ntrollers
6
How engi
ne
Price: Aust. $A19.80 plus $A10 P&P ($A12 P&P NZ; $A18 P&P elsewhere) – see
management
works
the order form in this issue or www.siliconchip.com.au for ordering details.
Order by phoning (02) 9939 3295 & quoting your credit card number; or fax the details to (02) 9939 2648; or mail your
order with cheque or credit card details to Silicon Chip Publications, PO Box 139, Collaroy, NSW 2097.
siliconchip.com.au
NZ $22.00 (inc
GST)
May 2010 39
SERVICEMAN'S LOG
The perils of salvaged computer parts
A little knowledge can be a dangerous thing
so why do people delve into the insides of
computers when they know almost nothing
about them? It can certainly make life
difficult for anyone who has to sort out the
inevitable problems.
My first two stories this month are
from A. F. of NSW. The first concerns
a computer user who definitely didn’t
know what he was doing. Here it is in
his own words . . .
Leon’s computer
Leon hammered on my front door
early one Sunday morning. According
to him, his monitor had just blown up
and he wanted to borrow mine so that
he could complete some urgent work.
I had not yet finished my coffee and
it was Sunday but I don’t charge my
neighbours for my services, in case I
need help from them one day.
I said I would be over in 30 minutes
with my spare flat screen and would
40 Silicon Chip
also take a look at his monitor for him.
When I got there, I found that Leon’s
CRT monitor presented a blank screen,
although the green power LED was on.
“See, it’s dead!”, Leon told me.
I did not want to expose his ignorance too rudely, so I told him that
another test would have to be made
to prove it one way or the other. This
involved unplugging the monitor cable
from the PC’s video card. I did this and
the “No Video Signal” warning immediately appeared in colours on the
screen, so the monitor was in fact OK.
Leon stared in disbelief and said
“But where is the XP start-up screen?”
He really wasn’t following what was
going on.
When I restarted the computer, I noticed an unusual silence from it – there
were no beep codes and no noises from
the hard disk drives. By now, Leon was
also silent and it was time to find out
why the computer was lifeless.
First, I removed the cover and closely examined the mainboard, looking
for any loose power cables or signs of
mechanical damage. It was then that
I noticed that the CMOS battery had
been installed upside down, as I could
see the circle of the insulating material
on the end of the battery. So how had
that happened? It was a strange “fault”
to say the least.
I removed the coin cell and it measured 2.98V under a 1mA load, which
was acceptable. I then re-installed it,
the right way up this time. It didn’t fix
the main problem of course but it was
still a fault that had to be corrected.
Next, I pulled the IDE cables off the
disk drives, explaining to Leon as I did
so that the best way to find the fault
was to simplify things by eliminating the plug-in hardware. There was
still silence from the mainboard, so I
removed the two sticks of dissimilar
RAM. This time, when the machine
was rebooted, there was a beep from
the mainboard, indicating that it was
now working.
By inserting the RAM sticks one at
a time, I soon found which one was
locking up the system and preventing
boot-up. The rest was easy. I reinstalled the good RAM stick, connected
the IDE cables and the monitor and
switched on. The computer immediately sprang to life, the desktop loaded
and after several successful restarts, I
pronounced that it was cured.
So how had this computer worked
with a reversed CMOS battery before
it finally halted with a faulty stick of
RAM? As I replaced the computer
cover, I explained to Leon the details
of this double-fault situation and said
he must be the unluckiest person
around, to have had such a weird
double failure.
So what was going on? It was only
then that finally Leon “fessed” up. He
explained that he had swapped his
mainboard from his old case to a better one he had found on the kerbside
during a council clean-up. During this
process, he had decided to install a
new CMOS battery but hadn’t realised that it could be installed upside
down. He had also decided to fit the
siliconchip.com.au
stick of RAM that was in the kerbside
computer into his own computer. It
fitted, so why not?
And so the mysteries ended. So
much for his original story of his monitor blowing-up! If he had told me the
full story in the first place, he would
have saved me a lot of time and effort!
I tried hard not to show my annoyance at being made a sucker, while
thinking that if I were charging him, a
threefold increase in the price would
have made me feel much better.
My neighbour Wally
Wally is undoubtedly the best neighbour I have. He is the kindest, hardestworking person I have ever known, a
truly “Bonzer Bloke”. When the steel
frame on my gate snapped during a
windstorm, Wally came around with
his arc welder on wheels, without me
even asking for his help.
Now it had been some years since I
had used a single phase welder at my
house and when Wally had trouble
striking the arc, it took me several
minutes to realise that he had blown
the 15A fuse. I crossed my fingers, gave
a silent prayer to the Patron Saint of
Housefires that my house would not
be consumed in a fireball, and used
a double strand of 15A fuse wire. I
swear I heard the arc welder give a
sadistic hum of pleasure before there
was a bang and molten copper balls
and smoke erupted from the fuse box.
Silence echoed through the house.
Wally’s solution was to use a sixinch nail instead of a fuse but I knew I
had already used up my prayer quota.
I then remembered that before the new
gas stove had been installed in our
kitchen, we had an electric stove and
this used a 30A fuse. When the stove
had been removed, the 30A fuse had
been changed to 15A and the wiring
had been terminated in an ordinary
15A wall socket.
I refitted the 30A fuse and Wally’s
welder sprang into life. Wally always
looked at peace when he had a cloud
of smoke floating around his head from
the welder electrode. And with 30A
of juice at his disposal, my gate was
soon repaired.
But of course, what goes round
comes round and when Wally asked
for my help with the wiring in his old
Transit Van, I readily agreed. What I
didn’t realise was that he had changed
his gearbox from a manual to an automatic and that he wanted me to
change the vehicle wiring, according
to a crude wiring diagram drawn on a
scrap of cardboard by some bloke behind the counter at the wrecking yard.
As an aside, Wally had also fitted a
new engine from the reconditioners
but had forgotten to fill it with engine
oil and seized it. I guess his workmates had nicknamed him “Wally” as
a warning to others that although he
was a good worker, Wally’s lift did not
always ascend to the top floor!
My immediate problem was to
translate the greasy pencil drawing on
a piece of cardboard into a working and
safe gearbox wiring conversion. The
worse part was the vehicle dropping
Items Covered This Month
•
•
•
•
•
Leon’s computer
My neighbour Wally
Grundig Elegance MFW703210/8 (CUC 1934 chassis)
A 5-minute job – not
The forgetful modem
sand into my eyes while I was looking up to find the wiring harness. The
grease on my hands later washed off
easily but it took days before my eyes
ejected all the gritty particles.
I suggested at one stage that maybe
he should wash the vehicle before we
did any further work on it but that just
produced a glazed look in Wally’s eyes.
The cardboard wiring diagram simply showed that the hot lead to the
ignition switch was wired through the
switch on the gearbox. If the gearbox
was in any of the Drive positions or
in Reverse, then there was no power
to the ignition coil or starter solenoid.
Conversely, in Neutral or Park, power
was applied via the switch.
Wally had not driven an automatic
before, so when the conversion was
complete, I had to show him how the
vehicle would only start in Neutral or
Park and not in any of the Drive positions. I also explained that he would
have to have my work and his conversion checked by a registered motor
mechanic, before he could have the
modifications registered with his in-
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May 2010 41
Serr v ice
Se
ceman’s
man’s Log – continued
surance company. But even as I spoke
I again saw that glazed look appear in
Wally’s eyes.
It was two weeks later that I heard
about Wally’s vehicle rear-ender. His
son had reversed the van into his own
car! It took two months to learn the full
story, as Wally always seemed to be out
when I called. Apparently, soon after
I finished wiring the gearbox, Wally
had driven up to the local store for
some cigarettes. When he got there,
he switched the engine off with the
gearbox in Reverse and left it there.
When he returned to the vehicle
it would not start, as it was still in
Reverse. He phoned his son for help,
who brought a handful of clip leads.
Using these, his son bypassed the gearbox interlock, routing power straight
from the battery to the coil and to the
starter solenoid.
The vehicle started and as it did,
Wally’s son blipped the throttle. And
because it was in Reverse, the vehicle
took off backwards and hit the vehicle
behind. Wally’s son was also in no
danger of being a tall poppy.
Of course, Wally was very matter of
fact about it all and was completely
unconcerned as evidenced by that
glazed look in his eyes.
Grundig TV set
My next story is from my own
service bench. I was called out to a
Grundig CRT TV that was dead. Once
again, the owner ignored my advice
that it wasn’t worth fixing and nor
could he be persuaded to bring the set
in himself. That meant that he was up
for a call-out fee on an old CRT set and
42 Silicon Chip
that was before I even started to fix it.
The reason he didn’t want to bring
it in quickly became obvious – his
house was on top of a fairly steep hill
overlooking the ocean. Ever a sucker
for punishment, I manfully climbed
about 1000 steps to reach the entrance,
by which time I probably felt worse
than his telly.
The set was a Grundig Elegance
MFW70-3210/8 (CUC 1934 chassis)
and I was convinced, sight unseen, that
the cause of the problem was corrosion
from the sea air. This had probably affected either the flyback transformer or
the capacitors in the voltage doubler
circuit (or perhaps both).
I also felt sure that when he discovered the cost of these parts, the owner
wouldn’t feel any better than I did!
Anyway, I thought I had better check
my theory before giving him the bad
news. When the set was switched on,
the front-panel LED went from red to
yellow but didn’t quite go to green. The
set was otherwise quite dead with no
+A voltage and yet it showed no signs
of stress or component failure.
I removed the chassis from the cabinet and examined it closely but could
not find any clues. There was nothing
for it – it had to go to the workshop,
minus the heavy CRT and cabinet. I
would have to suss it out there with
dummy loads, etc.
Anyway, I informed the owner of
this and also told him that it could
well be the flyback transformer and
that it could be expensive. I would
prepare a more accurate estimate for
him when I knew more and with that
I renegotiated the 1000 steps down
the mountain precipice, carrying the
chassis and my tools.
Back at the workshop, I ran a few
checks which, strictly speaking, I really could have done at the house had
I been in the mood. However, I was
more comfortable dealing with this
problem in my workshop. At least I
could make a mess on my own bench
and I wasn’t dead with exhaustion
after having climbed all those steps to
Mr Coulton’s castle in the sky. Machu
Picchu would be a snack after that.
I soon discovered that the 2A antisurge fuse (Si60501) measured open
circuit. I could not measure any shorts
in this 350V circuit and the fuse looked
perfect, with no signs of blackening.
So was the problem caused by a power
surge? I replaced the fuse with a shiny
new one and connected the TV to
the mains with a 200W light globe
in series.
I switched it on and the globe lit
brightly – there was a hidden short
circuit after all!
I was convinced that it was either
FET T60506 or a capacitor that was
faulty, so I removed all the likely suspects and checked them. They were all
OK except for a vital clue I found on
the FET heatsink. There was a small
but distinct round mark on it where
the metal had partly melted.
Next, I examined the insulating
washer and discovered a very small
hole/puncture in line with a corresponding mark on the FET. So it looked
like the FET had been arcing across to
the heatsink.
I fitted a new mica washer along
with a liberal smearing of thermal
grease and reassembled it all. This
time the set fired up with the globe
just beginning to glow. The +350V
rail was now OK, as was the +A rail,
siliconchip.com.au
so I removed the 200W globe and fitted it where the
horizontal deflection yoke would normally go.
This time, the chassis fired up without any distress
and all voltage measurements were correct. I resubmitted a cheaper estimate for Mr Coulton which he
gratefully accepted.
I returned to the mountain and reassembled the
chassis back into its case. To my relief, the set fired
up with a good picture and sound, so I collected the
moolah and hiked back to the car. I think my earnings
will be blown on a good physio though!
My next story comes from M. S. of Keilor in Victoria
and strikes a familiar chord.
A 5-minute job – not
ACOUSTICS
SB
We’ve all had customers who claim that a job should
take “no more than five minutes”. It invariably turns
out to be wishful thinking on the customer’s part but
then we all want to minimise labour costs.
I recently got a phone call from a bus company requesting my services. I’d never done any work for them
before and after this job, I’m not in any hurry to hear
from them again. This guy started straight out with the
“it’s only a 5-minute job” routine. “All I want you to
do is wire up the rear mount TV. We’ve wired it every
way possible and it doesn’t work”.
When I got there, sure enough, the TV didn’t work.
It was dead and the reason was quite simple – there
was no power to it. I eventually managed to trace one
of the main earths (negative power) all the way to the
front of the coach but this involved removing most of
the inside overhead panels and the ventilation system.
That was at the 16-hour point of his 5-minute job. The
look on the owner’s face was priceless when he saw
the inside of his coach but there was no other way if I
was going to fix the problem.
I eventually found the problem at the 23-hour point.
It was at the front of the coach and it turned out to be
a rusty earth bolt. And as I discovered, this was also
preventing other electrical items from working properly
although the owner didn’t think to tell me that up front.
Once the problem had been fixed, the TV not only
worked properly but so did all the other electrical items
in the coach, including the fuel gauge!
After about 36 hours, I finally had everything back together and I had an almost happy customer. An invoice
was negotiated and he promptly paid up, although it
was rather more than he originally bargained for. So
much for his 5-minute job – unless you think of it as
432 separate 5-minute jobs strung together!
My final story for the month comes from D. S. of
Maryborough in Qld and concerns a modem that kept
losing its settings. Here it is . . .
dynamica
The forgetful modem
This story began when a friend contacted me and
asked if I could help with her internet connection.
The issue was that the modem would lose the login
information and she would then have to reload this
information into the modem each time she wanted to
access the internet. Thinking it would be a 5-minute
fix, I said that I would pop around that afternoon and
sort it out. How wrong I was.
siliconchip.com.au
May 2010 43
Serr v ice
Se
ceman’s
man’s Log – continued
The modem in question was a DLink DSL-302G. Now this has been
a very successful modem and a large
number are still operating without
problems. It’s a small unit and does
not have all the bells and whistles
that some modems have but it works
very well. This particular model was
supplied by several ISPs to new ADSL
users and as such, the modem was
loaded with that ISP’s own version of
the firmware. In this case, the modem
was supplied by Optus and had the
Optus firmware installed.
First, I checked the PC’s network
and internet settings and checked that
the IP and DNS addresses were correct. Then I opened a CMD window
and using the ipconfig /all command,
checked the LAN and gateway settings.
The returned data told me that all was
well and confirmed that the modem’s
DHCP software was operating and assigning IP addresses as it should.
A quick “ping” command also gave
me the connection speeds and indicated that no data packets were getting
lost. So all was looking good so far. I
then checked all the cables and power
connections and again, everything was
just as it should be.
Now, if the modem was losing its
internal settings, maybe that was a
power supply issue, so I replaced the
original plugpack with a spare I had,
rechecked all the cables and rebooted
the modem. Everything worked fine
and after explaining my findings to
my friend, I went home thinking that
the problem had been solved.
44 Silicon Chip
Unfortunately, it wasn’t going to be
that easy because she was back on the
phone the very next day. “It’s done it
again” she told me with a rather miffed
tone in her voice. “Don’t touch it” I
said and went straight around to her
house with a spare modem.
When I arrived, I got into the modem’s configuration page (by entering
10.1.1.1 into the browser) and after
entering the username and password,
I began to scroll through the various
options. Sure enough, the ISP logon
details had returned to the factory
defaults!
After setting up my spare modem for
her, I returned home with the offending modem in my grasp. It was time for
some troubleshooting. First, I checked
with Optus to find out if any firmware
upgrades were available but no luck
there. I then powered the modem up,
entered my own ISP log-on information and left it hooked up.
It worked flawlessly for several days
until one morning, when I turned it
on, I couldn’t connect to the “net”.
On checking the Configuration page,
I found that it had lost all the log-on
settings again.
Now that I knew it wasn’t a PC or
network issue, I contacted D-Link and
asked their advice. The gentleman I
spoke to was extremely helpful. He
agreed that it was possibly a firmware
issue and emailed me an update for
the firmware. This proved to be easy
to install – the software simply found
the modem and installed itself.
This upgrade opened up a few extra
features in the modem but apart from
that, was identical to the Optus firmware. I then re-entered the settings
again and used the modem for the rest
of the day without a hitch. However,
when I tried to use it the next morning,
it had reset itself again.
It was time to take a look
under the bonnet!
After opening the
case, I could see immediately what the likely
cause of the problem
was. This modem runs
off a 9VAC plugpack and
its internal power supply
circuitry consists of quite
a few inductors, a few
surface-mount transis-
tors, several electrolytic capacitors and
two surface-mount power control IC’s.
The problem was that several of the
electros had “bulging top” disease. All
had leaked and two had even decided
to “launch” their cans, the latter only
coming half way off as the lid of the
case prevented them from going all
the way.
I made a list of the electros I would
need – a couple at 100µF 50V, three at
220µF 35V and a handful of 47µF and
100µF 25V units. All were 105°C types
and that indicated why they had failed.
My friend had placed the modem on
her desk but in a position where the
airflow through it was severely restricted. As a result, the electros had
overheated and eventually failed.
The circuit is protected by a fuse
which was still intact and the modem
still worked each time after the ISP’s
info had been re-entered. It’s a wonder
that it continued to work at all. The
case does have cooling vents and the
unit is supplied with rubber feet but
the feet had never been used and the
airflow around the modem was dismal.
Replacing the faulty parts was a
pain because the board is double-sided
and a ground plane covers nearly the
entire surface on the non-component
side. The resulting copper forms an
extremely good heatsink and so a great
deal of heat is necessary to remove
any parts.
As a result, some pads and tracks
were damaged and these had to be
repaired before the new parts were
fitted. A couple of the larger electros
also had to be fitted off the board but
I eventually got the job done.
The repaired modem has now been
running quite happily for several
weeks. It’s been fitted with the supplied feet and has been relocated on
my friend’s desk so that it now receives
an unrestricted airflow for cooling. I
was surprised at just how hot these
and other modems get during operation and I now advise other friends
to place their modems in open space.
Undoubtedly, there are many people
who would say “why bother, why not
just purchase a new modem?” Well, to
me, this “throwaway” society of ours
is irritating.
Once, you would repair anything.
Nowadays, it gets thrown out. It’s no
wonder that landfills are overflowing
and our planet is being slowly poisoned by the chemicals that leech out
SC
of the things we throw away.
siliconchip.com.au
Mega CCD Camera Clearance
MEGA MAY
A high performance colour CCD surveillance camera which
captures detailed flickerless video footage
even in the lowest of light levels.
Features auto iris control, auto
white balance, 2 stage
automatic gain control and
back light compensation.
Pocket sized gas torch for heatshrinking, soldering etc and uses
standard butane gas. Adjustable flame, all metal construction.
• Size: 205(L) x 13(Dia)mm
TS-1667
$11 95
Rare Earth Magnets
149
00
• Sony ExView 1/3" HAD CCD Sensor
$
• 380TVL, 500 x 582p resolution
SAVE $20 00
• Minimum illumination: 0.05 lux
• Shutter speed: 1/110,000 (sec)
QC-3298 Was $169.00
More Camera Clearance
lines on page 5
Also available:
Hi-Res ExView HAD Colour CCD Camera (470TVL)
Cat. QC-3299 Was $349.00 Now $249.00 Save $100.00
24 -12V DC-DC Converter
DC to DC converters are useful for running 12V devices from a
24V supply in a truck or bus. These have
switchmode technology for light weight
and compact design. Input and output is
via cigarette lighter plug and socket.
• Input voltage: 20 - 30VDC
• Output voltage: 13.8VDC
• Output current: 7A continuous, 10A max.
• Efficiency: 85%
• Dimensions: 160(L) x 48(W) x 48(H)mm
MP-3352
Great for Truckies!
Don’t forget Mother’s Day May 9th
Vehicle LED Daytime Running Lights
These Euro styled superbright LED bulbs will turn on
automatically on ignition, making your car more noticeable on
the road. With a lifespan of 50,000 hours, these long life and
energy saving DRLs are a much better daytime alternative than
using your fog lights or low beam headlights. Flush-mounted
brackets are included for easy installation and directional tiltadjustment.
149 00
$
69 95
$
• Energy efficient 12V 6.1W
• Emark 87R certificate
• Each lamp measures 190(W) x 30(H) x 43(D)mm
SL-3419
High Performance 12V Stereo Amp
Mega Car Amp Clearance
A compact and super affordable
4-channel amplifier that can
power an entire car audio
system. It includes variable
high and low pass filters, and pass
through RCA. This is an ideal first upgrade
amplifier from a basic factory installed system.
149 00
$
• Power / ch <at> 4 ohm 14.4V: 50WRMS x 4
SAVE $50 00
• Power / ch <at> 2 ohm 14.4V: 80WRMS x 4
• Power / bridged <at> 4 ohm 14.4V: 160WRMS x 2
AA-0422 Was $199.00 See P4 for more specials
15A Intelligent 5 Stage Battery Charger
Microprocessor controlled for charging and maintaining peak
performance of your batteries. Suitable for all flooded and gel
acid batteries, it compensates for temperature changes and
voltage drops in the cables. It's ultraportable with a handy storage pocket
in the back for the leads.
Charging current: 2 - 15A
Input voltage: 220 - 240VAC
Output voltage: 12VDC
Dimensions: 170(W) x 230(H)
x 140(D)mm
00
$
MB-3622
149
Pencil Butane Torch
Refer: Silicon Chip Magazine May 2010
An ideal project for anyone wanting a compact
stereo amp. It could be used for busking or any
application where 12V power is available. No mains
voltages, so it's safe as a schoolie's project
or as a beginner's first amp. Performance
is excellent with 20WRMS per
channel at 14.4V into 4 ohms
and THD of less than 0.03%.
Shortform kit only. Recommended
heatsink Cat. HH-8570 $6.95
• PCB: 95 x 78mm
• 12VDC
KC-5495
44 95
$
Super powerful rare earth magnets
with 4.5mm countersunk mounting holes
so you can fix them to your project to
latch a door closed, etc. Two sizes available:
FROM
16 95
$
Round 25(Dia) x 5mm Cat. LM-1626 $16.95
Rectangle 50(L) x 25(W) x 5(H)mm Cat. LM-1628 $19.95
Solar that Really Works
A highly informative and practical guide
showing the do's and don'ts of DIY solar
installation. From caravans to fishing
lodges, it features detailed descriptions
of working solar systems with
illustrations. Written by acclaimed
Australian author Collyn Rivers.
$
42 50
Softcover, 82 pages, 290 x 210mm
BE-1535
Also available in this series:
Motorhome Electrics
Cat. BE-1536 $42.50
Solar Success Cat. BE-1537 $47.50
Super Bargain Autoranging DMM
An automatic multimeter for checking
all sort of things!
• 10A AC & DC current range
• Built-in stand
• Backlit LCD
• AC & DC Voltage
• Resistor tester
$14 95
• Audible Continuity
00
$
• Size: 72(W) x 142(H) SAVE 10
x 32(D)mm
SUPER DEAL
QM-1528 Was $24.95
GREAT GIFT IDEAS FOR MUM
DON’T FORGET th
MOTHER’S DAY MAY 9
Pink 3 Piece Gardening Tool Set with Pouch
Ultrasonic Cleaner
If your Mum has a green thumb this is the Mother's Day gift for
her! This beautiful pink gardening tool set contains a mini hand
trowel, mini 3 tined rake, and a wonderful multi-tool featuring
secateurs, knife, weeder and two
serrated blades. The
$5 00
handy belt pouch holds
SAVE $4 95
everything secure and
within easy reach.
TD-2072 Was $9.95
All Mum's old jewellery can sparkle like new again! This
ultrasonic cleaner produces millions of microscopic bubbles to
clean items such as jewellery and small
silverware, as well as dentures, razor
heads, printer heads, and small
machined metal parts.
To order call 1800 022 888
www.jaycar.com.au
Prices valid until 23/05/2010. While stocks last. No rainchecks. All Savings are based on Original RRP
• 600ml capacity
• Mains powered
YH-5406 Was $99.00
79 00
$
SAVE $20 00
2
15 Piece Micro Driver Set
The set contains:
Slotted: 1mm, 1.4mm, 1.8mm, 2.4mm
Phillips: #000, #00, #0, #1
Torx: T5, T6,T7, T8 Drivers: 105mm long
Hex: 1.5mm, 2mm, 2.5mm
Case size: 192(L) x 130(W) x 26(H)mm
TD-2069
12V 100Ah Deep Cycle Gel Battery
Deep-cycle gel performance for
solar installations and other
alternative energy systems.
24
$
95
Heavy Duty Toggle Switches
Rated for 277VAC 20A with
11.5mm Mounting hole.
SPST
Cat. ST-0581 $4.95
SPDT
Cat. ST-0583 $5.45
DPDT Cat. ST-0585 $7.95
Also available: 12VDC 20A SPST Illuminated Red
Cat. ST-0587 $4.95
Deluxe Mains Power Meter
• Capacity: 100Ah
• Initial charge current: 30A
• Cycle voltage: 14.4 - 15V
• Standby voltage: 13.5 - 13.8V
• Weight: 31.5kg
• Dimensions: 330(L) x 173(W) x 223(H)
SB-1695
499 00
$
12/24V 25A Switchmode
Battery Charger
Plug in up to 3 mains appliances rated up to 10A and use
the remote to turn each one on or off individually or all
together. One of the outlets also has an LED night light
that's also operated with the remote. Not just for couch
potatoes, this also has obvious benefits for the elderly or
disabled.
499 00
$
POWER
4
High tech SLA battery charger for automotive, marine,
motorcycle, workshop or industrial use. Features switchmode
operation, multi-stage maintenance and charging, nearbulletproof performance and microprocessor control. It is
also IP rated for use in workshops and hostile environments.
See website for full specifications and data sheets.
MB-3608
IP67 Rated Illuminated
Pushbutton Switches
$17.50
$17.50
$17.50
$14.50
$14.50
9
$ 95
Cat. SP-0741
Cat. SP-0745
Cat. SP-0747
Cat. SP-0749
$9.95
$12.95
$9.95
$12.95
• High cranking capacity - 800A
• High input/output current - 200A
• Low power consumption - 15mA
• 3 year warranty
• Mounting hardware included
• Dimensions: 85(H) x 55(W) x 35(D)mm
MB-3678
SPST Heavy Duty
Pushbutton Marine Switch
Marine Keyswitch
24
44 95
$
Surge/Overload Protected Powerboards
With microprocessor control, this
indispensable device monitors
the output voltage of any 12V
lead-acid battery. If the
terminal voltage
drops below
11.9V, the
battery will be
automatically disconnected.
Essential for boats, camping, caravans, RVs,
4WD, solar power systems etc.
FROM
SPST heavy duty key switch with 2 keys.
21mm mounting hole in panels up to 25mm
thick. Screw terminals.
