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Contents
Vol.28, No.4; April 2015
SILICON
CHIP
www.siliconchip.com.au
Features
16 Airborne Weather Radar: Keeping Aircraft Safe
Airborne weather radar enables aircraft to avoid extreme weather to ensure
safety and passenger comfort. We take a look at the technology and the huge
advances that have been made in recent years – by Dr David Maddison
24 Review: National Instruments VirtualBench
VirtualBench is a computer-driven 2-channel 100MHz digital oscilloscope,
34-channel logic analyser, waveform generator, 3-output adjustable power
supply and multimeter, all in one box. It also mates with National Instruments’
LabView software for automated measurement & testing – by Nicholas Vinen
89 Review: Keysight MSO-X 3104T Oscilloscope
Appliance Insulation
Tester – Page 30.
Keysight’s updated MSO-X 3104T midrange scope adds a number of new
features, including a touch-screen, without a price increase. Nor is there any
need to return the unit to a service centre to upgrade the bandwidth all the way
from 100MHz to 1GHz – by Nicholas Vinen
Pro jects To Build
30 Appliance Insulation Tester
Do you think that your 230VAC-powered tools and appliances are safe because
they are double-insulated? The only way to be reasonably sure is to test them
using our new Appliance Insulation Tester – by John Clarke
42 A Really Bright 12/24V LED Oyster Light
Got a boat, RV or 4WD, etc? Here’s a low-cost, 1000+ lumen “Oyster” LED light
fitting for when you don’t have mains available (or even if you do). It runs from
12-24VDC or from 230VAC via an optional mains adaptor – by Ross Tester
58 Build A Low-Frequency Distortion Analyser
Concerned about the quality of your 50Hz 230VAC supply? Want to measure
the harmonic distortion of the lower frequencies from your loudspeaker system?
This unit will measure the distortion of any 3-20VAC sinewave signal in the
range of 20Hz-10kHz – by Nicholas Vinen
A Really Bright 12/24V LED Oyster
Light – Page 42.
72 WeatherDuino Pro2 Wireless Weather Station, Pt.2
Second article this month describes the transmitter circuit and the assembly
details. We also describe the software installation and look at the various
sensors that are available – by A. Caneira & Trevor Robinson
Special Columns
53 Serviceman’s Log
I hate letting anything beat me – by Dave Thompson
Build A Low-Frequency Distortion
Analyser – Page 58.
80 Circuit Notebook
(1) Hard Drive Brushless Motor Controller With Speed Control; (2) Lithium
Battery Cell Equaliser; (3) PICAXE-Based Next Number Display System
84 Vintage Radio
The AWA 897P: Australia’s first transistor radio – by Ian Batty
Departments
2 Publisher’s Letter
4 Mailbag
67 Product Showcase
siliconchip.com.au
92 Ask Silicon Chip
95 Market Centre
96 Advertising Index
96 Notes & Errata
WeatherDuino Pro2 Wireless
Weather Station, Pt.2 – Page 72.
April 2015 1
SILICON
CHIP
www.siliconchip.com.au
Publisher & Editor-in-Chief
Leo Simpson, B.Bus., FAICD
Production Manager
Greg Swain, B.Sc. (Hons.)
Technical Editor
John Clarke, B.E.(Elec.)
Technical Staff
Ross Tester
Jim Rowe, B.A., B.Sc
Nicholas Vinen
Photography
Ross Tester
Reader Services
Ann Morris
Advertising Enquiries
Glyn Smith
Phone (02) 9939 3295
Mobile 0431 792 293
glyn<at>siliconchip.com.au
Regular Contributors
Brendan Akhurst
David Maddison B.App.Sc. (Hons 1),
PhD, Grad.Dip.Entr.Innov.
Kevin Poulter
Dave Thompson
SILICON CHIP is published 12 times
a year by Silicon Chip Publications
Pty Ltd. ACN 003 205 490. ABN 49
003 205 490. All material is copyright ©. No part of this publication
may be reproduced without the written consent of the publisher.
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Subscription rates: $105.00 per year
in Australia. For overseas rates, see
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in this issue.
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Postal address: PO Box 139,
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Phone (02) 9939 3295.
Fax (02) 9939 2648.
E-mail: silicon<at>siliconchip.com.au
ISSN 1030-2662
Recommended and maximum price only.
2 Silicon Chip
Publisher’s Letter
We live in a time of plenty and
we should all be optimistic
Do you get sick of all the bad news on the media? Every day there seems to be another dire story about things
getting worse: more pollution, more floods, more fires,
deaths, more noise, more disease, scarcer resources,
energy becoming more expensive – the list goes on
and on. And yet for the vast majority of people, life is
not getting worse, life is getting better; profoundly so.
Consider, for example, the increasing cost of energy
and in particular, the burden that air-conditioners place on our electricity grid.
For me, that burden is not bad; that is good. Fifty or sixty years ago in Australia
virtually no households had air-conditioning; not even the richest people had
it. The same applied to most office buildings. So in summer we all sweltered
and many older people died of heat stress. In winter, we shivered and older
people were more likely to die of cold or succumb to influenza.
But now, most households can afford air-conditioning and unless people are
living in areas where they get cooling sea breezes in summer, they elect to have
it. And nor do they necessarily moan about the resulting electricity bills. You
want the comfort? That’s what it costs! Really, the only argument is whether
the electricity tariffs should be as high as they are. I would argue that they are
artificially high, partly because of subsidies for renewable energy. But by and
large, most people are significantly more comfortable, happier and probably
live longer because of air-conditioning. It is a blessing.
And what about air and water pollution, soil degradation, desertification
and so on? Again, it is pretty easy to gain the impression that everything is
getting worse. Well, in the cities of most developed countries of the world, air
and water pollution is demonstrably better than it was in past decades. Similar
comments apply to soil degradation. Better farming techniques in the advanced
countries are slowing the process of soil degradation and as living stands rise
in the developing countries, you can see the process of improvement again,
with China being a prime example.
And think about the range of entertainment that we now have. Fifty years
ago in Australia, we did have black and white television in the cities but many
households did not have it. Nor did most households have hifi systems. Indeed,
many homes did not even have a telephone. Microwave ovens, dishwashers,
automatic washing machines, clothes dryers – what were they? Computers,
smart phones? – science fiction! And what about developments in medicine
with heart, lung, kidney and even liver transplants, hip and knee replacements
and so on? Now look at us! The march of technology has brought unimaginable improvements to virtually every aspect of our lives – at least they were
unimaginable fifty or more years ago.
So why is the news so dire? Why are some people so worried about resources
getting scarcer or climate change? As far as natural resources are concerned,
I cannot think of one that is becoming scarcer. Sure, fish stocks have been
badly depleted in parts of the world but I have no doubt that, with the move
to large-scale fish farming, even that may be reversed in the future. After all,
look at the rising whale numbers around the world.
Which finally brings me to climate change. Why are we so worried? In the
past, human ingenuity has adapted to much more adverse conditions and man
has thrived. I have no doubt that the wonders of technology over the next fifty
years will again bring unimaginable improvements to our lives. We couldn’t
imagine them in the past and we cannot necessarily imagine future improvements right now, can we? Be optimistic; I certainly am.
Leo Simpson
siliconchip.com.au
DISCOVER MORE
siliconchip.com.au
April 2015 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”.
Help required for
kite record attempt
My world altitude record was included in “Reach For The Sky” in the
February 2015 issue; excellent article
by the way! I am by no means an
electronics expert and have a basic understanding of radio, GPS and telemetry. In 2006 I purchased a GPSFlight
telemetry system from the USA. This
includes on-board 900MHz spread
spectrum Maxstream radios coupled
to a u-blox GPS receiver. The ground
transceiver is a Maxstream connected
to a PC Win 7 laptop via USB.
The flight module was troublesome
for a couple of years, with two replacement units, however the original interface board had auxiliary pins for a
barometric altitude module (BAM) and
a temperature module. Unfortunately,
these units were lost in return mail
to the USA. My current board has six
spare pins and I am assuming these are
for those auxiliary modules.
GPSFlight suffered in the GFC and
has closed. The last units available
about three years ago had the optional
modules listed. I am hopeful of finding
temperature and barometric modules
that may work but the temperature is
most important as we plan on flying
a train of big kites to over 40,000 feet.
The software that interfaces with
the telemetry is called GPSFlight
Dashboard (the free version) and GPS
Team, the fully featured version. Both
these have barometric and temperature
on their displays. These spare pins
show about 3V. I was hoping that
suitable modules would be available
and work on my boards. I have seen
various small OEM modules but I have
no idea how they would interface with
the board or the software.
I have found images of the 2003
GPSFlight interface board as well as
the optional Baro sensor PCB, although
the latter is quite blurred. It has six
pins on one side and three on the other.
I’m looking for a pin assignment dia-
gram but it’s difficult as the company
shut three years ago.
The 2006 version is fairly close to
this design but has another row of three
pins in the middle of the interface
board. I don’t know what goes on the
2-pin auxiliary. I was hoping that your
team or readers may have some ideas.
Bob Moore,
Baulkam Hills, NSW.
Teething problems with
the $5 Wifi Server
I had some trouble setting up the $5
WiFi server described in the December
2014 issue and the following tips may
help others. The connection diagram
of Fig.4 on page 32 contains an error.
The Micromite COM1: TRANSMIT is
shown as pin 23 but is actually pin 21.
The Terminal Program listed on
page 35 opens COM1 at 115,200 baud
whereas the ESP8266 modules I purchased (vendor: www.ai-thinker.com/
Version:0.9.2.4) communicate at 9600
baud.
It is essential that the AT commands
sent to the ESP8266 are terminated
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siliconchip.com.au
siliconchip.com.au
April 2015 5
Mailbag: continued
Helping to put you in Control
IP67 Car Detection Sensor
The MB8450 car detection
sensor is a high performance,
low-cost USB ultrasonic proximity sensor that detects the
side of a vehicle. Great for
drive thru’s & where you need
to detect a car. It features serial output,
USB powered, it senses up to 5 m.
SKU: MXS-151
Price: $119.95 ea + GST
DC-DC Converter
DIN Rail isolated DC-DC converter accepts 9 to 36 VDC input &
gives a regulated 24 VDC output
<at> 0.25 A. It features status
LEDs, indefinite short-circuit protection and CE & RoHS marked.
SKU: NTP-010
Price: $89.95 ea + GST
Ratchet Crimping Tool Kit
Includes 5 popular die sets
which can easily be swapped
using the Allen key included
in the kit. The kit is housed in
a rugged easy to carry plastic
box.
SKU: HET-020
Price:$39.95 ea + GST
60W LED Lighting Transformer
Ultra compact electronic
lighting transformer is
suitable for halogen & LED
lightig installations. Screw
terminals for input & output.
60W, 1.8 m mains lead.
SKU: PSA-001
Price:$11.95 +GST
Photoelectric Detector
This through-beam photoelectric sensor can be used
to detect presence of an
intruder by using an infrared
transmitter & photo-electric
receiver. 12 to 24 VAC/DC
powered with detection distance up to 12
m. It features alarm output with NC & NO
contact.
SKU: HIS-002
Price: $48.53 ea + GST
TECO PLC
The SG2-12HR-D features 12 x
I/O points which can be expandable up to 34 x I/O points.
There’s a built-in 4x16 character
LCD & keyboard for operator
feedback & control. 20.4 to 28.8
VDC powered.
SKU: TEC-005
Price: $149.95 ea + GST
12 VDC Relay Card
Eight channel, 12 VDC powered, relay card with wide
range of input configurations.
Each relay can be activated
via HI or LO input voltage
via its screw terminals. Each
channel has an indicator LED. The relay is
rated to 7 A <at> 240 VAC or 10 A <at> 28 VDC.
SKU: RLC-128
Price: $85 ea + GST
For OEM/Wholesale prices
Contact Ocean Controls
Ph: (03) 9782 5882
oceancontrols.com.au
6 Silicon Chip
Errors in Spark
Energy article
I noticed the following errors in
the February 2015 issue of SILICON
CHIP.
(1) On page 48, in the righthand column in the section “Estimating Spark
Energy”, there is a sentence which
says “So for this example a -30mA
peak spark current has an average
spark current of about 15mA over a
2ms interval. The charge transferred
across a 1000V load (the spark) is
about 30mQ (millicoulombs) resulting in about 30mJ (millijoules) per
spark.”
The error is in the amount of
charge. 30mA for 2ms is 60μC (microcoulombs) not millicoulombs.
However, the maths is correct in the
following paragraph.
(2) Page 62 in the section titled “Calibrator circuit”” reference is made in
the test to “. . . with a repetitive 2ms
-5V pulse across the 150W 5W resistor.”. It should of course read 150Ω
5W resistor.
(3) Page 59 bottom right corner: the
text says “The inverting input, pin
3, normally sits . . .”. The inverting
input is pin 2 not pin 3.
I also wish to say that I thoroughly
enjoy Leo Simpson’s editorials. I
don’t always agree with them but I
always find that they give me food for
thought. I enjoy reading his thoughts
on the wide variety of subjects he
covers. Keep it up, please.
David Williams,
Hornsby, NSW.
Comment: these errors have now
been fixed in the online edition.
with CR+LF. My installation of Tera
Term defaults to Newline=CR. This
must be changed to Newline=CR+LF
for transmit in Setup->Terminal.
Greg Donnan,
Anakie, Vic.
itself up to begin scheduled recording. Ah – the wonders of technology!
Ian Thompson,
Duncraig, WA.
Mains Moderator saves power
& protects appliances
I used the Deluxe GPS 1PPS
Timebase (SILICON CHIP, April 2013)
project to provide the interface for a
Trimble Resolution-T GPS module.
This module runs off 3.3V, however
as its output signal HIGH level is only
about 2.85V, it is not compatible with
the 40106B specified for IC1 which
has a higher input threshold.
Substituting a 74HCT14 which has
a lower threshold but still shares the
same pin-outs fixed this issue. This
may be of interest to others contemplating the use of 3.3V modules.
The Trimble module has a particularly stable 1PPS output with
standard deviation jitter of less than
12ns and this makes it a good choice
for feeding a frequency counter or a
disciplined oscillator. Used modules
sell for about US$25 on eBay (my unit
had a build date of March 2013 and
looked near new). Trimble provides
excellent monitoring software which
is freely available – see www.trimble.
com/timing/resolution-smt-GG.aspx
and click on VTS software.
Our line voltage here in Perth sits
very close to 250VAC RMS, so I decided to build the Mains Moderator
from the March 2011 issue. I also fitted
the Soft Starter from the April 2012 issue down stream and a wireless GPO
controller up stream, to power our
LCD TV plus separate amplifier and
DVD player.
I used the Appliance Energy Meter
(SILICON CHIP, July & August 2004) to
measure the power with and without
the Mains Moderator and found a saving of 30W. This saving is all the time
the TV is on. Of course, I expect the
inverter life to be improved, as well.
Luckily, the TV memorises its status
and channel, so when it is switched
on with the remote power switch, up
it comes and with no “bang” as all
the capacitors in the TV and amplifier
charge up softly. On switch off, the
standby power is a little less than 2W.
The PVR is permanently powered from
a separate GPO, as it needs to wake
Deluxe GPS 1PPS Timebase
interface adaptation
siliconchip.com.au
To make full use of the many software features, forward control of the
module is required. I used a simple
NPN transistor circuit with a 10kΩ
base resistor and the collector connected to the module’s Rx input, with
the pull-up resistor reduced from 10kΩ
to 1kΩ. The base resistor then connects
to pin 3 of the DB9F serial connector.
As negative voltages can be present
on pin 3 of the connector, I placed a
protection diode between the base and
emitter of the transistor.
Software features include a Google
Earth view position map, satellite
almanac and ephemeris data. The default data protocol is proprietary TPIS
although the modules can be switched
to NEMA. The module does require an
external active antenna with an SMB
female connector (US$7 on eBay).
The module draws about 110mA
plus about another 10mA or so for the
antenna. Hence a 1A LM3940 or similar regulator must be used for REG1
and the output capacitor increased
from 10µF to 33µF.
Trevor Woods,
Albany, NZ.
Impact driver operation is more
complex than may be thought
The dynamics of impact drivers are
not as simple as some might have us
believe. Alan Torrens’ explanation on
page 6 of the March 2015 issue is essentially correct. However, the dynamics
are not that simple. For example, the
force (torque) on the nut or bolt is far
from constant and so in using the equation which expresses the Conservation
of Momentum what is the torque on
the nut or bolt?
Certainly, the torque exerted by the
wrist on the wrench can reasonably be
taken as a constant. In the case where
the wrench makes good progress with
each impact and the nut or bolt rotates
quite a bit with each impact then using
the Conservation of Momentum equations will give a good approximation.
But the maximum torque rating of the
device as quoted in the January question will not work with this equation.
A more complete explanation is as
follows. In the first instance, one needs
to focus on the fact there are three free
bodies involved: (1) the body of the
driver including the handler’s hand, (2)
the hammer inside the device and (3)
the anvil which is struck by the hammer and which is connected in some
way to whatever is being tightened.
The dynamics of an impact between
two otherwise free bodies needs to
be precisely stated. When two bodies
strike one another, the forces, which
each exerts on the other, are equal and
opposite. However, it is very important
to realise that in the case of an impact,
the magnitude of the forces referred to
here are rapidly changing with time. At
any instant in time, the force that the
first body exerts on the second body
is equal in magnitude and opposite in
direction to the force that the second
body exerts on the first body, so called
“equal and opposite”, but that the
magnitude of that force, is in general,
rapidly changing.
It is misleading and wrong to refer
to them as having a magnitude F. “F”
is not a constant but must be defined
as F(t), a time dependent quantity. In
some simplified configurations, the
magnitude of the forces resembles a
sinewave; certainly never a constant F.
The device repeats a process which
can be divided into three stages: (1)
time t1, when the hammer is accelerated towards the anvil; (2) time t2,
during which the hammer strikes the
anvil (the first time, t1, might be 100
or more times longer than time t2);
and (3) time t3, when the accelerated
anvil exerts a force on the nut or bolt
via the relatively elastic connections
involving the socket etc.
During period t1, when the free body,
which is the body of the device and
handler’s hand, exerts a force on the
hammer, which is inside the device,
the magnitude of that force might
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April 2015 7
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Mailbag: continued
8 Silicon Chip
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reasonably be taken as a constant,
say F1.