95
SM-1042
$
• 433MHz
• Remote battery included
• Remote measures:
125(W) x 45(H) x 17(D)mm
MS-6142
Low Voltage Battery Isolator
Illuminated IP65 Rated
DPDT Pushbutton Switches
IP65 rated for use in harsh
environments. Illuminated, metal
body, DPDT, on-off or momentary
action. Rated for 250VAC <at> 5A,
with 12VDC LED illumination.
Mounting hole 15mm.
Red Momentary
Red On/Off
Green Momentary
Green On/Off
29 95
$
Wireless 3 Outlet Mains Controller
Waterproof SPST large rocker actuator for
harsh environment applications.
• Rated for 240VAC 10A
$ 95
• Mounting hole 34 x 15mm
SK-0993
14
In addition to telling you the
cost of electricity
consumption of an appliance
plugged into it and the
amount of power used in
kilowatt hours, it will tell you
how many cumulative kg of
CO2 the appliance is putting
into the atmosphere.
Battery included.
• Dimensions: 120(L) x 58(W) x 40(H)mm
MS-6118
SPST IP65 Rated Rocker Switch
IP67 rated for industrial harsh
environments. 12VDC LED lluminated,
metal body, SPDT, on-off or
momentary action. Rated for 250VAC <at>
3A. Mounting hole 16mm.
Red SPDT
Cat. SP-0791
FROM
50
Green SPDT
Cat. SP-0792
$
Blue SPDT
Cat. SP-0793
Red SPDT Momentary
Cat. SP-0796
Green SPDT Momentary
Cat. SP-0797
Save On Your Electricity Bill!
SPST momentary action, brass body with large
chrome-plated actuator. Can accommodate
panel thickness of up to 22mm. Mounting
hole 16mm,
screw terminals.
SP-0701
19 95
$
Individually switched powerboards provide a high level of
protection from overload and surge, with extra-wide spacing to
take bulky mains plugpacks. Ideal for home theatre, computers,
TV and video or audio systems.
• Extra-wide spacing to take mains plugpacks
• Individually switched
• Surge and overload protected
• 4 or 6 way
99 95
$
19 95
$
4 Way Powerboard
Cat MS-4064 $19.95
6 Way Powerboard
Cat MS-4066 $24.95
Merit Plug to Cigarette
Lighter Socket
DIN Rail Mount
Relay Socket
DIN rail mounting base
for SY-4009. Also
has 4mm holes so
can be screw
mounted to a
chassis.
• Size: 71(L) x 29(W) x 30(H)mm
SY-4004
FROM
5
$ 50
Allows you to connect
mobile phone
chargers and other
cigarette lighter
plugged
devices into
vehicles equipped
with a Merit socket.
PP-2099
12 95
$
All Savings are based on Original RRP
Better, More Technical
To order call 1800 022 888
MEGA MAY
SIT THERE,
Don’t forget Mother’s Day - May 9th
Great Gift Ideas For Mum
She has style, she has flair, now Mum can have the keyboard
to match. Features 21 hot keys including 3 ACPI keys for easy
access to the internet, email and multimedia applications.
• Compatible with Windows
95/98/ME/NT/XP
• Dimensions:
95
$
460(L) x 180(D)mm
$
GH-1899 Was $59.95 SAVE 10 00
49
LED Night Light with Sensor
LED Night Light with Sensor
No need to stub your toe when you get up
in the middle of the night. Keep one of
these plugged in and it will give you
enough light to see where you're going.
Operates automatically.
9
$ 95
• Rotates through 360° to light any direction
• Automatically comes on in darkness
• Unobtrusive size - smaller than a double
adaptor
ST-3181
Designed for long life, and using the latest in high
intensity technology, these MR16 downlights
pump out brilliant lumens of white light.
Four port USB hub
with a different
bright colour for
each port. Funky
and compact, keep
one handy in the
notebook bag just in case.
XC-4878 Was $15.95
MR16 3 x 2W Cool White Cat. ZD-0353 $74.95
• Lumens: 450
• Colour temperature: White 5000 - 7000k
• Lens: 38 degree
• Dimensions: 50(D) x 63(L)mm
10 95
$
SAVE 5
$ 00
Wireless LED Wall Light
Switchmode Plugpacks
with USB Outlets
Slimline, lightweight, and featuring manually selectable
variable voltage outputs. All are MEPS compliant and each
come supplied with 7 plugs and a USB
output socket.
7.2 Watt 3 - 12VDC 600mA
Dimensions: 69(L) x
39(W) x 31(H)mm
Cat. MP-3310 $19.95
19 95
$
18 Watt 3 - 12VDC 1500mA
Dimensions: 80(L) x 60(W) x 50(H)mm
Cat. MP-3314 $29.95
27 Watt 3 - 12VDC 2250mA
Dimensions: 80(L) x 65(W) x 50(H)mm
Cat. MP-3316 $34.95
www.jaycar.com.au
14
95
$
• 7 Super bright LEDs
• One touch ON/OFF/DIMMER
SAVE $15 00
• Dimensions: 170(H) x 75(W) x 90(D)mm
• Stand alone requires 2 x AAA and 3 x AA batteries
ST-3178 Was $29.95
These fantastic X-Glow torches utilise
Cree® high performance LEDs,
which are renown for
providing superior light and
longer globe life than other
brands. Incredibly energy
efficient, Cree® LEDs produce a
clear smooth beam of brilliant
white light with minimal energy
lost through residual heat. These X-Glow torches feature
robust water resistant aluminium casings for heavy duty
use, and they will even cold start in sub-zero temperatures.
80 Lumens ST-3372 Was $47.95 Now $29.95 Save $18.00
136 Lumens ST-3374 Was $64.95 Now $34.95 Save $30.00
176 Lumens ST-3376 Was $69.95 Now $39.95 Save $30.00
LIMITED STOCK
Mains Powered Universal
Battery Charger
• Recharges AAA, AA,
C, D, and 9V batteries
• Recharges batteries
singularly or in groups
95
$
• Includes battery tester for
$
1.2V to 1.5V cells
SAVE 5 00
• Accepts various combinations of batteries
• 200(W) x 50(H) x 95(D)mm
• Note: will not discharge standard 9V batteries
MB-3505 Was $24.95
19
All Savings are based on Original RRP
95
74each
3 x 1W puck lights that can be surface mounted or recessed to
fit into your décor. They're powered by a single plugpack with
a distribution block on a 2 metre cable, and each light has its
own 600mm cable, so you can
easily install them yourself.
An economical unit that can charge Ni-MH batteries as well
as Ni-Cd batteries (Yes, even 9V Ni-MH). It has a
discharge function for proper Ni-Cd
battery cycling and a battery tester
for 1.2 & 1.5 volt batteries.
FROM
MR16 3 x 2W Warm White Cat. ZD-0354 $74.95
Lumens: 310
$
Colour temperature: 2700 - 3500k
Lens: 38 degree
Dimensions: 50(Dia) x 63(L)mm
3 Piece LED Puck Light Kit
This stylish wall light with super bright
LEDs is an extremely versatile lighting
solution that comes complete with
remote control and mounting brackets.
No need for an electrician - installation
is childsplay for the home handyman.
Includes DC socket for plugpack
connection.
Cree® LED Torch Clearance
The meter can tell you how much an
appliance is costing to run and tracks
the actual power being used. It can
also display the instantaneous
voltage or current
$19 95
being drawn as well
as peak levels etc.
SAVE $10 00
10A max rating.
MS-6115
‘000s Sold
Was $29.95
Every Month
18 Watt 3 - 12VDC 1000mA
Dimensions: 75(L) x 60(W) x
40(H)mm
Cat. MP-3312 $24.95
4 Port Coloured
Flexible USB Hub
• Fashionable cool white colour
• More than 30,000 hours life
• Power supply 12VDC 1A
• Light size: 72(Dia) x 28(H)mm
ST-3894
149 00
$
Protect your Home
Entertainment System
Surge protection and filtering are provided for the mains as
well as your telephone line, network connection,
satellite/cable TV, and the
TV antenna. Further
protection is
provided by the
built-in 10A circuit
breaker.
95
$
See website for detailed specs.
SAVE $15 00
MS-4024 Was $64.95
49
In-Car Ni-Cd &
Ni-MH Battery Charger
Recharges 2 x AA or 2 x AAA Ni-CD or Ni-MH batteries
using Delta V voltage detection which ensures the batteries
are charged to their optimal levels for long life. Keep
a spare set of batteries topped up and
ready to go, wherever you are.
• Includes bad cell detection
• Delta V detection
• 900mA charging current for AA batteries
• 450mA charging current for AAA batteries
• Dimensions: 130(L) x 45(W) x 30(H)mm
MB-3552 Was $18.95
10 00
$
SAVE $8 95
Also available:
Advanced ANSMANN Battery Charger
Cat. MB-3554 Was $89.00 Now $79.00 Save $10.00
POWER
Mains Power Meter
BUILD SOMETHING
MR16 3 x 2W CREE® Downlights
DON’T FORGET th
MOTHER’S DAY MAY 9
Rhinestone USB Keyboard
3
DON’T JUST
4
Mega Car Amp Clearance Sale
Response Car Amp 4 x 100WRMS
Precision Response 5 Channel
Full Range Car Amp
Precision Response Car
Amplifier 2 x 150WRMS
This amp can be used as a
standard stereo amp or
bridged to provide a
massive 500WRMS x 1
into a 4 ohm load. A powerful amp
at a great price. Features variable high and low
pass filters, bass boost and pass through RCA.
179
$
• 2 x 150WRMS <at> 4 ohms
• 2 x 255WRMS <at> 2 ohms
• 1 x 500WRMS <at> 4 ohms bridged
• Dimensions: 340(L) x 258(W) x 50(D)mm
AA-0424 Was $219.00 Limited Stock
00
SAVE $40 00
This award winning amplifier features
four full range channels plus
a subwoofer channel. The
main channels have
adjustable gain and variable
high-pass filters; the fifth channel
has adjustable phase, variable lowpass filter, and adjustable gain.
An ultra-powerful 4-channel amplifier with output
exceeding 100WRMS per channel or
300WRMS in bridged mode at 4
ohms. Features variable
high and low pass
filters, and pass
through RCA.
399 00
$
• 4 x 60WRMS + 1 x 225WRMS <at> 4 ohm
• 4 x 90WRMS + 1 x 340WRMS <at> 2ohm
• 2 x 180WRMS + 1 x 340WRMS <at> 4 ohm bridged
AA-0458 Was $449.00
• 4 x 130WRMS <at> 4 ohms
• 4 x 190WRMS <at> 2 ohms
• 2 x 380WRMS <at> 4 ohms
bridged
• Dimensions:
400(L) x 258(W) x 50(D)mm
AA-0426 Was $349.00
SAVE $50 00
299 00
$
SAVE $50 00
Precision Response 4 x 100WRMS Full Range Car Amp
Response 1000WRMS
Linkable Monoblock
Car Amp
A very efficient amp designed to drive full range speakers and is able to produce
550W bridged. It has insert-type connectors, variable high and low pass filters
and variable bass boost.
319 00
AUTO
• 4 x 130WRMS <at> 4 ohm
• 4 x 190WRMS <at> 2 ohm
• 2 x 380WRMS <at> 4 ohm
• Dimensions: 300(L) x 170(W) x 50(D)mm
AA-0456 Was $399.00 Limited Stock
Monstrous,
eardrumpuncturing
power. You also
get variable bass boost,
adjustable phase shift, low
pass filter and master/slave
operation. Optional remote bass gain
controller.
$
SAVE $80 00
Vifa 5" Component Car Speakers
SAVE
• 1000WRMS <at> 1 ohm mono
• 600WRMS <at> 2 ohms mono
• 1800WRMS <at> 2 ohm linkable, dual mono
AA-0460 Was $399.00
Vifa's patented Hearing Optimised Driving (HOD) technology
accounts for harsh in-car audio environments and drastically
improves the sound production quality of your car audio system.
Featuring super strong strontium magnets, Vifa's patented
complex cone design, 36mm silk dome tweeter and a
Butterworth crossover circuit; these component split systems
reproduce unparalleled crystal clear sound that sounds more
home theatre than car audio.
Vifa 5" Component Split Speakers
• 60WRMS <at> 4 ohms
• 50Hz-20kHz
Cat. CS-2398 Was $219.00
Vifa 6.5" Component Split Speakers
• 80WRMS <at> 4 ohms
• 45Hz-20kHz
Cat. CS-2399 Was $249.00
Car speaker grilles to suit our range
of Vifa car speakers, but will
suit many other car audio
applications. Made from
perforated steel,
finished in black.
179 00
SAVE $40 00
199 00
$
5" Car Speaker Grille
Pair Cat. AX-3600
6" Car Speaker Grille
Pair Cat. AX-3602
6 x 9" Car Speaker Grille Pair Cat. AX-3604
SAVE $50 00
If you value sound quality, true high fidelity mid range drivers like these are a
must for your car audio. All Vifa coaxials feature the legendary Vifa silk dome
tweeters, strontium magnets and composite diaphragms.
Available in 2 or 4-way configuration.
Vifa 5" 2 Way Speakers
• 60WRMS <at> 4 ohms
00
$
• 50Hz-20kHz
• 87.9 dB SPL <at> 1W, 1m
SAVE $20 00
Cat. CS-2393 Was $119.00
Vifa 6.5" 2 Way Speakers
00
• 80WRMS <at> 4 ohms
$
• 45Hz-20kHz
• 86.3dB SPL <at> 1W, 1m
SAVE $40 00
Cat. CS-2395 Was $169.00
Vifa 6 x 9" 4 Way Speakers
00
• 150WRMS <at> 4 ohms
$
• 35Hz-20kHz
• 90 dB SPL <at> 1W, 1m
SAVE $40 00
Cat. CS-2397 Was $229.00
99
129
189
All Savings are based on Original RRP Limited Stock on sale items
Better, More Technical
50 00
$
Vifa Car Speaker Grilles
$
Vifa Coaxial Car Speakers
349 00
$
$9.95
$12.95
$14.95
Vifa Premium Subwoofers
These premium range Vifa car subwoofers produce genuine high fidelity
sound quality. With dual voice coils, high power handling and die-cast
aluminium chassis, they don't just deliver brilliant low-register bass clarity
but also thump tremendous SPLs like only Vifa speakers can.
10" or 12" models available.
Vifa 10" Subwoofer
• 200WRMS <at> 2 x 4 ohms
• 30Hz - 1kHz
• 86.6dB SPL <at>1W, 1m
CS-2351 Was $299.00
Vifa 12" Subwoofer
• 250WRMS <at> 2 x 4 ohms
• 25Hz - 1kHz
• 87.2dB SPL <at>1W, 1m
CS-2353 Was $349.00
249 00
$
SAVE $50 00
299 00
$
SAVE $50 00
To order call 1800 022 888
MEGA MAY
Don’t forget Mother’s Day - May 9th
5
DON’T JUST
SIT THERE,
BUILD SOMETHING
Mega Security Clearance Sale - Up to 50% Off
Economy 4 Channel Multiplexing DVR
A combined multiplexer and digital video recorder with Ethernet port that
allows remote access and control via a web browser. Features MPEG-4
compression, advanced motion recording, video loss detection, remote
network record and back-up support. Supplied with a 250GB HD and can be
expanded up to 400GB. See website for specifications. 340mm wide.
B&W Underwater (1m) Day/Night CCD Camera
This camera features a water resistance rating to IP57 allowing it to be submerged
underwater. This makes it ideal for aquariums or virtually any underwater surveillance
application up to a maximum depth of 1 metre. The camera will operate down to 0lux, courtesy of 12 infrared LEDs mounted behind a protective glass shield.
299 00
$
SAVE $200 00
• Sensor: 1/3" CCD
• Connections: 12VDC/2.1mm, video BNC
• Lens: 3.6mm (92°)
• Dimensions: 65 (D) x 120 (L)mm
QC-3490 Was $99.00
• Ethernet capability
• MPEG-4 compression
• 250GB HDD included
QV-3079 Was $499.00
Day/Night 470TVL Colour CCD Camera
Also available:
Colour IP57 Day/Night CCD Camera 330TVL
Cat. QC-3492 Was $249.00 Now $119.00 Save $130.00
Colour by day, black and white by night. This high-resolution
CCD camera is perfect for use with infra red illuminators.
• 1/3" Sony Hi-Res SuperHAD CCD Sensor
• Auto Iris Control
• 470TVL resolution
• Minimum illumination: 0.2 lux
• Day / Night changeover level: 3 lux
QC-3301 Was $299.00
Colour IP57 Day/Night CCD Camera 480TVL
Cat. QC-3495 Was $299.00 Now $199.00 Save $100.00
229 00
$
Also available:
Day/Night 520TVL Colour CCD Camera
Cat. QC-3307 Was $299.00 Now $219.00 Save $80.00
Day/Night 350TVL Colour CCD Camera
Cat. QC-3309 Was $149.00 Now $119.00 Save $30.00
Was
$99.95
$549.00
$279.00
$129.00
$119.00
$79.00
$82.00
$249.00
$199.00
$199.00
$299.00
$89.00
Now
$69.00
$399.00
$179.00
$99.00
$99.00
$69.00
$69.00
$179.00
$179.00
$179.00
$219.00
$69.00
Dome Style B&W CCD Camera
This quality dome housing is fitted with a 1/3" Samsung® CCD
sensor, mounted on an adjustable bracket. The darkened
dome improves security by preventing would-be thieves from
seeing where the camera is pointed. Ideal for use in retail
stores and reception areas etc. Requires 12VDC.
00
$
• 380 TVL
• 0.5 Lux Min
Also available:
SAVE $34 00
• 92° Lens angle
B&W CCD Camera in
QC-3472 Was $89.00 Metal Case with Audio
Cat. QC-3474 Was $89.00 Now $59.00 Save $30.00
Save
$30.95
$150.00
$100.00
$30.00
$20.00
$10.00
$13.00
$70.00
$20.00
$20.00
$80.00
$20.00
A high quality colour CCD dome camera with 350TV line
resolution and 1/3" Sony sensor chip. The camera
features auto white-balance and shutter speeds
from 1/50 to 1/100,000 of a second and is
compact enough to be installed in the smallest of
rooms or corridors. The camera is mounted inside
a small dome making it ideal for security
application where a visible deterrent is helpful.
• Requires a 12VDC regulated
power supply. Use our MP301112VDC 300mA Regulated AC
Adaptor.
QC-3318 Was $179.00
SECURITY
Security Camera Clearance
Cat No.
QC-3259
QC-3381
QC-3498
QC-3569
QC-3570
QC-3571
QC-3573
QC-3727
QC-3728
QC-3729
QC-3297
QC-3291
SAVE $30 00
Colour CCD Dome Camera with Sony Sensor
SAVE $70 00
Description
Spare 2.4GHz Camera for QC-3258
IP67 Pro Outdoor Colour Camera with Sony Super HAD CCD Sensor
Dome Style Colour CCD Camera with Panasonic Sensor
2.4 GHz Mini Wireless CMOS Camera Kit
5.8GHz Wireless CMOS Camera with 4 Ch Receiver
5.8GHz Wireless CMOS Camera
5.8GHz Wireless CMOS Camera with IR Illuminator
Mini Colour CCD Reversing Camera
Flush Mount Colour CCD Reversing Camera
Clip-On CCD Reversing Camera
Vari-focal 480TVL Dome Camera
Low Cost Colour Mini Dome Camera - Sharp Sensor
69 00
$
89 00
$
SAVE $90 00
That’s 50% Off
Colour Dome Camera Kit with 2-Wire Connection
A simple 2 wire combined arrangement for power and video make this system a snap
to install. The system uses a CMOS image sensor with 350TV line resolution and will
automatically sense signal cable tampering or incorrect wiring and alert you
with a warning signal. Kit
00
$
includes camera, signal
processor, connecting cable,
$
SAVE 16 00
and mains adaptor.
QC-3264 Was $85.00
69
Also available:
Outdoor IR version
(IP56 rated)
Cat. QC-3266 Was $100.00 Now $89.00 Save $11.00
55
550TVL IR Dome Camera
A high quality colour IR dome camera with 550TV line resolution and a 1/3" Sony HR sensor
chip. The camera features a 3D gimble mount enabling the camera to be installed on the roof
or wall. Requires a 12VDC regulated power supply.
• Min. illumination: 0.4 Lux / F 2.0 (Day), 0 Lux (IR on)
• Power consumption IR On: 480mA max,
• IR Off: 200mA max.
• Dimensions: 140(Dia) x 81.4(H)mm
00
$
• Power supply: 12VDC
• Recommended power supply: MP-3011
SAVE $80 00
QC-8600 Was $299.00
219
www.jaycar.com.au
Personal Mini Alarm with LED Torch
A personal alarm made from tough ABS construction with a 120dB siren to
deter thieves and attackers. To activate simply pull the rip-cord
to pull out the pin. Replace the pin to deactivate the alarm.
Also includes a LED light. Great for travellers.
• 105-120dB
• Practical design
• Compact size
• Includes 3 x LR44 batteries
• Dimensions: 72(L) x 31(W) x 22(H)mm
LA-5183
All Savings are based on Original RRP
Limited Stock on sale items
9
$ 95
6
Great Gift Ideas For Mum
AV Clearance Sale
HDMI Extender
HDMI 3 Port Switch
This system expander will allow you to hook up, convert
and switch between a component video (YPbPr), DVIDigital, and a HDMI signal to one HDMI v1.3 output. Audio
is also combined with the video signal, so you can combine
stereo audio or optical digital audio with your YPbPr video
source and DVI-D can
be combined with
optical digital
audio. Includes an
IR remote control for
00
$
ease of use, as well as
the mains adaptor.
SAVE $10 00
139
• Dimensions: 258(W) x
120(D) x 28(H)mm
AC-1684 Was $149.00
Play your favourite MP3 tracks in any car
cassette player or use it as an
MP3 player.
AUDIO VISUAL / MULTIMEDIA
• Supports up to 1080p resolution
• Compatible with VGA, SVGA, XGA, SXGA, UXGA
• Automatic equalisation up to 1.6Gbps
95
$
• HDMI v1.3 compliant
• Dimensions: 50(L) x 28(W) x 18(H)mm
SAVE $10 00
AC-1697 Was $39.95
29
Dual Channel AV Sender
MP3 Player to Cassette Adaptor
• Supports SD, mini SD
and MMC cards
• Remote cable
450mm long
• USB cable and cigarette
lighter adaptor included
• 8 hours playing time
from one charge
AR-1764 Was $44.95
The typical maximum range of a HDMI signal is just 12m at
maximum - not very long if you are trying to send your high
definition A/V signal from one end of
the lounge room to the other. This
HDMI extender equalises and
boosts your HDMI signal so that
you can run cable up to 50m long.
39 95
$
SAVE $5 00
Slimline LCD/Plasma Brackets
Projecting only 10mm from
the wall, these ultra-slim
brackets are very easy to install
but will accommodate an LED,
LCD or plasma TV up to 80kg. The
spring-loaded cleats lock in
position so the TV can't be
accidentally knocked off. Two
sizes available for 23-37" TVs or
32-60" TVs.
Allows you to connect two AV
sources, such as your TV, Hi-Fi
sound system, video recorder,
DVD player, set top box, or
cable TV system, to the
transmitter, share them around
the house, and select either of
them from the other room,
without the hassle of running
wires. A selector button on the
receiver allows selection
between the two connected devices.
AR-1838 Was $79.95
39
Slimline LCD/Plasma Bracket
for 23 - 37", 45kg. Cat. CW-2821
$
Slimline LCD/Plasma Bracket
for 32 - 60", 80kg. Cat. CW-2823
$
95
49 95
• Celsius and Fahrenheit display
• Kg or lb
• Size: 200(Dia) x 22(H)mm
Note: Dish not included
XC-0161 Was $44.95
34 95
$
SAVE $10 00
Don’t Forget
Mother’s Day May 9th
She can seal her goodies in the reusable bag
and use the powerful pump to vacuum seal
it. Ideal for freezing or food drying.
69 95
$
SAVE $10 00
• 3 bags included
• Reduces plastic bag waste
• Requires 6 x AA batteries
• Measures: 270(L)mm
GH-1342 Was $24.95
19 95
$
SAVE $5 00
Automatic IR Liquid
Soap Dispenser
Additional Receivers With Remote Extender
available separately Cat. AR-1839 Was $54.95
Now $37.95 Save $17.00
A functional and stylish addition to any
kitchen or bathroom sink. It features a
blinking LED to indicate operation, a large
410ml (14 ounce) liquid soap reservoir
for fewer refills and a manual dispensing
button to provide continuous soap flow
for larger cleaning tasks. Just wave your
dirty hands - no mess, no fuss, no germs!
High Quality Lightweight
Stereo Headphones
• Frequency response: 150Hz - 20kHz
• Weight: 80 grams
AA-2061
Kitchen scales, clock and weather
station all rolled into one. It weighs
up to 3kg (6.6lb) in metric or
imperial, then can be used as a wall
clock that displays temperature and
humidity as well. Funky orange design.
Requires 3 x AAA batteries.
Vacuum Bag Sealer
Ultra-lightweight stereo
headphones that provide
outstanding performance
and comfort. Featuring
high output drivers with
neodymium magnets, they
produce crystal clear sound
with crisp highs and smooth bass
response. Soft leatherette swivel ear
pads, adjustable headset and 1.2m lead.
• Fits standard spacing wall studs
• Ultra-low profile
Kitchen Scales with
Clock and Temp Display
• Requires 4 x AA batteries
• Dimensions: 90(W) x 130(D) x 200(H)mm
GH-1187
24 95
$
Cat III Rated Banana Alligator Clip
24 95
$
Also available: High Quality Full Cup Stereo Headphones
Cat. AA-2063 $34.95
Takes standard and fully
insulated 4mm banana plugs
and turns them into an
alligator clip. CAT III
rated. Sold as a pair,
red and black.
PA-3696
9
$ 95
TV Accessories & AV Leads
TV Adaptors
Right Angle HDMI Adaptors
75 ohm TV plug
to F81 socket
• Right angle
Cat. PA-3673 $4.95
Adapts HDMI plug to socket at right
angles. Perfect for wall mounted
TV applications. Gold
plated connections.
Two types available:
75 ohm plug to
75 ohm socket
• Right angle
Cat. PA-3679 $4.95
Right Angle Down
PA-3646 $12.95
Right Angle Up
PA-3648 $12.95
High Quality
Concord Leads
RCA LEADS
• Video Lead RCA - RCA
• 0.5 metre
Cat. WQ-7221 $10.95
• 2 x RCA to 2 x RCA Plug Lead
• 0.5 metre
Cat. WQ-7227 $16.95
AV LEADS
• 3 x RCA to 3 x RCA
plug for
component video
• 0.5 metre
Cat. WQ-7239 $29.95
• Toslink Plug to
plug for optical audio
• 0.5 metre
Cat. WQ-7261 $16.95
All Savings are based on Original RRP
Better, More Technical
To order call 1800 022 888
MEGA MAY
7
DON’T JUST
SIT THERE,
Don’t forget Mother’s Day - May 9th
BUILD SOMETHING
Keyboard Bargains
USB Multimedia Keyboard
A slimline ergonomic keyboard that features 21 hot keys
including 3 ACPI keys for easy access to the internet, email
and multimedia applications.
Industrial IP68 USB Keyboard
Wireless Trackball Keyboard
Perfect for industrial, food & beverage, laboratories, garages
and even outdoor use. It also comes with a silicone sleeve for
added protection. Anti-bacterial rubber
construction.
This keyboard works like a games console with a trackball
and a set of mouse buttons conveniently located on the
underside (also a second set on top). No need for installation
software - simply plug in the USB wireless
receiver to your PC and you're good to go.
00
$
14 95
$
SAVE 4
$ 00
• Compatible with Windows 95/98/2000/ME/NT/XP
XC-5157 Was $18.95
Wireless Networking Antennas
Here's a quick and inexpensive way to improve
the range at either your base station or
terminal. These antennas are specifically
designed for 2.4GHz applications and 802.11
wireless networking is an ideal application.
2.4GHz Wireless Antenna 5dB Gain
• Height: 195mm
Cat. AR-3273 $19.95
89 00
$
• Full-sized QWERTY layout
SAVE $10 00
• USB connectivity
• Windows 2000/XP/Vista
• Measures 440(L) x 138(W) x 12(H)mm
XC-5141 Was $99.00
All-in-One Card
Reader & USB Hub
An ideal accessory for roving
photographers. With 6
card slots and an ability
to read a multitude of
formats, it also has a flip
open top to store a
number of micro, SD or XD
cards. If that's not enough, there is also a two
port USB 2.0 hub. The USB cable neatly tucks
into the back when not in use.
• Dimensions: 87(L) x 39(W) x 18(H)mm
XC-4924
High Quality IEEE1394 Cables
Also known as FireWire, i.Link or Lynx cables, IEEE1394 is
commonly used in digital audio/video and automotive
applications. This range of high quality IEEE1394
cables boast 24K gold plated
connectors, 99.9% oxygen free
copper conductors and are
shielded against EMI. If you require
near faultless data streams these
cables are hard to pass up.
IEEE1394 B 9-pin to IEEE1394 B 9-pin Cable - 1.8m
Cat. WC-7630 $19.95
IEEE1394 B 9-pin to IEEE1394 A 4-pin Cable - 1.8m
Cat. WC-7632 $19.95
IEEE1394 B 9-pin to IEEE1394 A 6-pin Cable - 1.8m
Cat. WC-7634 $19.95
USB Digital TV Micro Tuner
Couple your laptop with this tiny device and you can
enjoy your favourite free-to-air digital TV programs
from practically anywhere. Includes mini
MCX DVB-T aerial & remote control.
• Supports Time-shifting allowing
you to pause live TV
95
$
• Supports scheduled recording
• USB 2.0 interface
• Supports High Definition Digital TV (HDTV)
XC-4897
89
www.jaycar.com.au
• 2.4GHz with 8 channels
• 10 metre range
• Windows XP & Vista compatible
• 12 Internet/multimedia hot keys
• Integrated optical trackball & scroll wheel
• Requires 4 x AA batteries
XC-4941 Was $99.00 Limited Stock
10 Port USB Hub
Turn off non-essential peripherals while maintaining power to
others with this 10 port USB hub. The two position switch turns
all ports on, or only ports 7 - 10. 5VDC 2A plugpack required
for powered operation.
29 95
$
8 Port Hub Switch
High performance 8
port, 10/100/1000
N-Way switch increases
network performance and reduces congestion. The switch also
supports auto-negotiation which allows each port to be
operated at a different speed while maintaining maximum
throughput. Plugpack included.
• Max cable length: 100 metres
• Transmission speed: 10/100/1000Mbps
• Size: 180(W) x 103(D) x 27(H)mm
YN-8087
99
$
00
• USB 2.0
• USB or mains powered
• Key holes for wall mounting
• Windows 2000, XP, Vista
and Mac OS 10.0 compatible
• Dimensions: 172(L) x 36(W) x 27(H)mm
XC-4946
59 95
$
USB Leads
High Quality USB 3.0 Cables
Superior quality high speed USB 3.0
cables for your nextgen USB devices.
Conforms to USB 3.0 standard 4.8Gbps. That's 10x faster than USB 2.0.
High Quality USB 3.0 A (male) to
A (male) 2m cable - WC-7780 $19.95
SnapMusic Audio Capture for PC
Turn your PC into a mini recording studio. Record and
archive music from your old vinyl records, cassettes or any
other audio source directly to your
PC and save the files as highquality WAVs or MP3s. See
website for full
specifications.
• Audio capture box with line-in/out, S/PDIF
in/out and mic-in all-in-one
• Create your own podcasts from any program material
• Record live performances or lectures
• Convert audio files formats
• Burn high quality audio CDs
• Includes SnapMusic Studio 715 and
00
$
Roxy Easy Media Creator 9 LE
XC-4994
89
All Savings are based on Original RRP
High Quality USB 3.0 A (male)
to B (male) 2m cable - WC-7782 $19.95
High Quality USB 2.0 Leads
High quality USB 2.0 leads for your
PC peripherals, professional audio or
camera equipment. Superior shielding
protects against potential electromagnetic
interferences and ensures data continuity.
USB A (male) to USB B (male) 2.0m
USB A (male) to USB-Mini B (male) 2.0m
USB A (male) to USB A (male) 2.0m
USB A (male) to USB-Micro B (male) 2.0m
Cat. WC-7790 $14.95
Cat. WC-7792 $14.95
Cat. WC-7794 $14.95
Cat. WC-7796 $14.95
IT & COMMS
2.4GHz Wireless Antenna 11dB Gain
• Height: 380mm
Cat. AR-3277 $39.95
89
SAVE $10 00
4 Tray Tool/Storage Case
Wire Draw Fish Tape
Each compartment has a 233 x
122 x 32mm 13 compartment
storage box for small items with
dividers that can be removed to
accommodate larger things. All
the hinges and catches are the
durable pintle type and the top tray
has a generous 265 x 160 x 65mm
space for ancillary items.
The smart way to draw cable through call
cavities or conduit. 30m of rigid spring
steel with a built-in cable clip on one
end. No electrician or installer
should be without one.
• Length: 30m
• Size: 305(Dia) x 38(H)mm
TH-1869
49 95
$
Battery Powered 6W Soldering Iron
Ideal for on-site repairs and PCB work and heats to
soldering temperature in about 10 seconds.
Requires 3 x AA batteries.
19
Size: 175(L) x 36(W) x 18(D)mm
TS-1535
$
95
• Dimensions: 270(W) x
260(H) x 150(D)mm
HB-6302
Set of five 115mm cutters and pliers for
electronics, hobbies, beading or other crafts.
Stainless steel with soft ergonomic grips.
Contents:
• Flush cutters
• Long nose pliers
• Flat nose pliers
• Bent nose pliers
• Round nose pliers
TH-1812
14 95
$
9 Piece Folding Torx/Allen Key Sets
Handy folding sets of Torx or Allen keys with sturdy anodised
aluminium handles. The handles have M8, M10, E8 and E10
spanners built into them. Never lose a bit again.
Micro Drill Bit Set 0.7 - 2.2mm
Every hobby engineer needs a set of micro
drill bits in the workshop.
95
Quality HSS in incremental $
sizes from 0.7 to 2.2mm.
14
Ball Allen Key Set Metric
Cat. TD-2172 $7.95
F-Connector Tool Set
SUPER DEALS
Ball Allen Key Set Imperial
Cat. TD-2174 $7.95
All the tools you need for
cutting, stripping and
crimping F-connectors for
coax cable installations.
Put one in the tooly today.
The kit includes:
USB Slide/Film Scanner
29 Piece Tool Kit with Torch
DIY minor repairs are a breeze with this 29 piece tool kit. All
the basic essential tools, including a torch, all stored in a
stylish silver case.
• Coax cable stripper
• Compression crimp tool
95
$
• Heavy duty cable cutter
• 10 x F-59 plugs
• Nylon storage case: 152(W) x 220(H) x 45(D)mm
TH-1804
89
29 95
$
No more fluorescent tubes to replace on your
magnifying lamp. Sixty LEDs provide ample
illumination, and the 3x and 12x
magnifying lenses will enable you
to see what you're working on
with remarkable clarity and detail.
Being LED, there's no delay in start-up and
they'll never need replacing. Ideal for hobbies,
model making or jewellery.
• Case measures
200(L) x 145(W) x
45(H)mm
TD-2066 Was $34.95
Compression Crimping Tool
A precision crimp tool that employs a ratchet action ensuring
correct crimping pressure is applied for reliable, trouble-free
compression BNC, RCA, PAL and F-type coaxial connectors.
Adjustable compression depth.
TH-1801
49 95
$
YOUR LOCAL JAYCAR STORE
Australia Freecall Orders: Ph 1800 022 888
AUSTRALIAN CAPITAL TERRITORY
Belconnen
Ph (02) 6253 5700
Fyshwick
Ph (02) 6239 1801
NEW SOUTH WALES
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
Brookvale
Ph (02) 9905 4130
Campbelltown Ph (02) 4620 7155
Coffs Harbour
Ph (02) 6651 5238
Croydon
Ph (02) 9799 0402
Erina
Ph (02) 4365 3433
Gore Hill
Ph (02) 9439 4799
Hornsby
Ph (02) 9476 6221
Liverpool
Ph (02) 9821 3100
Convert negatives and slides to digital images quickly and
easily with this USB scanner. Each image is scanned in
about half a second for high-speed
$99 00
conversion and you can do some basic
editing using the included Arcsoft
SAVE $30 00
Photoimpression software or
one of many other image
management programs.
Breakdown & Emergency Road Flasher
Every car on the road should have a couple of these.
Simply switch them on and place them on the ground to
warn other motorists and guide them around a problem.
Flashing or steady mode.
• 90mm dia.
ST-3185
$9.95 each OR
buy 2 for $9.95
69 95
$
Maitland
Ph (02) 4934 4911
Newcastle
Ph (02) 4965 3799
Penrith
Ph (02) 4721 8337
Rydalmere
Ph (02) 8832 3120
Sydney City
Ph (02) 9267 1614
Taren Point
Ph (02) 9531 7033
Tweed Heads
Ph (07) 5524 6566
Wollongong
Ph (02) 4226 7089
NORTHERN TERRITORY
Darwin
Ph (08) 8948 4043
QUEENSLAND
Aspley
Ph (07) 3863 0099
Caboolture
Ph (07) 5432 3152
Cairns
Ph (07) 4041 6747
Capalaba
Ph (07) 3245 2014
Ipswich
Ph (07) 3282 5800
Mackay
Ph (07) 4953 0611
Maroochydore Ph (07) 5479 3511
Mermaid Beach Ph (07) 5526 6722
Nth Rockhampton Ph (07) 4926 4155
Arrival dates of new products in this flyer were confirmed at the time
of print. Occasionally these dates change unexpectedly. Please ring your
local store to check stock details. Prices valid to 23rd May 2010.
All savings are based on original RRP
PERFECT FOR
MOTHERS DAY
• Colour or B&W
film or slides
• Negative and slide
holders included
• 1,800 dpi resolution
• Windows XP, Vista
XC-4881 Was $129.00
SAVE $5 00
Desktop LED Magnifying Lamp
34 95
$
• Sizes: 0.7mm, 0.8mm, 0.9mm, 1.0mm, 1.2mm,
1.4mm, 1.6mm, 1.8mm, 2.0mm, 2.2mm.
TD-2407
Torx Key Set
Cat. TD-2170 $7.95
• Dimensions: 320(H) x 95(Dia)mm
QM-3544
Stainless Cutter / Pliers Set
Townsville
Ph (07) 4772 5022
Underwood
Ph (07) 3841 4888
Woolloongabba Ph (07) 3393 0777
SOUTH AUSTRALIA
Adelaide
Ph (08) 8231 7355
Clovelly Park
Ph (08) 8276 6901
Gepps Cross
Ph (08) 8262 3200
TASMANIA
Hobart
Ph (03) 6272 9955
Launceston
Ph (03) 6334 2777
VICTORIA
Cheltenham
Ph (03) 9585 5011
Coburg
Ph (03) 9384 1811
Frankston
Ph (03) 9781 4100
Geelong
Ph (03) 5221 5800
Hallam
Ph (03) 9796 4577
Melbourne
Ph (03) 9663 2030
Ringwood
Ph (03) 9870 9053
Springvale
Ph (03) 9547 1022
Sunshine
Ph (03) 9310 8066
Head Office
320 Victoria Road, Rydalmere NSW 2116
Ph: (02) 8832 3100 Fax: (02) 8832 3169
Thomastown
Werribee
WESTERN AUSTRALIA
Maddington
Midland
Northbridge
Rockingham
NEW ZEALAND
Christchurch
Dunedin
Glenfield
Hamilton
Hastings
Manukau
Mt Wellington
Newmarket
Palmerston Nth
Wellington
NZ Freecall Orders
Online Orders
Website: www.jaycar.com.au
Email: techstore<at>jaycar.com.au
Ph (03) 9465 3333
Ph (03) 9741 8951
Ph (08) 9493 4300
Ph (08) 9250 8200
Ph (08) 9328 8252
Ph (08) 9592 8000
Ph (03) 379 1662
Ph (03) 471 7934
Ph (09) 444 4628
Ph (07) 846 0177
Ph (06) 876 0239
Ph (09) 263 6241
Ph (09) 258 5207
Ph (09) 377 6421
Ph (06) 353 8246
Ph (04) 801 9005
Ph 0800 452 922
PRODUCT SHOWCASE
PowerShield Home Theatre Powerboard with the lot!
With powerboards available for under $3 these days, one which sells for
$149 is going to need to be something
extra special!
The PowerShield Theatreguard
home theatre powerboard from Altronics is something extra special!
For a start, it’s the appearance – in
It also has inbuilt surge, spike and
lightning protection (144,000A or 3672
joules is the claim!) along with jacks
for phone/fax protection (one line in,
two lines out) and both F and standard
superb “piano black” finish it’s not
something to hide away – it’s something to show as a feature of your home
theatre system!
With three “always on” and five slave
3-pin mains outlets (the slaves power
up when a master device is turned on)
you’re going to save a lot of “standby”
electricity. We’re told that up to 10% of
our power bills are from standby power.
But that’s not unusual, lots of powerboards can do that. What is unusual is
that any of your existing device infrared
remote controls (eg TV, DVD, etc) will
also control the powerboard. It will
even power down automatically three
minutes after the master device goes
into standby mode.
aerial antenna sockets for TV antenna
and cable antenna surge protection.
But wait, there’s more: a large blue
digital display reads the total power
being used at any instant (in watts)
through the slave outlets, so you can
make a conscious effort to save power.
The device itself uses only 0.85W
on standby.
The PowerShield Theatreguard is
available from Altronics stores, resellers and via their website (Cat P8140).
Contact:
Altronic Distributors Pty Ltd
PO Box 8350, Perth Busn Centre, WA 6849
Tel: 1300 780 999 Fax: 1300 790 999
Website: www.altronics.com.au
Tool box and parts
storage in one!
Jaycar have a
great new tool
box which can
also hold parts
in its four
233 x 122
x 32mm
storage
trays. The
13 tray compartments
can be
removed
to fit larger items.
All the hinges and catches are the
durable pintle type, not a flimsy bit
of folded plastic that will snap after
a week. The tool box has a generous
265 x 160 x 65 space and it’s finished
in a tasteful shade of industrial yellow and black.
Retail price is $14.95 (Cat HB6302),
available from all Jaycar stores, resellers and their website.
SC
Contact:
Jaycar Electronics
(All stores and web Techstore)
Tel: 1800 022 888
Website: www.jaycar.com.au
Avcomm’s new tiny multiband receivers have Digital Signal Processing
They might be small (135 x 85 x 27mm) but these two new Tecsun
multiband receivers pack some outstanding features, including DSP.
DSP offers the highest possible sensitivity, selectivity and provides
a continuous display of received level and signal-to-noise ratio. It is
particularly suited to those who desire broadcast band reception.
The Tecsun PL300 (left) covers 64.00MHz to 108.00MHz (FM – including the FM broadcast band) – and from 153KHz to 1710KHz (long
wave and AM broadcast band) plus 3150KHz to 21950KHz in 1KHz
steps. This model features a world-time dial and display. It normally
retails for $89.00 but SILICON CHIP readers who mention that they saw
it in the magazine can get it for just $79 (May 2010 only).
The Tecsun PL310 receiver covers the same bands but offers several added features, including keyboard direct frequency entry and an
external antenna socket while still offering DSP across all bands. The
PL310 retails for $90.00
Both have earphone sockets (and earphones are included) and are
powered by 3xAA batteries but the PL-310 includes a mini USB socket
so can be powered via a computer or standard USB supply. Both also
offer LCD clocks and frequency displays.
siliconchip.com.au
Contact:
Av-Comm Pty Ltd
24/9 Powells Road, Brookvale NSW 2100
Tel: (02) 9939 4377 Fax: (02) 9939 4376
Website: www.avcomm.com.au
May 2010 53
By NICHOLAS VINEN
Compact High-Performance
12V Stereo Amplifier
Amplifiers which run from 12V DC generally don’t put out much
power and they are usually not hifi as well. But this little stereo
amplifier ticks the power and low distortion boxes. With a 14.4V
supply, it will deliver 20 watts per channel into 4-ohm loads
at clipping while harmonic distortion at lower power levels is
typically less than 0.03%.
T
HIS IS AN IDEAL project for anyone wanting a compact stereo amplifier that can run from a 12V battery.
It could be just the ticket for buskers
who want a small but gutsy amplifier
which will run from an SLA battery
or it could used anywhere that 12V
54 Silicon Chip
DC is available – in cars, recreational
vehicles, remote houses with 12V DC
power or where ever.
Because it runs from DC, it will be
an ideal beginner’s or schoolie’s project, with no 240VAC power supply
to worry about. You can run it from
a 12V battery or a DC plugpack. But
while it may be compact and simple
to build, there is no need to apologise
for “just average” performance. In
listening tests from a range of compact
discs, we were very impressed with
the sound quality.
siliconchip.com.au
Long-time readers might recall that
we presented a similar 12V power amplifier design back in May 2001. It was
a similar configuration to this one but
it is now completely over-shadowed by
the much lower distortion and greatly
improved signal-to-noise ratio of this
new design. In fact, let’s be honest: the
previous unit is not a patch on this
new design. It used two TDA1519A
ICs which resulted in distortion figures
above 1% virtually across the board
and a signal-to-noise ratio of only
-69dB unweighted.
However, by using the TDA
7377
power amplifier IC and making some
other improvements, the THD (total
harmonic distortion) of the new design is about 50 times better than the
older unit (see performance graphs
for details). The bottom line is that
the THD under typical conditions is
around just 0.03% or less. It is also
able to deliver more output power due
to the improved output transistors in
the new power amplifier IC.
In addition, its idle power consumption is low – not much more than 1W.
As a result, if you don’t push it too
hard it will run cool and won’t drain
the battery too quickly. And because
the IC has self-protection circuitry,
it’s just about indestructible. It will
self-limit or shut down if it overheats
and the outputs are deactivated if they
are shorted.
Obtaining enough power
With a 12V supply, the largest voltage swing a conventional solid-state
power amplifier can generate is ±6V.
This results in a meagre 4.5W RMS
into 4Ω and 2.25W RMS into 8Ω, without considering losses in the output
transistors. Even if the DC supply is
around 14.4V (the maximum that can
normally be expected from a 12V car
battery), that only brings the power
figures up to 6.48W and 3.24W for 4Ω
and 8Ω loads respectively – still not
really enough.
There are three common solutions to
this problem. The first is to boost the
supply voltage using a switchmode
DC converter. This greatly increases
the cost and complexity of the amplifier but it is one way of getting a lot of
power from a 12V supply. However, we
wanted to keep this project simple and
that rules out this technique.
There are variations on the boosting method, such as the class H architecture used in the TDA1562Q IC
siliconchip.com.au
It may only be small but the 12V Mini Stereo Amplifier puts out up to 20W
per channel into 4Ω loads at low distortion. It uses just two ICs and is very
easy to assemble.
featured in the Portapal PA Amplifier
(SILICON CHIP, February 2003). It is
able to achieve 40W/channel but with
>0.1% THD. In that case, the amplifier
output itself provides the switching for
a charge pump.
The second method is to lower the
speaker impedance. Some car speakers have an impedance as low as 2Ω,
which allows twice as much power to
be delivered at the same supply voltage. However, we don’t want to restrict
this amplifier to 2Ω loudspeakers.
The remaining solution is to use
bridge mode, also known as BridgeTied Load (BTL). It requires two amplifier circuits per channel. The TDA
7377 IC is ideal for this purpose – it
contains four amplifiers in a single
package and is intended for a bridged
stereo configuration.
In the TDA7377, two of the four
amplifier circuits have inverting inputs, so all we need to do is to feed
the same signal to one of each type
and the outputs will swing in opposite
directions – when one voltage goes up
the other will go down and vice versa.
Instead of connecting the speakers
between the amplifier output and
ground, we connect them between the
two outputs. This doubles the voltage across the speaker and multiplies
the maximum power delivered by
four (P = V2/R). It also eliminates the
AC-coupling capacitor at the output,
which is needed with a standard single
supply amplifier.
Practically speaking, virtually any
4Ω or 8Ω speaker is suitable for use
with this amplifier; the more efficient,
the better. Avoid anything less than 4Ω,
as that would be asking each amplifier
circuit to drive a load under 2Ω, which
the IC is not rated for.
Circuit description
Fig.3 shows the full circuit. As can
be seen, it’s based on the aforementioned TDA7377V monolithic stereo
BTL amplifier (IC2) plus a TL074 quad
FET-input op amp package (IC1). The
latter provides the tone control stages
in both channels.
May 2010 55
03/19/10 16:16:20
2
2
1
1
0.5
0.5
0.2
0.2
0.1
0.1
0.05
0.05
0.02
0.02
0.01
03/19/10 16:19:59
THD+N % vs Power, 8 , 14.4V
5
THD %
THD %
THD+N % vs Power, 4 , 14.4V
5
0.01
60m
100m
200m
500m
1
2
5
10
20
30
60m
100m
200m
Watts
56 Silicon Chip
1
2
5
10
20
30
Watts
Fig.1: THD+N vs output power at 4Ω (one channel driven
only). The supply is 14.4V and the measurement band
width is 20Hz-22kHz. The distortion increase below 1W
is due to noise.
As shown, the input signals are fed
via 4.7µF non-polarised capacitors to
a 10kΩ dual-gang potentiometer (VR1)
which serves as the volume control.
From there, the signals are AC-coupled
via 470nF capacitors to op amps IC1a
& IC1b. These act as unity-gain buffer
stages to provide a low source impedance for the following Baxandall tone
control stages based on IC1c & IC1d.
In operation, IC1c & IC1d and their
associated potentiometers (VR2 & VR3)
provide bass and treble boost of ±15dB,
with a centre frequency of 700Hz. The
frequency response is very flat when
the pots are centred (see Fig.11).
To understand how the tone control
stages work, let’s consider the bass and
treble sections separately. We’ll concentrate on the bass sections first but
will initially ignore the 10nF capacitors. This leaves us with an inverting
amplifier (IC1c or IC1d), where the
resistors (including the pots) form the
feedback network and thus control
the gain. With the bass pot turned all
the way clockwise, the gain is set at
122kΩ/22kΩ or about 5.5. If it is turned
in the opposite direction, the gain is
22kΩ/122kΩ or 0.18.
Adding the 10nF capacitors across
VR2a & VR2b adds a low-pass filter to
each gain network, so that turning the
knob affects low frequencies more than
high frequencies. As a result, we can
adjust the gain of the bass and hence
achieve bass boost/cut.
500m
Fig.2: THD+N vs output power at 8Ω with both channels
driven. The supply is 14.4V and the measurement band
width is 20Hz-22kHz. The disparity between the channels
is primarily due to tone control pot tracking errors.
The treble section (VR3a & VR3b)
works similarly except that the capacitors (4.7nF in this case) are in series
with the resistors, thus forming a highpass filter instead.
The 10pF capacitors on the inverting
inputs of IC1c & IC1d reduce their gain
at high frequencies, thereby preventing oscillation in case there is RF pickup in the filter network. Similarly, the
10Ω resistors at the outputs of IC1c &
IC1d attenuate any RF signals which
may make it through before they go
into the power amplifier (IC2).
Power amplifier
Only a few external components are
required by the single TDA7377V IC
(IC1). It’s very clever – not only does it
contain the four low-distortion amplifiers we need to drive stereo speakers
in BTL configuration but it has virtually rail-to-rail swing on the outputs
and is inherently stable with a fixed
26dB gain (see the separate article in
this issue for more details on how the
TDA7377V works).
We have used its standby pin (pin
7) to switch the amplifier on and off.
This avoids having high current passing through on/off switch S1. In fact,
S1 only switches the power to pin 7 of
IC2 and to the quad op amp IC1. Hence
the power supply and IC1 remain energised as long as the supply voltage is
present but only the capacitor leakage
and standby current are drawn, a total
of around 100µA. Switching the amplifier on raises the quiescent (no signal)
current to around 100mA.
As soon as switch S1 is turned on,
the 100µF filter capacitor is charged
via diode D1. The standby pin (pin
7) has a low-pass filter consisting of
a 22kΩ resistor and 1µF capacitor so
that the power amplifier is not enabled
until the op amp is on. This avoids
turn-on thumps.
Similarly, when you switch S1 off,
the 22kΩ resistor at the anode of diode
D1 pulls down the standby pin voltage,
turning the power amplifier IC off almost immediately. This avoids switchoff thumps from the loudspeakers.
Reverse polarity protection
The main power supply components
are the four 2200µF 25V electrolytic
capacitors plus two 470nF MKT capacitors in parallel for high-frequency
filtering. Mosfet Q1 provides reverse
polarity protection for this section.
Although the TDA7377 IC can
withstand negative supply voltages,
the electrolytic capacitors cannot. In
the May 2001 design, a 3A diode was
placed across the supply rails so that
it would conduct and blow the fuse if
the supply polarity was accidentally
reversed. In this circuit, however, we
have connected an IRF1405 Mosfet in
series with the supply ground lead.