During period t2, the free body,
which is the hammer, exerts a force
on the free body which is the anvil,
the dynamics of which are relatively
complicated. The interaction depends
on the shape and elasticity of the anvil
and hammer. If the two bodies were in
fact two rigid bodies and they met each
other at the ends of an elastic spring,
then the motions would be described
as a sinewave starting at zero angle at
first impact and ending when the angle
is equal to PIE when they separate: half
a sinewave.
Note that there is no single value
involved. However, an impact wrench
is most effective if the impact is as
short as possible and it is desirable to
eliminate as far as possible any spring
between the hammer and the anvil.
What happens can best be visualised
by thinking of two jellies hitting one
another. All sorts of vibrations are set
up. These can be calculated and are
the Eigen Functions but suffice it is say
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that t2 is very much shorter than t1.
During period t3, measured also
from the start of the impact, the free
body which is the anvil winds up the
shaft connecting the anvil to the nut
or bolt. It is desirable for this connection to be as rigid as possible. During
t3, the torque in the connecting shaft
between the anvil and the nut or bolt
can reasonably be described as a portion of a sinewave up to the moment
when the torque exceeds the friction in
the threads etc, when the torque will
remain relatively constant during the
time when sliding occurs. The time t3
is longer than t2 but shorter than t1.
The softer the connection between the
anvil and the socket the less effective
the impact wrench.
A non-critical observer might note
that because there is a small torque
exerted by the wrist for a long period
of time and a large torque exerted on
the nut or bolt for a short period of
time, then these numbers seem as if
they might fit into the equation stating the Conservation of Momentum.
www.virtins.com
But the mechanics and dynamics are
more complicated than this equation
describes. One needs to note what the
equation expressing the Conservation
of Momentum purports to describe.
As stated above, when the wrench
is making good progress tightening
something, working well under its
rated capacity, then for that situation
alone, where the torque on the nut or
bolt is constant at the sliding friction
level for the time while the nut is
moving, and because the wrist torque
is also reasonably constant, then the
equation expressing the Conservation
of Momentum can be used correctly.
But for the situation where the
wrench is developing its highest torque
the torque on the nut or bolt will have
a sinewave shape and the equation expressing the Conservation of Momentum does not apply. Maximum torque
is highly dependent on the elasticity
of the connection to the socket. Any
extension shaft will greatly diminish the magnitude of the maximum
tightening torque, as expressed in the
January 2015 question on page 101.
Dr Kenneth E. Moxham,
Urrbrae, SA.
siliconchip.com.au
Recycling a cordless drill
I was interested in the letter from B. D., of Hope Valley SA in the “Ask SILICON CHIP” pages of the February
2015 edition and it has prompted me to record my own
experience in this regard. I retrieved a cordless drill from
a rubbish dump because apart from the fact that there was
no battery in it, it appeared to be in reasonable condition.
Also it was a Bosch brand and made in Switzerland.
The voltage rating was 14.4V, the same as a LiPo battery
I had bought having read the article in SILICON CHIP about
these batteries. I wired the battery to the drill using Anderson Powerpole connectors and was pleasantly surprised
by the performance which was excellent – plenty of power
and with the 4Ah battery, it goes for ages. The battery is
attached to the base of the drill with cable ties and as the
DC connectors are accessible, the battery can be recharged
easily. It’s new life for a good old drill.
Keith Gooley,
One Tree Hill, SA.
Wireless audio repeater for PA system
I recently had occasion to build a PA system for my
club. One consideration I wanted was to feed the signal
to the rear of the room wirelessly. The distance was about
15 metres and running cables to rear speakers was really
not acceptable.
I spent a great deal of time and effort on systems like
Bluetooth – unacceptable latency – FM transmitters and
hours on the internet looking for suitable systems. In the
end I hit on the idea of modifying a wireless microphone
and it works really well. I just thought I’d pass it on to you
and your readers should it be of interest.
Briefly, I used one of the dual BNK B701 microphones
at $50 plus shipping off eBay (also used for the club’s two
wireless microphones). The board was removed from the
microphone and a 3.5mm mono socket was substituted
for the microphone. There was a 47kΩ resistor in series
with the compander input so I raised that to 470kΩ and
replaced the washer shaped antenna with a telescopic
version. As the regulations only specify input power into
the antenna it is still legal.
It was installed into a plastic box from Jaycar with a front
LED replacing the internal microphone LED, an ON/OFF
switch and a 9V battery compartment with external access.
It transmits from the front amplifier to the BK701 receiver, then to a $25.00 Lepai 2020A+ amplifier and then
two stereo speakers, one each side at the rear of the room.
I used a 15-metre 250VAC extension lead from Bunnings
with the plug and socket cut off and a 0.25-inch mono
plug to connect the second speaker.
I used an ALDI Livingston FA-30 I had lying around
at the front which as well as the repeater also drives (by
cable) a second Lepai 2020A+ which in turn drives two
Pioneer car speakers in pods mounted one above the other,
which I also had lying around.
I did find that the with the Lepais mounted on the side of
the speakers, vibration caused the volume control to alter.
I moved them and I have also successfully replaced one
volume pot with a $15 20kΩ linear stepped attenuator from
ROLEC OKW
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April 2015 9
Mailbag: continued
LED lighting can
cause interference
LED lighting is very popular as it
is efficient and the LEDs last a long
time. I used to work in the predecessor to the ACMA as an interference
investigator, hence I still get asked
by people about the causes and cures
of severe interference to television
and radio reception that they may
be experiencing. LEDs themselves
do not cause interference but the
power supplies to change the input
supply voltage to that needed for the
LEDs in many instances do.
I would suggest that current and
eBay. At 220-230MHz, these wireless
microphone transmitters go through
walls very nicely – at least they did for
me. I also tried converting a GT-TECH
GT-02 wireless microphone but the
quality is not so good.
Josh Stevenson.
Moe, Vic.
Improvements to Poor Man’s
High-Voltage Probe
With respect to my high-voltage
probe circuit, as featured on page 84 of
the March 2015 issue, I found that in
practice it was better to make the 4.7pF
capacitor a 10pF variable type. This
allowed me to adjust rise time for both
potential users of LED lighting make
sure that the lights do not cause interference. They should have a compliance sticker on them to indicate
that all relevant EMC/EMI standards
are met. However, I have found items
with compliance stickers on them
have created considerable interference (compliance labels are quite
cheap!). Many of the interfering LED
lights are sourced cheaply over the
internet. I have made sure that all
my LED lighting does not cause any
interference.
Rodney Champness,
Mooroopna, Vic.
(+) and (-) inputs independently to get
optimum “no overshoot” rise times for
each input. The nett effect was to get
a very clean rise time for both singleended and common mode responses
and optimised high frequency CMRR
(common mode rejection ratio).
In future, I may modify my unit to
use ±15V external supplies, to allow
±1200V signals to be monitored. I
have used it successfully to monitor
voltages in a 240VAC CFL light power
supply. The 1mV p-p output noise limits measurement to >100mV p-p at the
input but adding a 100kHz low pass filter (10kΩ/150pF) to the output allows
high-frequency noise to be suppressed
so you can make measurements above
20mV p-p referred to the input.
If you are interested in <10kHz responses then the output filter could
be reduced to 10kHz (10kΩ/1500pF).
Peter Kay,
Dromana, Vic.
Suggestion for a CAN bus
watchdog project
I have an automotive EFI engine
that I would like to have monitored
by a watchdog device, ie, an alarm/
relay would operate when a monitored
engine parameter is operating outside
of a pre-programmed window (eg,
coolant temperature or oil pressure).
This is particularly useful for engine
protection.
A project such as this would suit
people who do not want to or can’t be
looking at their engine instruments
regularly. It would especially suit
engines that are fitted to vehicles that
don’t include an OEM CAN bus style
instrument cluster, such as boats, race
cars, kit cars, engine upgrades.
In particular, I have a requirement
for an MIL (malfunction indicator
light) for registration purposes. I have
a kit car with a Ford Coyote engine installed. In its native application (Ford
Mustang), the MIL light is part of the
instrument cluster which receives its
status via the CAN bus. As this instrument cluster is not used in my car, there
is no simple way of driving a MIL. This
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April 2015 11
Mailbag: continued
How to determine transformer
winding voltages
I have just read Nicholas Vinen’s article in Serviceman’s Log pages of the February 2015 issue and I want
to comment on his derivation of winding voltages. In
the case of the input winding being open circuit and
a good guess at the voltage of one of the secondary
windings, the easier way is to feed a mains frequency
voltage of say half the nominal voltage into the known
winding and then measure the voltage on the remaining winding(s).
The ratio of these voltages will give the no-load
voltage of the unknown winding. Also, if none of the
winding voltages are known and a Variac is available,
an estimate of the voltage can be obtained by monitoring the input current (the magnetising current) while
increasing the voltage. The current will rise quite
quickly just after the nominal voltage is reached due
to magnetic saturation.
Sometimes it is possible to gain access to the thermal fuse and short it out. Of course, this removes the
protection but it is no worse than the solution adopted
in the article.
Charles Borger,
Croydon, Vic.
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is a very common problem for people installing modern
engines into vehicles with custom instrumentation.
I thought I would mention this idea for a project as I
have not been able to find anything commercially available
other than industrial engine controllers for generator sets
and marine diesels. There are certainly plenty of people in
the kit car, hot rod and race scenes that would make good
use of such a project.
As said by many others before me, thank you for an
excellent magazine, with a great technical balance.
Nigel Allen,
Magill, SA.
NBN connection at last
I finally bit the bullet and had the NBN connected. I went
with TPG because they offered far and away the best deal
($79.95 per month with unlimited just about everything).
I cannot fault their service; everything went very smoothly and it all just works. Pulse dialling is not supported but
everything else (fax, answering machine etc) works seamlessly. I can talk on my old phone and pick up calls with
it but I have to dial out with a different phone.
Ironically, I picked up the very first call that came in with
my 60-year-old phone and it was a man with a very strong
Indian accent trying to tell me he was from Microsoft and
that my computer has a virus in it!
The only minor snag was that even though Telstra had
disconnected my service and ported my number to TPG,
the phone line was still connected to something, so when
I plugged a phone cable into the NBN box and plugged the
other end into a phone point, I just got a horrible growling
siliconchip.com.au
noise. Anyway, I just snipped the wires where they enter
my garage and that was that.
Which brings up an interesting point: since my internal
phone wiring is now only connected to the outside world
by a fibre-optic cable, I should be able to connect anything
I like and modify the wiring any way I like.
Keith Walters,
Riverstone, NSW.
Climate change
& technology
With regard to the Publisher’s Letter in the February 2015
issue, I don’t fully agree with your policy that peripheral
electrical/electronic subjects should be covered in SILICON
CHIP magazine. I don’t buy it for that.
One aspect of Climate Change (about which I’m happy
to be called a sceptic) that has an electronic/engineering
dimension is how the temperature of the Earth (absolutely
or relatively) can be meaningfully defined – to within a few
degrees, let alone tenths or hundredths of degrees.
The definition has to include the atmosphere somehow
or other I would think, not just the surface. And whether
one averages daily maximum and minimum for a daily
figure – and why. And how to average say seaside/sea-level
Sydney with inland/altitude Canberra?
Assuming a definition can be agreed somehow, how
can meaningful measurements be made to within tenths
or hundredths of degrees, even at ground level, let alone
altitude? And assuming all the above can be done, how can
today’s measurements be melded with historical numbers?
And finally, why are solutions to possible future problems only looked at in the context of today’s technologies?
SILICON CHIP readers, especially the older ones, have seen
enormous technological changes contributing to improved
quality of life for many if not most.
Surely it is at least equally appropriate to be optimistic,
rather than pessimistic, about the future ingenuity of the
human race in mitigating any problems, and coming up
with brand new solutions and initiatives. This seems far
more likely to me, as a retired engineer, compared with
any problems which might flow from unlikely, small temperature rises in some places.
Mike Dinn,
Canberra, ACT.
Time domain reflectometry on the railways
With respect to the articles on Time Domain Reflectometry
in the November & December 2014 issues and a subsequent
letter in the Mailbag pages, you may find this of interest.
Many years ago I was told that VicRail used a TDR to
find the location where a train overhead power line had
come down. From memory this is how it worked: I was
told that they had an overlay that they would put over the
TDR screen. The overlay showed what the trace should
look like if the power line was OK. The point where the
measured TDR trace was different would show where the
power line was down.
Also marked on the overlay were the locations of road
crossings and buildings. The point where the traces were
different with reference to road crossings etc indicated
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April 2015 13
Mailbag: continued
where to look and fix the overhead
power line – an interesting application where reflections are normally
there when the line is OK. The fault
location is where the reflection is not
as expected.
It would be interesting to know if
they still use this method today.
Roderick Wall,
Dandenong, Vic.
Vintage radios should
be kept original
In recent years we have come to
realise that not all old equipment be
it cars, motorcycles, trucks, military
weapons and radio sets should be
fully “restored” to what the restorer
imagines to be new condition.
To illustrate, I recently visited the
Portland Power Museum and among
their beautifully restored motorcycles
is an ancient machine in poor condi-
tion with side car that proudly boasts
the sign, “Do not clean me – I am meant
to look like this”. The machine is the
classic “barn find” and is original in
every way, including the patina caused
by years of use and abuse. Interestingly,
this exhibit drew much favourable
comment from visitors.
Don’t get me wrong – there is a place
for restoration but just as importantly,
we should sometimes conserve items
that come our way so that future generations can see the originals without
our early 21st century makeover. And
that is why I was horrified when reading the Vintage Radio pages in the
March 2015 edition which described
the “restoration” of a Tela-Verta 1948
Musiclock Model 204C Mantel Radio.
The source of my horror was the caption: “Left: the clock mechanism (to the
left of the tuning gang) was in a poor
state and was replaced by a modern
quartz clock movement”.
Instantly the value of the restored
radio in a historical sense has been
destroyed. Also, I venture that the
value to astute vintage radio collectors
would be far less than if the inoperable
clock was left in the radio. If the clock
has to run, I venture that most electronics enthusiasts can run a lathe or mill
to make replacement parts. After all,
these machine tools are far easier to
use than a modern oscilloscope.
So, may I recommend to those bent
on restoring old electronic equipment
that they consider the conservation
approach occasionally. Leave the
marks and dings in the cabinet and the
yellowed dials – these are the ghosts
of our grandparents sitting in smoky
lounge rooms listening to John Curtin
say those famous words: “Every Australian should consider himself at the
service of the government – whether
he likes it or not”.
Gerard Dean,
SC
Glen Iris, Vic.
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April 2015 15
Helping to keep the skies safe . . .
by
Dr David Maddison
Airborne Weather Radar
Airborne Weather Radar enables flight routing to avoid extreme weather
in order to keep passengers and crew safe and more comfortable – and
to avoid damage to the aircraft. Huge advances have been made in this
technology in recent years, including Rockwell Collins new “MultiScan”
ThreatTrack Radar, released only last year at the Singapore Airshow.
D
espite the fact that flying is the safest way to travel,
the year 2014 was perceived by many as a bad year
for aviation – although that really depends upon
how you analyse the statistics.
According to the Geneva-based Bureau of Aircraft Accidents Archives (BAAA) there were 111 aircraft accidents
in 2014, the lowest number of accidents since 1927. The
BAAA counts any aircraft crash in which the aircraft is
certified for at least six people plus the crew. It also counts
shoot-downs but does not count military aircraft except
troop carriers and other aircraft that can carry more than
six passengers.
Deaths are a different matter, however and 2014 saw
1,328 people die in aircraft crashes and shoot-downs, the
most since 2005, according to BAAA statistical methods.
Cause
1950s 1960s 1970s 1980s
Pilot Error
42
36
25
29
Pilot Error weather related
10
18
14
16
Pilot Error mechanical related 6
9
5
2
Total Pilot Error
58
63
44
57
Other Human Error
3
8
9
5
Weather
16
9
14
14
Mechanical Failure
21
19
20
21
Sabotage
3
5
11
12
Other Cause
0
2
2
1
1990s 2000s Average
29
21
5
55
8
8
18
10
1
34
18
5
57
6
6
22
9
0
32
16
5
53
6
12
20
8
1
Fatal accident causes for commercial aircraft with 19 or
more passengers on board from 1950 to 2010. Over that
period weather-related fatalities, both involving and not
involving weather-related pilot error have been a factor in
28% of accidents. (www.planecrashinfo.com/cause.htm).
16 Silicon Chip
However, according to the Aviation Safety Network (which
counts only civilian planes which are certified for 14 passengers or more and does not count corporate jets, shootdowns or sabotage) in 2014 there were 692 people killed in
aircraft incidents making it the safest year since 1945. This
would obviously exclude the 298 killed when Malaysian
Airlines flight MH17 was shot down over the Ukraine.
According to the BAAA there were 163 weather-related
fatalities in 2014 and 162 of those were on Air Asia flight
QZ8501 that crashed into the Java Sea off Indonesia. The aircraft was an Airbus 320-200. Historically, weather-related
aircraft fatalities due to crashes are a factor in 28% of cases.
Avoiding weather of sufficient severity to put an aircraft
Adverse weather effect on an aircraft: a lightning strike.
siliconchip.com.au
World’s first airborne weather radar – the ECKO airborne
“cloud and collision warning search radar” from 1950.
at risk is of particular importance. Planning to avoid potentially dangerous weather starts at the flight planning stage
but after take-off weather continues to be monitored both
from reports radioed to the aircraft and on-board weather
monitoring systems, the most important of which are the
pilot’s Mark I eyeballs!
Some aircraft operating in some areas also transmit
weather data to meteorological authorities where it is fed
into weather models to supplement data from weather
balloons and other sensors.
Apart from the possibility of severe weather causing fatal
aircraft crashes, a much more common occurrence is injury
to passengers and damage to aircraft caused by turbulence.
In order to assist aircraft operators avoid bad weather
once in flight they use aircraft mounted weather radar
systems (radar is an acronym for RAdio Detection And
Ranging).
Airborne weather radar detects bad weather in the
aircraft’s flight path and allows the pilot(s) to avoid the
worst of it.
Another primary purpose of airborne weather radar is
to ensure that course deviations to avoid bad weather are
kept to the minimum that is necessary to avoid the adverse
weather, without adding excessively to the distance to be
flown which increases the time taken and adds to operating costs.
A problem?
The ability for radar to detect weather conditions was first
noted during World War II where it was seen as a problem
as radar returns from certain weather systems containing
rain, snow and sleet could mask enemy activity. Ways were
then developed to filter out such undesirable returns but
scientists and engineers started studying the phenomenon
after the war as a means to monitor weather and it has been
extensively developed ever since.
The first airborne weather radar was from the UK company ECKO who, in 1950, developed the “cloud and collision warning search radar”.