In essence, the Mosfet acts like a
diode with a very low forward voltsiliconchip.com.au
siliconchip.com.au
May 2010 57
100k
VR1a
10k A
470nF
47 F
VOLUME
470nF
VR1b
10k A
1k
1k
6
5
100k
100k
2
3
1
IC1b
7
IC1: TL074
IC1a
4
NP
4.7 F
NP
4.7 F
100nF
12V MINI STEREO AMPLIFIER
100k
4.7 F
NP
4.7 F
NP
100 F
22k
4.7nF
4.7k
10nF
VR2b 100k
22k
VR3b 50k
4.7k
4.7nF
22k
A
D1
22k
4.7nF
4.7k
TREBLE
VR3a 50k
22k
VR2a 100k
BASS
4.7k
4.7nF
22k
10nF
K
10pF
13
12
10k
10k
10
9
10pF
11
IC1d
IC1c
A
K
10
470nF
1 F
22k
470nF
22k
10
10k
ZD1, ZD2
14
8
10k
A
STBY
G
D
S
IRF1405
47 F
D
PG
8
470nF
10
SG
9
OUT4 14
OUT3 15
DIAG
OUT2 2
2
1
2200 F
25V
2200 F
25V
OUT1 1
3 13
Vcc Vcc
IC2
TDA7377V
SVR
6
11 IN4
12 IN3
7
5 IN2
4 IN1
470nF
2200 F
25V
2200 F
25V
S1 POWER
Fig.3: the complete circuit is based on a TL074 quad FET-input op amp (IC1) and a TDA7377V quad power amplifier (IC2). IC1a-IC1d
and their associated stereo potentiometers (VR2-VR3) form a Baxandall tone control circuit and this drives IC2 which is wired in bridged
stereo mode. Mosfet Q1 provides reverse polarity protection.
2010
SC
10
RIGHT IN
CON2
10
CON1
LEFT IN
K
D1 1N4004
4
6
A
8
K K
A
10
RIGHT
OUT
TDA7377V
14 15
+
Q1
IRF1405
F1 6.5A
LEFT
OUT
–
CON5
–
+
12
S
D
CON4
–
ZD2
15V
ZD1
15V
G
100k
+
CON3
–
+
DC
IN
in fact, than if a standard diode had
been used.
IC2 TDA7377V
BASS
TREBLE
+
R IN
+
10k
CON2
470nF CON1
4.7 F 4.7 F
NP
NP
1k
100k
10k
10k
22k
VR3 2x50k B
470nF
10k
100k
100k
10
10
GND
NP
10pF
VR2 2x100k B
100k
1k
4.7 F
10pF
100 F
47 F
L IN
CON5
4.7 F
22k
10nF
D1
100nF
4.7nF
4.7nF
4.7k
4.7k
4.7k
4.7k
22k
22k
22k
22k
10nF
4.7nF
4.7nF
15V
2200 F
4004
22k
Power source
RIGHT
OUTPUT
2200 F
NP
ZD1
ZD2
470nF
22k
SWITCH
S1
10
10
47 F
470nF
470nF
470nF
CON4
Q1
IRF1405
1 F
IC1 TL074
15V
CON3
–
–
12V DC
INPUT
+
100k
+
2200 F
–
2200 F
+
LEFT
OUTPUT
VR1 2x10k A
VOLUME
Fig.4: follow this layout diagram to build the PC board. Make sure that all
polarised parts are correctly oriented and don’t get the pots mixed up.
The maximum current consumption
depends on the speaker impedance
and how far up you turn the volume.
As a rough guide, full power with a
14.4V supply and 8Ω speakers requires
at least 3A. For 4Ω speakers, the current consumption can exceed 6A.
At a minimum, use a 7.2Ah SLA
battery for 8Ω speakers or a 12Ah SLA
for 4Ω. They should last 2-24 hours
depending on how hard you’re driving the amplifier (larger batteries will
last longer).
You can charge the battery while
using the amplifier, although this may
slightly prejudice the sound quality
due to the supply ripple that charging
introduces. Power supply rejection
is >50dB at 300Hz and thanks to the
large supply bypass capacitors, the
additional noise should be kept to a
low level.
If you want to run the amplifier from
a mains power supply, both linear and
switchmode types are suitable. A 6A
linear supply is likely to be large and
expensive so switchmode is probably
the way to go. A higher supply voltage
(ie, up to 16V) will give more power.
The absolute maximum operating
voltage is 18V, so make sure whatever
you use can never exceed that.
Construction
This view shows the completed prototype. The pot bodies are connected
together using a length of tinned copper wire which loops across them and
is terminated in pads on either side of the board.
age, typically less than 25mV at 5A
(we measured 8.7mV at 2.5A). This
compares with around 1V at 5A for a
58 Silicon Chip
standard rectifier diode. This means
that the amplifier can deliver significantly more power, about 15% more,
All the circuitry, including the potentiometers for the volume and tone
controls, is mounted on a PC board
measuring 97 x 78mm and coded
01104101. This is mounted in a compact metal case with an aluminium
base and steel lid.
Fig.4 shows the parts layout on the
PC board. Start by checking the board
for defects, such as shorts or breaks in
the copper tracks and undrilled holes.
If it’s OK, start the assembly by installing the four wire links using 0.71mm
tinned copper wire. Make sure they are
straight and flat before soldering, since
some of the links pass near exposed
component legs.
Next, install the fixed value resistors. It’s a good idea to check each
value with a DMM, as the colour codes
can be notoriously hard to read.
After that, solder in the two zener diodes. They are identical but make sure
that you get their orientation correct.
Once the zeners are in, bend the
siliconchip.com.au
03/19/10 16:09:53
2
2
1
1
0.5
0.5
0.2
0.2
0.1
0.1
0.05
0.05
0.02
0.02
0.01
03/19/10 16:08:31
THD+N % vs Frequency, 8 , 14.4V, 5W
5
THD %
THD %
THD+N % vs Frequency, 4 , 14.4V, 5W
5
0.01
20
50
100
200
500
1k
2k
5k
10k
20k
20
50
100
200
500
Hz
Fig.5: THD+N vs frequency for 5W into 4Ω. The supply is
14.4V and the measurement bandwidth is <10Hz-80kHz.
The reading at 1kHz is slightly higher than in Fig.1 due to
the wider measurement bandwidth.
Mosfet’s leads down at right angles
about 5mm from its tab using small
pliers. That done, insert its leads into
the PC board and check that its mounting hole lines up. Adjust the leads if
necessary, then secure the tab to the
PC board using an M3 x 6mm machine
screw, spring washer and nut. Once
it is firmly in place and cannot move,
solder and trim the three leads.
Next, install the three terminal
blocks. Push them all the way down so
that they sit flush with the board and
check that they are correctly oriented
before soldering their pins. The three
polarised polarised headers can then
be installed, again taking care with
their orientation.
Follow with the MKT capacitors and
the two ceramic types. The polarity
doesn’t matter here but don’t get the
values mixed up. The four bipolar
electrolytic capacitors can then be
installed, followed by the four small
polarised electrolytics but don’t install
1k
2k
5k
10k
20k
Hz
Fig.6: THD+N vs frequency for 5W into 8Ω. The supply is
14.4V and the measurement bandwidth is <10Hz-80kHz.
The reading at 1kHz is slightly higher than in Fig.2 due to
the wider measurement bandwidth.
the larger 2200µF units just yet.
Next, install the TL074 IC, making
sure it goes in the correct way around.
We used a socket in our prototype
but there’s no reason why it cannot
be directly soldered to the PC board.
done, check that the pins are all still
properly inserted and that the package
is parallel with the edge of the board.
When it is all straight, solder a couple of leads and recheck its orientation
before finishing the job.
The four 2200µF electrolytic capacitors can now be installed. Make sure
that each of these sits flush against
the PC board and is oriented correctly.
Installing the TDA7377
It’s now time to install the
TDA7377V. You must do this slowly
and carefully since it’s difficult to
remove if it’s misaligned.
Start by gently inserting its leads
through the board, taking care not to
bend any of them. You may need to
adjust them using needle-nose pliers if
they have been bent during transport,
so that they line up properly.
Once the pins have been pushed
all the way down, place the metal tab
of the IC on a flat, horizontal surface
with the PC board vertical. Hold
the IC down against the surface and
adjust the angle of the board so that
they are exactly at right angles. That
Cutting the pot shafts
Before fitting the potentiometers
(VR1-VR3), it’s necessary to cut their
Table 2: Capacitor Codes
Value
470nF
100nF
10nF
4.7nF
10pF
µF Value IEC Code EIA Code
0.47µF
470n
474
0.1µF
100n
104
0.01µF
10n
103
.0047µF 4n7
472
NA
10p
10
Table 1: Resistor Colour Codes
o
o
o
o
o
o
o
siliconchip.com.au
No.
5
8
4
4
2
4
Value
100kΩ
22kΩ
10kΩ
4.7kΩ
1kΩ
10Ω
4-Band Code (1%)
brown black yellow brown
red red orange brown
brown black orange brown
yellow violet red brown
brown black red brown
brown black black brown
5-Band Code (1%)
brown black black orange brown
red red black red brown
brown black black red brown
yellow violet black brown brown
brown black black brown brown
brown black black gold brown
May 2010 59
up with four 21mm spacers. Note: the
spacers at the rear of the board are
later removed when it is attached to
the heatsink.
Initial checks
Follow this photo and the text to complete the wiring inside the case. Note
the use of shielded cable to connect the RCA input sockets.
If you have a bench supply, set it to
12V with a current limit of 200mA.
Otherwise, use a 12V plugpack or
similar supply – if possible, one which
is too small to provide much current.
First, connect your DC supply to
the power block (CON3), with a DMM
wired in series and set to read amps.
Now switch the supply on and check
the current reading. With no power
switch attached, the current should
be negligible (<1mA) and the DMM
will probably read 0 (once the 2200µF
capacitors have charged).
If it reads more than a few milliamps, switch off and check the board
for mistakes.
Now short the switch header pins
(ie, for S1) together using a piece of
wire. The current should now increase
to around 100mA and possibly as high
as 160mA. If you remove this short,
the reading should drop back to 0mA
within a second or so.
If you have made a mistake with the
Mosfet or zeners, it’s possible no current will flow at all. If that happens,
check that area of the board. It could
also be a problem with the standby
RC filter components (22kΩ and 1µF).
Drilling the case
shafts to length so that the “D”-shaped
sections (ie, the flat sections) are about
10mm long. This is done by clamping
the end of each shaft in a vice and then
cutting it with a hacksaw. Deburr the
ends when you have finished, so that
the knobs can later be fitted.
VR1-VR3 can now be installed on
the board. They each have a different
value, so be sure to mount each one
in the correct location.
Earthing the pot bodies
To prevent noise pickup, it’s necessary to earth the bodies of the pots.
This is done using a length of tinned
copper wire which loops across the top
of the pots and is terminated at both
ends to pads on the PC board.
To install this wire, first solder
one end to the pad immediately to
the right of the volume control. That
done, stretch the wire across the tops
of the three pots and feed the free end
into the pad to the left of the bass pot.
60 Silicon Chip
Finally, pull the wire down tight and
solder it in position, then solder the
wire to the top of each pot body.
Note that it will be necessary to
scrape away the passivation material
on each pot body in order for the solder to take. You will also need to use
a hotter-than-normal soldering iron in
order to heat the pot bodies sufficiently
for soldering.
In practice, the pot bodies will later
all be in contact with the bare metal
of the case, so it should not be necessary to connect the GND pad on the
PC board to the case itself. However,
if you elect to house the board in a
plastic case, it will be necessary to
connect the GND pad to the ground
(-) terminal of CON3.
The PC board assembly can now
be completed by attaching an M3 x
12mm spacer to each corner, secured
by M3 x 15mm machine screws. That
done, thread M3 x 9mm spacers over
each end so that you effectively finish
Fig.7 shows the drilling details for
the front and rear panels of the case.
This can either be copied and used
as a template or you can download a
PDF file from the SILICON CHIP website,
print it out and use that instead.
Start by attaching the front panel
template section to the case. Once
that’s done, centre-punch the location
of each hole, then remove the template
and drill a small pilot (eg, 2mm) hole
at each location. Before going further,
place the board assembly in the case
and check that the three righthand
holes line up correctly with the centres
of the pot shafts.
Once you are satisfied that everything is correct, drill the three potentiometer holes to 6.5mm, then check that
the pot shafts (included the threaded
portions) go all the way through).
Enlarge the holes if necessary using a
tapered reamer until it fits correctly.
The switch cutout is made by first
pilot-drilling the two marked posisiliconchip.com.au
130
23.5
31
23.5
44.5
13.25
31
33
4
B
A
A
A
11
B
70
4
10
6.5
(FRONT PANEL)
HOLES A: 6.5mm DIAM. HOLES B: 5.5mm DIAM. (FOR SWITCH CUTOUT)
ALL DIMENSIONS IN MILLIMETRES
HOLES C: 8.0mm DIAM.
HOLES D: 9.5mm DIAM.
HOLE E: 12.5mm DIAM.
130
22
34
D
C
24
C
C
D
24
20
70
E
C
15
C
20
25
30
25
15
(REAR PANEL)
Fig.7: this diagram shows the drilling templates for the front and rear panels. Centre-punch each hole position and
drill small pilot holes before carefully enlarging them to size using progressively larger drills and a tapered reamer.
tions, then enlarging them to 5.5mm
and drilling a third hole between them.
The centre piece can then be knocked
out and a small flat file used to gradually enlarge the cutout to the marked
rectangular outline.
Slowly enlarge it in each direction
until the switch snaps into place and
is locked in by its plastic tabs. It will
take a good 10-15 minutes of patient
filing, so take it slowly and make sure
you don’t make the hole too large or
crooked.
should each be marked on the underside of the case and are positioned
6mm in from the front panel and 21mm
in from the sides. Drill them to 3mm
then slide the board into position and
fit the mounting screws.
Don’t worry about securing the pots
to the front panel at this stage —that
step comes later. For the time being,
just check that everything lines up
correctly, then remove the board and
power switch so that the rear panel
can be drilled.
Installing the PC board
Rear panel drilling
In order to later secure the PC board,
it’s necessary to drill mounting holes
in the base of the case for the front (but
not the rear) spacers. The two holes
Eight holes have to be drilled in
the rear panel – two for the insulated
RCA input sockets (D), four for the
loudspeaker terminals (C), one for
siliconchip.com.au
the DC power socket (C) and one for
the fuse (E).
Begin by securing the drilling template accurately in position (use tape),
then centre-punch each hole location,
and drill small pilot holes. The template can then be removed and the
holes enlarged to the sizes indicated
using drills and a tapered reamer (ie,
8mm for the binding posts and DC
connector, 9.5mm for the RCA sockets and 13-15mm for the fuseholder,
depending on the exact type).
Use an oversize drill to deburr the
holes, then install the rear panel hardware as shown in the photos. Make
sure all the nuts are done up tightly
so the components can’t rotate. By
the way, insulated RCA input sockets
May 2010 61
Using A Mosfet As A Diode
In this project we have used a Mosfet
instead of a diode for reverse polarity
protection, for the reasons explained in
the article.
Fig.8 shows how an N-channel Mosfet
is typically used for motor control, lamp
flashing or any other task where a high
current DC electronic switch is required.
Because a Mosfet’s source is generally
connected to the substrate, a parasitic
diode known as the “body diode” is present. This is shown in the symbol and it
cannot be avoided.
Because its source is connected to
ground, Q1 is on whenever the gate voltage is above the Mosfet’s on-threshold
(usually 2-4V). The body diode is reverse
biased and does not conduct unless the
load is inductive and switch-off causes
a large enough positive voltage spike to
trigger reverse breakdown (avalanche).
What we want to do, though, is use
a Mosfet to prevent current flow if VCC
becomes negative. In the case of Fig.8,
if this were to happen, the body diode
are mandatory if you want to get low
distortion.
Pay attention to the orientation of
the holes in the binding posts. The
upper two (red) should have the holes
vertical, while the lower two (black)
should be orientated with the holes
30-45° from vertical so that you can
insert the speaker leads from the side.
Attaching the heatsink
The specified heatsink is a 55 x
105mm “fan” type. It is quite heavy, so
it will need to be attached to the base
of the case using two right-angle steel
INSULATING
BUSH
TDA7377V
brackets (obtained from Bunnings).
To do this, stand the heatsink vertically on a flat surface and place a
bracket flush against the flat side at one
end. Mark the centre of the mounting
hole, then repeat this procedure at
the other end. The two holes are then
centre-punched and drilled to 4mm.
Remove any swarf from around the
holes using an oversize drill, then
attach the brackets using two M4 x
10mm machine screws, spring washers and nuts.
Now remove the rear spacers from
the PC board, install it in the case and
INSULATING
PAD
SPRING M3
WASHER NUT
HEATSINK
M3 x 15MM
SCREW
would conduct and it would be impossible
for the Mosfet to provide reverse polarity
protection. Hence, we must reverse the
Mosfet and connect it so that the source
is positive with respect to the drain, as
shown in Fig.9.
Note that the body diode is now forward
biased when VCC is positive. If we also bias
the Mosfet on, all of the current will flow
through the channel (ie, source to drain)
instead. The channel path will have a much
lower voltage drop than the body diode.
We achieve this by connecting a resistor
between the supply input and the gate.
When the supply voltage is positive, the
Mosfet is turned on and if it becomes negative it will be turned off and of course, the
body diode will be reverse-biased!
Because the source is no longer connected to ground it may seem that we
can no longer turn the Mosfet on. In fact,
the source is pulled to ground via the
body diode.
The final refinement adds two backto-back zener diodes between the gate
Fig.10: this diagram shows how the TDA7377V amplifier IC is attached
to the heatsink. It must be electrically isolated from the heatsink using an
insulating bush and pad.
62 Silicon Chip
+ VCC
ILOAD
RLOAD
D
VCONTROL
G
Q1
IRF1405
S
Fig.8: using a Mosfet as a switch
(typical connection).
D
VCONTROL
RPULLUP
G
RLOAD
Q2
IRF1405
S
ILOAD
+ VCC
Fig.9: using a Mosfet as an active
rectifier.
and source terminals. They are included
to prevent a supply voltage spike of more
than ±20V from destroying the Mosfet.
slide the heatsink up to it so that it sits
flush against IC2’s metal tab. Check
that the heatsink is correctly centred,
then mark the mounting holes for the
heatsink brackets on the bottom of the
case. The heatsink and PC board are
then removed and the marked locations drilled to 4mm.
The next step is to drill a mounting
hole in the heatsink for IC2’s metal
tab. That’s done by first reinstalling
the PC board in the case and securing
the heatsink to the base using two M4
x 10mm machine screws and nuts. It’s
then just a matter of marking the hole
location, then removing the heatsink,
centre-punching the marked location
and drilling to 3mm.
Now use an oversize drill to carefully deburr the mounting hole. This
step is most important —if there’s any
metal swarf around the hole, it could
punch through the insulating washer
that’s used to electrically isolate IC2’s
tab from the heatsink and create a
short circuit. Basically, it’s just a matter of checking that the mounting area
is perfectly smooth by running your
finger over the hole.
Attaching IC2 to the heatsink
IC2’s tab must be electrically isosiliconchip.com.au
Performance
Total harmonic distortion plus noise: typically <0.03%
Signal-to-noise ratio: 93dB (96dB A-weighted) with respect to 10W into 8Ω
Channel separation: -72dB at 1kHz
Input sensitivity: 500mV RMS for 10W into 8Ω
Input impedance: 8.3kΩ
Stability: unconditional
This view inside the
prototype clearly
shows the heatsink
mounting details.
Note that the speaker
polarity has been
reversed in the
final version (ie, the
positive speaker leads
should go towards
the rear of terminal
blocks CON4 & CON5
on the PC board).
lated from the heatsink using an insulating bush and washer – see Fig.10.
It’s just a matter of fitting the heatsink
back in the chassis, then attaching
IC2’s tab as shown. It’s secured using
an M3 x 15mm machine screw, spring
washer and nut. Do the screw up firmly
to ensure good thermal contact, then
use your multimeter (set to a low ohms
range) to confirm that IC2’s tab is correctly isolated from the heatsink.
By the way, if you use a mica washer
rather than a thermal insulating pad,
be sure to smear both sides of the
washer with thermal grease before
bolting the tab down.
Front panel
A front panel for the specified case
can be downloaded from the SILICON
siliconchip.com.au
CHIP website (as a PDF file) and printed
out on a colour printer. It’s attached using double-side tape and this should be
done with the PC board and heatsink
assembly out of the case. You will also
have to temporarily remove the rocker
switch if it’s in place.
Once the front panel is in position,
cover it with some wide strips of
adhesive tape, then cut out the holes
for the switch and pot shafts using a
sharp hobby knife. The adhesive tape
covering will protect the label from
scratches and finger marks and will
provide a durable finish.
The PC board and heatsink assembly
can now be permanently installed in
the chassis. Before sliding it in, fit a
nut onto the threaded boss of each pot
and wind it all the way up to the pot
body. That done, place the assembly in
the case and secure it via the heatsink
brackets and the screws that go into
the front spacers.
Now wind the pot nuts forward
until they contact the rear of the front
panel, then fit three more nuts to the
pots from the front. The six pot nuts
can now all be tightened to lock the
pots firmly in place and prevent the
front panel from flexing. Once they
are secure, fit the knobs and reinstall
the rocker switch.
Chassis wiring
All that’s left is the chassis wiring.
First, cut a short length of red heavyduty hook-up wire, strip the ends and
solder it between the centre pin of the
DC socket and the middle tab of the
May 2010 63
Frequency Response, 4 , 5W, 14.4V
02/23/10 09:56:35
03/19/10 16:33:59
THD+N % vs Power, 4 , 12.0V
+10
5
+8
2
+6
1
+4
0.5
THD %
dBr
+2
-0
-2
0.2
0.1
-4
0.05
-6
0.02
-8
-10
10
20
50
100
200
500
1k
2k
5k
10k
20k
50k
100k
0.01
60m
100m
200m
Hz
2
5
10
20
30
Fig.12: this graph of THD+N vs power is similar to that
shown in Fig.1 except that the amplifier is powered from a
12V 4A switchmode supply. As you can see, performance
doesn’t suffer much except that full power output is
reduced due to the lower supply voltage.
run from CON4 & CON5 to the binding
post terminals on the rear panel and
should be made long enough so that
they don’t touch the heatsink.
Note that we’ve reversed the output
terminal polarity compared to our prototype to compensate for the inverting
preamplifier stage. Ultimately, though,
it doesn’t matter greatly, as long as
both pairs of binding posts are connected the same way around (ie, the
loudspeakers are not in anti-phase).
The power switch wiring is next.
This can be run using two 95mm
lengths of medium-duty hook-up wire.
Begin by stripping about 8mm from
one end of each wire and crimping
them to two polarised header pins
using pliers. Once you have crimped
Connecting The GND Terminal
If you build the unit into the specified metal case, then it will not be necessary to connect the GND terminal to the case. That’s because the circuit earth
is connected to the case via the DC power socket, while the pot bodies are
earthed to the case via the nuts used to secure them.
In fact, if you do connect the GND pad to the case under these circumstances,
you could get an earth loop.
Conversely, if you elect to house the board in a plastic case, then it will
be necessary to connect the GND pad to the ground (-) terminal of CON3.
Alternatively, it can be connected to the negative terminal of the DC socket.
Similarly, if the pots are not directly secured to a metal chassis (ie, you don’t
fit the nuts), then the GND terminal should be connected to metalwork. You
can do this by securing a solder lug to the base of the case and then running
a short lead between it and the GND pad on the board.
64 Silicon Chip
1
Watts
Fig.11: this shows the amplifier’s frequency response
for a 4Ω load with the tone controls centred. The -3dB
point is around 25Hz. This is purposefully a little high
to reduce the chance of “motor-boating” with a sagging
supply voltage under load.
fuseholder. A 70mm length of red wire
is then run from the end fuseholder
tab to the +12V input terminal on the
board (ie, at CON3).
Now connect the two remaining tabs
on the DC socket together and run a
90mm length of black heavy-duty wire
to the ground (-) terminal of CON3. In
fact, the easiest way to do this is to strip
the insulation from the hook-up wire
back at least 15mm and wrap the wire
around both these tabs before flowing
solder over it. Because one of the tabs
goes to the metal thread of the DC
socket, this connects the negative rail
to the case and improves the shielding.
Next, connect the speaker outputs,
again using heavy-duty red and black
hook-up wire (see photos). These leads
500m
them, flow some solder into each junction so that it can’t come apart.
After soldering, insert the two pins
into one of the plastic header blocks
then strip about 5mm from the other
ends of the wires. These ends are then
attached to 4.8mm female spade connectors (a ratcheting crimper will do
the best job) which are then pushed
onto the switch terminals.
Alternatively, solder the wires directly to the switch terminals if that’s
what you prefer but be careful not
to overheat and damage the plastic
switch body.
Wiring the RCA sockets
All that remains is the wiring to the
RCA input sockets. These are connected using two lengths of shielded
cable which run back to two polarised
pin headers situated behind the volume control.
Begin by cutting two 150mm sections of shielded cable, strip 20mm
of insulation from each end and twist
the copper shield wires together. Then
strip 5mm of insulation from the inner wires.
At one end, tin the shield and inner
wires, then crimp them into polarised
header pins and flow solder into the
crimp pin so it can’t come apart. Note
that it’s necessary to twist the shield
wires tightly before soldering them,
so that they fit into the header pins.
After soldering, insert the pins into
siliconchip.com.au
the two remaining plastic header
blocks. In each case, the inner wire of
the shielded cable must go to the “+”
side of the header block (see Fig.4).
This means that when the headers
are plugged in, the inner wire of each
header must be to the left, as viewed
from the front of the PC board.
The shield leads must be to the right,
so that they connect to the earth pattern of the PC board when the headers
are plugged in.
The other ends of the shielded leads
can then be soldered to the RCA sockets. In each case, the inner lead goes
to the centre terminal of the socket,
while the shield wire is soldered to
the solder tab.
As stated above, it’s necessary to use
insulated RCA sockets for the inputs.
After connecting them, it’s a good idea
to check that neither RCA socket surround is shorted to the case (if they
are, the performance will suffer). You
can do this by using your multimeter
to check for continuity between the
outside metal surround of each RCA
socket and the case. You should get an
open circuit reading for both sockets.
If the meter does indicate a short,
check that the shield wires are not
touching the case at the metal tabs. If
they are, just bend the tabs forward
slightly until the short is cleared.
The assembly can now be completed
by plugging the other ends of the
shielded leads into the headers on the
PC board. Don’t get them mixed up –
the left input (white socket) should go
to the header on the left side of the PC
board and vice versa.