In later developments in 1953 a researcher with the Illinois State Water Survey produced the first radar image of
a “hook echo”, a particular type of weather radar signature
associated with tornadoes. This demonstrated the viability
of using radar to detect severe weather conditions and even
siliconchip.com.au
The first weather radar image of a “hook echo” which is
associated with tornadoes, taken in 1953.
provide early warning of developing severe conditions.
Early ground-based and airborne weather radars provided
information on the reflectivity of whatever targets they illuminated but could give no information on the speed, of
say, water droplets in a storm which would be indicative
of wind speed.
Initial research on weather radar systems focused on
observations of the precipitation within a weather system
and its development, movement and structure, as well as
making observations of the relationship between the characteristics of the radar echo and precipitation rate. When
there was a greater precipitation rate there were more water
droplets for the radar beam to reflect from and therefore
the radar return was greater.
Doppler radar for weather
In 1950s research began on Doppler radar for weather
applications although the earliest Doppler radar systems
were developed during World War II.
The Doppler effect is the familiar property of a moving
noise source such as a siren changing in frequency as it
approaches an observer and then moves away. The same
phenomenon applies to radar signals whose return echo is
influenced by the velocity of the target they are bouncing
off, such as rain drops.
Early Doppler radars used large and sensitive analog
filters and were not practical for airborne operation except
under special circumstances. It required the development
Feet, Nautical Miles & Flight Levels
While Australia (and indeed most countries) have
adopted the metric system, in aviation Imperial units are
still used: heights are generally expressed in feet, distances
in nautical miles and speed in knots (which is of course
nautical miles per hour).
You may also come across the term “flight level” with
values between zero and perhaps 500. While a flight level
strictly speaking is a barometric pressure (based on an international standard air pressure at sea level), it is conveniently used to express a height above sea level expressed
in thousands of feet. Therefore an aircraft said to be flying
at flight level 360 means it is 36,000 feet above sea level.
April 2015 17
VISUAL TOP
RADAR TOP
A primary threat to en-route weather
avoidance is the fact that thunderstorm cell
tops are non-reflective because they contain
ice – a poor radar reflector.
of fast computers and digital signal processing in the 1970s
and the development of digital Doppler radar to enable
useful and easy to visualise weather information to be interpreted from such Doppler shifts in the return radar echoes.
As an aside, it is interesting to note that an unexpected
Representative values of radar reflectivity as a function of
height for equatorial oceanic and continental geographical
areas and mid-latitude areas. For a given cruise altitude
of 35,000 feet note the very large variation of reflectivity
between the equatorial oceanic (black vertical bar) regions
and the mid-latitude continental (yellow vertical bar)
regions, corresponding to almost a 20dB range or 100
times power ratio. Note also the dramatic loss of radar
reflectivity above the typical altitude for freezing of water
at 16,000 feet. dBZ is a a logarithmic measure used for
radar systems representing the radar echo intensity.
(Diagram courtesy Rockwell Collins.)
18 Silicon Chip
problem during the development of early radar systems
was that the Doppler shift induced by the reflection of a
radar pulse from a fast moving object effected a phase shift
in the returning signal, causing the signal to be cancelled
and thus reverse phase-shift compensation had to be built
into the radar set.
The development of Doppler radar enabled not only the
shape and location of a weather pattern to be determined
but also the velocity of precipitation within that weather
pattern, and by inference, wind speed. Doppler radar also
allows the elimination of returns travelling at a particular
velocity. For example, with airborne radar, ground returns
can be eliminated.
Airborne weather radar can be classified as either the
more conventional and familiar two dimensional radar,
or the more recently developed three dimensional radar.
It might also come as a surprise to some that modern commercial aircraft do not have general purpose radars that
indicate the presence of other aircraft or terrain. Avoidance
of these is effected by pilot observation, flight planning,
transponders on aircraft and automated aircraft systems.
What you see is not what you get!
Monitoring weather systems with radar might seem
straightforward but there are many complicating factors.
For a start, what is visible to the naked eye may not be visible to radar. For example, the cloud tops of thunderstorms
contain mainly ice and that is a very poor radar reflector.
Typically, above 16,000 feet the temperature will be
below zero centigrade and so water will be in the frozen
state. The cloud top will be visible to the naked eye but
not to the radar, or there will be very poor radar visibility
so the flight crew have to correlate in their mind what
they see with their eyes and how that relates to the radar
information being received.
As a general rule, the lower two thirds of a cloud are visible to radar and the top one third is invisible, due to the
presence of non-radar-reflective ice crystals. Of course, even
though the cloud top may be invisible to radar it does not
mean it is not of concern and there can be turbulence within
that area of the cloud which can affect flight operations.
The presence of certain weather patterns that are visible
to the radar below 16,000 feet can be used to infer that there
will be certain formations above them and what their properties may be. This important point will be discussed later.
By convention, a display for weather radar is coded by
three different colours according to precipitation activity.
Green or Level 1 refers to light precipitation activity, little
or no visibility and possible reduced turbulence; yellow
or Level 2 corresponds to moderate precipitation, very low
visibility, moderate turbulence and passenger discomfort;
while red or Level 3 refers to heavy precipitation, possible
thunderstorms, severe turbulence and the possibility of
aircraft damage. Black corresponds to no return. A typical
cloud will have heaviest precipitation at the bottom, with
less higher up in the cloud.
It should be noted that the radar reflectivity varies enormously for different types of weather and is dependent on
several factors. Mid-latitude continental thunderstorms
have a much greater radar reflectivity than, say, equatorial
oceanic thunderstorm clouds. This has lead to problems in
the past as a weather radar might be optimised for typical
weather conditions in, say, the United States where it is
siliconchip.com.au
manufactured and where most of its planes fly (mid-latitude
continental area) but it would not work so well for an
Australian operator in areas where many of its planes fly
(equatorial oceanic). In fact the variation in radar return
from these two types of conditions may vary by a factor of
20dB or 100 times (see graph).
Some examples of the different radar characteristics of
thunderstorms are as follows: continental land-based thunderstorms (eg, USA) typically have high moisture content at
high altitude and are more radar reflective than other types.
Oceanic thunderstorms (eg, Bay of Bengal) have low radar reflectivity as their moisture is located at low altitudes
and the cloud tops are invisible to radar. Mid-latitude land
based thunderstorms (eg, Brazil) have an intermediate
radar reflectivity between that of continental land-based
thunderstorms and oceanic thunderstorms.
In addition to geographical variation in the radar reflectivity of storms, there is also a seasonal variation. An
additional problem is how to determine the severity of a
thunderstorm cell. They may look the same to the eye and
on the radar but one might be much more risk for hail and
lightning than the other. Thus it is clear that a weather
radar should ideally take all these factors into account.
When monitoring weather patterns from aircraft it is
important to get a complete view of meteorological activity.
With conventional 2D airborne weather radar the image provided is in one field of view like a slice and so the flight crew
have to manually tilt the radar beam up and down to get a
full picture of the weather. There is a fairly significant flight
crew workload associated with obtaining comprehensive
weather information with 2D radar. For an instruction guide
on the operation of a typical
modern 2D airborne weather
radar you may
wish to see the
video “EJETS
WEATHER RADAR OPERATION” http://
youtu.be/VusX0V2zvU8
Ground-based
weather radar
For those interested,
there are numerous
weather-related websites
along with radar Apps for
smart phones.
We featured the Australian
Bureau of Meterology Doppler
Weather Radar in the January
2010 issue (also see www.
bom.gov.au/australia/radar/
3D Radar
or www.weatherzone.com.au/
I n r e c e n t radar/, among others).
times two companies have
developed
airborne 3D
weather radar.
One company
is Honeywell
with their IntuVue RDR-4000
system and the other company is Rockwell Collins with
their WXR-2100 MultiScan ThreatTrack system. The objective with 3D radar is to reduce flight crew work load and to
provide a more comprehensive picture of weather activity.
This leads to greater safety and airline efficiency.
The Honeywell system is currently used on the Boeing
737NG, 777, C-17, and Airbus A380 aircraft and has been
A typical MultiScan radar display showing various weather threats.
siliconchip.com.au
April 2015 19
A typical MultiScan
display and how
it correlates with
what is seen out
of the cockpit
windows.
selected for the Airbus A350, Gulfstream G650 and KHI
CX aircraft platforms.
Rockwell Collins system
The Rockwell Collins system has been installed on all
Qantas aircraft, and is standard on all new Boeing 787
Dreamliners, Boeing 747-800s and Boeing Business Jets
and is an option for the Airbus A320s, A330s and A340s,
and Boeing 777s and Next-Generation 737s.
Qantas is a pioneering operator of the Rockwell Collins
Milestones in radar development
1865 James Clerk Maxwell publishes “A Dynamical Theory of the
Electromagnetic Field” with the original four Maxwell’s Equations
which describe how electric and magnetic fields are generated
and relate to each other.
1887 Starting in November of that year, Heinrich Rudolf Hertz
discovers electromagnetic waves, proves Maxwell’s Equations
and publishes a series of papers, the first being “On Electromagnetic Effects Produced by Electrical Disturbances in Insulators”.
1899 Guglielmo Marconi recalls his 1899 work in 1922 and says
a “ship could radiate or project a divergent beam of these
[electromagnetic] rays in any desired direction, which rays, if
coming across a metallic object, such as another steamer or
ship, would be reflected back to a receiver screened from the
local transmitter on the sending ship, and thereby immediately
reveal the presence and bearing of the other ship in fog or thick
weather.”
1900 Nikola Tesla in Century magazine wrote “by their [standing
electromagnetic waves] use we may produce at will, from a
sending station, an electrical effect in any particular region of
the globe; [with which] we may determine the relative position or
course of a moving object, such as a vessel at sea, the distance
traversed by the same, or its speed.”
1904 Christian Hülsmeyer demonstrates detection of a ship at a
distance with his “Telemobiloskop” and is sometimes credited
with the invention of radar but it does not give the range of
20 Silicon Chip
an object direct. It is the first patented device that can detect
objects at a distance.
1917 Lucien Lévy invents the superheterodyne receiver.
1921 The magnetron is invented by Albert Wallace Hull.
1922 US Naval Research Laboratory engineers Albert H. Taylor
and Leo C. Young detect a wooden ship in the Potomac River
by accident when conducting communications experiments and
later in 1937 develop a practical ship-based radar.
1930 Lawrence A. Hyland at US Naval Research Laboratory demonstrates the reflection of radio waves from an aircraft.
1936 The development of the klystron at General Electric by George
F. Metcalf and William C. Hahn (the invention has also been attributed to the brothers Russell and Sigurd Varian of Stanford
University in 1937).
From this time on radar was rapidly developed, especially as the
Second World War loomed and was soon started.
For more details on the history of radar you may wish to look at
http://en.wikipedia.org/wiki/History_of_radar Some YouTube
videos of interest are:
“Radar: Technical Principles: Mechanics” pt1-2 1946 US Army
Training Film” http://youtu.be/64LUeQ4DAqg and “Heroes
and Weapons of WWII : 01. The Men Who Invented Radar”
http://youtu.be/5x37BVCvFRk
siliconchip.com.au
Rockwell Collins WXR-2100 as installed in aircraft cockpit and displayed on the central monitor.
system and has been using it since it was first released to
the market in its original version in 2002. In fact, Qantas
played a major role in its development. Qantas flies across
the Pacific Ocean frequently, often at night and thus had
a particular incentive to want better weather radar than
Air Turbulence
In Australia, there are about 25 in-flight turbulence related
injuries every year according to the Australian Transport
Safety Bureau (ATSB) with many more unreported. Some
injuries are serious with broken bones and head injuries. In
a typical severe turbulence event, 99 percent of passengers
will not be injured.
Since Australia has some of the best flying conditions in the
world, it is expected that flights outside of Australia will encounter more serious problems than flights within Australia.
From 2009 to 2013 there were 677 turbulence related instances reported to the ATSB on flights to and from Australia
with 197 minor injuries and 2 major injuries.
Australia’s Civil Aviation Safety Authority (CASA) classifies several types of turbulence and their causes as follows.
Types of turbulence
Light turbulence - briefly causes slight, erratic changes in
altitude and/or attitude.
Light chop - slight, rapid and somewhat rhythmic bumpiness
without noticeable changes in altitude or attitude.
Moderate turbulence - similar to light turbulence, but greater
intensity. Changes in altitude/attitude occur. Aircraft remains in control at all times. Variations in indicated air
speed.
Moderate chop - similar to light chop, but greater intensity.
Rapid bumps or jolts without obvious changes in altitude
or attitude.
Severe turbulence - large, abrupt changes in altitude/atsiliconchip.com.au
conventional 2D weather radar which requires a lot of
flight crew interpretation and represents a high work load.
While both Honeywell and Rockwell Collins make superb radar systems, the Rockwell Collins system has an
Australian connection and it is the focus of the remainder
titude. Large variation in indicated airspeed. Aircraft may
be temporarily out of control.
Extreme turbulence - aircraft is violently tossed about and
is impossible to control; may cause structural damage.
The causes
Thermals - Heat from the sun makes warm air masses rise
and cold ones sink.
Jet streams - Fast, high-altitude air currents shift, disturbing
the air nearby.
Mountains - Air passes over mountains and causes turbulence as it flows above the air on the other side.
Wake turbulence - Near the ground a passing plane or
helicopter sets up small, chaotic air currents.
Microbursts - A storm or a passing aircraft stirs up a strong
downdraft close to the ground.
Preventing injury from air turbulence
Occasional injuries are sustained by passengers due to
air turbulence, mainly by being thrown about the cabin or
by having items fall on them from open overhead lockers.
Almost all air turbulence related injuries can be avoided
by ensuring objects are securely placed in overhead lockers
and the lockers are kept closed and that seat belts are worn
at all times, not just during take off and landing.
Also, crew instructions should be followed at all times and
you should familiarise yourself with the safety information
card in the seat back pocket.
April 2015 21
Rockwell Collins MultiScan ThreatTrack
Radar – features and development
milestones
2002 Release of first model and it is put into immediate
service by Qantas. This version was called MultiScan.
2003 On delivery flights of Qantas aircraft from the USA
to Australia the flight time was used to test and develop
the next version of the system. The aircraft flew with
both a certified version of the radar and also the test
unit. Data obtained were eventually incorporated into
the 2008 model.
2006-2007 Rockwell Collins rented a Boeing business jet
and flew around the world for three months to verify
what was learned during the Qantas flights and this
information was incorporated into the 2008 model.
2008 A major upgrade was made from the 2002 model.
Storm top prediction was possible due to the addition
of a geographic database of storm models in different
areas at different times of the year. This was called
MultiScan VI.
2014 Hail and lightning detection was added (predictive
overflight). The ability to track 48 different thunderstorm cells and vertical analysis of thunderstorm
cells were added. This version was called MultiScan
ThreatTrak.
Note that the essence of the radar system is in its
smart software, it represents a revolution in software
rather than a revolution in hardware. Earlier model systems can be upgraded to the current specifications by
software upgrades and some minor hardware changes
in some cases.
Windshear is a hazard pilots dread because in the vast
majority of cases they receive no visual warning of the
phenomenon. Here the red and black stripes represent the
actual windshear location along with a warning reminder
at upper right.
22 Silicon Chip
of this article but the same general principles apply to the
Honeywell system.
A video of the Honeywell IntuVue radar is available at
“IntuVue® 3-D Weather Radar” http://youtu.be/w8IYyFmJcF0 and a training video for its use “RDR-4000 IntuVue™
Weather Radar Pilot Training for Boeing Aircraft | Avionics | Honeywell Aviation” http://youtu.be/WNVtJeccNSM
A video of the MultiScan radar can be seen on YouTube
at “MultiScan ThreatTrack weather radar -- The worst
weather is the one you can’t see coming” http://youtu.
be/zJDduGPvOEA and Boeing crew training videos can
be seen at “MultiScan Weather Radar Module 1 Boeing”
http://youtu.be/EUjxFVRTdtw and “MultiScan Weather
Radar Module 2” http://youtu.be/Ai_P-MwlrOw
The Rockwell Collins MultiScan ThreatTrack has the
following technologies:
Geographic Weather Correlation: Recall from earlier
in this article that there is significant regional variation
in the radar reflectivity of thunderstorm cells as well as
variation according to the time of year. This is a relatively
recent discovery that occurred from 1997 onwards after
the launch of the TRMM satellite (Tropical Rain Forest
Measuring Mission).
This satellite has amassed a vast database of thunderstorm
reflectivity information which, along with the work of leading climatologist Dr Ed Zipser, has enabled Rockwell Collins
to embed thunderstorm models into the radar which are
specific to particular geographic locations and time of year.
As previously noted, the tops of storm clouds are invisible
to radar but the radar model is able to make predictions of
the altitude of the true top of the storm cell and its level of
hazard by knowing the location and time of year.
Core Threat Analysis: The radar can track up to 48
thunderstorm cores at once and also predict their severity.
Automatic Temperature-Based Gain: As the outside air
temperature decreases, the cloud tops become less radar
reflective so this feature increases the radar energy used to
This particular windshear occurred during taxiing. In these
pictures from the cockpit the windshear can be seen in the
form of a line squall approaching the aircraft down the
taxiway. The pilot delayed his takeoff for 30 minutes until
the thunderstorm had passed the airport and took off safely.
siliconchip.com.au
illuminate the cloud, effectively decreasing the proportion
of the cloud that is invisible to radar.
OverFlight Protection: Traditional manual operation of
2D weather radars involves pointing the radar beam at the
lower radar reflective portion of storm clouds. As a matter
of simple geometry, if no adjustment to the beam angle is
made, as the aircraft approaches the cloud the beam moves
higher and higher until it is in the non-reflective part of
the cloud and the storm cell disappears from view. The
overflight protection feature keeps the beam pointed 6,000
feet beneath the flight path to keep the reflective portion
of the cloud in view.
Predictive OverFlight Protection: Storm cells can grow
at up to 6,000 feet per minute and when this happens a
“bubble” of turbulent air is pushed above the cloud top.
This feature tracks the rate of growth of storm cells and
warns if there is a fast-growing cell in the vicinity, which
is to be avoided.
SmartScan: As an aircraft turns with traditional radar
there is a black wedge indicated a lack of data in the direction of the turn. This feature ensures that data is immediately acquired in the direction of the turn.
Two Level Enhanced Turbulence: USA FAA regulations require turbulence with a ±0.3G RMS severity to be
displayed on weather radars but in addition to displaying
that, areas with a less severe but still uncomfortable level
of turbulence are also displayed.
Flight Path Hazard Assessment: The radar system looks
for different hazards according to those relevant to the
phase of flight.
For example during take off and landing the main concern is storm cells with convective activity and the Core
Threat Analysis feature is used to evaluate the threat;
during cruise the main threat is accidental penetration
of thunderstorm cloud tops, so the Geographic Weather
Correlation, Automatic Temperature Based Gain and the
Predictive Overflight Protection features are invoked to
prevent flying through the cloud tops.
In addition to these features there is also a wind-shear
alert and an attenuation alert to warn when a storm cloud
has absorbed so much radar energy that nothing behind it
will be visible (radar shadow).
Quiet, dark cockpit
In keeping with modern aircraft flight philosophy of
minimising the pilot workload (the “quiet, dark cockpit”)
the MultiScan radar ensures that only relevant information
is displayed. Threatening weather can be detected out to a
maximum range of 320 nautical miles while non-threatening weather 6,000 feet beneath the aircraft is not displayed.
In order to minimise the display of unnecessary information ground clutter is removed by the use of a global terrain
model so that returns from the ground can be ignored.
With so many aircraft flying around the world, many
fitted with the same model of radar, one might wonder if
there is potential for the radars to interfere with each other.
This is not a problem as each radar pulse is sent out
with a slightly different frequency and the radar will reject
any pulse it receives that is not at the frequency that was
sent out.
The radar dish for this system is around 70cm in diameter and sweeps side to side and up and down every four
seconds.
siliconchip.com.au
Radar and the pulse repetition
frequency and Doppler
compromise
Traditional radar works by sending out a short
signal pulse and then turning off the transmitter and
listening for any signals reflected back to the radar
antenna. Knowing that the radar signal travels at the
speed of light, it is possible to determine the distance
to an object, by dividing the total time for the pulse to
return by two.
The required length of the period between pulses
has to be enough time for the signal to travel out from
the radar set to the target object and return. A long
period between pulses allows objects to be seen at
a long distance compared to a short inter-pulse period which will only allow objects to be seen a short
distance away.
A compromise short inter-pulse period, corresponding to a high pulse repetition frequency (PRF) allows
a potential target to be illuminated with more radio
energy. This makes an object easier to see than if
illuminated with a low pulse repetition frequency.
However, a low pulse repetition frequency is needed
if distant objects are to be observed and they are
illuminated with less radio energy due to a lower
number of pulses.
In fact, the energy reflected from the target back to
the transmitter is also subject to the inverse square
law so the energy received back at the radar set has
a fourth root dependence, not a square root dependence. A consequence of this is that to double the effective range of a radar system the power has to be
increased by a factor of 16.
With Doppler radar there is a further compromise
which is that there is an inverse relationship between
the distance that the radar can see to and the velocity
that can be measured. When the PRF is low a long
distance can be measured but only a low range of velocities. When the PRF is high, a much higher range of
velocities can be measured but the range is reduced.
A more recent development in radar, at least as
far as commercial augmentation is concerned, is
Frequency-Modulated Continuous Wave, or “Broadband” Radar, which unlike traditional radar doesn’t
use a high-energy pulse but is “always on”. Contradictory though it may sound, FMCW radar uses a lot
less energy, is a lot safer to operate close to and is
particularly applicable to marine use (see the feature
in November 2010 SILICON CHIP).
Conclusion
Great advances have been made in radar since it was
first invented. The most recent advances are being made
not so much in radar hardware but in the software used to
interpret and make use of the radar data.
As applied to airborne weather-radar, recent developments in 3D radar which serve to both reduce pilot work
load and greatly increase the analysis of weather systems
and the possible threats posed will make our skies even
SC
safer than they are now.
April 2015 23
VirtualBench is a computerdriven 2-channel 100MHz
digital oscilloscope, 34-channel logic analyser,
waveform generator, 3-output adjustable power
supply and multimeter, all in one box. It can
be driven wirelessly using an iPad or from a
PC via USB. Importantly, it integrates with
National Instruments’ LabView software for
automated measurement and testing.
VirtualBench 5-in-1
F
ollowing the trend of integrating
test equipment into one unit,
VirtualBench is an instrument
which can be used to test and debug
many projects all by itself.
As you can see from the photos,
it’s “headless”, with no screen and
virtually no controls. The interface is
handled by a PC or tablet.
This has some significant advantages. For one, you aren’t stuck with
whatever size or resolution screen the
manufacturer has decided to put on
the device.
We’ve seen many multi-thousanddollar test devices with screens that
are inferior to today’s bargain basement tablets! So this “bring your own
screen” philosophy can work quite
well.
On the other hand, if you forget to
bring your tablet/laptop or its battery
is flat, you’re out of luck; VirtualBench
24 Silicon Chip
is effectively tethered to a computer.
Physically, as the name should suggest, the VirtualBench is very convenient for bench-top use.
At 255mm wide, 190mm deep and
73mm high it doesn’t take up a great
deal of space. In fact, since it has a flat
top, you can argue that it doesn’t take
up any space at all.
At the very least, you can stack
similar-sized equipment on top. An
iPad fits quite nicely.
All the connectors you need frequent access to are on the front. The
power button and Wi-Fi power indicator are at upper left, with the IDC
connector for the logic ribbon cable in
the middle and the two BNC scope inputs, calibration terminals, waveform
generator BNC output and external
trigger input at upper right.
Along the bottom, from left-to-right
are the digital I/O terminal block, DC
power supply output terminal block
and DMM insulated banana sockets.
Features
The digital I/O block provides a 3.3V
power source (but only up to 20mA),
ground connections and eight general
purpose I/Os which can be used for
controlling the equipment you are debugging or testing (more on that later).
The power supply outputs are 0-6V
at up to 1A, 0-25V at up to 0.5A and
0 to -25V at up to 0.5A. Each can be
set independently in 1mV steps and
a current limit can also be set for each
output.
So between these three adjustable
outputs and the (fairly limited) fixed
3.3V, you can power a large range of
devices from the VirtualBench without
resorting to an external power supply.
Interestingly, the ground terminal
for the ±25V adjustable supply is insiliconchip.com.au
“Hands on” review
by
Nicholas Vinen
The front panel houses most of the input/
output sockets, including those for the
oscilloscope and function generator at top
and digital I/O, power supply and DMM
underneath. The rear panel, by comparison,
is spartan, with just mains and USB sockets,
an earth point, a Kensington lock socket, WiFi
antenna and ventilation.
dependent of other grounds, although
in most applications it would be connected to the main circuit ground.
The DMM is a 5.5 digit type with
relatively high accuracy. It has four
input terminals and six modes, covering all the most common functions: DC
or AC voltage (true RMS, up to 300V
DC/265V RMS), DC or AC current (up
to 10A), resistance (up to 100M),
diode test (forward voltage up to 2V)
and continuity test with audible tone,
via iPad/PC speakers.
When measuring DC voltages up to
10V, a high input impedance (>10G)
option is available which can be quite
handy when measuring sensitive
circuits. DC current measurement
resolution goes down to 0.1A while
resistance measurement resolution is
down to 1m; however there is no
4-wire test mode. Still, such resolu-
tion is quite useful for finding shorted
tracks or components.
iPad interface
Most of the VirtualBench’s features
are usable from an iPad, over WiFi
(see screenshot opposite). At the time
of writing this review, there is no
Android support but this is expected
relatively soon; presumably, before the
end of 2015.
When controlling the VirtualBench from LabView, many options are available. Fortunately, the built-in help explains
them in detail. This screen shot shows the details for setting up the waveform generator.
siliconchip.com.au
April 2015 25
The VirtualBench PC interface allows control over all the MSO, DMM, power supply and signal generator features. There
are many digital channels so several serial buses can be monitored.
The interface is not difficult to figure
out. The scope traces are displayed in
the middle of the screen and can be
moved around by dragging. Vertical
scaling and the timebase can similarly
be adjusted using two-finger gestures.
The other displays and controls are
above and below the scope traces,
including the DMM features, scope
measurements, power supply controls
and function generator.
What we couldn’t find in the iPad
interface are the serial bus decoding
options (which are present on the
equivalent PC software) or controls
for the eight-pin digital I/O bus on the
front panel of the VirtualBench.
Presumably these more advanced
features have been left out because
they wanted to keep the iPad app
simple.
Like a lot of WiFi peripherals, rather
than joining your network, the VirtualBench requires that you connect your
iPad to its WiFi network (ie, it acts as
an access point).
The annoying aspect of this is that
26 Silicon Chip
this means you lose Internet access
while using it, so if you want to say
download a data sheet during a debugging session, you will have to disconnect from the VirtualBench’s WiFi and
then reconnect to it again later.
It also means that each time you
turn the VirtualBench on, you have to
remember to re-join its WiFi network
before running the app or it won’t
work. That’s because the iPad will automatically re-connect to your normal
WiFi network when the VirtualBench
access point disappears.
As we said, this is a pretty typical
way to interface with a device using
WiFi and it does avoid the need to
program your SSID and WEP password
into the device but in the long run that
would probably be a more satisfying
solution.
PC interface
You have two options for using the
VirtualBench on a PC. First there is
the dedicated interface software which
works similarly to the iPad software
but with the extra features mentioned
that are missing in the iPad version,
such as the serial protocol decoding
(SPI/I2C/Parallel); see the screenshot
above.
We found this software particularly
easy to use.
For example, the menu for setting
up serial decoding appears next to the
button to turn the digital channels on
and off when you move your mouse
near it, and similarly other set-up
menus appear next to related buttons.
The layout is visually clean and you
really don’t need a manual to figure the
software out; most users will be up and
running right away and will be able
to figure all the functions out easily.
In some ways using a scope this way
is very convenient because we often
find when debugging a project that we
refer to schematics, PCB overlays and
software on a computer when trying
to figure out what’s going on.
Thus we often end up swapping
constantly between the PC and a scope
when troubleshooting a project.
siliconchip.com.au
In this case, the PC is the scope interface, avoiding the need to constantly
switch between two different screens
and sets of buttons. This also makes it
easy to do things like save screen grabs
to the computer.
All the basic functions work well.
As a mixed signal scope, its performance is on a par with a typical,
good quality 100MHz unit. Similarly,
the DMM has reasonable accuracy if
somewhat limited functions.
The power supply is convenient
but with a maximum of 1A on its
0-6V output, won’t necessarily cover
all possible uses and so you may well
require a separate power supply with
a bit more grunt.
LabView integration
The other option for driving the VirtualBench from a PC is LabView and
this unleashes the full power of the device. It allows you to create automated
testing procedures and control them
via a graphical programming interface.
Automated testing is not only useful in a production environment, eg,
for QA where you need to do a quick
check that all the functions of a device
are operating correctly before sending
it out the door but also in a test, service
and debug environment, such as the
sort of development and testing work
we do at SILICON CHIP.
For example, say you have a device
which has a glitch after power up,
if a certain sequence of buttons are
pressed in a particular order. You’re
trying to eliminate this glitch by making changes to the software and/or
hardware but each time you make a
change, you need to check whether it
has fixed the glitch or not.
You can design a test procedure in
LabView which uses the VirtualBench
to power up your device, wait for it to
be ready, simulate button presses via
its configurable digital I/Os, then run
whatever tests are necessary using
the MSO and DMM to verify correct
operation.
The LabView software can then report whether the glitch is still present
and if so, you can make further changes
and try again. That makes such testing
a lot easier and more repeatable and
is especially handy if the glitch you’re
looking for is short-lived.
The image below shows the LabView software interfacing with our VirtualBench review unit. This is one of
the example programs provided on the
National Instruments website which
uses the adjustable power supply and
DMM features of the device to plot a
This demo program steps the power supply output through a range of voltages and uses the DMM to measure current and
produce the plot at the bottom of the screen.
siliconchip.com.au
April 2015 27
V/I curve for the device under test.
This sort of test works well because
the adjustable power supply has such
fine-grained control over output voltage.
The program itself is shown at top.
This consists of a variety of blocks
representing different parts of the
VirtualBench device and different
stages in the test, which are “wired
up” together to determine a sequence
of events. It is broken into five sections
and the control sequence flows from
left to right, with the five different
steps labelled below.
The first step is initialisation and
this involves the software connecting
to the VirtualBench device and preparing the sections which are to be used
(ie, power supply and DMM).
The configuration step sets the various test parameters such as what mode
the DMM section will operate in (DC
current in this case), the voltage range
over which the power supply will be
stepped and so on.
Parameters such as the voltage range
and number of steps are set by the user
in the “Front Panel” interface in the
middle of the screen.
This makes it easy to adjust the parameters and run a new test without
having to change the block diagram.
The selected values are automatically
fed by the software into the orange
and blue rectangles in the block diagram which then feed into the control
process.
The grey box outlined in the middle,
above “Perform Operation” is a “for
loop” which performs a set of tasks a
fixed number of times.
In this case, it’s used to step the
power supply through the test voltage
range and read the current level from
the DMM each time. The voltage and
current figures are then fed to the X/Y
plot in the bottom pane via the pink
“Analog Data” item at right.
The remainder of the items in the
top pane deal with shutting the VirtualBench down once all the data has
been acquired and telling the user
whether there were any problems
during the test (eg, if the multimeter
input range was exceeded).
At left of the display is the “palette”
with some of the blocks that you can
place in the block diagram at top in
order to perform different functions.
For this test, we connected a 3.9V
zener diode across the power supply
terminals and the plot at bottom shows
28 Silicon Chip
its soft knee characteristic over the
0-10V test range and 0-500mA capability of the adjustable +25V power
supply output.
Ease of use
LabView can seem daunting at first
even for an experienced computer
programmer, partly because of the
large number of built-in functions but
mostly because its graphical nature is
quite different from the more common
text-based programming systems.
However with the aid of examples
and a little experimentation, it doesn’t
take long to figure out the basics. We
managed to build a test from scratch
and get it working in less than half
an hour.
The supplied examples help a lot. In
addition to the one described above,
others include creating Bode plots,
frequency response plots and stimulus/response measurements using
the signal generator and oscilloscope
modules.
The built-in context-sensitive help
is excellent, once you’ve figured out
how to get to it – you need to right-click
on one of the block objects using the
correct selection tool and then choose
“Help” and you’ll get a clear explanation of how the block works – see the
earlier screen grab.
If you have programming experience, you should become comfortable with LabView after using it for a
short time but it is a complex piece of
software and will certainly take some
time to master. The advantage of this
complexity is that it’s very powerful
once you get used to it.
We decided to see just how practical the combination of LabView and
VirtualBench is and to do this, we
wanted to set it up to perform a function that wasn’t mentioned in the
documentation and for which there
are no examples.
We succeeded in setting up a real
time distortion analyser with spectrum
display and this only took about 30
minutes to figure out. It would have
been much quicker if we had more
experience with the software.
We set up the waveform generator to
produce a sine wave and fed this to the
scope input. Our distortion analysis
software then reported 0.1% THD+N
with the second harmonic at -65dB,
third at -61dB and fourth at -72dB as
sas read off the spectrum plot.
While this set-up would be no match
for our Audio Precision system in
terms of performance, that certainly
demonstrates the unit’s flexibility
when teamed with the LabView software.
From what we can see, there are a
lot of other analysis tasks which would
be possible to perform using this sort
of set-up.
Note though that to do this sort of
advanced analysis, you need to buy
the more expensive “Full” version of
LabView rather than just the “Base”
version.
For the list of differences, see this
web page: www.ni.com/labview/buy/
Signal processing functions available in the “Full” version include
waveform and signal generation and
conditioning (useful in combination
with the Arbitrary Waveform Generator VirtualBench function), waveform
measurements, windowing, filtering,
spectral analysis, transformations and
PID control.
Conclusion
If you’re a die-hard iPad user you
may appreciate the WiFi connectivity
functions of this unit but in our opinion, to get the full benefit, you really
need to use LabView on a PC.
While LabView is available for Mac
OSX, the VirtualBench driver appears
to be Windows-only for the moment.
The way that the various functions
of the VirtualBench are integrated,
combined with the power of the LabView software is by far its best aspect.
And note that LabView will also
integrate with other National Instruments products, including their large
range of data acquisition and signal
generator devices.
So if you like the idea of a PCcontrolled all-in-one test instrument
and are interested in taking advantage
of the automated testing capabilities
available in conjunction with the LabView software, VirtualBench could be
for you.
Pricing & availability
The VirtualBench is available direct
from National Instruments, PO Box
382, North Ryde, NSW 2113. It retails
for $2987, including GST. LabView is
$550 (incl. GST) for the Base version
and $1100 for the full version.
For enquiries or to purchase, go to
www.ni.com/virtualbench/buy/ or call
them on 1800 300 800.
SC
siliconchip.com.au
siliconchip.com.au
April 2015 29
Appliance
Insulation
Tester
By JOHN CLARKE
Do you think all your 230VAC-powered tools and appliances are
safe because they are double-insulated? If so, you could be in for a
rude shock – literally! Or do you think you are safe because your
home (or workplace) is fitted with RCDs (Residual Current Devices)?
Again, you could still be at risk of a severe electric shock. The only
way to be reasonably sure about appliance and power tool safety is
to test them regularly. That is where our Appliance Insulation Tester
is a crucial tool.
L
ET’S BE BLUNT: an RCD will not
save you from electric shock if you
use a faulty power tool or appliance.
Nor will it necessarily save you from
death. Have we got your full attention
now?
An RCD (commonly called a safety
switch) will switch off the 230VAC
power if it detects an imbalance
between the Active and Neutral currents in the appliance circuit. That
imbalance could mean that current
is flowing through your body rather
than the mains wiring. At least 30mA
of current needs to flow through your
30 Silicon Chip
body for a typical RCD to switch off the
power – but depending on the fault, the
current could be a lot more than 30mA
and the time before it is switched off
could be up to 150 milliseconds. That’s
long enough to experience a very nasty
electric shock and one which could
possibly kill you!
Well hopefully, it would not kill
you but you could still be seriously
injured. Say you get the shock while
using the faulty tool and standing on
an aluminium ladder. The shock could
throw you off the ladder and you could
be seriously injured or killed (again!).
And anyway, how you do know the
RCDs in your home are working properly? Have they been tested recently?