Once the wiring is complete, use
some cable ties to secure the various
leads as shown in the photos. This not
only keeps them looking tidy but will
also prevent them from coming adrift.
That’s it —construction is complete.
Final testing
Now for a final test. Install the 6.5A
fuse into the fuseholder and connect
a signal source (eg, a CD player) and
a pair of speakers. Be sure to connect
the speakers in phase and don’t crosswire the leads.
Now turn the volume knob all the
way down, switch on and slowly turn
the volume up. If you hear audio loud
and clear then all is well! If not, switch
off immediately and check the chassis
wiring carefully. If there’s a problem,
it’s a good idea to first measure the
voltage across the power terminal
siliconchip.com.au
Parts List
1 vented aluminium case (Jaycar
HB-5444)
1 PC board, code 01104101, 97
x 78mm
1 55mm “fan”- type heatsink
(Jaycar HH-8570, Altronics
H-0250)
1 SPST mini rocker switch
(Jaycar SK-0975, Altronics
S-3202/S-3247)
2 4.8mm female spade lugs
2 small steel brackets (Bunnings
RAB020)
4 M4 x 10mm machine screws
4 M4 nuts
4 M4 spring washers
1 2.1mm I.D. chassis-mount
DC socket (Jaycar PS-0522,
Altronics P-0622)
1 low-voltage M205 chassismount fuseholder (Jaycar
SZ-2020, Altronics S-5992)
1 M205 6.5A fast-blow fuse
2 red insulated binding posts
(Jaycar PT-0453, Altronics
P-9252)
2 black insulated binding posts
(Jaycar PT-0454, Altronics
P-9254)
1 red insulated RCA socket
(Jaycar PS-0276, Altronics
P-0218)
1 white insulated RCA Socket
(Jaycar PS-0278, Altronics
P-0220 [Black])
2 16mm knobs (Jaycar HK-7762,
Altronics H6040)
1 24mm knob (Jaycar HK-7764,
Altronics H-6044)
3 2-pin terminal blocks (5.08mm
spacing)
3 2-pin polarised headers
(2.54mm spacing)
3 2-pin polarised header connectors (2.54mm spacing)
1 TO-218 mica or silicone insulating washer (with bush)
5 M3 x 6mm machine screws
1 M3 x 10mm machine screw
4 M3 x 15mm machine screws
2 M3 spring washers
2 M3 nuts
block, to make sure power is actually
reaching the board.
If that doesn’t solve the problem,
you’ll need to recheck the component
placement and orientation, as well as
the solder joints. If the fuse blows, then
4 M3 x 12mm tapped Nylon
spacers
4 M3 x 9mm tapped Nylon
spacers
1 500mm length of red heavyduty hook-up wire
1 500mm length of black heavyduty hook-up wire
1 300mm length of medium-duty
hook-up wire
1 400mm length of single-core
shielded cable
1 300mm length of 0.71mm
tinned copper wire
Heatsink compound (if using a
mica insulating washer)
8 100mm cable ties
3 additional nuts for pots
Potentiometers
1 100kΩ linear dual gang 16mm
potentiometer (VR2 – B100k)
1 50kΩ linear dual gang 16mm
potentiometer (VR3 – B50k)
1 10kΩ log dual gang 16mm
potentiometer (VR1 – A10k)
Semiconductors
1 TL074 quad op amp (IC1)
1 TDA7377V quad power amplifier
(IC2) (available from Futurlec)
1 IRF1405 MOSFET (Q1)
2 15V 1W zener diodes
(ZD1,ZD2)
1 1N4004 diode (D1)
Capacitors
4 2200µF 25V electrolytic
1 100µF 25V electrolytic
2 47µF 16V electrolytic
4 4.7µF non-polar (NP) electrolytic
1 1µF 25V electrolytic
6 470nF MKT
1 100nF MKT
2 10nF MKT
4 4.7nF MKT
2 10pF ceramic
Resistors (0.25W, 1%)
5 100kΩ
4 4.7kΩ
8 22kΩ
2 1kΩ
4 10kΩ
4 10Ω
you likely have a short circuit in your
chassis wiring, because the earlier tests
on the board would have shown up
any shorts on the board itself.
Assuming all is well, put on your
favourite CD and enjoy the sound! SC
May 2010 65
By NICHOLAS VINEN
Low-Power Car/Bike
USB Charger
Looking for an efficient USB charger that can operate from a
12V car battery? This unit functions at up to 89% efficiency and
can charge USB devices at currents up to 525mA. Best of all, it
won’t flatten the battery if it’s left permanently connected, as
long as you remember to unplug the USB device.
T
HERE ARE LOTS of USB chargers
on the market but this device has
two stand-out features: high efficiency
and low standby current. In fact, its
standby current is just 160µA, a figure
that’s well below the self-discharge
current of most lead-acid batteries.
This means that you can leave the
device permanently connected and it
will not cause that battery to go flat (or
at least, not much faster than it would
of its own accord).
Why is this useful? Well, in September 2009’s “Ask SILICON CHIP” section,
D. E. of Ainslie, ACT asked if it was
possible to connect a 12V-to-5V USB
charger directly to the battery on a motorbike. His reason for wanting to do
this is that doing anything else might
void the warranty. Our reply was that
it is possible but that it would need to
66 Silicon Chip
have a quiescent current (IQ) of less
than 1mA to avoid draining the battery
between uses.
While USB car chargers are cheap
and plentiful, finding one with a low
enough quiescent current for permanent battery attachment is difficult.
Even those marketed as “low idle
power” devices don’t specify how
much current they draw on standby.
We tested a regular charger and
found that it consumed 13mA with
no load. Like many others, it has an
integrated power LED and that would
contribute significantly to the standby
current consumption. However, since
the cigarette lighter socket is only
powered when the engine is running,
there is no real reason for the designers of these car supplies to keep the
quiescent current low.
Cigarette lighter plugs are also pretty
lousy DC connectors. They often don’t
fit well and can easily fall out. With
this project, you can use whatever type
of connector is most convenient. In
many cases, this will mean input wires
terminated in spade or eyelet lugs.
While this may seem like a very
specific application, there are many
other uses for a low-quiescent current
12V DC to 5V DC converter. For example, remote monitoring stations often
run from a 12V SLA battery topped
up by a solar panel. These stations
invariably contain a microcontroller
and other circuitry which needs a
3.3V-5V supply.
The current consumption in these
devices will be low most of the time
but occasionally the microcontroller
will wake up and activate a radio
siliconchip.com.au
5.05
100%
90%
80%
Efficiency %
60%
50%
5.00
40%
30%
Output Voltage (V)
70%
20%
10%
0%
0
100
200
300
400
Output Current (mA)
500
4.95
600
Fig.1: this graph plots the efficiency and output voltage over the full
output current range. As shown, the efficiency is over 80% for any
output current above 10mA.
module or other circuitry which can
draw more current. This charger can
deliver that current – up to 500mA –
while still being miserly with battery
power when the load is light.
In addition, because its efficiency is
high (up to 89%), hardly any battery
power is wasted even when the load
is drawing 500mA.
What is quiescent current?
So what exactly is quiescent (or
standby) current? This term often
comes up in IC data sheets. Its simple
meaning is “idle current”, although
when talking about regulators, it sometimes refers to the current consumed
by the device itself, rather than by what
it is supplying.
In most fixed regulators, this is the
same as the “ground pin current”.
There are typically two current flows
in a regulator – from the input to the
output and from the input to ground.
The ground pin current is the power
consumed by the regulator itself.
At higher currents, most regulators
consume more current than they do at
idle. As a result, the quiescent current
may be specified for different output
currents, including the no-load case.
Although the device is arguably no
longer “quiescent” when it is delivering an output, the term is often used
this way.
Since we primarily want to minimise power consumption with no
USB device attached, the idle current
is critical for this design. What’s more,
siliconchip.com.au
a device with low idle current will
usually also have low ground pin current at higher loads. This is just what
we want since the overall efficiency
is determined by the combination of
the conversion efficiency and ground
pin current.
USB charging issues
Basically, this device is a DC-DC
converter. You feed 12V DC (or there
abouts) in at one end and it delivers a
5V DC output at the other end. It complies with the USB 2.0 specifications
with regard to power, ie, it supplies at
least 500mA at 4.75-5.25V.
However, for some devices, this
current level is insufficient for them
to operate and charge their battery
simultaneously. Many of these devices
require a custom cable or special USB
data pin connection arrangement before they will attempt to draw more
than 500mA so that they can do both
at the same time.
This shouldn’t be a big problem
since such devices should be able to
operate without simultaneously charging the battery. The battery can then be
charged when they are switched off (ie,
no longer being used). Unfortunately,
many USB-powered devices provide
no way to switch modes like that.
However, if your device can operate
normally from a computer’s USB port,
it should work fine with this charger,
since they supply the same amount
of power.
There’s just one wrinkle here. If your
USB device switches to a data transfer
mode when plugged into a computer
USB port, it may behave the same
way when connected to this charger,
even though the data lines (D+ and D-)
aren’t connected. Its battery will still
charge but the device may have to be
unplugged to be used.
Devices which typically behave in
this manner are car GPS units. Plug
them into a PC’s USB port and they
immediately switch to data transfer
mode (ie, for downloading software
upgrades and map updates). This
doesn’t stop the internal battery from
charging via the USB port – it’s just
the the device must be unplugged in
order to use it as a GPS.
Design considerations
The first step in designing this
device was to find an appropriate
switchmode regulator IC. One candidate that satisfies all the requirements
is the Linear Technology LTC1174HV.
The HV (high-voltage) version can
run from 6-17.5V (for 5V output) and
consumes only 130µA at idle, with a
maximum output of around 500mA
(this is also the most current that can
be drawn from a single USB port). The
LTC1174HV is quite efficient too.
Unfortunately, it’s hard to get the HV
version in a DIP package. None of our
usual vendors stock it, so we had to
order the low-voltage version, which
has an absolute maximum rating of
only 13.5V.
This problem was solved by adding
a low quiescent current linear preregulator to the design. This prevents
the IC’s supply from exceeding 13V,
regardless of the battery voltage. The
only drawback is that it reduces the
efficiency slightly at higher battery
voltages, although it doesn’t add much
to the idle current.
However, since the battery will only
be above 13V while it is being charged,
the loss of efficiency under this condition doesn’t really matter.
The other issue is that while the data
sheet says that switching will occur at
around 100kHz with the components
we are using, at light loads the burst
mode causes switching to occur at
much lower frequencies – in some
cases, well into the audio range. As a
result, the inductor used in the circuit
makes some noise with light loads.
We managed to tweak the design
to minimise this noise. If you listen
carefully you can hear it but once the
May 2010 67
C
A
3
LB IN
1N5819
GND
4
K
VFB 1
D2
1N5819
IC1
LTC1174
100nF
USB CHARGER FOR CARS & BIKES
SC
C
–
12V
IN
E
B
1M
Q2
BC549
C
10M
B
Q3
BC559
E
TVS1
1.5KA
36CA
+
CON1
2010
VR1
200k
2x
22 µF
470nF
270k
2
A
ZD2
12V
A
ZD1
15V
Fig.2: the circuit is based on an LTC1174 switching regulator IC (IC1), while Mosfet Q1 and transistors Q2 &
Q3 form a pre-regulator circuit. The pre-regulator prevents the supply to IC1 from exceeding 13V, regardless
of battery voltage.
A
A
K
5
SW
LB OUT
6
7
8
VIN SHTDWN IPGM
2.2M
1k
K
G
K
Output voltage: 4.75-5.25V
Output current: approximately 525mA
Input voltage range: 6-16V DC
Input current requirement: maximum 300mA at 12.0V
Input current with output shorted: 4.3mA
Output ripple: 110mV p-p, 30mV RMS at 500mA
Load regulation: 50mV at 12V, 0-500mA (1%)
Line regulation: 16mV at 450mA, 7.0V-13.0V (0.32%)
No load input current: 160µA
Efficiency: up to 89% (see Fig.1)
Switching frequency: 10Hz – 120kHz
K
ZD1, ZD2
470nF
E
B
BC549, BC559
2x
47 µF
110k
330k
G
D
S
CON2
IRF9540
D
USB
TYPE A
SOCKET
OUTPUT
–
+
CON3
L1 100 µH
A
K
D3 1N5819
CON4
D
Q1 IRF9540
S
K
A
D1 1N5819
68 Silicon Chip
Performance
board is mounted in a box and placed in a moving vehicle, it will be inaudible.
Circuit description
Refer now to Fig.2 for the circuit details. IC1
is the main switching regulator IC, while Mosfet
Q1 and its associated parts form the pre-regulator
circuit.
Power from the external 12V DC source is fed
in via CON1. Immediately following this, a 36V
AC transient voltage suppressor (TVS1) across
the input damps any positive voltage spikes that
may appear on the supply line (eg, due to devices
switching on or off). Diode D1 then provides
reverse polarity and negative spike protection.
The pre-regulator circuit (based on Q1) was
published previously in Circuit Notebook for
March 2010. It is a low quiescent current Mosfetbased design, especially developed for this type
of application. Its operation was fully explained
in the Circuit Notebook entry, so we’ll just cover
the basics here.
Essentially, the transconductance of the Mosfet
Q1 is controlled so that the voltage at its drain
will not exceed a preset value. This is done using
zener diode ZD2, trimpot VR1 and transistors
Q2 & Q3.
In this case, the voltage on Q1’s drain is set
to 13V and VR1 allows you to trim this value.
We need to make sure the LTC1174 can’t be
damaged and this provides a small safety region
(ie, 0.5V) between its supply voltage and its
maximum rating.
The circuit works as follows. When power
is applied, Q1’s gate is pulled low via a 1MΩ
resistor, turning it on. Q1’s output voltage then
rises until ZD1, a 12V zener diode, begins to
conduct and pass current to trimpot VR1. Once
VR1’s wiper exceeds 0.65V, Q2 turns on and this
then turns on Q3.
As a result, current now flows though Q3 and
the 1MΩ resistor. This in turn increases Q1’s gate
voltage and switches it off. By suitably adjusting
VR1, Q1’s output can be accurately set to 13V.
siliconchip.com.au
The nominal 13V supply from the
pre-regulator is decoupled using two
22µF 16V tantalum capacitors and a
470nF MKT capacitor. Tantalum capacitors were chosen for two reasons:
(1) they have much lower leakage than
aluminium electrolytics and (2) they
have a lower ESR at high frequencies
than other electrolytics.
Any capacitor leakage across the
input or output of the switchmode
regulator adds to the quiescent current
of the circuit and we want to keep leakage to a minimum. The switchmode
circuit can operate at frequencies in
excess of 100kHz (occasionally as high
as 1MHz) in burst mode, so we need
to make sure the capacitors will be
effective at high frequencies.
The switchmode regulator section is
based on the schematic shown in the
LTC1174 data sheet (“High Efficiency
3.3V Regulator”). However, the 50µH
inductor has been increased to 100µH
and we’ve added a voltage divider
since we need a 5.0V output instead
of 3.3V.
Pins 7 & 8 of IC1 are tied to the positive supply rail. Keeping pin 8 high
ensures that the IC is always enabled,
while pulling pin 7 high selects the
higher peak current limit (600mA).
That way, the current limiting will
not kick in until an average of almost
exactly 500mA is being supplied.
The 330kΩ and 110kΩ resistors
across the output form a 4:1 voltage
divider. This sets the output voltage.
In operation, the LTC1174 adjusts its
output voltage so as to keep its VFB pin
(pin 1) at 1.25V. This means that the
output voltage will be 1.25 x 4 = 5.0V.
If you want to change the output
voltage, use the formula R3 = R4 x
((VOUT/1.25) - 1), where R4 is 110kΩ.
For example, to set the output to 3.3V,
replace R3 with 180kΩ. In this case,
the output would be taken from CON3
(which is a polarised 2-pin header)
rather than from the USB socket.
The 2.2MΩ and 270kΩ resistors form
a voltage divider which is applied to
the LBIN (Low Battery Input) pin of IC1.
If the supply falls below 11V, pin 2 will
sink current (ie, it goes low). Header
CON4 enables a high-brightness LED
to be fitted to indicate the low-battery
condition but note that once it comes
on, it will then run the battery flat
even faster!
In short, this LED is optional and
should be left out unless you have a
specific reason for using it.
siliconchip.com.au
By contrast, diode D3 is necessary.
It’s included to protect IC1 from an
input supply short circuit – as unlikely as that may be. Without it, if an
input short were to occur, IC1 could
be destroyed.
Following L1 (which serves as the
switchmode energy storage element),
the output voltage is filtered by two
47µF tantalum capacitors and a parallel 470nF MKT capacitor. This is not a
great deal of capacitance but thanks to
the good high-frequency performance
of tantalum capacitors, the output ripple is typically no more than 110mV
peak-to-peak and 30mV RMS. Larger
capacitors could be used here but their
leakage currents would be higher.
The 5V output is fed to two different
output sockets connected in parallel.
CON2 is a Type A USB socket for
recharging USB devices. For other
devices, the output can be taken from
2-pin polarised header CON3.
Note that the operating temperature
range for the LTC1174CN8 is specified
as 0-70°C. If you live in a cold or extremely hot climate and will be using
this device outdoors (eg, mounted
outside the cabin of a vehicle), then
you may need to use the LTC1174IN8
IC instead. This can operate from -40°C
to 85°C.
Input limitations
Normally, the supply voltage will be
in the range of 12-14.4V. However, the
regulator will operate just fine over a
range of at least 9-15.6V. In a vehicle,
it is not unusual to get short-term voltage spikes in both directions. TVS1,
D1 and the pre-regulator combine to
protect the device from these spikes.
Voltages between -36V and 0V will
not harm the regulator since D1 will
not conduct. D1’s reverse breakdown
voltage is -40V but TVS1 should absorb
spikes below -36V anyway.
Above 15.6V, the regulator will
continue to operate normally, all the
way up to 36V at which point the
TVS clamps the supply voltage. We
tested the regulator to 30V and it ran
normally. However, if you were to run
the regulator at high current and high
voltage, Q1 would eventually overheat
since it has no heatsink.
This means that while the regulator
will run off voltages above 15.6V, as
can happen in a vehicle from time to
time, it must not be run at high voltages
for extended periods. With a maximum
input current of about 220mA at up to
Parts List
1 PC board, code 14105101, 62
x 49mm
1 2-pin terminal block (5.08mm
pitch)
1 PC-mount horizontal Type A
USB socket (Jaycar PS0916,
Altronics P1300)
2 2-pin polarised headers
(2.54mm pitch)
2 2-pin polarised header connectors (2.54mm pitch)
1 100µH high-frequency 1.13A
bobbin inductor (Altronics
L6222)
1 small rubber grommet
1 M3 x 6mm machine screw
1 M3 star washer
1 M3 nut
1 8-pin machine tooled socket
(optional)
1 200kΩ horizontal single-turn
trimpot (VR1)
Semiconductors
1 LTC1174CN8 (IC1) (available
from Farnell)
1 IRF9540 Mosfet (Q1)
1 BC549 transistor (Q2)
1 BC559 transistor (Q3)
1 1.5KE36CA transient voltage
suppressor (TVS1)
1 12V 1W zener diode (ZD1)
1 15V 1W zener diode (ZD2)
3 1N5819 Schottky diodes
(D1-D3)
Capacitors
2 47µF 16V tantalum
2 22µF 16V tantalum
2 470nF MKT
1 100nF MKT
Resistors
1 10MΩ
1 300kΩ*
1 2.2MΩ
1 270kΩ
1 1MΩ
1 110kΩ
1 360kΩ*
1 1kΩ
1 330kΩ
* May be necessary to adjust
regulator output – see text
15.6V, Mosfet Q1’s dissipation will not
normally exceed 572mW.
Buck regulation
The LTC1174 has several modes
but works similarly to a normal “buck
converter” at high output currents.
A “buck converter” is the most
common type of step-down DC/DC
May 2010 69
SWITCH S1
There are losses in this process,
which is why switchmode regulator
efficiency is never 100%. However, it
is still a great deal better than linear
regulation. With a 13V input, a 5V
output and 500mA output current, the
input current is around 220mA. This
gives an efficiency of (5 x 0.5)/(13 x
0.22) = 87%. A linear regulator under
these conditions would have just 5/13
= 38.5% efficiency (assuming that the
input and output currents are equal).
If the instantaneous current through
the inductor exceeds the IC’s internal
current limit (nominally 600mA), the
internal transistor switches off and
the switch off-time is extended from
4µs to around 12µs. This gives the inductor time to discharge if the output
is shorted.
One reason for this current limit,
apart from stopping IC1’s internal
transistor from overheating, is that
inductors with non-air cores can “saturate”. Essentially, the core can only
hold a certain amount of magnetic flux
and its inductance rapidly drops when
that level is reached. When it drops far
enough, the inductor is essentially just
a wire and if the switch is still on, a lot
of current can flow through it.
Because the current through the
inductor is ramping up and down as
the transistor switches, the average
current is less than the peak current.
That is why, with a 600mA limit, we
can only draw up to 500mA. The current limit kicks in soon after that and
the output voltage drops until the current draw decreases below the limit.
This protects against short-circuits
INDUCTOR L1
+
+
iL
PATH 1
DIODE
D1
VIN
PATH 2
C1
VOUT
LOAD
Fig.3: basic scheme for a switchmode buck converter. Voltage regulation
is achieved by rapidly switching S1 and varying its duty cycle. Current
flows via path 1 when S1 is closed and path 2 when it is open.
converter. It requires a single switch
(normally a transistor), an inductor
and a capacitor. Fig.3 shows the basic
scheme and it works as follows.
When the switch is closed, current
flows through inductor L1 into the load
(Path 1). This current slowly builds up
from zero to a peak value. When this
peak current is reached, the switch
opens and current flows through diode
D1 to discharge the inductor’s energy
into the load (Path 2).
C1 is included to act as a reservoir,
to smooth out the voltage produced
across the load. This voltage is dependent on the load and duty cycle of
switch S1 (ie, the time that it is closed
compared to the time that it is open).
It’s also dependent on the peak current
through L1 and the input voltage.
This type of circuit can be very
efficient because voltage control is
achieved by rapidly switching the
input. The small amount of power dissipated is mainly due to voltage losses
in the switching device (in practice,
S1 is a switching transistor or Mosfet)
and in L1 and D1.
The USB Charger operates in similar
fashion but in this case the the switching is performed inside IC1 (LTC1174).
Many buck regulators operate at a
fixed frequency, using PWM to control
the switch duty cycle and thus the output voltage. By contrast, the LTC1174
has a “fixed off-time” configuration. It
varies the switch duty cycle by controlling the length of the “on-time”, ie,
how long the switch is kept on for each
pulse. This is a power saving feature
– it means that the frequency drops
at light loads and the less the internal
Mosfet has to switch, the less power
is consumed by the IC itself.
When the internal Mosfet switches
on, current flows from VIN (pin 6) to
SW (pin 5) and through inductor L1,
charging the output capacitors. During
this period, the magnetic field generated by the inductor increases.
Conversely, when the internal Mosfet switches off, the magnetic field collapses and this continues driving current into the output capacitors. Since
the internal transistor is off, the current
instead flows from ground through D2
and then through the inductor.
It is this charging and discharging
of the inductor’s magnetic field which
allows for efficient voltage conversion.
When the internal transistor is on,
the inductor nominally has 12V at its
switch end and 5V at the output end.
If the inductor was a resistor, then
more than half the power would be
wasted as heat.
Table 2: Capacitor Codes
Value µF Value IEC Code EIA Code
470nF 0.47µF 470n
474
100nF 0.1µF
100n
104
Table 1: Resistor Colour Codes
o
o
o
o
o
o
o
o
o
o
No.
1
1
1
1
1
1
1
1
1
70 Silicon Chip
Value
10MΩ
2.2MΩ
1MΩ
360kΩ
330kΩ
300kΩ
270kΩ
110kΩ
1kΩ
4-Band Code (1%)
brown black blue brown
red red green brown
brown black green brown
orange blue yellow brown
orange orange yellow brown
orange black yellow brown
red violet yellow brown
brown brown yellow brown
brown black red brown
5-Band Code (1%)
brown black black green brown
red red black yellow brown
brown black black yellow brown
orange blue black orange brown
orange orange black orange brown
orange black black orange brown
red violet black orange brown
brown brown black orange brown
brown black black brown brown
siliconchip.com.au
ZD1
15V
Q2
Q3
BC559
D2
D3
L1
100 µH
5819
5819
BC549
VR1
200k
1
3
2
4
100nF
+
+
47 µF
CON3
330k
IC1
LTC1174
5819
10M
1M
+
12V
TVS1
1.5KA
D1
1k
2.2M
110k
CON1
270k
+
10150141
CON2
470nF
CON4 +
Q1
IRF9540
–
B SU ra C
12V
IN
22 µF
22 µF
USB OUTPUT SOCKET
47 µF
470nF
ZD2
©
0102
Fig.4: follow this parts layout diagram and the accompanying photo to assemble the PC board. Make sure that all
polarised parts are correctly oriented and don’t get the transistors mixed up.
at the output as well as inductor
saturation.
Burst mode
At lower currents, the IC goes into
“burst mode”. What it does is deliver
several very fast pulses of current to
the inductor over a short period, bringing the output voltage slightly above
5V. It then switches off and waits for
the output voltage to drop below 5V
and then starts pulsing again.
As it is waiting for the voltage to
drop, the IC is in “sleep mode” and
consumes very little power. The result is that at light loads, ground pin
current is substantially lower than
it would otherwise be without this
burst mode.
While the delay between the bursts
makes the effective frequency of operation much lower than at full power,
the frequency of the bursts themselves
is actually quite high. We measured
frequencies as high as 1MHz.
This means that the noise generated
by the inductor is a sub-harmonic of
the switching frequency and is caused
by magnetostriction of the inductor’s
core.
If there is nothing attached to the
regulator’s output, the feedback volt-
age divider becomes the only load.
Because the output voltage decays
very slowly, the period during which
the IC sleeps in burst mode becomes
several hundred milliseconds. It is
this long sleep period which allows
the regulator to have a very low quiescent current with light loads or no
load (approximately 140µA).
Construction
Building this unit is easy. All the
parts mount on a small PC board
coded 14105101 (62 x 49mm) and this
snaps into the integral channels in a
standard UB5 plastic box. The USB
socket is accessed through a hole cut
in one side of the box, while a hole at
one end provides access to the input
screw-terminal block.
If you want something that’s a bit
more robust, a small IP67-rated box
can be used instead. In this case,
the board can be mounted on M3 x
12mm tapped stand-offs and secured
using M3 x 6mm machine screws and
washers.