You can now see that appliances
and power tools should be tested
regularly. So we have produced our
Appliance Insulation Tester which
checks whether the insulation resistance is adequate to protect you from
serious shock on double-insulated or
earthed appliances and power tools. It
does this by applying 250V or 500V DC
between mains Active and Neutral to
the Earth on the 3-pin plug of earthed
appliances (Class 1 appliance) or to
siliconchip.com.au
10-LED BARGRAPH
HIGH VOLTAGE
GENERATOR
(IC1, IC2, Q2, T1,
D1–D4, VR1
ENA
λ
OUT
3.9M
FB
VOLTAGE FEEDBACK
100n
+
–
OUTPUT
ADJUST
VR1
λ
λ
λ
λ
λ
λ
λ
IC3c
BARGRAPH DRIVER (IC5)
CALIBRATE
VR2
100k
250V
λ
OVER
LED4
22k
500V
λ
TEST
TERMINALS
3.0k
22k
λ
100k
S2
D6
K
200k
FEEDBACK
MONITOR
(IC4,LED1)
GENERATOR
DISABLE
(Q4, LED2)
SAFETY CIRCUIT
A
POWER OFF
DISCHARGE
(Q5, S1)
DISCHARGE
(Q3)
K
D8
TRIP
COMPARATOR
A
IC3a, D5
REFERENCE
(REF1, IC3b)
Fig.1: block diagram of the Appliance Insulation Tester. It uses a high-voltage generator (top, left) to produce either 250V
or 500V DC which is applied to the test terminals. The resulting leakage current through the appliance under test and the
associated 3kΩ resistor is monitored by op amp IC3c which then drives a 10-LED bargraph via IC5. IC3a monitors IC3c’s
output and shuts down the high-voltage generator via Mosfet Q4 if the voltage across the 3kΩ resistor exceeds 3V.
exposed metal on double insulated
appliances (Class 2) and then the
insulation resistance is measured. In
general, an insulation resistance (IR)
below 1MΩ is deemed unsafe.
There are a couple of appliances
where this 1MΩ value does not apply.
The first is with a portable RCD that
has a functional earth (ie, requires
an earth for correct operation) and
the second is for appliances which
have mineral insulated metal sheath
heating elements. Check with the AS/
NZS3760 standard for more information. Our Appliance Insulation Tester
is not suitable for these devices.
Another instrument required
While our Appliance Insulation
Tester will check most appliances, it
does not apply 230VAC mains voltage
and therefore cannot conduct an IR test
on appliances that have a “soft” or a
non-mechanical power switch such
as in most appliances with remote
controls (eg, DVD players and TV
sets). These appliances can only be
tested with an instrument that permits
energising with the normal 230V supsiliconchip.com.au
ply voltage to measure the actual earth
leakage current. We plan to feature an
Appliance Earth Leakage Tester next
month as a companion instrument.
Testing safely
We mentioned that the testing voltage used is 500V or 250V DC. 500V DC
is the usual test voltage while 250V DC
is used where an appliance has overvoltage protection. These voltages are
high enough to give you a nasty shock
if you come into contact with both the
test probes, so we have incorporated
three safety features.
The first is the use of shrouded
banana sockets for the high voltage
output terminals. Secondly, there is a
1mA (or 500µA depending on output
voltage) trip current detector that shuts
off the high voltage if this current is
exceeded. So if you do make contact
with both the test probes you will
get an unpleasant “tickle” instead of
possibly a more severe electric shock.
As well, the Tester has a Trip Test
pushbutton which verifies that the unit
will shut down if you make contact
with the probes. It also lights a LED
to indicate that it has been tripped.
To restore operation, the unit has to be
switched off and then on again.
Finally, a check LED is included to
indicate if the high-voltage generator
is not working correctly.
Simplified circuit
Fig.1 shows the simplified circuit
arrangement of the Appliance Insulation Tester. It comprises a high-voltage
generator that can be set to produce
either 250V or 500V DC, with voltage
feedback to maintain the required voltage with varying load. IC4 includes
two comparators which detect if there
is a fault in the high-voltage output. A
high or low voltage is indicated with
LED1 (HV Error).
The positive high voltage becomes
the “+” test output while the negative (-) test output is connected to the
supply ground via a 3kΩ resistance.
When the test terminals are connected
to an appliance to test for insulation
resistance, any leakage current will
flow through this 3kΩ resistance and
so develop a voltage. This voltage is
monitored by IC3c, a high input imApril 2015 31
POWER S1
OFF
A
+9V
ON
10 µF
16V
9V
BATTERY
LOW
ESR
1k
6
Q1
IRF540
D
4x
1Ω
470 µF
16V
100nF
IC1
MC34063
REVERSE
POLARITY
PROTECT
Ct
3
GND
4
λ LED1
IC4b
5
IC4a
A
100nF
630V
S
VR1 1M
(VR25/VR37)
100k
(VR25/VR37)
100k
250V
100k
(VR25/VR37)
+9V
20k
Q3
TK7A60W
IC3: LMC6484
10k
13
100Ω
12
1.2V
IC3d
14
10k
820Ω
100k
C
2.2k
1M
10k
4
FEEDBACK MONITOR
K
S2
6
2
K
+500V/
+250V
OUTPUT
ADJUST
1.3V
3
A
22k
500V
IC4: LM393
SC
22k
820Ω
8
K
3.9M
+2.5V
K
20 1 5
2
A
A
Q2
IRF540
G
5
VOLTAGE FEEDBACK
HV
ERROR
1
10Ω
3
IC2
7555
6
1
1nF
7
5
K
D
4
10 µF
2.2k
A
8
7
1nF
+9V
T1
2.2k
100nF
1
SwC
FB
SwE
2
D1–D4
4x UF4007
TRIPPED
λ LED2
10k
K
7
Ips
8
DrC
Vcc
G
S
2.2k
A
λ LED3
+2.5V
BATTERY VOLTAGE MONITOR
LOW
BATTERY
D
Q4
2N7000
S
B
E
Q5
BC337
NC
NO
D
S
S3
TRIP TEST
G
10Ω
D8 1N4148
A
K
10Ω
G
10k
DISCHARGE MOSFET
K
APPLIANCE INSULATION TESTER
Fig.2: the circuit of the Appliance Insulation Tester. The high-voltage generator consists of an MC34063 DC-DC converter
(IC1), a 7555 CMOS timer (IC2), Mosfet Q2, step-up transformer T1 and bridge rectifier D1-D4. IC3c monitors the leakage
current through the two series 1.5kΩ resistors and drives IC5, while IC3a is the trip comparator for the safety circuit.
pedance, low input current op amp.
IC3c operates as a unity gain buffer
for the 500V setting or with a gain of
two when 250V is selected. So for
example, a 1MΩ leakage resistance
between the test terminals with a 500V
DC test voltage would produce a current of 500µA. This gives 1.5V across
the 3kΩ resistance and thus 1.5V at
IC3c’s output.
For 250V DC, the current with the
same 1MΩ leakage resistance would
give 250µA and there would be 750mV
across the 3kΩ resistance. However, we
still get 1.5V at IC3c’s output because
it now operates with a gain of two.
The pin 8 output of IC3c is attenuated and fed to IC5, an LM3915 dot/
bar display driver (used in dot mode)
and 10-LED bargraph display. The display shows resistance in 10 3dB steps:
32 Silicon Chip
<707kΩ, 1MΩ, 1.4MΩ, 2MΩ, 2.8MΩ,
4MΩ, 5.6MΩ, 8MΩ, 11MΩ and 16MΩ.
A separate LED lights for resistance
values of more than 16MΩ.
Op amp IC3a compares the output of
IC3c with a 2.5V reference voltage set
by IC3b. If the voltage across the 3kΩ
resistance reaches 3V, IC3a’s output
goes high to turn on Mosfet Q4 and
disable the high-voltage generator. At
the same time, Mosfet Q3 discharges
the high-voltage generator’s 100nF
output capacitor via a 200kΩ resistance and the display will show a low
ohm (<707kΩ) reading. In addition,
LED2 indicates that the high-voltage
generator has been disabled.
Finally, since the high-voltage output will be zero, the feedback monitor
will turn on the high-voltage error
indicator, LED1.
As already noted, to restore operation, the unit has to be switched off
and then on again. Note that if the unit
is switched off, Mosfet Q3 discharges
the high-voltage capacitor, under the
control of transistor Q5, which monitors the on/off switch.
Full circuit
The full circuit is shown in Fig.2.
The high-voltage generator comprises
an MC34063 DC-DC converter (IC1),
a 7555 CMOS timer (IC2), Mosfet Q2
and transformer T1. If this circuit did
not have the trip current protection
feature, IC1 & IC2 could have been
used in a slightly simpler configuration, with the 7555 used as a rail-to-rail
Mosfet gate driver and with no gating
function via Q4.
IC1c’s oscillator runs at a nominal
siliconchip.com.au
+
TEST
TERMINALS
–
A
λ
16MΩ
A
λ
8MΩ
A
λ
11MΩ
4MΩ
A
λ
5.6MΩ
A
λ
A
A
A
λ
λ
λ
150Ω
A
E
10k
B
K
C
λ 10-LED
BARGRAPH
10k
>16MΩ
λ LED4
Q6
BC557
A
2.2k
16
15
13
14
10
11
12
17
18
O2
O3
O8
O7
O6
O10 O9
O4
O5
100k
4
10
(VR25/VR37)
9
10k
A
λ
D7
1N4148
2.0MΩ
A
CLAMP
2.8MΩ
K
1MΩ
10 µF
1.4MΩ
+9V
<707kΩ
+9V
IC3c
10nF
6.8k
8
5
IN
+9V
DOT/ 9
BAR
10 µF
IC5 LM3915
VREF
7
CALIBRATE
DISPLAY
VR2
10k
1nF
3
V+
11
BUFFER/AMPLIFIER
1
O1
RHI
6
RLO
4
REF ADJ
8
V–
2
1.5k
3.3k
100k
CURRENT
MONITOR
RESISTANCE
K
1.5k
1W
A
1.5k
FORCE
DISPLAY
LOW
D6
1N4148
D5 1N4148
IC3: LMC6484
1W
K
A
20k
5
LATCH
+2.5V REF
3
1
IC3a
7
K
LEDS
A
K
A
K
A
K
REF1
LM285Z-2.5
REFERENCE VOLTAGE BUFFER
A
100nF
100k
1N4148
6
2
TRIP COMPARATOR
UF4004
IC3b
LM 285 Z-2.5
BC 33 7 ,
BC557
2N7000
B
A K
NC
D
G
S
E
IRF540,
TK7A60W
G
C
D
D
S
Main Features
30kHz, as set by the 1nF capacitor at
pin 3. IC1’s output pins (1&8) are opencollector transistors that are pulled up
to the 9V supply by a 2.2kΩ resistor.
The 30kHz output signal is coupled to
IC2, a 7555 which is mainly used as
an inverting buffer/gate which drives
Mosfet Q2.
When Q2 is switched on, current
flows through the primary winding of
transformer T1 until it peaks at about
1.2A. This current flows through the
four paralleled 1Ω resistors between
pins 6 & 7 of IC1 and when it reaches
1.2A, IC1 stops its oscillator and
Mosfet Q2 is switched off. Thus, the
magnetic field in the transformer core
collapses, producing high voltage in
the primary winding. The secondary
winding steps up the voltage and feeds
a bridge rectifier comprising diodes
siliconchip.com.au
•
Displays insulation resistance in 10 steps from 707kΩ to 16MΩ with acceptable
resistance in green and unacceptable resistance in orange and red
•
•
•
•
•
•
•
500V DC and 250V DC test voltages
•
Not suitable for mineral insulated metal-sheathed heating elements
1mA/500µA over-current trip for safety
Over-current trip test and trip indicator
Low battery indicator
High voltage fault indicator
High voltage discharges to safe levels at power off and over-current trip out
Not suitable for portable residual current devices that incorporate a functional
earth
D1-D4 to produce a 500V (or 250V)
DC supply and this is filtered with a
100nF 630V DC capacitor.
Note that a single diode could
have been used instead of the bridge
rectifier. However, a single diode rectifier would require the transformer
windings to be correctly phased and
this can be problem for constructors
winding their own transformers. Using
April 2015 33
Appliance Insulation Tester: Parts List
1 double-sided PCB, code
04103151, 86 x 133mm
1 front panel PCB, code
04103152, 90 x 151mm
1 UB1 plastic utility box 158 x 95
x 53mm
1 ferrite pot core and bobbin set
(Jaycar LF-1060 & LF-1062,
Altronics L 5300 & L 5305)
(T1)
1 pot core spacer eg 0.25mm
cardboard 11mm OD or similar
(see text)
1 9V battery clip lead
1 9V battery
1 9V battery U-shaped holder
1 20-pin wire wrap SIL socket
strip for LED bargraph
2 SPDT toggle switches, PCBmount (S1,S2) (Altronics S
1315)
1 SPDT pushbutton PCB-mount
switch (S3) (Altronics S 1393)
1 red safety banana socket (Jaycar PS-0420)
1 black safety banana socket
(Jaycar PS-0421)
1 shrouded safety multimeter test
lead set (Altronics P 0404A,
Jaycar WT-5325)
3 M3 tapped 9mm Nylon spacers
3 M3 tapped 6mm Nylon spacers
3 M3 x 12mm screws
3 M3 x 5mm screws
1 M3 x 10mm countersink screw
1 M3 x 25mm Nylon screw
8 M3 Nylon washers
2 M3 nuts
1 6.5m length of 0.25mm-dia.
enamelled copper wire
1 700mm length of 0.5mm-dia.
enamelled copper wire
1 40mm length of 230VAC rated
red wire
1 40mm length of 230VAC rated
black wire
3 PC stakes
1 1MΩ multiturn trimpot (VR1)
1 10kΩ multiturn trimpot (VR2)
a bridge rectifier makes transformer
winding and termination easier.
Since the load on the high-voltage
supply can vary, we have voltage feedback to pin 5 of IC1 via a 3.9MΩ resistor and 100kΩ trimpot VR1, together
with a 22kΩ resistor at pin 5 of IC1 to
ground. VR1 is adjusted to provide
an output of 250V DC. An extra 22kΩ
resistor is switched via S2 to provide
the 500V setting.
Either way, the feedback divider
reduces the high voltage to a nominal
1.25V at pin 5 and this is compared
against an internal 1.25V reference in
IC1. If the output voltage drops, the
duty cycle of the output waveform
from pins 1 & 8 is increased to compensate (and vice versa).
Note that the 3.9MΩ feedback resistor is a VR37 or VR25 type, rated at
3500V DC or 1600V DC, respectively.
Note also that IC2 has its pin 4 reset
pin connected to other parts of the
circuitry. This is used to shut down
the high voltage generation when required. Under normal operation, pin
4 is pulled high via a 10kΩ resistor to
allow IC2 to operate.
34 Silicon Chip
Semiconductors
1 MC34063AP1 DC-DC converter (IC1)
1 7555 CMOS timer (IC2)
1 LMC6484AIN quad CMOS op
amp (IC3)
1 LM393N dual comparator (IC4)
1 LM3915N dot/bar display
driver (IC5)
1 10-LED green/yellow/red LED
bar (Altronics Z 0964)
2 IRF540 100V 33A N Channel
Mosfets (Q1,Q2)
1 600V low gate threshold Nchannel Mosfet (Q3) (Toshiba
TK7A60W or equivalent) (RS
Components Cat. 799-5201)
1 2N7000 Mosfet (Q4)
Voltage fault indication
As mentioned above, the circuit
has voltage fault indication and this
comprises IC4, an LM393 configured
as a “window” comparator. It drives
LED1 when the voltage feedback signal
fed to pin 5 of IC1 is outside the limits
set at its pins 5 & 2 (of IC4). Normally,
with feedback voltage in the range of
1.2-1.3V, the paralleled open-collector
outputs of IC4 at pins 1 & 7 will remain
high and LED1 will be unlit.
If the feedback voltage drops below
1.2V, pin 1 of IC4a will go low to light
LED1. Similarly, if the feedback voltage goes above 1.3V, pin 7 of IC4b will
go low instead to again turn on LED1.
So if LED1 lights, it indicates that the
1 BC337 NPN transistor (Q5)
1 BC557 PNP transistor (Q6)
1 LM285Z 2.5V reference (REF1)
4 UF4007 1000V 1A fast diodes
(D1-D4)
4 1N4148 diodes (D5-D8)
3 3mm red high brightness LEDs
(LED1-LED3)
1 3mm green high brightness
LED (LED4)
Capacitors
1 470µF 16V low ESR electrolytic
4 10µF 16V PC electrolytic
3 100nF MKT polyester
1 100nF 630V metallised polyester
1 10nF MKT polyester
3 1nF MKT polyester
Resistors (0.25W, 1%)
1 3.9MΩ VR37/VR25 (3500V DC
or 1600V DC)
1 1MΩ VR37/VR25 (for calibration)
(3500V DC or 1600V DC)
3 100kΩ VR37/VR25 (3500V DC
or 1600V DC)
1 1MΩ
1 1.5kΩ
4 100kΩ
2 1.5kΩ 1W
2 22kΩ
1 1kΩ
2 20kΩ
2 820Ω
8 10kΩ
1 150Ω
1 6.8kΩ
1 100Ω
1 3.3kΩ
3 10Ω
5 2.2kΩ
4 1Ω 5%
DC-DC converter is not producing the
correct high voltage.
It is not a completely foolproof
check of output voltage because if one
of the feedback resistors should fail or
change its value, the feedback voltage
could be correct but the output voltage
will not. However, it is still a useful
indicator as it will light up when the
DC-DC converter is shut down or if
the output cannot provide sufficient
voltage under load. Of course, test
voltages can be periodically checked
with a multimeter.
Output terminals
As can be seen on the circuit, the
positive output of the high voltage generator connects directly to the positive
(red) test terminal while the negative
test terminal is connected to circuit
ground via two 1.5kΩ 1W resistors
connected in series. These provide a
means of monitoring the load current
siliconchip.com.au
for the Insulation Tester.
IC3c monitors the voltage across the
resulting 3kΩ resistance via a 100kΩ
resistor. This 100kΩ resistor protects
the op amp’s input should one of the
1.5kΩ resistors go open circuit and
allow the full 250V or 500V to be applied. Diode D7 clamps the input to
just over the +9V supply.
IC3c amplifies the voltage across the
3kΩ resistance by a factor of two when
switch S2 is in the 250V position. In
the 500V setting, S2 disconnects the
associated 100kΩ resistor from ground
and connects another 22kΩ resistor
between pin 5 of IC1 and ground. As
well as doubling the output from the
high-voltage generator, it converts IC3c
to a unity gain voltage follower. So
either way, the following LED display
circuitry involving IC5 gets the correct
signal range which is fed via a 6.8kΩ
resistor and 10kΩ trimpot VR2.
IC5 is an LM3915 logarithmic dot/
bar driver and this drives the 10-LED
display. An internal 1.25V reference at
pin 7 sets the full-scale input voltage.
IC5 is set in dot mode, meaning that
only one LED in the 10-LED bargraph
is driven at any one time.
For our circuit, full scale is when the
LED at pin 10 is lit and this is labelled
707kΩ. Other LEDs show 1MΩ, 1.4MΩ
etc, as mentioned above. If any of the
10 LEDs in the bargraph is lit, the resulting LED current through the 150Ω
resistor from the +9V rail will produce
a voltage to switch on transistor Q6
and it shunts LED4 so it cannot light.
If all the bargraph LEDs are off, Q6
will be off and LED4 will light, indicating that the load across the tester’s
terminals is more than 16MΩ. So in
practice, with nothing across the test
terminals, LED4 will be lit.
Over-current trip
As noted above, the trip circuit shuts
down the high voltage if the leakage
current exceeds 1mA in the 500V setting and 500µA for the 250V setting.
The over-current detection circuitry
comprises op amps IC3a, IC3b, Q3
& Q4 and REF1. REF1 is an LM285
2.5V reference and IC3b buffers it
and feeds the inverting input of IC3a
at pin 2. IC3a’s non-inverting input at
pin 3 monitors the output of IC3c via
a voltage divider comprising a 20kΩ
and 100kΩ resistor.
IC3a is connected as a comparator. If
IC3c’s output goes above 3V, the load
current through the two 1.5kΩ current
siliconchip.com.au
Fig.3: this scope
grab shows the
action of the trip
circuit when
the load current
exceeds 1mA (for
the 500V setting).
The green trace
shows the voltage
across the 3kΩ
monitor resistance
and the orange trace
shows the resulting
exponential drop in
the high voltage in
less than 40ms.
monitoring resistors will evidently be
above 1mA (for the 500V DC setting).
So with a voltage just above 3V from
IC3c, IC3a’s output goes high and D5
pulls pin 3 up even further to ensure
IC3a then stays latched. IC3a’s high
output then switches on Mosfet Q4 and
it pulls down pin 4 (the reset input) of
IC2. IC2 now acts as a gate and shuts
off the drive to Mosfet Q2 to kill the
output of the high voltage generator. At
the same time, LED2 lights to indicate
that the high voltage is off and the overcurrent circuit has tripped.
In addition, diode D8 drives the gate
of Mosfet Q3 to discharge the 100nF
high-voltage supply capacitor via two
100kΩ resistors. And finally, diode D6
drives the input of IC3c to well over
3V so that the LED display will show
a low reading, ie, “<700kΩ”.
As mentioned previously, the highvoltage error LED (LED1) will also light
to indicate that the high voltage has
shut down. To return to normal operation, the Insulation Tester is simply
switched off and on again.
Pushbutton switch S3 connects the
two 100kΩ VR25/VR37 resistors on
the positive high-voltage supply to
the negative test terminal. The resulting current through the 3kΩ monitor
resistance causes the circuit to trip
out as described earlier. The trip test
current is 2.5mA at 500V and 1.25mA
at 250V. These test currents are more
than twice the rated trip current but
will at least verify that the trip current
circuit will work.
If you are unfortunate enough to get
a shock from this Appliance Insulation
Tester, it shuts down the high voltage
to safe levels within 40ms (much faster
than any RCD is supposed to disconnect the 230VAC mains supply in the
event of a fault or shock).
9V battery
A 9V battery powers the circuit and
it is connected via switch S1 in the
positive lead. Mosfet Q1 is connected
in the negative lead to the battery and
provides protection against reversed
polarity (ie, when you connect the
battery the wrong way around). If the
polarity is correct, the internal diode
in Q1 will conduct and Q1’s gate will
be driven to 9V via a 1kΩ resistor to
switch it on. If the 9V is reversed, Q1’s
internal diode will be reverse biased
and the Mosfet will remain off.
A low battery indicator is provided
by op amp IC3d, connected as a comparator. It compares the 2.5V from
Specifications
Power: 9V at 25mA for a 500V output, 18mA for 250V (with >16MΩ leakage
resistance), 110mA at 600kΩ leakage and 500V test voltage
Low voltage indication: 7.5V. Circuit operates down to 5V
Output voltage: 500V and 250V with <1% variation from no load to 1mA trip point
Leakage trip current: 1mA at 500V, 500µA at 250V
Trip test current: 2.5mA at 500V, 1.25mA at 250V
High voltage discharge rate: the 500V output drops below 50V in 40ms
April 2015 35
WIRE STRESS
RELIEF LOOP
TO BATTERY
10-LED BARGRAPH
1k
470 µF
2N7000
100nF
10k
4148
20k
2.2k
10Ω
2.2k
D1-D4
(600V)
10 µF
TP GND
Q4
SOCKETS
PANEL)
10nF
1M
10k
100k
100k
100k
Q3
1N4148
1nF
20k
–
Q5
BC337
1.5k 1W
REF1
500V
100k*
10k
IC3 LMC6484
S2
D5
10k
1
LM285
100k
22k
1.5k
10k
250V
+
100k*
10Ω
HV ERR.
100nF 630V
100k*
VR1
1M
820Ω
* VR25 or VR37
3.9M*
4148
A
HV ADJ.
4148
LED1
1
4148
k
IC4
LM393
10 µF
22k
2.2k
1nF
C
UF4007
10Ω
Q2
IRF540
820Ω
10k
100nF
TWO MORE
1 Ω UNDER
NC
NO
1
IC2
7555
100Ω
1Ω
1Ω
10k
2.2k
1nF
MC34063
Q6
A
OVER RANGE
TRIP TEST
15130140
PRIMARY--T1--SECONDARY
100nF
+
Low ESR
1
S3
A
10 µF
IC1
LED4
k
6.8k
S1
POWER
LM3915
TEST LEAD
(ON FRONT
IC5
1.5k 1W
LOW BATT.
TRIPPED
LED2
k
10k
IRF540
LED3
04103151
C 2015
1
BC557
Q1
k
A
APPLIANCE INSULATION TESTER
3.3k
10k
2.2k
–
150Ω
VR2
10 µF
9V
+
DISPLAY CAL.
D6 D7 D8
Fig.4: follow this parts layout diagram and the photo at right to build the PCB but don’t solder
the LEDs or connect the insulated banana sockets until after the front panel PCB is attached
(see text). Figs.5&6 on the following pages show the transformer winding details.
REF1 with a sample of the battery
voltage fed via the 20kΩ and 10kΩ
resistors on pin 13. This will cause
the comparator to switch its output
to turn on LED3 for battery voltages
of less than 7.5V. The 1MΩ resistor
between pins 14 & 13 provides 135mV
of hysteresis to stop any flickering of
the LED. Note that the circuit will
continue to operate down to about 5V.
Note also that we have not provided
a separate power indicator LED since
either the LED bargraph or LED4 will
light whenever power is on.
Assembly
The assembly is straightforward,
with all parts installed on a doublesided PCB coded 04103151 and meas
uring 86 x 133mm. A second PCB
(coded 04103152, 90 x 151mm) is used
36 Silicon Chip
as the front panel and this replaces the
lid of the UB1 plastic utility box that’s
used to house the unit.
The two PCBs can be obtained either
as part of a complete kit (ie, from parts
retailers) or can be purchased as separate parts from the SILICON CHIP Online
Shop (www.siliconchip.com.au).
Fig.4 shows the parts layout on
the main PCB. Begin by installing
the resistors and diodes, taking care
to ensure that the latter are correctly
orientated. Table 1 overleaf shows the
resistor colour codes but you should
also check each one with a multimeter
before fitting it to the PCB.
Two 1Ω resistors must be installed
on the underside of the PCB. These are
mounted directly under the two 1Ω
resistors (located adjacent to IC1) and
are installed in parallel with these two
resistors. It’s just a matter of soldering
their leads directly to the pigtails of
the top resistors.
Note that VR25 or VR37 resistors
must be used in the positions marked
with an asterisk (*). In addition,
two different diode types are used –
1N4148 and UF4007. Be sure to install
the UF4007 diodes adjacent to T1.
Once the resistors are in, install the
three PC stakes. These are used for
the positive and negative terminals
adjacent to the test lead sockets and
for the TP GND terminal (near Q4 at
bottom left).
The ICs can now be installed. Make
sure that the correct IC goes in each
position and that it is orientated as
shown on Fig.4. IC1, IC2 & IC4 are all
8-pin devices, so be careful not to get
them mixed up.
siliconchip.com.au
foul the front panel PCB). Q1 and Q2
are both IRF540 types, while Q3 is a
TK7A60W type (or equivalent).
Begin by soldering these Mosfets in
at full lead length, taking care to ensure
that each is orientated correctly (Q1 &
Q2 face in opposite directions). That
done, grip the leads of each device in
turn using needle-nose pliers and bend
it over so that its body sits horizontally
above the PCB.
Note that if Q3 has a metal tab, it
should be covered with heatshrink
tubing as the tab will have a high voltage on it. The specified TK7A60W has
a plastic insulated tab and so does not
require heatshrink insulation.
Installing the LED bargraph
The primary & secondary leads that emerge from the bottom of the transformer
are soldered directly to their respective pads on the underside of the PCB. Note
that two 1Ω resistors (circled) are also soldered to the underside of the PCB.
These go directly under the two 1Ω resistors on the top of the PCB and are
soldered directly to their solder pads, so that all four resistors are in parallel.
Follow with the capacitors, taking
care to install the electrolytics with the
correct polarity. Note that the 470µF
capacitor (near power switch S1) must
be a low-ESR type. Note also that the
top of each electrolytic capacitor must
be no more than 15mm above the PCB,
to allow clearance for the front panel
PCB. It may be necessary to mount the
470µF low-ESR capacitor on its side
to meet this requirement, as shown in
the photos.
Transistors Q5 & Q6 and Mosfet Q4
can now go in. Q5 is a BC337 NPN
type while Q6 is a BC557 PNP type, so
don’t get them mixed up. The LM285Z
(REF1) be also now be installed – it
goes in to the left of IC3.
Multi-turn trimpots VR1 & VR2 are
next on the list. VR1 (1MΩ) goes in
with its adjustment screw towards the
siliconchip.com.au
top edge of the PCB, while VR2’s adjustment screw goes to the right. VR1
(1MΩ) could be marked as 105, while
VR2 (10kΩ) may be marked as 103.
Now for the three switches. S1 &
S2 can be installed either way around
– just push them all the way down
onto the PCB and make sure they are
seated correctly before soldering their
terminals. By contrast, S3 (at top right)
must be orientated with its common
pin towards the lower edge of the PCB.
This pin is marked with a “C” on the
switch side.
Power Mosfets
As shown in the photos, Mosfets
Q1-Q3 must be mounted horizontally,
with their leads bent down through 90°
to go into their respective PCB holes
(this is necessary so that they don’t
The LED bargraph is mounted using a 20-way wire-wrap socket strip.
First, break the socket strip into two
10-way strips and plug these into the
bargraph pins. That done, insert the
socket strips into the holes on the
PCB with the bargraph’s anode at top
right, as indicated by the chamfer on
one edge (see Fig.4).
Finally, solder the pins so that the
top of the display is 18mm above the
PCB. It’s best to solder one end pin
first, the adjust the display as necessary before soldering the diagonally
opposite end pin. The remaining pins
can then be soldered once everything
is correct.
Winding the transformer
Fig.5 shows the transformer winding details. It’s wound on a plastic
bobbin which is then fitted into a pot
core assembly.
The primary goes on the plastic bobbin first and is wound using 10 turns of
0.5mm enamelled copper wire (ECW).
These turns are wound on side-by-side
(ie, close-wound), with the wire ends
brought out through the notched exit
April 2015 37
BOBBIN
SECONDARY WINDING
3 LAYERS OF 40 TURNS
EACH; 0.25mm
ENAMELLED COPPER
WIRE (120T TOTAL)
PRIMARY WINDING
10 TURNS OF 0.5mm
ENAMELLED COPPER
WIRE
Fig.5: the transformer primary consists of 10 turns of 0.5mm-diameter
enamelled copper wire (ECW), while the secondary is wound using
120 turns of 0.25mm-diameter ECW in three 40-turn layers. Note that
one lead of each winding is brought out at the top of the bobbin, while
the other is brought out at the bottom (see text & photos).
M3 x 25mm NYLON SCREW
M3 x 5mm SCREWS
NYLON WASHERS
NYLON WASHERS
M3 x 9mm TAPPED
NYLON SPACER
T1 HALF
CORE
M3 x 6mm
NYLON SPACER
T1 HALF
CORE
M3 x 9mm TAPPED
NYLON SPACER
PCB
M3 x 6mm
NYLON SPACER
NYLON WASHERS
NYLON WASHERS
M3 NYLON NUT
M3 x 12mm SCREWS
Fig.6: this diagram and the two photos at right show the mounting details for the transformer. It’s secured in place
using three sets of Nylon spacers, Nylon washers and Nylon screws.
points on the top and bottom of the
bobbin. Once it’s on, cover the winding
with a layer of 10mm-wide insulating
tape to hold it in place.
By contrast, the secondary consists
of 120 turns of 0.25mm ECW and is
wound using three 40-turn layers, each
separated by a layer of insulation tape.
As before, the start and finish windings
exit from two notched exit points on
the top and bottom on the bobbin.
The secondary is also close-wound
but note that 40 turns will not fit sideby-side across the bobbin. This means
that some of the turns in each layer
will have to go directly over the top of
the others. Ideally, each layer should
start on one side of the bobbin and be
wound progressively toward the opposite side of the bobbin. Make sure
that all three layers are wound in the
same direction.
Secure the top secondary winding
layer with another layer of insulation
tape to hold it in place.
The next step is to cut an 11mm OD
spacer from 0.25mm-thick cardboard.
This spacer is used to separate the two
Table 1: Resistor Colour Codes
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
No.
1
2
7
2
2
8
1
1
5
1
1
2
1
1
3
4
38 Silicon Chip
Value
3.9MΩ
1MΩ
100kΩ
22kΩ
20kΩ
10kΩ
6.8kΩ
3.3kΩ
2.2kΩ
1.5kΩ
1kΩ
820Ω
150Ω
100Ω
10Ω
1Ω
4-Band Code (1%)
orange white green brown
brown black green brown
brown black yellow brown
red red orange brown
red black orange brown
brown black orange brown
blue grey red brown
orange orange red brown
red red red brown
brown green red brown
brown black red brown
grey red brown brown
brown green brown brown
brown black brown brown
brown black black brown
brown black gold brown
pot core halves (it produces an air gap
which prevents saturation in the ferrite
cores). Once you’ve cut the spacer to
size, cut a neat 3mm hole in its centre.
The pot core halves can now be
placed over the bobbin with the spacer
between them (ie, the spacer fits inside
the bobbin). Check that the four leads
Table 2: Capacitor Codes
Value
100nF
10nF
1nF
µF Value IEC Code EIA Code
0.1µF
100n
104
0.01µF 10n
103
0.001µF 1n
102
5-Band Code (1%)
orange white black yellow brown
brown black black yellow brown
brown black black orange brown
red red black red brown
red black black red brown
brown black black red brown
blue grey black brown brown
orange orange black brown brown
red red black brown brown
brown green black brown brown
brown black black brown brown
grey red black black brown
brown green black black brown
brown black black black brown
brown black black gold brown
brown black black silver brown
siliconchip.com.au
The front panel PCB (with the insulated banana sockets fitted) is secured to the main PCB assembly by fitting it over the
three switch shafts and doing up nuts on either side. Once it’s in place, the LEDs are pushed through the front panel and
soldered and the banana sockets connected to their respective test terminal pads.
from the bobbin exit through the core
notches, then secure the core assembly
using an M3 x 25mm screw, two Nylon
washers (one at the top and one at the
bottom) and an M3 nut (see Fig.5).
Cut off any excess screw length using
side cutters.
The transformer is now fitted into
its hole in the PCB with its 0.5mm primary leads to the left (ie, near Q2) and
its 0.25mm secondary leads to the right
(near D1-D4). One lead on each side
will exit on the top of the PCB, while
the other two leads exit the transformer
on the underside of the PCB.
Once it’s in position, secure the
transformer in place using three M3 x
9mm tapped Nylon spacers, three M3
x 6mm Nylon spacers and M3 screws
and washers – see Fig.6. The ends of
the windings can then be trimmed,
striped of insulation using a sharp
knife and soldered to their respective
pads on the PCB.
All that remains before the calibration procedure is to install the battery
snap connector. Loop its leads through
the two strain relief holes as shown
on Fig.4 before soldering them to
their pads.
Note that LEDs1-4 and the two banana socket terminals are not installed
at this stage.
Test & calibration
Before going further, note that the
This adaptor cable makes it easy to connect one of the Insulation Tester’s
probes to both the Active & Neutral leads of the appliance being tested at the
same time. It’s made by cutting the socket and about 150mm of lead from the
end of an extension cord, then connecting the socket’s Active and Neutral
wires together and terminating them in a solder eyelet. The Earth wire is cut
back out of the way and the cable sleeved in heatshrink and marked. The
appliance to be tested is plugged into this socket and one of the Insulation
Tester’s probes connected to the solder lug while the other probe goes to the
appliance’s external metalwork or chassis.
inverter circuit generates a high voltage (up to 500V DC) and this can give
you a nasty shock. In particular, note
that the trip current protection circuit
only works for connections between
the “+” and “–” high-voltage terminals.
It’s there to provide protection against
accidental contact with the output
terminals, mainly when the unit is
installed in its case.
Conversely, any contact between
the circuit ground (or any other low-
voltage point on the circuit) and high
DC voltage on the “+” output will not
cause the circuit to shut down. So
take care and apply power only when
your other hands are safely away from
the PCB.
To test the unit, you will need to
first solder short lengths (eg, 10mm)
of red and black mains rated wire to
the “+” and “–” high-voltage PC stakes
(the output sockets are not installed
at this stage). The test and calibration
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siliconchip.com.au
April 2015 39
to the top of the switch threads and
tighten them down to hold the assembly together.
The four LEDs can now be pushed
into their front panel holes and their
leads soldered. In addition, you will
need to solder the high-voltage output
leads to the banana socket terminals.
Preparing the case
This is the view inside the completed Appliance Insulation Tester. The
battery is clipped into a holder that’s attached to the lefthand side of the
case 15mm up from the bottom and between two sets of internal ribs.
procedure is as follows:
(1) Connect a multimeter using clip
leads across these “+” and “–“ highvoltage leads and set S2 to the 500V
position.