Note that because this unit is likely
to be exposed to a lot of vibration, we
have not specified a socket for the IC.
You can use one if you prefer but make
sure it is a machine-tooled type, as the
IC is less likely to work its way loose.
Before starting the assembly, carefully check the PC board for defects.
Most of the underside is covered by a
ground plane. Make sure that there are
no unintentional connections between
this ground plane and any of the other
tracks, as could occur if the board is
under-etched.
If you are going to install the board
in a UB5 case, check that it fits correctly by snapping it into place. It may
be necessary to file the edges slightly
if it is too large. Even if it’s just 0.1mm
too wide, that can make the plastic
case bulge slightly when it is in place.
Once you are satisfied the board is
OK, install the resistors. Check each
resistor with a DMM before installing
it on the board, to ensure the values are
correct. That done, install the diodes,
starting with the two zeners (ZD1 &
ZD2), then the three 1N5819 diodes
(D1-D3). Don’t mix them up and be
careful with their orientation.
Next, bend the Mosfet’s leads down
by 90° exactly 5mm from its body and
mount it on the PC board. Check that
its tab mounting hole lines up with
the board, then fasten it to the board
using a 3mm machine screw from the
top and a star washer and M3 nut on
82
6
7
12
28.5
15
(SIDE OF UB5 BOX)
ALL DIMENSIONS IN MILLIMETRES
Fig.5: this diagram can be copied and used as a drilling template for the USB socket cut-out in the side of the case.
siliconchip.com.au
May 2010 71
Fig.6: this shows the output voltage (yellow) and switching (green) waveforms at 10mA. The long off-time relative
to the on-time can be seen. The device is operating in
discontinuous mode – the inductor current falls to zero,
causing the oscillations in the green trace.
the underside. Do the nut up firmly,
then solder and trim the leads.
Note: don’t solder the Mosfet’s leads
first. If you do, you could stress and
crack the the copper tracks on the PC
board as the mounting screw is tightened. Always install the mounting
screw before soldering.
Next, install the IC socket if you
have decided to use one. Follow this
with the transient voltage suppressor
(TVS1) – its orientation doesn’t matter – then install the two small-signal
transistors (Q2 & Q3). Note that Q2
& Q3 are different types, so don’t get
them mixed up. Q2 is a BC549 NPN
transistor, while Q3 is a BC559 PNP
type.
Fig.7: this scope shot shows the output voltage waveform
at 450mA. The device is switching continuously and
so the frequency is much higher. There is evidence of
occasional burst-mode operation, as can be seen near the
centre of the trace.
If their leads are too close to fit
through the holes, bend them outwards near the body of the transistor
using small pliers, then back down
again.
The PC-mount USB socket (CON2)
is next on the list. Be sure to press it
down firmly so that it sits flush against
the board, then solder its two metal
tabs to secure it in place. That done,
solder the four pins, taking care to
avoid bridging them.
Trimpot VR1 and the three MKT
capacitors can now go in, followed by
the four tantalum capacitors, inductor
L1 (this can go in either way around)
and the screw terminal block (CON1).
Push the terminal block down firmly
onto the board and make sure its entry
holes face outwards before soldering
its pins.
Be careful also with the orientation
of the tantalum capacitors. A “+” will
be printed on the case above the positive lead – just line it up with the “+”
sign on the board overlay.
Vibration proofing
If the unit is to be used in a vehicle,
it’s a good idea to apply some silicone
sealant around the base of each tantalum capacitor and TO-92 transistor.
The idea is to glue them to the PC
board so that they can’t vibrate and
break their leads.
Be sure to use neutral-cure silicone
Recharging Apple USB Devices
+5V
+5V
+5V
27k
22k
2.5V
D–
2.0V
22k
D+
Vcc
USB TYPE A
SOCKET
GND
16k
~3.3V
1
2
3
4
0V
18k
0V
Fig.8: the data pin biasing arrangement for iPOD NANO 2nd generation players.
Some USB devices require their D+ and
D- pins to be biased for charging to occur.
These devices include the iPOD NANO
1st generation and 2nd generation music
72 Silicon Chip
30k
D–
D+
Vcc
GND
USB TYPE A
SOCKET
2.8V
1
2
3
4
D–
2.0V
47k
10k
0V
33k
33k
D+
Vcc
USB TYPE A
SOCKET
GND
1
2
3
4
22k
0V
Fig.9: the biasing arrangement for
iPOD NANO 1st generation players
and 5th generation iPOD video.
Fig.10: the biasing arrangement for
the iPhone 3G and iPOD Touch 2nd
generation player.
players, the 5th Generation iPOD video,
the iPhone 3G and the iPOD Touch 2nd
generation player.
This biasing can be achieved using
resistors, as shown in the accompanying
diagrams. All resistors are 0.25W and
they can be installed by adding them to
the copper side of the PC board.
siliconchip.com.au
sealant (ie, the stuff without acetic
acid).
Set-up & testing
Before soldering in the IC, it’s a
good idea to adjust the pre-regulator
voltage. To do this, connect a power
supply which can provide somewhere
between 14-30V to the input terminal
block, with an ammeter
in series. It’s best to
start at the lower end
of that voltage range.
Turn on the supply and check the
current. It should
be less than 1mA. If
it is more than 1mA, then something
is wrong – turn it off and check for
assembly errors.
Now check the voltage between
pads 8 & 4 for IC1. It should be in the
range of 12-14V. Adjust trimpot VR1
until it reads 13V (or just under). If you
want to be extra cautious, you can set it
to 12.5V for a slight loss in efficiency.
Once the reading is correct, disconnect the power and install the IC to
the PC board. Make sure it goes in the
right way around!
Now power the board using a 9-16V
supply and check the output voltage.
The easiest way to do this is to check
the voltage across pin header CON3.
The output should be very close to
5.0V, or if you have changed the output
divider, your target voltage. It will be
moving up and down slightly due to
the burst mode regulation but should
not vary by more 0.2V. If it is not being
properly regulated to 5V, disconnect
the power and check for faults.
It’s possible that the output voltage could be below 4.85V, due to a
combination of the tolerance of the
voltage feedback divider resistors and
the tolerance of the LTC1174’s internal
reference voltage. If this is a case, replace the 330kΩ feedback resistor with
a 360kΩ resistor. This will increase the
output voltage by 6.8%, ensuring that
it never drops below the minimum
USB supply limit of 4.75V.
Conversely, if the output is above
5.2V, replace the 330kΩ feedback resistor with a 300kΩ resistor, to reduce the
output voltage by 6.8%. However, in
most cases, the output will be within
50mV of the programmed voltage with
the recommended 330kΩ resistor.
Installation
If you are going to install the board
siliconchip.com.au
The PC board snaps into the side channels
of a standard UB5 plastic case. A blob
of hot-melt glue can be used to stop the
grommet for the input leads from working
loose.
Fig.11: this shows
the output voltage
during standby
operation. Note
the low frequency
of operation due to
the long sleep time
and burst mode.
in a UB5 box, you will first need to
make a cut-out for the USB socket.
Fig.5 shows the cutting details and
this diagram can be copied and used
as a template. You will also have to
drill a hole in one end of the box to
accept a grommet for the input leads
or connector.
After that, the board should simply
snap into place. It’s best to introduce
the side with the USB socket first and
then gently push the board into place.
Alternatively, as previously stated,
you can mount the board in the case of
your choice and secure it on threaded
standoffs using M3 x 6mm machine
screws. A 500mA in-line fuse on the
input side is a good idea, although the
IC’s current limiting should normally
protect the power supply.
As a final check, once the supply
is wired up, it’s a good idea to use a
multimeter to measure the voltage at
the USB socket before attaching any
devices. There are four pins in the USB
socket – touch the multimeter probes
to the two outer pins, being careful to
avoid shorting them to adjacent pins or
the surround. If the multimeter reads
close to 5.0V (or your target voltage),
then it’s working properly.
That’s it! If you are using the USB
Charger to power USB devices in a
vehicle, don’t forget to unplug them
when they are not in use, or you could
still flatten the battery.
Alternatively, if you power the device via the cigarette lighter socket,
it will be automatically switched off
when the ignition is switched off. SC
May 2010 73
In the March and
April 2010 issues, we
described the design
and construction of
our new Digital Audio
Signal Generator.
The final article this
month has the driving
instructions.
By NICHOLAS VINEN
A High-Quality Digital Audio
Signal Generator; Pt.3
D
RIVING THE Digital Audio Signal
Generator is straightforward. In
operation, it delivers an output signal (analog and/or digital, depending
on the configuration) as soon as it is
switched on and the LCD initially
shows the current signal generation
mode. There are five such read-outs,
one for each mode: locked, independent, mixed, pulsed and sweep.
In each case, the Up and Down
buttons change the current mode
and the display adjusts to show the
corresponding reading. Pressing the
Select button (in the centre of the main
cluster) switches the LCD from the
signal generation mode read-out to the
setting read-outs. When this is done,
signal generation continues according
74 Silicon Chip
to the last mode selected.
Changing the setting read-out (done
using the Up and Down buttons) has no
affect on the current signal generation
mode. There are seven different setting
read-outs. Pressing the Select button
again returns the unit to the signal
generation mode read-out.
In other words, the Select button
toggles between the current signal
generation mode read-out and the
setting read-out. The active generation
mode is always the mode which was
last selected.
Left & right buttons
On most read-outs, the left and right
buttons allow you to move a cursor
across the display. The only excep-
tion is the Status read-out where these
two buttons have other effects (more
on this later). In practice, the cursor
can only move to locations which
show values that can be adjusted or
activated.
When the cursor is visible, pressing the Up and Down buttons will
modify the indicated setting rather
than changing the current read-out.
Pressing the Select button or moving the cursor past the first or last
setting hides the cursor and the Up
and Down buttons can once again be
used to change the current mode and/
or read-out.
This system may sound complicated
but once you try it, it will quickly
start to make sense. In other words, it
siliconchip.com.au
sounds more complicated that it really
is and the process is quite intuitive
once you understand the basics.
Table 1: Signal Generation Mode Readouts
Locked Mode Readout: top line = signal frequency
(both channels) and left channel amplitude; bottom
line = channel phase difference and right channel
amplitude.
The mute buttons
There are two additional buttons on
the unit – Left Mute and Right Mute.
Pressing them toggles the mute status
of the corresponding channel at any
time. For example, if you press the
Left Mute button and the left channel
is currently enabled, it will be disabled
and vice versa.
The mute status is shown on the
status read-out and also on each mode
read-out. For sweep mode, if a channel
is muted, an “l” (indicating the left
channel) and/or an “r” (indicating the
right channel) is shown at the top of
the display. For the other four modes,
a muted channel is shown by changing
the minus sign in front of each amplitude setting to an underscore.
If you press the two Mute buttons
simultaneously, the left and right
channel settings will be swapped.
This includes frequency, amplitude
and phase (when applicable), as well
as the mute status.
Table 1 shows what each generation
mode read-out looks like by default
and highlights all the settings that can
be changed. There is also a description
of the function for each setting.
More mode information
As stated in the original article, the
output frequency can be set at up to
half the sample rate (ie, 48kHz) in steps
of 1Hz. Depending on which frequency
digit you select with the cursor, pressing the Up and Down buttons will add
or subtract 1Hz, 10Hz, 100Hz, 1000Hz
or 10,000Hz.
The amplitude is set in similar
fashion and the range is from 0dB to
-98dB in 1dB steps.
If you increase the attenuation past
-98dB, the read-out changes to “off”
and the signal is muted.
Note that as you get close to -98dB,
the actual signal amplitudes become
so small that the error increases and
some values have an identical result.
In fact -96dB, -97dB and -98dB generate the same amplitude due to the
16-bit precision of the scaling factor.
However, for attenuation down to
-60dB, the scaling is basically perfect.
Beyond that, the measured values are
as shown in Table 2.
Note that these measurements also
include scaling errors from the DAC
siliconchip.com.au
Independent Mode Readout: top line = left channel
frequency and amplitude; bottom line = right
channel frequency and amplitude.
Mixed Mode Readout: top line = frequency and
amplitude of wave 1; bottom line = frequency and
amplitude of wave 2.
Pulsed Mode Readout: top line = frequency (both
channels) and pulse-on amplitude; bottom line =
pulse-on time (0-9999ms), pulse-off time (0-999ms)
and pulse-off amplitude.
Sweep Mode Readout: top line = start frequency
and amplitude (both channels); bottom line = finish
frequency (both channels), sweep time (0.1 - 99.9s)
and off-time (0-98s & manual).
Note: values inside green boxes can be selected and varied using the front panel pushbuttons.
itself, so they are only a guide as to the
unit’s actual precision.
Keep in mind that when adjusting
the attenuation, pressing the Up button increases the attenuation and thus
decreases the signal amplitude.
The only other mode settings (aside
from frequencies and amplitudes) are
time periods. In the case of pulsed
mode, they are specified in milliseconds and have a range of 0-9999 (just
under 10 seconds) or 0-999 (just under
one second). In sweep mode, they are
specified in tenths of a second and
seconds, with a range of 0-99.9 seconds
and 0-99 seconds respectively.
If you switch away from a mode and
then back again later, the previous settings are typically retained. However,
some are shared between the modes.
For example independent and mixed
mode share all their settings, differing
only in how they output the signal
(independently to each channel or
mixed on both). As a result, changing
a setting in one changes both.
The left/right channel amplitudes
are shared between all modes except
pulse and sweep. Most other settings
are independent.
Configuration details
Table 3 shows each setting read-out
and describes each field. Some require
more explanation, as follows:
Status readout: the Status readout is
very useful in sweep mode. Not only
Table 2: Attenuation Accuracy
Setting
Measured Value
-60dB
-59.92dB
-70dB
-69.80dB
-80dB
-79.16dB
-90dB
-89.35dB
does it show the frequency as the
sweep occurs (it’s updated four times a
second) but you can pause and restart
the sweep. Pressing the Left button in
this readout mode pauses or resumes
the sweep, while pressing the Right
button starts/restarts it.
This is especially useful when you
are optimising crossover networks or
matching a subwoofer to other drivers. If you hear a peak in the output
amplitude, you can pause the sweep
and read off the frequency.
There may be times when you want
a manual sweep, ie, rather than having it loop repeatedly, you can trigger
it manually. To do this, set the sweep
off time to maximum via the sweep
mode read-out – it will show “man”
(manual).
It will then only start when you
trigger it manually from the status
read-out using the Right button.
Sweep setting readout: this simply
allows you to choose between Exponential or Linear sweep. Exponential
sweep is the default and is usually
May 2010 75
Table 3: Setting Readouts
Output/wave type setting read-out: top line = output
type (44100Hz, 48000Hz [default], 96000Hz, Analog);
bottom line = signal type (Sine, Square, Triangle,
SawtoothUp, SawtoothDn).
Status read-out: indicates the current generation
mode and mute status. In pulsed and sweep mode,
it shows the current frequency and amplitude. “LR”
becomes “lr” when both channels are muted.
Sweep setting read-out: first line = setting; second
line = sweep type (Exponential [default] or Linear).
S/PDIF setting read-out: line 1 = encoding type
(Consumer [default] or AES/EBU) plus pre-emphasis
setting (Normal [default] or PreEmph); line 2 =
battery voltage display.
Battery setting read-out: Line 1 = 3.3V regulator
output voltage calibration; line 2 = low battery
warning voltage setting.
LCD setting read-out: line 1 = LCD backlight brightness (0-100%); line 2 = LCD contrast (0-100%).
EEPROM setting read-out: line 1 = Select EEPROM
bank (0-9); line 2 = Load all settings from specified
bank and Save all settings to specified bank.
Note: values inside green boxes can be selected and varied using the front panel pushbuttons.
what you want. In this mode, the frequency doubles or halves at a fixed
rate.
Linear sweep simply increases the
frequency by a set amount over time.
As a result it spends less time at low
frequencies and more time at higher
frequencies. This mode could be
useful if you are using a computer to
capture and analyse the output, as it
may make analysis simpler.
Keep in mind that while the generator attempts to reach your programmed
finish frequency after the specified
time has elapsed, in practice this is
very difficult to achieve. As a result,
with long sweep times, it may be off
by a few milliseconds and occasionally
the final frequency may actually be a
few Hz below that specified.
S/PDIF setting read-out: this lets you
configure the S/PDIF output format
as well as view the current battery
voltage.
The first setting, “Consumer” or
“AES/EBU”, determines the format
of the Channel Status data sent with
the S/PDIF stream. “Consumer” is
the typical format that most CD and
76 Silicon Chip
DVD players use. On some equipment, this format is limited to 20 bits
of precision in the audio data, so you
may get slightly higher distortion and
worse amplitude control on this setting. However, it is the most widely
supported.
“AES/EBU” is the professional
standard used by DATs, mixers and
high-end sound cards. It allows the full
24-bit precision in the audio samples
as well as sending more complete
meta-data. In general, AES/EBU mode
is better provided the equipment that’s
receiving the signal can handle it.
The second setting allows you to
enable the pre-emphasis bit in the
S/PDIF stream. This has the effect of
enabling the de-emphasis hardware in
the receiver (if it has any) and is mainly
useful for testing. For example, you
can run a 20Hz-20kHz sweep with and
without this bit set and check that the
higher frequencies are properly attenuated (ie, de-emphasised) when it is set.
The battery voltage readout lets you
keep track of the charge state. Note,
however, that the reading is actually
a little lower than the real battery
voltage (by about 0.3V) due to the
Schottky diode (D2) in series with it.
This means that if you consider your
cells flat when the battery reaches 4.0V
(for example), you’ll actually want
to switch the device off or attach the
plugpack as soon as it reads near 4.3V.
Battery setting readout: this lets you calibrate the battery voltage monitor – see
the “Calibration” section in Pt.2 in the
April 2010 issue. It also lets you set the
low-battery warning voltage threshold.
Once the battery has dropped below
this level, the backlight will dim and
flash, warning you to charge the battery
or switch it off.
During this time, you can continue
using the generator. The recommended
settings are 3.9V for alkaline cells (actually 3.6V) and 4.3V for NiMH cells
(actually 4.0V).
Regardless of this setting, if the
voltage reading drops below 3.5V for
some time, the microcontroller will go
into sleep mode. The “Battery flat!”
message is then displayed and all
other functions cease. Backlight flashing continues although at a reduced
brightness.
When that happens, the current
drain drops from 100mA or more to
about 30mA. This will still drain the
battery but not as quickly.
LCD setting readout: here you can adjust
the display contrast and backlight
brightness. You may need to change
them according to lighting conditions,
viewing angle or temperature. If you
manage to reduce the contrast so much
that the display becomes unreadable,
switching the power off and on will
typically restore it to the default.
The backlight brightness selection is a compromise because as you
increase it, you increase the current
drain at the expense of battery life.
The default value of 25% is sufficient
for good display visibility under most
conditions and only adds about 30mA
to the battery current.
EEPROM setting readout: this lets you
define the default settings (ie, those
loaded at power on), as well as store
up to nine other setting configurations.
Bank 0 is loaded at switch-on, so if
you save to bank 0 you are setting the
defaults.
To save settings, select the appropriate bank number, then move the cursor
to “Save” and press the Up or Down
button. The read-out will change to
“Saved” and the current configuration
and mode settings will be stored in that
siliconchip.com.au
slot. You can then switch the generator
off, or continue using it. You can even
change the bank number and save to
another one if you wish.
To load settings, the procedure is essentially the same. You select the bank
number you want, move the cursor to
“Load”, and press the Up or Down button. The read-out changes to “Loaded”
and the current settings are replaced
with those stored in EEPROM. Almost
everything will be set just as it was
when you saved to that bank.
Note that attempting to load a bank
that has nothing saved in it has no
effect.
The additional banks can be handy
if you often repeat certain tests and
they involve a specific configuration.
You can store commonly used configurations in banks 1-9 and save yourself
the time of having to adjust multiple
settings to the same values again later.
Table 4: Example Wave Types
Internal DAC
Sine
External DAC
Sine
Wave types
Table 4 gives an example of each
wave type. Each has been sampled
using both the analog outputs of the
Digital Audio Signal Generator and
also the SILICON CHIP High-Quality
Stereo DAC (September-November
2009), the latter fed from the generator’s S/PDIF output.
The high-frequency oscillations apparent in both the square and sawtooth
signal outputs from both DACs are a
result of their delta-sigma architecture.
These types of waveforms are unnatural due to their discontinuous nature –
ie, they contain vertical lines whereas
natural waveforms normally do not.
As a result, the digital sinewave
signal interpolation is smoothing
the abrupt transitions, with the filter
inserting some high-frequency waves
before and after each transition to
cover up the discontinuity. The result
is what you see here. We know that the
digital circuitry must be responsible
for the oscillations because they occur equally both before and after each
transition.
On the other hand, the external DAC
has some overshoot with the square
and sawtooth waves, which is presumably due to the analog filter circuitry
after the DAC chip itself. It only occurs
post-transition.
The sinewave signal does not suffer
from this issue because it is continuous. The triangle signal does have a
discontinuous first derivative (at the
point of each triangle) but since it has a
siliconchip.com.au
Square
Square
Triangle
Triangle
Sawtooth Up
Sawtooth Up
Sawtooth Down
Sawtooth Down
May 2010 77
Fig.1: the effects of aliasing start to become noticeable at
44kHz. Note the subtle variations in the signal amplitude.
Fig.2: at 47kHz, aliasing effects are quite severe (the input
data in this case actually has constant amplitude).
Fig.3: this scope grab shows the analog output distortion
residuals (0.06%) for a 1kHz sinewave & 0dB attenuation.
Fig.4: the distortion residuals drop to just 0.0006% (1kHz,
0dB attenuation) when using the High-Quality Stereo DAC.
continuous waveform it is not badly affected. There is a little rounding at the
tips, again likely due to the digital sine
signal interpolation, but it is minimal.
Aliasing
There is an additional issue related
to the digital filtering and that is aliasing. In fact, all DACs suffer from it to
some extent.
When the sample rate is set to
96kHz, the highest frequency signal
you can generate is 48kHz. There is a
wrinkle, though – as you get very close
to 48kHz, there are so few samples
per signal that the signal form can no
longer be properly represented.
Basically, the digital data becomes
ambiguous – while the frequency information can still be extracted, the
amplitude of each wave is no longer
clear. Aliasing starts to be become no78 Silicon Chip
ticeable above 44kHz (note the subtle
variations in amplitude shown in the
scope shot of Fig.1) and it is quite
severe at 47kHz (Fig.2).
The input data for the second capture actually has a constant amplitude.
However, aliasing does not increase
monotonically with frequency. There
is no aliasing at exactly 48kHz, for
example.
What this means is that you should
generally avoid frequencies between
45% and 50% of the sample rate,
except for exactly half (ie, 48kHz in
this case). That way, aliasing will not
typically be an issue.
By the way, if you want to make
sound effects for a science fiction film,
try setting the signal type to triangle
and the sample rate to 48kHz, then
initiate a sweep from 12-24kHz. What
you then hear is due to the aliasing
causing frequency shifts in the output.
Distortion
There’s another issue to keep in
mind when selecting the sample rate.
When the output frequency is below
about 10kHz, the sinewave signal
distortion is actually lower at 48kHz
sampling than at 96kHz sampling. So
if you’re only going to generate low-tomid frequency sinewaves and need the
least distortion, stick with the 48kHz
sampling rate. You can still switch
to 96kHz when necessary for higher
frequency output signals.
Finally, if you have an oscilloscope,
it’s a good idea to connect the generator’s outputs to it and try out the
various modes. By doing this, you will
quickly get used to the interface and
get a feel for how the various modes
SC
work.
siliconchip.com.au
Tektronix DMM4050
6½ Digit
Precision Multimeter
This bench-top multimeter features 6½ digit readings, a graphic LCD
and a number of advanced features such as trend plot, histogram
and dual measurement mode. With front and rear panel inputs,
its short term and 1-year accuracy figures are outstanding.
Review by Nicholas Vinen
siliconchip.com.au
May 2010 79
T
he Tektronix DMM4050 has all the usual features
you would expect in a high accuracy bench-top
multimeter.
The main modes are DC voltage and current, AC voltage
and current (with true RMS), resistance (2- and 4-wire),
continuity, diode testing, capacitance and temperature.
Temperature measurement is via RTD (resistance temperature detector) only and can be use 2-wire or 4-wire sensing.
The unit measures 225mm wide, 330mm deep and sits
150mm above the bench surface when using the integrated
carrying handle as a tilting bail (which provides two different angles). It comes with a pair of high quality needle
probes, a power cable, an RS-232-to-USB cable and two
CDs with documentation and software.
A calibration certificate is provided along with a booklet
that contains installation and safety instructions, as well
as listing the accuracy figures.
The basic DC voltage precision is 0.0024% over one year;
other modes feature similarly excellent figures. Maximum
DC voltage resolution is down to 100nV and DC current
to 100pA.
Also on the rear panel are the external trigger terminal
block, the Ethernet, RS-232 serial and GPIB (General Purpose Interface Bus) ports, the IEC power connector and
the power switch.
All functions (including power on/off) are easy to access
via the front panel buttons. The interface response is instant
– the only time there is a noticeable delay is the first time
the unit is turned on after being connected to mains power.
In any mode, extended functions are generally provided
via the five “soft buttons” which are labelled at the bottom
of the LCD. This allows them to change function to suit
the mode. Less commonly accessed functions are available
via the “Analyze”, “Measurement Setup” and “Instrument
Setup” buttons.
Features
One of the more outstanding features of this unit is the
display. It is a wide-format cyan-on-black graphic LCD
which is easily visible from any angle. There are three
brightness settings available.
Having a graphic (dot matrix) display means that the
format can change depending on the mode. For example,
a larger font is used when taking a single measurement
compared to dual measurement mode, making the display
easier to read. The display also permits graphical features
such as the trend plot and histogram.
In addition to the six banana sockets on the front, there
are five on the back; the low current sense terminal is duplicated but the 10A terminal is not. Two buttons on the
front panel switch between the two sets. This could be
used for several purposes, eg, to switch between different
sets of probes or for connection to an external test interface
with less clutter.
Virtually all modes provide optional digital and analog
filters to remove noise and high frequency variations from
the readings. AC measurements can also be displayed in dB
or dBm and have more filtering options. The diode tester
has a few selectable voltage and current levels.
Most modes give a choice of 4, 5 or 6-digit readout and you
can configure how many power line cycles (PLC) the readings are sampled over, for a speed/accuracy trade-off. The
longer the sampling time, the less noise affects the reading.
The DMM4050’s dual measurement mode is handy
but more limited compared to some other bench meters.