(2) Apply power (keep your hands
away from the leads) and check the
high-voltage output. Assuming you get
a reading, carefully adjust VR1 (using
an insulated screwdriver) for a reading
of 500V DC on the multimeter
(3) Set S2 to its 250V position and
check that the reading is 250V.
(4) Switch off and connect a 1MΩ
VR25 or VR37 resistor across the highvoltage terminal wires.
(5) Set S2 for 500V, apply power and
adjust VR2 anticlockwise until at least
the third LED (from the left) in the LED
bargraph lights.
(6) Adjust VR2 clockwise until the
second LED (the 1MΩ indicator) just
lights, then set S2 to 250V and check
that the unit shows the same 1MΩ reading on the LED bargraph. That’s it – the
calibration procedure is complete.
Final assembly
Now for the final assembly. First,
insert LEDs1-4 into their PCB holes,
40 Silicon Chip
noting that LED4 is green and that all
LEDs mount with their anode lead
towards the lower edge of the PCB. If
the LEDs all have a clear body, you can
usually determine which is the green
LED by using the diode test feature on
your multimeter. The LEDs may only
glow dimly using this test but that’s
all that’s needed to reveal the colours.
Don’t solder the LEDs at this stage
but just leave them sitting in place on
the PCB.
Next, wind a single nut all the way
down onto each switch mounting
thread. Once these are in place, fit the
red and black shrouded banana sockets
to the front-panel PCB and secure them
with the supplied nuts. Do the nuts up
tightly, then fit the front panel over
the three switches and push it down
so that the LED bargraph goes into its
rectangular hole.
Note that the corners of this rectangular hole may need to be “squared off”
using a file so that the bargraph will fit.
Now adjust the three previouslyfitted switch nuts so the LED bargraph
display sits flush with the top of the
front panel. Check also that the panel
is parallel to the PCB, then fit nuts
Only a small amount of work is required on the case. The first step is to
attach a mounting clip for the 9V battery to the inner lefthand side. That’s
done by drilling a 3mm-diameter hole
some 15mm up from the outside bottom of the box and between two sets
of ribs (see photo). The mounting clip
can then be attached using an M3 x
10mm screw and nut.
In addition, the internal ribs on the
case ends must be cut down, as they
prevent the front panel from sitting
directly onto the four corner pillars.
This can be done using side cutters
or a sharp hobby knife.
The 9V battery can then be clipped
into its holder and the completed PCB
and front panel assembly lowered
into position and secured using the
supplied screws. That done, switch it
on and check that the output voltages
(250V and 500V DC) are correct.
Finally, press S3 to check that the
Trip function works correctly. If it
does, LED2 should light to indicate
that this has occurred.
Testing appliances
When testing appliances, the condition of the mains plug, lead and
earth connection (where used) will
need to be checked. Make sure that
mains wires are not frayed, repaired
with insulation tape, broken or exposed. For earthed appliances, check
the resistance between the Earth pin
on the mains plug and any exposed
metal. There should be less than 1Ω
resistance when measuring with a
multimeter set to the low ohms range.
The accompanying photos show
how the Appliance Insulation Tester
is used to test a mains appliance. One
probe is used to simultaneously connect to both the Active and Neutral
pins of the mains plug, while the other
probe connects to any exposed metal
parts on the appliance. The appliance’s power switch must be on.
Note that some metal parts may be
painted or anodised and so contact
with bare metal will not be made with
siliconchip.com.au
POWER SWITCH
SET TO ON
SIGNAL
HOUND
USB-based spectrum
analyzers and RF recorders.
SA44B:
•
Up to 4.4GHz
•
USB 2.0 interface
•
AM/FM/SSB/CW demod
SA12B:
This jigsaw gave an insulation
resistance measurement of
>16MΩ on the 500V test range,
indicating that it is safe to use.
•
•
•
Up to 12.4GHz plus all
the advanced features
of the SA44B
AM/FM/SSB/CW demod
USB 2.0 interface
BB60C:
An insulation resistance
reading of around 4MΩ was
the result when testing this old
soldering iron. This indicates
some leakage but it’s still
safe to use. By contrast, any
appliance with an insulation
resistance of 1MΩ or less is
unsafe.
•
Up to 6GHZ
•
Simultaneously monitor two
stations or stream the entire
FM radio band to disc.
•
•
Facility for GPS time-stamp
of recorded RF streams
USB 3.0 Interface
Vendor and Third-Party
Software Available.
Ideal tool for lab and test bench
use, engineering students, ham
radio enthusiasts and hobbyists.
Tracking generators
also available.
the probe. The way around this is to
scrape away any coating (without
causing too much unsightly damage)
so that a proper connection is made
to the metal.
The Active and Neutral mains plug
connection can be made using a large
clip attached to the probe. Alternatively, the appliance could be plugged
into an extension cord mains socket
which has its Active and Neutral leads
brought out, connected together and
terminated in a crimp eyelet for easy
connection to the tester – see photos.
siliconchip.com.au
Note that normally a 500V insulation resistance test should be made but
when an appliance test fails because of
internal over-voltage protection (eg, if
MOVs are fitted), then a 250V test can
be made instead.
Any appliance that has a measured
insulation resistance of 1MΩ or less is
unsafe. Note that this does not apply to
portable RCDs that have a functional
earth or for mineral insulated metal
sheath heating elements (for more
information refer to the latest AS/NZS
SC
3760 standards).
Virtins Technology USB based
DSO’s and Signal Generators.
Bitscope Digital and Analog
USB test and measurement.
Silvertone Electronics
1/8 Fitzhardinge St
Wagga Wagga NSW 2650
Ph: (02) 6931 8252
contact<at>silvertone.com.au
April 2015 41
Got a Boat, Van, RV, 4WD, etc?
Need Light?
Really Bright
12/24V LED
Oyster Light
By Ross Tester
Here’s a low-cost, 1000+ lumen, attractive “Oyster” LED light fitting for
when you don’t have mains available. Or even if you do! It runs from 1224VDC or even from 230VAC with an optional (low cost) mains adaptor.
A
few months ago (gad, was it
really January 2013?) we presented a “LED Solar Skylight”
from Oatley Electronics. It was (and
still is!) very popular for introducing
light into dark corners.
Now they’ve come up with another
low-voltage LED-based light fitting
which is ideal for boats, caravans, RVs
and mobile homes, trucks, 4WDs . . .
in fact, anywhere you have 12-24V
DC available.
And it could also be used as a mainspowered LED light with a low cost,
optional AC adaptor (albeit with a bit
of fiddling).
There’s virtually nothing to build
with this one. The Oyster-style lamp
housing is already fitted with a PCB
containing 24 ultrabright, pure white
LEDs in two concentric rings,
connected in series/
parallel.
In the centre of
these is a driver
PCB which
supplies the
40V <at> 260mA
required by the
LEDs
Overall current
drawn from a 12V sup42 Silicon Chip
ply is around 1.1A, dropping to about
550mA from a 24V supply.
Light output from the Oyster fitting
is more than 1000 lumens. Looking
directly at it, you’d swear it was a
lot more!
Incidentally, for comparison a traditional 36W fluoro tube puts out about
3500 lumens but that’s over a much
wider length.
Oyster size is about 260mm diameter x 75mm deep, so it’s not too
dissimilar to other domestic light
fittings. An integral 235mm diameter
aluminium backing plate/heatsink is
designed to be screwed to a ceiling/
wall/bulkhead/etc and the Oyster diffuser mounts on that via a twist onto
three pins.
Now a quick word to the wise: the
diffuser is made of quite thin (and
somewhat fragile) plastic so if you go
at it like a bull at a gate, you’re liable
to put your thumb or fingers right
through it (we speak from sad experience, don’t we boss. . .).
When disassembling, which is
simply a matter of turning the diffuser
with respect to the base, treat with a
bit of care!
The LED driver
The driver PCB circuit is shown
in Fig.1.
You don’t need to worry about polarity of the DC supply as this is taken
care of by a bridge rectifier at the input.
However, this results in a not-soinsignificant voltage drop across the
two bridge rectifier diodes (2 x ~0.6V
or about 1.2V).
Therefore you’re
effectively throwing
away 10% if it is a
12V supply.
Directly
feeding the
filter capacitor (C1) rather
than through the
bridge would be
more efficient, albeit at
siliconchip.com.au
rent boost LED driver.
Inside IC1 is a switching Mosfet
which turns on and off at about
180kHz. Every time it turns off, the
magnetic field built up in L1 collapses,
inducing a higher voltage at the anode
of diode D5.
This is rectified by D5 and stored
by capacitor C3/C4. Ordinarily, this
voltage could be quite high but is
limited to 56V by zener diode ZD1
(IC1’s maximum voltage is 60V). If the
voltage across C3/C4 exceeds 56V, the
Zener conducts and stops the inverter
by applying a voltage to IC1’s feedback
pin (pin 5).
The output voltage is further
clamped to approximately 40V by the
24 high-brightness LEDs connected
in series/parallel at the output. Effectively there are 12 LEDs in series, each
dropping about 3.3V (12 x 3.3 40V).
The voltage at the feedback pin of
IC1 (pin 5) controls the duty cycle of
the Mosfet, while pin 2 (the enable
pin) can be shorted to ground to stop
the inverter working. We use this pin
to allow it to “soft start” the inverter
so it can be used with a switch-mode
supply, as detailed shortly.
24 ultra-high-brightness white LEDs are powered by an integral 12/24V driver
(ignore the DC12V sticker!). The backing hardware also doubles as a LED heatsink.
the expense of the reverse-polarity
protection provided by the bridge.
If you wanted to, you could feed
the circuit with AC (obviously via
the bridge) – say from 8 to 18 volts.
However, this would require a much
larger “filter” capacitor – the existing
one is 100F; you would need at least
ten times this for AC (preferably more
– 2200 or 3300F would not be too
much if it woud fit). This capacitor is
bypassed by a 100nF.
Power is applied directly to inductor
L1 and IC1, a 60V, 4A switching cur-
Operating on 230VAC
Oatley Electronics have a verylow-price switch-mode power supply
(KC24) which can deliver 24V DC at
up to 1A. On first glance, this would
appear to be ideal for powering the
Oyster LED light from the mains.
D5
L1
A
+
K
A
C3
100F
K
ZD1
D1 – D4
K
12–24V DC
OR
8–18V AC
A
K
A
K
4
A
100nF
IC1
XL6005
Vin
FB
A
A
1k
K
K
A
A
260mA
50V
10F*
LED OYSTER LIGHT DRIVER
K
APPROX
40V
C1
100F
WHEN POWERED BY
AC THIS CAPACITOR
SHOULD BE >1000F
K
5
GND
1
EN
2
K
A
K
A
A
25–35V
siliconchip.com.au
C4
100nF
56V
3
SW
A
K
50V
A
*SEE TEXT
1.2
(OATLEY ELECTRONICS)
2.2
–
K
K
24 x 0.5W LEDS IN
SERIES/PARALLEL
Fig.1: here’s the LED driver which is
contained in the white container at the
centre of the photo above. It supplies
around 40V DC <at> 260mA from a low
voltage DC or AC source.
April 2015 43
XL6005
D1 – D5, ZD1
(SW)
Oatley’s KC24
230V to 24V <at>
1A switch-mode
power supply.
It’s suitable for
use with the
Oyster LED
light but that
requires a small
modification, as
described in the
text to stop the
power supply
shutting down at
turn-on.
Unfortunately, appearances can be
deceiving!
By its very nature, the Oyster LED
lamp has quite a high surge current
at switch-on, which is enough to trip
the over-current protection circuitry
in the KC24 supply, which turns off
almost straight away. The high surge
current disappears, the power supply
again tries to start, resulting in a high
surge current . . . etc etc!
The result is that the Oyster LED
Lamp “strobes” - a neat feature if
you’re having a party but not quite so
good if you’re looking for light!
The KC24 power supply is sealed,
so no adjustment is possible there
(not that we’d want you to because it
is a mains-powered device and can
therefore “bite” very hard).
But it’s easy enough to open up the
LED driver in the Oyster LED Light
and modify it slightly so that it “soft
starts”, eliminating that surge current.
All you need do is insert a small
(say 10F) capacitor in series with the
“enable” pin of the IC, which introduces a delay of a few seconds before
operation is enabled. In fact, if you buy
the Oyster LED light and power supply kit from Oatley Electronics, they
will include a 10F, 35V electrolytic
capacitor for this purpose.
You’ll need to lift the enable pin (pin
WARNING: 230V LED Driver
An alternative 230V AC LED driver
(285MACC) is also available but WE
STRONGLY RECOMMEND THAT YOU DO
NOT USE THIS DRIVER .
It is not an isolated supply so the whole
LED mounting base can become live – indeed, we checked this driver with the Appliance Insulation Tester described elsewhere
in this issue and it instantly tripped it (ie,
isolation <700k).
Stick to the SAFE 12/24V LED driver and
if you want to run it from the mains, use
the KC24 switch-mode supply as detailed
above. Incidentally, we checked the KC24
supply with the same tester and it passed
with flying colours.
2) off the PCB. It’s not hard to do this
as it is a surface-mount device – melt
the solder with your soldering iron
and use a hobby knife to prise the pin
up, ensuring you’ve removed all the
solder underneath (Solder Wick is
handy for this).
Solder the positive lead of the capacitor to the pin (not the PCB!) and
the negative lead to a suitable earth
point – we used the top end of resistor
R3, as shown in the photo. That’s all
there is to it.
Power supply connections
Power wires, either 12-24V DC or
8-18V AC go through a hole in the back
of the Oyster LED light, very close to
the push-button terminal block. As
we mentioned before, you don’t need
to worry about polarity so simply
connect either wire to either terminal.
Mains supply
The KC24 power supply from Oatley
comes with a short length of mains
cable, fitted with a “figure 8” plug on
one end (the end which plugs into
the supply). The opposite end is bare
– you’ll need to fit it with a standard
mains plug.
Make sure you connect the two leads
Here’s that modification required to the LED driver – a 10F capacitor is added
in series with the “enable” pin of the IC to slow its start down. This prevents it
overloading the power supply and shutting it down. The PCB first meeds to be
removed from the white housing in the middle of the LEDs.
44 Silicon Chip
to the Active and Neutral terminals
in the plug – they’re either labelled
“A” and “N” or in some cases colour
coded, usually red (Active) and black
(neutral). In newer plugs, the colour
coding may conform to the IEC colours
of brown (Active) and blue (Neutral).
Do NOT connect anything to the
plug’s Earth terminal (“E”, green or
green-gold) and make sure that you
slide the rear cover all the way onto
the plug body.
The DC end will probably have a
4-pin DIN plug on it which has to be
cut off. Stripping the outer insulation
back will reveal four wires – red and
black (positive) and green and white
(negative). Note that – the black wire
is definitely positive – it’s a trap for
young players.
You only need to use one pair of
wires (ie, there’s no need to parallel
them), say the red and the green wires,
for DC out. These go through the hole
in the back of the Oyster LED light to
the push-button terminal block. As we
mentioned before, you don’t need to
worry about polarity.
SC
Where from, how much?
The LED Oyster Light is available from
Oatley Electronics, PO Box 139, Ettalong
Beach, NSW 2257; phone [02] 4339 3429
(www.oatleyelectronics.com).
On its own, the LED Oyster Light as
described here (with 12/24V LED driver)
sells for $25.00, inc. GST, (Cat No K400).
The KC24 230V AC to 24V DC switch-mode
supply sells for $9.95 inc. GST.
However, at the time of writing Oatley
Ekectronics are selling BOTH the LED
Oyster and switch-mode supply for just
$28.00 (Cat No K400P1), inc. GST.
And if you want two sets, the price
reduces to only $50.00 for both inc. GST
(Cat No K400P2). All prices are plus freight.
siliconchip.com.au
2015
CATALOGUE
OUT NOW!
GET YOUR FREE* COPY WHEN YOU SPEND OVER $30.
With every order of $30 or more placed via our TechStore website. *Offer valid until 23/04/2015.
NEW
QC-3840
$
8995
N600 Dual-Band Wi-Fi
Entertainment Bridge
4
$ 95
2-Channel Active
Speakers XC-5120
Connect your PC or
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• 100(D) x 97(W) x 95(H)mm
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They are the most cost-effective tablet/Smartphone connected security
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• ¼” colour CMOS sensor
• 1280x720 at 30fps
• Supports up to 32GB microSD card
(sold separately)
• Supports iPhone®, iPad®, Android® Smartphones
NEW
$
3495
INDOOR QC-3840 $149
OUTDOOR QC-3846 $169
ALSO AVAILABLE:
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Single Board Mini PC + Arduino = pcDuino! NEW
pcDuino is a high performance and cost-effective mini PC combined
with connectivity to Arduino shields. Capable of running KODI and
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Take your pcDuino projects to the next level by adding a 7” LVDS*
colour LCD screen with capacitive touch capability (XC-4356).
Extremely easy to install, this 1024x600 pixel interactive touchscreen
display is the perfect addition for the pcDuino V3.
†
LVDS & Wi-Fi only on XC-4350 * LVDS = Low-Voltage Differential Signaling
PCDUINO V3.0 NANO XC-4352
PCDUINO V3.0 WITH WI-FI XC-4350
7” LCD TOUCHSCREEN TO SUIT XC-4350 XC-4356
NOW OPEN: WARWICK FARM
siliconchip.com.au
Catalogue Sale 24 March - 23 April, 2015
$
DOUBLE
POINTS
8995
XC-4352
NEW
$
139
XC-4356
NEW
$
129
XC-4350
CNR OF SAPPHO ROAD & HUME HIGHWAY
WARWICK FARM NSW 2170 PH: (02) 9821 3100
To order phone 1800 022 888 or visit www.jaycar.com.au
April 2015 45
DOUBLE POINTS ON OUR HIGH PERFORMANCE WIRELESS MODEM ROUTERS FOR REWARDS CARD HOLDERS*
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*
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DOUBLE
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Why pay more for the same features? Our range of
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• Wi-Fi Protected Setup (WPS) fast setup for
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• Supports UPnP, IP/MAC filtering, DMZ and
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Wireless N150
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YN-8325
Functions as a router, access
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• 1 x RJ-45 WAN port
FASTEST
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$
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YN-8327
Functions as a router, access
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• 802.11b/g/n
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• 1 x RJ-45 WAN ort
REWARDS CARD HOLDERS:
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$
Wireless N300
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WITH USB SHARING
9995
Wireless AC750
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YN-8342
Provides full ADSL2/2+
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• 802.11b/g/n
• Up to 300Mbps (2.4GHz band)
YN-8329
Functions as a router, access point, Wi-Fi range
extender, Wi-Fi bridge or a WISP with 3 x high gain
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• 802.11ac/b/g/n
• Up to 433Mbps (5GHz band) /
Up to 300Mbps (2.4GHz band)
• 1 x RJ-45 WAN port
BUY 2 & SAVE UP TO 35% FOR REWARDS CARD HOLDERS*
*Valid for selected products shown below. See Page 8 for details or ask us how in stores.