In DC volts mode you can also measure AC volts. In AC
volts or amps mode you can measure the DC component
or frequency simultaneously. In DC amps mode you can
measure AC amps, DC volts or volt-amps. In frequency
mode, period can also be displayed. In temperature mode,
the sensor resistance can be displayed.
In DC volts mode, the default input impedance is 10MΩ
but it can be set to 10GΩ for the 10V range and below. This
could be critical for getting accurate readings on a voltage
with a high source impedance.
There is another very useful DC voltage measurement
feature: the sense terminals can provide a reference voltage and display the reading as a ratio to it. That could be
Fig.1: this PC screen shot of the provided software (“NI
LabVIEW SignalExpress Tektronix Edition” Light Edition
for Windows”) shows the real-time reading taken from the
DMM4050 along with the control panel which allows you
to configure it from the PC. A USB-to-RS232 serial cable is
also included.
Fig.2: the software can log measurements over time and
display them in an auto-scaled graph which is updated as
measurements are taken.
Display, inputs & controls
80 Silicon Chip
siliconchip.com.au
control the meter and record the readings (see Fig.1 & 2).
Serial interface protocol documentation is also provided.
This allows custom software to be written which has full
control over the meter. For example, such software could
allow for automated testing in a production environment.
While the built-in trend plot and histogram features of
the meter are impressive, off-loading the data to a personal
computer for analysis or plotting provides a great deal more
power and flexibility.
The busy rear panel of the DMM4050. Along with the
second set of inputs, there are the external trigger terminal
block, the Ethernet, RS-232 serial and GPIB ports, the IEC
power connector and the power switch.
handy for measuring voltage dividers etc.
The capacitance measurement range is from 1pF to
100,000F – allowing measurement of virtually any capacitor you might come across.
The meter has quite a few mathematical and analysis
features. Mathematical options include limit testing, offset
nulling, arbitrary offsetting, ratio measurements and mX+B
measurements. An interesting feature is “stats” mode which
shows reading minimum, maximum, average and standard
deviation over a configurable number of samples.
The DMM4050 can be triggered from an external source
and can also send a pulse after each measurement is completed, via the 3-way terminal block mounted on the rear
panel. The trigger delay and number of samples collected
when triggered are adjustable via the front panel interface.
Storage and logging
The DMM4050 has a 10,000 reading internal memory
and can also store multiple configurations internally, to
save time repeating particular test set-ups.
If a USB flash drive is plugged into the front panel, it
is possible to store another 999 files with the same 10,000
reading limit for each. This provides a handy way to get data
to a computer for analysis regardless of where the meter is
installed. Readings can also be saved to a USB flash drive
from the internal memory.
The unit can be controlled and measurements taken from
a computer via an RS232 serial interface, GPIB or over
Ethernet. The supplied RS232-to-USB adaptor cable makes
connection easy with virtually any modern computer.
“NI LabVIEW SignalExpress Tektronix Edition” (Light
Edition) Windows software is included. With it you can
Clever accessories
The DMM4050 has a very clever optional accessory – the
TL705 4-wire test lead. It has just two banana plugs and
two leads – in fact it is only superficially different from a
regular set of probes in that both plugs are moulded from
the same piece of plastic.
The trick is that the multimeter’s input sockets have split
contacts that allow all four wires to be connected with just
two plugs. The TL705 leads contain a pair co-axial wires
connected to copper-tipped Kelvin probes.
So despite being able to use them like regular probes,
measurements down to a few milliohms are possible in
the 4-wire mode.
The copper tips avoid any dissimilar metal junctions in
the probes. Such junctions can act like thermocouples and
bias voltage readings.
Conclusion
While the DMM4050 has a decent set of features, its focus is on precision. We can’t list all of the accuracy figures
here but the data sheet, available from www.tek.com, has
that information. In this sense, you get what you pay for –
the measurement errors of this unit are much lower than
cheaper 6½ digit multimeters.
Many DMM4050 purchasers will also want to spend the
extra for the TL705 4-wire test lead since it makes accurate
resistance measurement so much easier and accuracy is
this unit’s forte.
Availability
The DMM4050 with a standard three-year warranty is
available from TekMark for AU$1885 plus GST and delivery. The DMM4040 (without capacitance or temperature
mode) is AU$1531 plus GST. The 5.5 digit DMM4020
is AU$1044.00 plus GST. To contact TekMark, e-mail
enquiries<at>tekmarkgroup.com or call (02) 9911 3888.
Further details are at www.tekmarkgroup.com/au SC
Issues Getting Dog-Eared?
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To order, simply call (02) 9939 3295 with your credit card handy . . . or fill in the handy order
form in this issue and fax it to (02) 9939 2648, or mail it to PO Box 139, Collaroy NSW 2097.
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Written in Australia, for Australian conditions by one of Australia's foremost
satellite TV experts. If there is anything you wanted to know about setting
up a satellite TV system, (including what you can't do!) it's sure to be covered in this
176-page paperback book.
Substantially updates coverage for low-speed and high-speed applications,
and provides step-by-step walk-throughs for design and selection of op
amps. Huge 648 pages!
PROGRAMMING 32-bit MICROCONTROLLERS
IN C By Luci di Jasio (2008) $79.00
NEWNES GUIDE TO TV & VIDEO TECHNOLOGY
By KF Ibrahim 4th Edition (Published 2007) $49.00
Subtitled Exploring the PIC32, a Microchip insider tells all on this powerful
PIC! Focuses on examples and exercises that show how to solve common,
real-world design problems quickly. Includes handy checklists. FREE CD-ROM includes
source code in C, the Microchip C30 compiler, and MPLAB SIM. 400 pages paperback.
It's back! Provides a full and comprehensive coverage of video and television technology including HDTV and DVD. Starts with fundamentals so is
ideal for students but covers in-depth technologies such as Blu-ray, DLP,
Digital TV, etc so is also perfect for engineers. 600+ pages in paperback.
USING UBUNTU LINUX
RF CIRCUIT DESIGN
by J Rolfe & A Edney – published 2007 $27.00
by Chris Bowick, Second Edition, 2008. $63.00
Ubuntu Linux is a free and easy-to-use operating system, a viable alternative to Windows and Mac OS. Introduces Ubuntu, tells how to set it up,
covers the various Open Office applications and gives troubleshooting
hints and tips. Highly recommended. 222 pages in paperback
DVD PLAYERS AND DRIVES
by K.F. Ibrahim. Published 2003. $71.00
A guide to DVD technology and applications, with particular focus on design issues and pitfalls, maintenance and repair. Ideal
for engineers, technicians, students of consumer electronics
and sales and installation staff. 319 pages in paperback.
The classic RF circuit design book. RF circuit design is now more important
that ever in the wireless world. In most of the wireless devices that we use
there is an RF component – this book tells how to design and integrate in a very practical fashion. 244 pages in paperback.
PRACTICAL RF HANDBOOK
See
Review
Feb
2004
by Ian Hickman. 4th edition 2006 $61.00
A guide to RF design for engineers, technicians, students and enthusiasts.
Covers key topics in RF: analog design principles, transmission lines,
couplers, transformers, amplifiers, oscillators, modulation, transmitters
and receivers, propagation and antennas. 279 pages in paperback.
ELECTRIC MOTORS AND DRIVES
PRACTICAL VARIABLE SPEED DRIVES &
POWER ELECTRONICS
Se
By Austin Hughes - Third edition 2006 $51.00
Intended for non-specialist users of electric motors and drives,
filling the gap between academic texts and general "handbooks".
Explores all of the widely-used modern types of motor and drive
including conventional & brushless DC, induction motors, steppers, servos, synchronous and reluctance. 384 pages, soft cover.
e
Review
Feb
An essential reference for engineers and anyone who wishes
2003
to design or use variable speed drives for induction motors.
by Malcolm Barnes. 1st Ed, Feb 2003. $73.00
286 pages in soft cover.
BUILD YOUR OWN ELECTRIC MOTORCYCLE
AC MACHINES
by Carl Vogel. Published 2009. $40.00
By Jim Lowe Published 2006 $66.00
Applicable to Australian trades-level courses including NE10 AC Machines,
NE12 Synchronous Machines and the AC part of NE30 Electric Motor Control
and Protection. Covering polyphase induction motors, single-phase motors,
synchronous machines and polyphase motor starting. 160 pages in paperback.
Alternative fuel expert Carl Vogel gives you a hands-on guide with
the latest technical information and easy-to-follow instructions
for building a two-wheeled electric vehicle – from a streamlined
scooter to a full-sized motorcycle. 384 pages in soft cover.
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PROGRAMMING and CUSTOMIZING THE
PICAXE By David Lincoln (2nd Ed, 2011) $65.00
by Douglas Self 2nd Edition 2006 $69.00
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A collection of 35 classic magazine articles offering a dependable methodology for designing audio power amplifiers to improve performance at every
point without significantly increasing cost. Includes compressors/limiters,
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A great aid when wrestling with applications for the PICAXE
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2011
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along with anyone who works with PICAXEs. 300 pages in paperback
SMALL SIGNAL AUDIO DESIGN
PIC IN PRACTICE
By Douglas Self – First Edition 2010 $88.00
by D W Smith. 2nd Edition - published 2006 $60.00
The latest from the Guru of audio. Explains audio concepts in easy-to-understand language with plenty of examples and reasoning. Inspiration for audio
designers, superb background for audio enthusiasts and especially where it comes to
component peculiarities and limitations. Expensive? Yes. Value for money? YES! Highly
recommended. 558 pages in paperback.
Based on popular short courses on the PIC, for professionals, students and
teachers. Can be used at a variety of levels. An ideal introduction to the world
of microcontrollers. 255 pages in paperback.
PIC MICROCONTROLLER – your personal introduc-
AUDIO POWER AMPLIFIER DESIGN HANDBOOK
tory course By John Morton 3rd edition 2005. $60.00
by Douglas Self – 5th Edition 2009 $81.00
A unique and practical guide to getting up and running with the PIC. It assumes no knowledge of microcontrollers – ideal introduction for students,
teachers, technicians and electronics enthusiasts. Revised 3rd edition
focuses entirely on re-programmable flash PICs such as 16F54, 16F84 12F508 and
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"The Bible" on audio power amplifiers. Many revisions and
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OP AMPS FOR EVERYONE
PRACTICAL GUIDE TO SATELLITE TV
By Carter & Mancini – 3RD EDITION $100.00
Substantially updates coverage for low-speed and high-speed applications,
and provides step-by-step walk-throughs for design and selection of op
amps. Huge 648 pages!
By Garry Cratt – Latest (7th) Edition 2008 $49.00
Written in Australia, for Australian conditions by one of Australia's foremost
satellite TV experts. If there is anything you wanted to know about setting
up a satellite TV system, (including what you can't do!) it's sure to be covered in this
176-page paperback book.
PROGRAMMING 32-bit MICROCONTROLLERS
IN C By Luci di Jasio (2008) $79.00
NEWNES GUIDE TO TV & VIDEO TECHNOLOGY
Subtitled Exploring the PIC32, a Microchip insider tells all on this powerful
PIC! Focuses on examples and exercises that show how to solve common,
real-world design problems quickly. Includes handy checklists. FREE CD-ROM includes
source code in C, the Microchip C30 compiler, and MPLAB SIM. 400 pages paperback.
By KF Ibrahim 4th Edition (Published 2007) $49.00
It's back! Provides a full and comprehensive coverage of video and television technology including HDTV and DVD. Starts with fundamentals so is
ideal for students but covers in-depth technologies such as Blu-ray, DLP,
Digital TV, etc so is also perfect for engineers. 600+ pages in paperback.
USING UBUNTU LINUX
by J Rolfe & A Edney – published 2007 $27.00
RF CIRCUIT DESIGN
Ubuntu Linux is a free and easy-to-use operating system, a viable alternative to Windows and Mac OS. Introduces Ubuntu, tells how to set it up,
covers the various Open Office applications and gives troubleshooting
hints and tips. Highly recommended. 222 pages in paperback
DVD PLAYERS AND DRIVES
by K.F. Ibrahim. Published 2003. $71.00
A guide to DVD technology and applications, with particular focus on design issues and pitfalls, maintenance and repair. Ideal
for engineers, technicians, students of consumer electronics
and sales and installation staff. 319 pages in paperback.
by Chris Bowick, Second Edition, 2008. $63.00
The classic RF circuit design book. RF circuit design is now more important
that ever in the wireless world. In most of the wireless devices that we use
there is an RF component – this book tells how to design and integrate in a very practical fashion. 244 pages in paperback.
See
Review
Feb
2004
PRACTICAL RF HANDBOOK
by Ian Hickman. 4th edition 2006 $61.00
A guide to RF design for engineers, technicians, students and enthusiasts.
Covers key topics in RF: analog design principles, transmission lines,
couplers, transformers, amplifiers, oscillators, modulation, transmitters
and receivers, propagation and antennas. 279 pages in paperback.
ELECTRIC MOTORS AND DRIVES
By Austin Hughes - Third edition 2006 $51.00
PRACTICAL VARIABLE SPEED DRIVES &
POWER ELECTRONICS
Se
Intended for non-specialist users of electric motors and drives,
filling the gap between academic texts and general "handbooks".
Explores all of the widely-used modern types of motor and drive
including conventional & brushless DC, induction motors, steppers, servos, synchronous and reluctance. 384 pages, soft cover.
e
Review
Feb
An essential reference for engineers and anyone who wishes
2003
to design or use variable speed drives for induction motors.
by Malcolm Barnes. 1st Ed, Feb 2003. $73.00
286 pages in soft cover.
AC MACHINES
BUILD YOUR OWN ELECTRIC MOTORCYCLE
By Jim Lowe Published 2006 $66.00
Applicable to Australian trades-level courses including NE10 AC Machines,
NE12 Synchronous Machines and the AC part of NE30 Electric Motor
Control and Protection. Covering polyphase induction motors, singlephase motors, synchronous machines and polyphase motor starting. 160
pages in paperback.
by Carl Vogel. Published 2009. $40.00
Alternative fuel expert Carl Vogel gives you a hands-on guide with
the latest technical information and easy-to-follow instructions
for building a two-wheeled electric vehicle – from a streamlined
scooter to a full-sized motorcycle. 384 pages in soft cover.
NOTE: ALL PRICES ARE PLUS P&P – AUSTRALIA ONLY: $10.00 per order;
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Vintage Radio
By RODNEY CHAMPNESS, VK3UG
Automatic gain control (AGC) –
what it is & why it’s necessary; Pt.1
Manufactured around 1948, the Astor GR/GRP receiver was a simple
3-valve TRF receiver. It had no AGC and featured a simple volume
control which varied the back-bias on its 6G86 variable-mu RF valve.
W
HEN RADIO (or “wireless”)
first made its appearance, it was
necessary for receivers to use every
bit of RF (radio frequency) and audio
frequency gain available. However,
as receivers became more sensitive
and gains improved, this situation
quickly changed. Receivers became
much more capable of pulling in weak
signals but there was one drawback. If
a receiver was tuned to a weak signal,
the gain then had to be manually reduced when tuning to a strong station
in order to produce the same audio
output level or volume.
On a set with a loudspeaker, there
would be a burst of quite loud and
probably distorted audio until the
volume control was hastily wound
84 Silicon Chip
back. That was bad enough but if the
listener was using headphones, their
ears would be ringing for quite some
time afterwards.
Once caught, most listeners would
turn the volume control down while
they tuned across the band. This meant
that strong stations were easily heard
but it had the disadvantage that weak
stations might be inaudible. So it
was a compromise as to just how far
the volume control was wound back
while tuning.
DXing
In the early days of radio, many listeners became interested in the hobby
of “DXing” which involved receiving
and identifying distant stations. Of
The development
of AGC (automatic
gain control)
circuits in the late
1920s and early
1930s was an
important milestone
in domestic radio
receiver design. It
allowed stations to
be received at the
same volume when
tuning across the
band, regardless of
signal strength.
course, these stations were much
weaker than any local stations and it
was all too easy to get a sudden loud
burst of sound from the loudspeaker
as one of the local stations was tuned.
Coupled with the inevitable static
crashes, this ran the distinct risk of
not only damaging the loudspeaker but
also frightening hell out of the listener
(and any innocent bystanders). Permanent damage to the listener’s hearing
was also possible if headphones were
being used.
To minimise this problem, it was
therefore necessary to keep one hand
on the volume control as the set was
tuned. That made tuning receivers
with no AGC (automatic gain control)
a rather tedious and awkward job.
siliconchip.com.au
In the simpler receivers, the regeneration control acted as the volume
control but more complex receivers
did have a separate audio-stage volume control. In fact, many of the more
complex receivers were likely to have
both audio and RF stage gain controls.
Another problem with early receivers was the variations in audio level
due to signal fading. At night, the
signal strength from a distant station
often varied continuously, from almost
non-existent at times to quite high at
other times. This signal “fading” was
inevitable and forced the listener to
continuously vary the volume control
to keep the audio at an almost constant
level.
Distant stations were also likely to
suffer from selective fading which
introduced considerable distortion
on AM signals. Unfortunately though,
AGC cannot overcome this particular
problem. It can be overcome to a large
extent by using phase-locked single
sideband (SSB) reception but this is a
specialised technique that’s used more
in communications equipment rather
than in domestic receivers.
Enter automatic gain control
In summary then, the problem was
how to stop the set from blasting the
listener out of the room on strong signals while still allowing weak signals
to be received at usable volume. The
answer was Automatic Volume Control (AVC) or as we more accurately
call it today, Automatic Gain Control
(AGC).
Basically, AGC works by automatically reducing the gain of the receiver
when a strong signal is received. The
stronger the signal, the greater the AGC
action. As a result, the audio output
is kept reasonably constant for all
stations regardless of signal strength.
AGC was invented in the US in 1925
by Harold Wheeler but did not come
into common usage until well into the
1930s. However, some late-model TRF
The Mullard Meteor 600 4-valve receiver (circa 1947) was another economy
receiver with no AGC. The volume was controlled by varying the backbias to the first two valves (both variable-mu types) in the line-up (ie, to the
ECH35 converter & EBF35 IF amplifier stages).
(tuned radio frequency) receivers using sharp cut-off valves did use AGC
circuits. This was not particularly successful as only a very limited amount
of AGC could be achieved before the
valve cut off completely.
The designers understood that varying the bias on the valves could alter
the gain to some degree. The problem
was that the gain of sharp cut-off valves
does not vary a great deal until the
valve is actually near cut-off. Once
the valve is near cut-off, very little
increase in the bias voltage is needed
to fully cut it off and reduce its gain
(or amplification) to zero.
When these valves are near cut-off,
distortion, overloading and various
spurious signals are generated. This
makes listening to an AGC-controlled
set with a sharp cut-off valve rather
unpleasant. This can occur if, say, a
6AU6 is plugged into the valve socket
for an RF or IF stage designed to use a
6BA6 with AGC. The cut-off voltage
for the 6AU6 is between -4V and -6V,
depending on the operating conditions
set for the valve. However, it is around
-20V for a 6BA6.
The main difference between these
two valves is the structure of the signal grid. The 6AU6 has a grid which
consists of close, evenly-spaced turns
of wire. By contrast, the 6BA6 has
closely-spaced turns of wire at each
end of the grid structure, with the
spacing widening towards the centre
of the grid. This is known as a “variable mu” valve.
Progressive cut-off
In operation, as the negative voltage on the grid of a variable mu valve
increases, it progressively cuts off the
electron flow at the ends of the grid
structure. Eventually, with increasing
negative bias, only a small section in
the middle of the valve is left to do
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First marketed in 1954, the AWA
Radiola 653P was a 5-valve portable
with simple AGC applied to the RF
amplifier and converter stages.
the amplifying. However, because the
remaining grid structure is so open,
large AGC voltage variations now
cause only relatively small changes
to the plate signal, compared to when
the entire valve is operating.
As a result, the gain is progressively
and smoothly reduced as the grid bias
increases.
Remote cut-off valves
Two early remote cut-off RF tetrodes
were the 35 and 51. Introduced around
1931, they were nearly identical and
became the 35/51. Basically, they were
an adaptation of the sharp cut-off 24
but with a variable-pitch grid.
In operation, the 24 required just
-8V of bias to cut it off but the 35/51
required around -40V. In addition, the
latter’s gain was reduced smoothly as
the bias increased.
The 39/44 RF pentodes with remote
cut-off characteristics appeared a little
later, followed by the 58. More modern
valves with remote cut-off characteristics include the 78, 6D6, 6U7G,
6K7, 6SK7, 6AD8, 6AR7GT, 2B7, 6B7,
6B8G, 6G8G, 6BA6, 6BH5, 6BY7 and
the 6N8. The relevant battery valve
types include the 1D5GP, 1C4, 1M5G,
1P5G and 1T4.
The AGC voltage
Having established that varying the
negative bias on a remote cut-off valve
would alter its gain, it was necessary to
come up with a method of developing
this control voltage. The device that
found almost universal favour to do
this was the humble diode detector.
Some receivers did use valves that
acted purely as diode detectors, eg,
the 6H6 and the 6AL5. However,
valve envelopes were expensive and
as the manufacturers became even
more innovative, they included one
and sometimes two signal diodes in
the same envelope as an audio triode.
Basically, the cost of producing a valve
with two diodes and a triode was not
much more than the cost of producing
a single-function valve.
The 55 and the 85 are two such
triode/diode valve types. In each case,
the triode section was similar to the
proven 27 valve. They were successful
and this prompted the development of
similar valve types, some even including tetrode or pentode elements.
The 55 and 85 are not the same,
however, as their triode gains are quite
different. The 85 has a gain of about
six while the 55 (or, in its octal guise,
the 6SQ7GT) has a gain of about 60 in
a practical circuit. Other valves that
proved successful in the duo-diode
audio triode role are the 2A6, 6B6G.
6BD7 and the 6AV6.
The duo-diode audio triode valve
suited the standard 5-valve superhet
receiver, which used a converter, an
IF (intermediate frequency) amplifier,
a combined detector and first audio
stage, an audio output valve and a
rectifier. By contrast, economy sets
using just four valves omitted the first
audio amplifier. As a result, in these
sets, the detector and AGC diodes
were incorporated into the IF amplifier
valve, eg, the 6AR7GT, 6G8G, 6AD8,
6N8 and EBF35 (to name a few).
into VIDEO/TV/RF?
Television & Video
Technology – by KF Ibrahim
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Practical Guide To
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The book written by an Aussie for
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An in-depth look at the
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There’s something to suit every
RF fan in the SILICON CHIP
reference bookshop: see the
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– by Chris Bowick
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text - tells how to design
and integrate RF components
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74
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! Audio ! RF ! Digital ! Analog ! TV ! Video ! Power Control ! Motors ! Robots ! Drives ! Op Amps ! Satellite
86 Silicon Chip
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The impressive 5-band STC Capehart A8551 radiogram dates from the mid1950s and uses eight valves plus a magic-eye tuning indicator. It is also fitted
with a very effective delayed AGC system.
One or two audio output pentodes
had diodes built into them too, such
as the 6BV7.
Early problems with AGC
Once suitable valves had been developed, AGC certainly kept the audio
output level reasonably constant, even
with wide variations in signal level. It
made normal signal level fading much
easier to accept but “selective” fading
still made listening to distant stations
difficult. It did take set designers a few
years to get AGC systems working really well, however.
One early problem brought about
by AGC occurred because of the way
some people tuned their sets. AGC
meant that the audio output level
remained virtually the same even if
the station was slightly mistuned. As
a result, many users had difficulty
in accurately tuning their sets even
though a mistuned station resulted in
audible distortion and sibilants and
was unpleasant to listen to (I know
because my father could never get it
right, so I’d sneak up and retune the
set when he wasn’t looking).
Eventually, some manufacturers
solved this problem by fitting “magiceye” valves to many of the up-market
siliconchip.com.au
receivers. The pattern on the magic eye
indicated the correct tuning position.
Another early problem with AGC
was that it emphasised the hiss, crackles, pops and other forms of interference when tuning between stations.
That’s because the sets were at their
most sensitive when tuning between
stations due to the increased gain. As
a result, set manufacturers came up
with various schemes to minimise
this problem.
These schemes invariably used the
AGC voltage to forward bias a valve
or diode in the signal path when the
signal exceeded a preset level. However, although these systems worked,
any station that was only just strong
enough to reach the threshold would
give distorted audio. In addition, if the
RF signal strength was fading up and
down, it may be heard quite well for a
short time but then, as it faded down
below the threshold level, the audio
would suddenly disappear before suddenly reappearing again as the signal
level increased.
This system is called “Quiet Automatic Gain Control”, or QAGC. And
although it wasn’t particularly successful on early domestic receivers,
variants of it are still used in com-
These binders will protect your
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Photo Gallery: Fisk Radiola Model R49G
ceiving an extremely weak signal. In
practice, however, this did not really
cause a problem, as it was quite practical to slightly reduce the standing bias
on the AGC-controlled valves to make
up for this. In these sets, a single diode
usually performed the dual function
of detector and AGC diode.
By contrast, delayed automatic
gain control (DAGC) uses two diodes
– one as the detector and the other as
the AGC diode. The detector circuit
is usually the same as in sets with
simple AGC.
DAGC is obtained by biasing the
second diode so that it does not conduct until the signal voltage applied
to it is above a preset level (usually
between -2V and -3V). The AGC bias
developed once that level is reached
is then applied to the AGC-controlled
valves in much the same manner as
for simple AGC. However, by delaying the application of AGC until the
preset level is reached, DAGC allows
a receiver to amplify weak signals at
full gain.
Early servicing problems
R
ELEASED IN 1939, the AWA Fisk Radiola Model R49G was a 4-valve batteryoperated receiver that operated on the broadcast band. It was housed in an
attractive wooden cabinet, had an IF (intermediate frequency) of 460kHz and
included following valve line-up: 1C6 converter, 1D5G IF amplifier, 1K6 IF amplifier, detector, AGC & audio amplifier and 1D4 audio output. Photograph by Kevin
Poulter for the Historical Radio Society of Australia (HRSA). Phone (03) 9539
1117. www.hrsa.net.au
munications receivers. However, it is
now called “Mute” or “Squelch” and
even some domestic FM receivers
use a muting circuit to reduce noise
between stations.
To overcome the limitations of
QAGC, a number of manufacturers
designed receivers with preset tuning. However, although the idea was
fine, this meant that the frequency
stability of the local oscillator had to
be very good, otherwise the set would
eventually drift off station. When this
happened, the oscillator had to be serviced, which was very inconvenient
and costly for the owner.
Mechanical preset tuning was
subsequently used extensively in car
radios in the 1960s but by then oscil88 Silicon Chip
lator frequency stability was much
better than in 1930s receivers.
Simple & delayed AGC
Initially, AGC circuits were of the
simple variety, in that as soon as a
signal, no matter how weak, was presented to the diode detector, a bias was
applied to the AGC line. This meant
that the receiver’s gain on even quite
weak signals was reduced. In fact, the
noise picked up by the antenna when
the receiver was tuned off-station
was often enough to generate some
AGC bias and this was used in some
receivers as the standing bias for the
AGC-controlled valve stages.
It might seem poor design to reduce
the gain of a receiver when it is re-
In earlier times, radio servicemen
were mostly self-taught. As a result,
many didn’t understand AGC circuits
and so were reluctant to work on them.
There was a widespread belief in the
trade that they were difficult to work
on but this was mainly due to their
lack of knowledge and adequate test
equipment.
What made it hard was that AGC
circuits have high resistance values
and the average serviceman had ineffective instruments for testing them.
As a result, servicemen often had to
guess whether this part of the circuit
had a problem in it.
Remember also that components
were expensive in those days. When
I was servicing back in the late 1950s,
my wages were $18 per week and a
standard RF valve cost $2 or $3. Capacitors were around 15 cents each,
so radio parts in earlier times were
much more expensive in relation to
the average wage. These days, we can
afford to replace multiple components
when tracking down a fault but that
technique wasn’t economic until the
1980s.
Next month, we’ll take a look at a
variety of AGC circuits and describe
how they work. We’ll also take a look at
some of the faults which can be found
SC
in such circuits.
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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. Write to: Ask Silicon Chip, PO Box 139, Collaroy Beach, NSW 2097 or
send an email to silicon<at>siliconchip.com.au
Changing the Zapper to
suit 8V batteries
I recently purchased and built the
Battery Zapper (SILICON CHIP, May
2006) and it works perfectly. However,
is it possible to change the 6V setting
to 8V or 9V. There are a lot of 8V batteries used in golf carts etc. I feel that
it would be better to treat batteries independently instead of in 24V banks,
don’t you?
I would use a 9VDC 1A plugpack
during zapping and then revert to the
normal 48V charger when zapping is
completed. (T. Q., via email).
• We would suggest treating 8V leadacid batteries independently instead
of in 24V banks.
Only one modification is needed to
change the 6V range for checking 8V
batteries. This involves swapping the
connection from the “6V” position of
switch S2b from the junction of the
270Ω and 220Ω resistors in the metering voltage divider down to the other
end of the top 220Ω resistor (ie, to the
junction of that resistor and the 220Ω
resistor below it).
However, for improved operation of
the Condition Checker section of the
project, we suggest that you also make
some of the changes incorporated into
the “Mk3” battery checker which was
described in the August 2009 issue.
Manual controller for
thermoelectric cooler
I want to build a simple controller
to manually adjust a 96W 12V thermoelectric cooler. Your 12V Speed Controller/Lamp Dimmer project (SILICON
CHIP, November 2008) seems ideal but
only handles up to 50W. The earlier
12V/24V 20A design featured in the
June 1997 issue is more than I need
(and costs twice as much).
Can the 12V Lamp Dimmer be
upgraded to handle a 100W cooler
by simply changing the Mosfet? If
so, which component should I use in
place of the one included in the kit?
(R. M., via email).
• For an 8A load, the MTP3055 is
not suitable (as you suggest) because
it is only rated at 12A and has an onresistance of 0.15Ω. Its dissipation
Twin Settings For 12V Battery Charge Controllers
I have built six 12V Battery Charge
Controllers (S ILICON C HIP, April
2008) for the club VHF/UHF repeaters, myself and several others. They
seem to perform excellently.
However, for the first time, I
needed two sets of parameters for
different charge rates. It seems that I
cannot do this because setting trimpots VR1-4 on link 5 also sets those
parameters on link 6. That means
that I cannot set two sets of values
and switch them via a 2-way switch,
connected to the pins of links 5 and
6, on the front panel.
The instructions read as if two
sets of parameters can be set, stored
and changed at will with links 5 and
6. Can you help me, please? (T. B.,
North Albury, NSW).
90 Silicon Chip
•
You can have two sets of parameters and switch between them with
LK5 and LK6.
With LK5 inserted, adjust the
required parameters using trimpots
VR1, VR2 and VR3 for one type of
battery and press switch S2. Then
use LK6 and set the parameters again
using VR1, VR2 and VR3 and press
S2. This will make the two alternative parameter settings available,
depending on whether the LK5 or
LK6 setting is being used.
The VR1-VR3 settings are dualpurpose and set the parameters depending on the position of LK5 and
LK6. These settings are not stored
unless S2 is pressed. This is detailed
at the end of the article headed “Setting the parameters”.
would be just under 10W at full power
to the motor. It therefore should be
changed to an IRF1405 (169A, 5.3mΩ).
This has a much lower on-resistance,
so there will be less heat generated
within the Mosfet.
The fuse should be rated at 10A and
the tracks leading from the screw connectors to the fuse, the Mosfet’s drain
and source and to diode D2 should
be thickened by running solder along
the tracks or add some tinned copper
wire between the connections on the
PC board if it is solder-masked.
24V mod for battery
charge controller
Would it be possible to use the 12V
Battery Charge Controller from the
April 2008 issue for 24V batteries? I
expect the voltage divider involving
R1 and R2 would need to be changed
to match the 24V rail but could I leave
the rest basically alone having consideration for the larger heat dissipation?
(C. M., via email).
• For charging 24V batteries, R1
should be 12kΩ and R2 2.2kΩ. The
470µF 25V capacitor at the input
should be increased to 35V or 50V,
while the 100Ω 0.5W resistor in series
with switch S1 should be 220Ω 0.5W.
Using a relay to change
motor direction
I’ve purchased two PWM controllers
(SILICON CHIP, June 1997) to control
two 200W 12V fixed magnet brushed
motors. I am wondering if I can run
these motors also in reverse by putting a switch in after diode D2 and the
capacitor which are wired across the
motor, to reverse the polarity at the
motor. (A. J., via email).
• Yes, a DPDT (Double Pole Double
Throw) relay can be used to switch
the polarity applied to the motor
terminals. For these relays, there are
two separate contacts called poles
and each pole has a common (COM),
a normally-open (NO) and a NormallyClosed (NC) contact.
siliconchip.com.au
If we call the poles Contacts 1 and
Contacts 2, then the COM terminal
of each pole connects to each of the
motor terminals. The NO of contact 1
and the NC of the contact 2 connect
to the “+” output of the Motor Speed
Controller. The NC of contact 1 and the
NO of the contact 2 connect to the “-”
output of the Motor Speed Controller.
The diode connects across the NC of
contact 2 (cathode) and the anode to
the NO of contact 2.
Note that for a 200W motor you
would need at least 20A and preferably
a higher contact rating for the relay.
Also the motor should be stopped
before switching it to change direction, otherwise the surge current will
be very high.
External power supply
for Class-A amplifier
I built the 15W Class A Amplifier
some years ago and have enjoyed it
tremendously. I have now purchased
the Altronics kits for the new 20W
Class Amplifier (ie, L & R channel
amplifier kits and a power supply kit).
I wish to use the toroid from the
original 15W amplifier which is 160VA
and has 21V secondaries rather than
purchase a new one with 16V secondaries. I’m happy to keep the new power
supply in a separate box.
Can I use the regulated 20V supply
from the original design? Alternatively, what changes would I need to
make to the new unregulated supply
in order to use the 160VA/21V toroid?
(A. F., via email).
• If you are going to keep the original
power supply box, then there is nothing to stop you from using the original
power supply itself.
A new use for the
GPS Car Computer
I have a possible application for the
GPS Car Computer (SILICON CHIP, January & February, 2010). I drive a Toyota
Camry V6 and a Proton Jumbuck ute
which has a 1500cc 4-cylinder, both of
which have air-conditioning. In South
Gippsland where I live, the Proton ute
is often one gear better off on long hills
with the air-conditioning off and while
there is no noticeable difference with
the Camry, it would undoubtedly save
petrol on those occasions when it is
working hard on a hill.
My suggestion is that a combination
siliconchip.com.au
Noise-Cancelling Circuit Wanted
Recently, I built a Bionic Ear (Jay
car Cat. KJ-8226). I have used the
unit in conjunction with a parabolic
reflector and recorder to record bird
calls in the bush. One problem that I
have encountered is relatively high
levels of ambient noise.
I have written to Jaycar suggesting that they consider developing
a kit which incorporates a variable noise-cancelling feature. This
would involve the use of two microphones. The first microphone
faces the direction that the sound
the listener wishes to hear emanates from. The second microphone
registers the ambient sound. The
second microphone’s signal is then
electronically subtracted from the
first microphone’s signal so that the
difference is basically the sound that
the listener wishes to hear.
Such set-ups have been used
in hearing aids for some time. I
believe that, some years ago, your
magazine featured a project which
involved an audio amplifier similar
of high fuel consumption and possibly
higher revs without a proportionate
distance travelled could be used as parameters to turn off the air conditioning compressor until conditions revert
to more normal settings. Presuming the
car computer is receiving pulses from
an injector, all the necessary external
data is already available.
This would also come into play
under acceleration which is a feature
appealing to the sports car fraternity.
An override may be necessary when
towing. (J. M., via email).
• We did publish an air-conditioning
controller in January 2007. This optimised the compressor running for best
economy and allowed extra power on
acceleration. This approach would be
much simpler.
Nitrous fuel controller
is not working
I have constructed the Nitrous Fuel
Controller (Performance Electronics
for Cars, 2004) and on applying 12V
DC with a 5W globe to check its operation, I found that it starts up only
now and then and when it does, the
to the Jaycar kit. I realise that this
noise-cancelling feature adds to the
complexity of the unit and as such
may be considered for a standalone
project for inclusion in your magazine. (G. H., Camden, NSW).
• While we are not familiar with
the Bionic Ear project, it is evidently
similar in principle to the “Sooper
Snooper” project described in the
September 2001 issue.
The fact that you are experiencing
a lot of extraneous noise suggests
that your mike set-up may not be
sufficiently directional. This may be
because your parabolic dish is not
big or deep enough or perhaps the
microphone is not set at the focus of
the parabola.
Having said that, we did describe
a project with noise-cancelling
microphones in an FM Motorcycle
Intercom (SILICON CHIP, October &
November 1989) and the relevant
part of the circuit with noise cancelling could be adapted to your
application.
frequency and pulse width jump all
over the place. I had the board checked
for soldering defects and incorrect
placement by staff at the Jaycar store
at Mermaid beach and they said my
construction was spot on and the soldering was excellent.
I also found the 100Ω resistor and
12V zener diode (ZD1) were overheating (you could fry an egg on them). I
have replaced the 7555 timer, trimpot
VR1 and the MTP3055 Mosfet with no
success. When I turn the trimpot the
light changes intensity and flashes erratically. Please help. (G. C., via email).
• Check the positioning of transistors
Q1 and Q2. The heavy load current
causing the 100Ω supply resistor to
overheat is possibly due to Q1 and
Q2 being in the wrong positions. This
would also cause the erratic behaviour.
Halogen lamps
with dimmers
I am a little confused on the subject
of using halogen downlights with light
dimmers and hope that you can help.
I have always thought that at a certain
filament temperature, the tungsten
May 2010 91
How Do Electromagnetic Waves Penetrate Barriers?
I’ve been reluctant to ask this question for fear that it may be regarded as dumb!
For many years, I’ve remained
curious as to how electromagnetic
waves could possibly penetrate barriers such as brick walls, internal
stud and plaster walls, and especially the metal-clad bodies of trains,
trams, buses, various other motor
vehicles, ships and aircraft, so that
mobile phones, GPS devices, laptops
and AV senders can happily work.
I’m happy with the thought of
radiation from the Sun penetrating
glazing, giving a potential window
to EM radiation. However, with the
relative absence of glass, how does
EM transmission successfully penetrate all those barriers, particularly
metal?
I also had in mind Faraday mesh
shields for exclusion of EM radiation. Presumably mobile phones etc
will not work inside such shields.
Yet how do the phones and other
electronic devices work within steelclad bodies?
What finally triggered this enquiry
atoms liberated from the filament react
with the gas and the glass envelope
in a way that results in the tungsten
being deposited back on the filament,
thereby increasing the operating life
of the lamp.
If I’m correct, it would stand to
reason that using a halogen downlight
with a light dimmer would reduce the
lamp’s life due to the fact the filament
would not reach the required temperature for the abovementioned reaction
to take place. This has me confused,
because everywhere I go I see halogen
downlights used with dimmers.
My question is does using a light
dimmer with a halogen lamp reduce
the lamp life?
• For the halogen cycle to work, the
silica glass bulb itself must run at such
a high temperature that tungsten is
not deposited on it. Hence any atoms
driven off the tungsten filament are
eventually deposited back onto it.
When run with a dimmer, the hal
ogen lamp runs much cooler and therefore the halogen cycle does not work.
Lamps continually run in a dimmed
92 Silicon Chip
was a recent comment in SILICON
CHIP that the “GPS Clock” will even
work inside a steel filing cabinet.
Huh?
Hot on the heels of this dilemma
was an enquiry from a colleague
regarding the failure of a cordless
phone to work inside a dwelling
with multiple internal brick walls.
There may be another logical reason
for this aberration and I’m mindful
of the fact that I’ve used a cordless
telephone inside and outside our
home (with multiple “barriers” to
EM radiation) without trouble for
many years. Conversely, a fairly
typical AV sender installation has
been disappointing.
So I’d be very grateful if you could
put me out of my misery; curiosity is
getting to me! I’ll assume it’s related
to the wavelength of the radiation
but I’m not entirely satisfied with the
hypothesis, nor the physical realisation. My enquiry could even form
the basis for a more detailed article
in SILICON CHIP, assuming that many
other readers might have similar
doubts, simply accepting that what
condition will eventually blacken and
will have a shorter life. Apart from
that, running halogens with a dimmer
greatly increases their inefficiency
– it’s a bad idea but people like the
facility of a dimmer.
Modifying the
Energy Meter
I would like to use the Appliance
Energy Meter (SILICON CHIP, July &
August 2004) to measure the electrical
power used in my home workshop. My
workshop has a single phase sub main
protected by a 63A circuit breaker. The
total rated load is 14.5kVA, so obviously the Energy Meter would need
to be modified.
I propose using a 60:5 current transformer to measure the current in the
sub main Active. I would delete R2 and
move R1 so that it connects between
the two 1kΩ resistors at the input of
AMP1. R1 would serve as the shunt
load for the CT and its value would
be changed to 0.02Ω .
Using a 60:5 CT with a shunt load
occurs is “normal” without understanding why. (B. G., via email).
• That is a big subject. Electromagnetic waves will certainly penetrate
solid materials such as brick walls
but they are heavily attenuated,
depending on the moisture content
of the material. Multiple brick walls
inside a dwelling can cause a great
deal of RF signal attenuation which
can be a real problem if you are attempting to set up a WiFi network
or A/V transmitter in a home.
Solid metal stops all RF signals, as
will wire mesh, provided the signals
of interest have a larger wavelength
than the holes in the mesh. That is
why mobile phone signals can easily
be received inside a vehicle – the
signals come in via the windows.
The reason that GPS signals can
be received inside a filing cabinet
is that the metal drawers and their
fronts are not a tight fit. The signal
can easily pass through the gap
and while it is probably heavily attenuated in the process, there is still
enough signal for the GPS receiver
to work – incredible but true.
(R1) of 0.02Ω would give the same
input to AMP1 of 100mV RMS at 60A
load and 150mV RMS at 150% rated
load. As I do not require the brown-out
protection option, I propose deleting
LK1 & 2, the 10Ω & 68Ω resistors, relay
RLY1, D6 and Q1, as well as all of the
load side wiring.
I would also change the value of F1
to, say, 1A as it would only protect the
mains voltage sense circuit and the
mains side of T1.
I have two questions: how do I scale
the output to give the correct readings
and will the phase shift adjustment be
sufficient to deal with any phase shift
introduced by the CT?
I think I may have the answer to
question one. I have a copy of Geoffrey Graham’s C code for this project
(thanks, Geoffrey). In his code, he
reads the watts value from the ADE
7756AN but before using it he divides
it by 472,149, which he describes as a
calibration constant.
If I divide this value by 6 and use
78,691.5 as my calibration constant,
this should (I think) get me close to
siliconchip.com.au
displaying the correct power value.
I am a qualified electrician so there
are no problems for me doing my own
electrical work. (B. P., Murrumbateman, NSW).
• A current transformer could be used
to reduce the current as measured by
the Energy Meter. The phase adjustment in the ADE7756AN is there to
compensate for current transformer
phase shifts and so will provide sufficient adjustment.
Calibration has more to do with
the actual numbers displayed on the
LCD. So when the calculations have
been made, the values will need to be
multiplied by 6 when the 60:5 current
transformer is used and R1 changed to
0.02Ω instead of 0.01Ω. However, the
calibration constant of 472,149 could
be changed to 78,691 instead.
Float charger
modification for 24V
I have built several 12V SLA Float
Chargers (SILICON CHIP, March 2003)
to avoid sulphation in stored batteries. I now need to do the same for a
24V battery.
Could I have your advice please on
some circuit changes? I have a 25V
transformer and will raise the voltage rating of the filter capacitors. My
real query is about the output voltage
divider chain. I propose doubling the
values: 120Ω to 240Ω, 1kΩ to 2kΩ and
VR7 to 1kΩ. Any comments? (K. O.,
via email).
• For 24V operation, the 16V and
25V capacitors need to be rated at 50V.
Both 2.2kΩ resistors feeding the LEDs
should be 4.7kΩ. The series 1kΩ resistor and trimpot VR7 should be 2.2kΩ
and 1kΩ respectively. Do not double
the 120Ω resistor.
Also the relay should preferably be
Digital Camera Won’t Work With Rechargeable Cells
A few months ago I made the
mistake of buying an Olympus digital camera. This particular model
takes two AA cells but will not run
off rechargaables because the voltage is too low. Alkalines last about
15 shots. Lithiums are the only
remaining alternative but they are
expensive.
What if I was to somehow mount
an extra rechargeable cell externally
and connect it in series with a power
diode? This should result in (3 x 1.2)
- (0.6) = 3V. What are your thoughts
on this arrangement? (G. H., Mt
Martha, Vic).
• Unfortunately, the voltage drop
across a silicon diode is not constant
and increases with current. So if you
have a nominal 3.6V from the NiMH
a 24V type (eg, Altronics S4162A) and
the 220Ω 0.5W resistor supplying the
relay current should be changed to 1kΩ
0.5W. Alternatively, if the original 12V
relay is retained, then the 220Ω 0.5W
resistor would need to be changed to
820Ω 5W.
In addition, take care that the input voltage to the LM317T does not
exceed 40V.
Knock sensor
for a go-kart
I bought the Knock Sensor kit (SILICHIP, June 2007) to use with the
Ignitech CDI I use on my super kart.
The Ignitech has a function whereby
when pin X is grounded, the timing
is retarded. When I build the Knock
Sensor kit, what type of output will
it give when knocking is detected? Is
CON
cells, the voltage following the diode
could range from about 3.3V at light
loads to below 2.6V under load.
This lower voltage may prevent the
camera from working and the higher
voltage at low loads may cause damage to the camera, as freshly charged
NiMH cells can have a much higher
voltage than 1.2V per cell.
If you are prepared to risk it, you
could try the diode in series with the
cells. A 3A diode would probably
be required and maybe a Schottky
diode would be needed to provide
a lower voltage drop at high current.
Ideally, a better approach would
be to use a 3V regulated supply that
can deliver the required current for
the camera. Lithium cells are probably the best alternative.
it a positive voltage? If so, I will use
a very small solenoid to earth the pin
in the CDI or is there another part of
the circuit I can tap into? I am using
a GM knock sensor out of a 2000 V6
Commodore. (J. J., via email).
• The knock sensor project was
specifically designed to be used in
conjunction with the SILICON CHIP
Programmable Ignition system (March
to May 2007). It is not designed to pro. . . continued on page 95
Notes & Errata
Battery Capacity Meter, June 2009:
the circuit on page 22 shows pins 15
& 16 of IC1 reversed. The PC board
is correct and does not need to be
modified.
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
Trade Practices Act 1974 or as subsequently amended and to any governmental regulations which are applicable.
siliconchip.com.au
May 2010 93
Silicon Chip Magazine May 2010
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94 Silicon Chip
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Ask SILICON CHIP –
continued from page 93
vide a knock signal independently
from the Programmable Ignition
which monitors the knock sensor signal only during the period
of ignition and ignores the signal
otherwise.
For use with the Ignitech CDI, the
knock signal will require further
processing where the output signal
is monitored to produce a low-going
(grounded) voltage with knock detection. A means to switch low when
knock is detected would be required.
The Voltage Switch (SILICON CHIP,
December 2008) would be suitable.
Note that the 10nF capacitor connecting to pin 12 of IC1 in the Knock
Detector will need to be increased
in value to around 1µF to increase
the signal detection period so that
ignition retard will have time to
take effect.
The first is an analog meter utilising a stepper motor as the movement
with, say, a 0-1V or 0-0.1V input for
full-scale deflection. A meter such as
this could have numerous applications where an analog indicator with
a quick response that’s free of overshoot is useful. Dumped computers
with floppy drives are plentiful on
the streets these days and can be a
source of stepper motors.
Secondly, how about an engine
knock detector? It could be as simple
as having just a warning light giving
indication of single or continuous
engine knocks and utilise a commonplace sensor. (A. G., via email).
• We produced a Knock Indicator
for cars in the April 1996 issue. It
used an LM3914 bar graph indicator
and 10 LEDs to show the severity of
knocking.
Changing the knock
signal frequency
Simulating a knock
sensor signal
My engine knock frequency is
at 6.8kHz but the low-pass filter in
your Knock Detector circuit is set to
6.4kHz. I can’t find any software to
recalculate the low-pass to higher
values. Is it possible to use precision
trimmers to set the knock frequency
window with a few modifications?
Can I add a microcontroller to the
output with 5V ADC? (J. B., Barkau,
Germany).
• The low-pass filter can be chang
ed to suit a knock frequency of
6.8kHz by decreasing the 3.3nF capacitor to 2.7nF and increasing the
12nF capacitor to 10nF. The signal
output can swing to not much more
than 5V, as IC1d’s output does not
go to the full supply of 8.2V.
The 2.2kΩ series resistor will limit
current into a microcontroller’s ADC
input when the input protection
diode clamps and prevents damage
should signal output go above 5V.
I have purchased the article on the
Knock Detector (SILICON CHIP, June
2007) and would like to know if this
can be used on its own with a LED
to detect knock in a engine while I
am tuning it.
At this point, I am not sure what
the output is between 4.8kHz and
6.4kHz because I cannot simulate
this signal to see if the unit works.
Your help would be appreciated.
(L. N., Johannesburg, South Africa).
• As noted elsewhere on this page,
the Knock Detector is not suitable for
use as a standalone knock indicator.
That function would be better performed by our Knock Indicator from
our April 1996 issue. While there is
no kit available for this project, all
the parts are still readily available.
Having said that, you would probably be better off monitoring the
knock sensor signal with an oscilloscope. Ideally, you should use a
dual-trace oscilloscope so you can
also display the ignition signal for
each cylinder compared with engine
firing. Knock will precede the ignition signal in each case.
To find out what the knock signal
looks like, just gently tap the sensor
SC
with a screwdriver.
Knock indicator to
avoid engine damage
I have a couple of project suggestions that may be of interest to SILICON CHIP. They are along the lines of
the salvaged parts series a while ago.
SC
May 2010 95
Do you eat,
breathe
and sleep
TECHNOLOGY?
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Jaycar Electronics is a rapidly growing, Australian owned, international
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Why not do something you love and get paid for it?
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Advertising Index
4D Systems..................................... 94
Altronics.......................................Flyer
Aust. Valve Audio Transformers....... 95
Cleverscope...................................... 9
Dick Smith Electronics............... 24-25
Emona Instruments......................... 41
Front Panel Express........................ 11
Grantronics..................................... 94
High Profile Communications.......... 95
Instant PCBs................................... 95
Jaycar..............................IFC,45-52,96
Keith Rippon................................... 95
Kitstop............................................. 94
LED Sales....................................... 94
Oatley Electronics......................... IBC
Ocean Controls............................... 10
OzComfile....................................... 94
PCBCART....................................... 11
Pymble Software............................. 95
Quest Electronics............................ 94
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There’s something to suit every
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A reference work for technicians,
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90
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Provided your idea is workable
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49
You’ll find many more technical
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elsewhere in this issue
96 Silicon Chip
RCS Radio...................................... 94
Rohde & Schwarz............................. 3
RF Modules.............................OBC,96
Sesame Electronics........................ 94
SC Performance Elec. For Cars...... 85
Do you have a good
circuit idea? If so,
sketch it out, write
a brief description
of its operation & send it to us.
– by Garry Cratt
The reference written by an Aussie
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Silicon Chip Publications,
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Silicon Chip Binders........................ 87
Silicon Chip Bookshop............... 82-83
Silicon Chip Order Form................. 89
Siomar Battery Engineering......... 7,95
Soundlabs Group.............................. 9
Splat Controls................................. 94
Terry’s Transistors........................... 94
Trio Smartcal..................................... 5
Truscotts Electronic World............... 95
Wagner Electronics......................... 43
Worldwide Elect. Components........ 96
PC Boards
Printed circuit boards for SILICON CHIP
designs can be obtained from RCS
Radio Pty Ltd. Phone (02) 9738 0330.
Fax (02) 9738 0331.
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O/circuit: 20.9V
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be used to control the speed. Both of the kits have
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These panels are waterproof, aluminium framed and
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covered with tempered glass. Connections are made to
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the screw terminals that are inside the small box at the
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is a PWM speed controller
[K281]
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heatsink (not supplied).
INTRODUCTORY PRICE without the reversing circuitry.
The
reversing
NEW K273 and K273IR
8W SOLAR ARRAY + K251A REGULATOR
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RELAY DRIVER AND INFRA-RED TRIGGER KITS
Includes two 4W small
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THE K273IR kit uses an IR LED and IR receiver to
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K275 is a
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Connect in parallel
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It can be powered from
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Or connect in series
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$12.50 reversing circuitry that employs
The K273 kit is
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This kit will not change direction until the motor has
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It uses an input from a switch
20W-12V MONOCRYSTALLINE SOLAR PANEL
current flowing as relays can carry more current than
or other circuit like our K273IR to
Peak: 20W, Open
they can switch.
allowing control of higher motor Circuit: 21.5V, Short
switch a relay. The kit comes with a relay
currents.
rated at 10A <at>250VAC. There is an optional
Circuit: 1.3A, Max.:
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Turning on warm
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Optional large 20A relay
Note: The above solar panels may vary slightly from
[OR20] $6
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[K275A]
I
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SC_DEC_09
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