REWARDS CARD OFFER
BUNDLE DEAL!
$
99
SAVE OVER $48
REWARDS BUNDLE: VALUED OVER $147
BUNDLE DEAL INCLUDES:
HIGH POWER WIRELESS OUTDOOR ROUTER/RANGE EXTENDER
802.11N YN-8330 $89.95
Extend your wireless network coverage with this high power outdoor router/range
extender. With a built-in 12dBi directional antenna and wireless power of 600mW,
this unit is ideal for long range wireless network up to 150Mbps.
• 802.11b/g/n standards
• LAN port 10/100 (featuring PoE)
1995
$
$
FROM
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2495
YN-8077
Power Wireless
Add Additional Ethernet Ports
network performance with these N-Way
Points WITHOUT MAINS Improve
unmanaged Ethernet switches. Features 8 x RJ-45
YN-8410
This PoE (Power Over Ethernet)
kit allows you to power wireless
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without the need to have a
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• Includes input and output leads
• 2.1mm DC plug/socket
ports and supports auto-negotiation and cable
length detection. Mains or USB powered.
10/100MBPS SWITCH YN-8077 $24.95
10/100/1000MBPS GIGABIT SWITCH
3495
Add Wi-Fi
Connectivity YN-8326
Plug-and-play N300 PCI-E
wireless network card for PC
motherboards lacking Wi-Fi.
Up to 300Mbps.
YN-8078 $59.95
YN-8352
N150 NANO USB 2.0 WIRELESS NETWORK ADAPTOR
YN-8309 $19.95
$
CAT5E LEAD 30M TO SUIT EXTENDER INSTALLATION
YN-8208 $37.95
WB-2030 $1.65/m
46 Silicon Chip
Page 2
$
YN-8328
Handy USB2.0 devices to extend your wireless network.
CAT5E 1GBPS 350MHZ:
5M YN-8204 $8.95
10M YN-8205 $14.95
15M YN-8206 $21.95
20M YN-8207 $24.95
30M YN-8208 $37.95
CAT6A 10GBPS 750MHZ: NEW
DOUBLE
2M YN-8294 $6.95
POINTS
3M YN-8295 $8.95
5M YN-8296 $12.95
10M YN-8297 $21.95
CAT5/6 CABLES SOLD BY METRE: also available in 100m bulk rolls.
CAT 5 8-CORE STRANDED NETWORK CABLE
CAT 6 SOLID CORE UTP NETWORK CABLE
FROM
Connect to High Speed Wireless Network
DOUBLE POINTS FOR
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WB-2020 $1.35/m
FROM
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99
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INDOOR YN-8328 $39.95
Extend your network range up to 300m using your
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OUTDOOR YN-8348 $49.95
SINGLE PORT KIT YN-8352 $99
THREE PORT KIT YN-8354 $129
AC600 Dual Band, max 150 + 433Mbps.
N150 9dBi 5M cable, max 150Mbps.
Improve 3G/4G Signals
Connect these 3G antennas with FME connector to your 3G/4G
wireless modem to speed up wireless Internet and boost reception.
5DBI 2M AR-3310 $49.95
7DBI 3M AR-3312 $69.95
FME CABLES AVAILABLE SEPARATELY:
SUITS INDUCTION 3G AR-3316 $16.95
SUITS SIERRA 312U AR-3317 $16.95
SUITS HWAWEI E160/618 AR-3318 $16.95
SUITS SAMSUNG S2/S3 AR-3319† $16.95
SUITS TELSTRA 4G USB MODEM AR-3320 $16.95
Available in selected stores only. Call ahead to check stock.
†
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1695
ea
$
REWARDS CARD OFFER
$
FROM
49
95
50%
OFF*
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*Valid with purchase of
AR-3310 or AR-3312.
siliconchip.com.au
Catalogue Sale 24 March - 23 April, 2015
DATA CONVERTERS
$
$
FROM
2795
RS-232 DB9 Converters
Connect a variety of RS-232 devices to your
modern computer with these adaptors.
5995
$
SAVE $20
XC-4135
RS-232 DB9 TO USB ADAPTOR XC-4927 $27.95
RS-232 DB9 TO USB 1.5M XC-4834 $29.95
RS-232 DB9 TO USB MICRO-B 600MM XC-4135 $29.95
99
SAVE $30
RS-485/422 to USB Converter
XC-4132 WAS $79.95
Wire up an RS-485/422 device to the 4 socket terminal block to
give your hardware USB connectivity. Surge protected. Suitable for
industrial, military, marine, science and custom built applications.
• 610mm USB A Male to Male cable included
Serial to Ethernet Converter
XC-4134 WAS $129
This smart device allows computers to connect to serial devices over
Ethernet and remotely accessed through a simple web interface.
• Supports 10/100Mbps
• Converts RS-232 , RS-485 and RS-422
REWARDS CARD HOLDERS:
PORTABLE MEDIA BUNDLE DEAL
DATA LEADS & ADAPTORS
YN-8426
FROM
9
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USB 2.0 Leads
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USB A MALE TO A MALE 1.8M
WC-7704 $9.95
USB A MALE TO B MALE 1.8M
WC-7700 $9.95
USB A MALE TO MINI-B MALE 2M
WC-7792 $14.95
FROM
9
$ 95
USB 2.0
Extension Leads
USB A Male to A Female leads
to extend the range of your PC
peripherals.
1.8M WC-7702 $9.95
3.0M WC-7703 $11.95
USB A MALE TO MICRO-B MALE 2M
$
FROM
2495
All units feature built-in extenders to run
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USB 2.0 5M
USB 3.0 5M
USB 2.0 10M
USB 2.0 20M
XC-4839 $24.95
XC-4126 $34.95
XC-4120 $39.95
FREE USB 2.0 OTG ADAPTOR FOR
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Valid with purchase of XC-4884.
*
9
WC-7725 VALUED AT $4.95
$ 95
1495
ea
$
USB 3.0 Leads
High quality data leads providing 10 times faster
speed than USB 2.0 leads. 1.8m long.
USB A MALE TO A MALE
WC-7770 $14.95
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WC-7772 $14.95
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WC-7774 $14.95
RS232 Serial Cables
Variety of DB9 and DB25 serial
cables to suit your applications.
1.8m long.
DB9 MALE TO DB9 MALE
WC-7535 $9.95
$
2995
USB RJ45
Extension Adaptor XC-4884
DB9 MALE TO DB9 FEMALE Connect USB devices to a computer
WC-7534 $9.95
DB25 MALE TO DB9
FEMALE WC-7516 $11.95
DB25 MALE TO DB25
FEMALE WC-7508 $13.95
XC-4946
XC-5176
XC-4124 $49.95
WC-7796 $14.95
FROM
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Active Extension Leads
from up to 50m away via a standard Cat5
network cable (sold separately).
• PC and MAC compatible
• Supports USB 1.1
• Transmitter and Receiver included
REWARDS BUNDLE:
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BUNDLE DEAL INCLUDES:
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READER YN-8426 $59.95
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BUNDLE DEAL!
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SAVE OVER $50
Share and transfer files from memory
cards/USB storage devices wirelessly
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hotspot. Rechargeable, USB charge cable included.
• 105mm x 650mm x 11mm
USB 2.0 10 PORT USB HUB XC-4946 $49.95
Powered by USB or mains, this handy USB hub features a twoposition switch which can turn all ports on, or only ports 7 - 10.
MINI USB/MICROSD CARD SPEAKER XC-5176 $24.95
Rechargeable amplified stereo speaker that plays MP3 files off a
microSD card or a USB dlash drive. Recharges via USB.
• 74(L) x 50(W) x 52(H)mm
FLEXIBLE 10-LED USB LIGHT ST-2807 $14.95
A handy on/off touch lamp for computers. Gooseneck 315mm long.
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4
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Serial SATA Cables
A range of SATA data and power cables for use with
computers and external serial ATA devices.
SATA TO SATA DATA PL-0978 $5.95
HDD POWER TO 2xHDD PL-0750 $4.95
HDD POWER TO 2xSATA PL-0759 $7.95
siliconchip.com.au
$
3495
SATA to USB 3.0 Adaptor
XC-4149
A simple way to access files on a SATA hard drive
you no longer have installed. Includes USB 3.0
cable and mains adaptor.
To order phone 1800 022 888 or visit www.jaycar.com.au
$
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USB 3.0 3.5” SATA
HDD Enclosure XC-4667
Easy installation, just two screws to remove the
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• Plug ‘n’ Play, hot swappable
• Supports SATA I/II/III
See terms & conditions on page 8.
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USB 3.0 SATA HDD Docks
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Suits 2.5”/3.5” SATA HDD’s (not included). USB 3.0
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SINGLE XC-4696 $39.95
DUAL XC-4697 $59.95
SINGLE CLOUD DOCK XC-4691 $59.95
April 2015 47
Page 3
FREE 3m HDMI CABLE FOR REWARDS CARD HOLDERS* WV-7916
Valid with purchase of AC-1639, XC-4973 or AC-1617.
*
WV-7916 VALUED AT $24.95
Convert Your PC To
A Modern Media Centre
$
$
99
AC-1639
AC-1617
Enjoy high definition video with audio on your big screen. These smart
devices convert your VGA equipment (computers, laptops) to newer
HDMI equipped displays via the VGA or USB 3.0 ports.
SAVE $15
VGA/USB TO HDMI CONVERTER AC-1639 WAS $79.95
USB 3.0 (VIDEO/AUDIO) TO HDMI CONVERTER XC-4973
VGA & R/L AUDIO TO HDMI SCALER CONVERTER AC-1617
$
8995
XC-4973
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FREE LCD SCREEN CLEANING KIT
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*
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*
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$
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VGA to Composite
and S-Video Converter XC-4871
USB to DVI Adaptor XC-4879
Connect your monitor to the computer via
the USB 2.0 port without buying additional
A versatile device that lets you use your wide screen
graphics cards. Use up to 6 simultaneously to
plasma or LCD screen as a computer monitor. Great
run screen arrays. Powered via USB.
for watching DVDs, gaming, presentations, or just
having a big screen on your computer. No software
is required and powered from USB Port.
$
DVI-A Plug to VGA Socket
VGA CONVERTER WQ-7440 $29.95
HDMI CONVERTER WQ-7442 $29.95
DVI CONVERTER WQ-7444 $29.95
6995
DOUBLE
POINTS
1295
ea
Connect modern computers with a Mini
DisplayPort® to a VGA, HDMI or DVI equipped
monitor or projector. All leads 1.8m long.
• Mini DisplayPort® 1.1a compliant
• Supports up to 1080p resolution
DOUBLE
POINTS
Limited stock.
Available in-store only.
DOUBLE
POINTS
Mini DisplayPort
Converter Leads
$
Ideal for connecting an old game console, VHS
player, etc to your computer monitor or plasma TV.
Has VGA loop through so you can have a computer
and composite/S-video source connected to the
same display.
Securely mounts onto a variety of desk thicknesses
for landscape or portrait positions. Features fully
adjustable arms and standard VESA mounting with
10kg per monitor load. Monitors not included.
WQ-7440
4995
Composite and S-Video to
VGA Video Converter XC-4906
4995
LCD Monitor Desk Brackets
SINGLE CW-2831 $49.95
DUAL CW-2833 $69.95
DOUBLE
POINTS
PA-0897 $12.95
For connecting DVI-A or DVI-I video cards with
VGA monitors.
ALSO AVAILABLE:
DVI SOCKET TO SOCKET ADAPTOR
PA-0896 $14.95
Compatible with DVI-I, DVI-D and DVI-A male
connectors.
DOUBLE
POINTS
6995
$
2-Port VGA/Audio Splitter
YN-8075
Splits a computers VGA and audio signal to two
identical streams. The splitter provides fast, flexible
solutions for test bench facilities, data centres or
video broadcasting. Includes mains power adaptor
and 1.8m male to female VGA cable.
• Bandwidth up to 500MHz
• Resolution up to 1920 x 1200 and 1080p
9995
2-Port KVM Switch
WITH HDMI/MIC/AUDIO SUPPORT
YN-8094
Control 2 computers with one keyboard and mouse.
Will also share stereo audio and mic so only one
set of speakers/mic is needed.
• 1 x input cable with 2 x HDMI, 2 x USB and 2 x
3.5mm plugs
• 3 x HDMI to DVI adaptors included
(1 for monitor, 2 for PCs)
TELECOMS
WC-7590 DOUBLE
POINTS
FROM
$
Monitor Cables
1195
A variety of DVI, VGA and XVGA
cables to suit your unique applications.
1.8M VGA DB15HD MALE TO
DB15HD FEMALE WC-7500 $11.95
1.8M VGA DB15HD MALE TO
DB15HD MALE WC-7582 $11.95
2.0M DVI TO DVI WC-7590 $29.95
5M XVGA DB15HD MALE TO
DB15HD MALE WC-7588 $39.95
10M XVGA DB15HD MALE TO
DB15HD MALE WQ-7258 $49.95
48 Silicon Chip
Page 4
7
$ 95
REWARDS CARD OFFER
RJ12 6P/4C Wall
Phone Bracket YT-6062
Designed to allow easy installation of telephones
which have standard US modular wall mountings.
• Fits standard Australian electrical switch plate
• ACA approved
RJ12 6P/4C LEADS SOLD SEPARATELY:
5.0M YT-6049 $7.95
10M YT-6041 $11.95
15M YT-6043 $14.95
BUY 2 FOR
Cat 5 UTP
Splitter
$
23
90
SAVE $10
YT-6090 $16.95
Save time, money and space! Usually used in pairs,
this UTP splitter enables two different devices to
share the same Cat5 cable.
NOTE: Cannot be used to run two computers from one
network and not suitable for gigabit networks.
Follow us at twitter.com/jaycarAU
FROM
1495
$
IP67 RJ45 Connectors
High quality RJ45 connectors suitable for harsh
environments.
RJ45 SOCKET PS-1450 $27.95
RJ45 PLUG PP-1452 $14.95
siliconchip.com.au
Catalogue Sale 24 March - 23 April, 2015
FREE IN/OUT THERMOMETER FOR REWARDS CARD HOLDERS* XC-0321
Valid with purchase of HB-5120 / 25 / 30 or HB-5170 / 74 / 80 / 82 series of Rack Mount Cabinets.
*
XC-0321 VALUED AT $19.95
19” Rack
Mount Cabinets
Jaycar’s 19” rack mount cabinets are ideal for IT
or phone system installations, studios and PA
systems, with a size and configuration to suit your
application. These cabinets are solid steel powder
coated to provide high strength and rigidity under
load and are packed flat for convenient transport.
Coupled with our wide range of accessories and
options, these 19” rack mount hardware are value
for money and offer you outstanding features found
on more expensive units. Unbeatable value!
TECH TIP! SAVE TIME & MONEY
Jaycar also stocks highly practical and
value-for-money network installation and
troubleshooting testers.
See our website or ask us now.
HB-5125
FROM
FROM
6495
SAVE UP TO $20
139
SAVE UP TO $40
Equipment Cabinet
Fixed Frame
$
$
ALUMINIUM FRONT PANEL
1U HB-5120
HB-5170
WAS $69.95 NOW $64.95 SAVE $5
CLEAR TEMPERED GLASS DOOR
6U HB-5180
WAS $219 NOW $199 SAVE $20
WAS $159 NOW $139 SAVE $20
12U HB-5182
12U HB-5174
WAS $109 NOW $99 SAVE $10
HB-5182
Swing Frame
CLEAR TEMPERED GLASS DOOR
6U HB-5170
2U HB-5125
FROM
199
SAVE UP TO $40
$
WAS $299 NOW $259 SAVE $40
WAS $229 NOW $189 SAVE $40
3U HB-5130
WAS $129 NOW $109 SAVE $20
HANDY TOOLS FOR
NETWORK INSTALLERS
15% OFF THESE 19” RACK MOUNT ACCESSORIES FOR REWARDS CARD HOLDERS*
*See Page 8 for list of products.
HB-5432
YN-8046
$
FROM
$
2495
Rack Cable Supports
2995
Patch Lead
Take the pain out of wiring and fault-finding rack
Management Panel HB-5434
cabinets. These high quality supports keep your
1U size, keeps all your patch leads under control.
cables organised and neat, and provides strain relief
at the same time.
1U HB-5430 $24.95
2U HB-5432 $29.95
HB-5454
$
FROM
$
4995
Cat 5/6 24-Port Patch Panels
Sleek attractive looking rack mount 24 port patch
panel with a hard metal exterior. Numbered ports
and a labelling area for each port.
1U, SUITS CAT5E YN-8046 $49.95
1U, SUITS CAT6 YN-8048 $69.95
2295
Cat5 Adjustable
Punch-Down Tool TH-1740
Designed for seating wire into terminal blocks
and has an adjustable internal impact mechanism.
Supplied with 88 blade. 152mm long.
ALSO AVAILABLE:
110 REVERSIBLE KRONE BLADE TO SUIT
TH-1743 $17.95
HB-5420
FROM
FROM
1050
$
Blank Panels
Black powder coated panels for filling in unused
space or configuring to your own requirements.
Mount hardware included.
1U BLANK PANEL HB-5420 $10.50
2U BLANK PANEL HB-5422 $12.95
1U BLANK VENTED HB-5424 $18.95
1U BLANK VENTED HB-5426 $27.95
$
$
49
Rack Shelves
6995
6-Way Power
Distribution Unit MS-4094
Ideal for equipment that you want to include in your
19” rack but doesn’t have rack-mounting ears. Each
Power up to six 240VAC components in
shelf is punched with ample slots for ventilation and
your rack setup. Surge/overload protected
takes loads of up to 20kg.
and fits any standard 19” rack. Includes
1U FIXED SHELF HB-5452 $49
1.6m power lead.
• 1U rack space
2U FIXED SHELF HB-5454 $69
$
1995
6P/8P Modular Crimp Tool
TH-1935
This tool will crimp 6P2C, 6P4C-RJ11, 6P6C-RJ12
and 8P-RJ45 plugs. Also cuts and strips the cable.
1U SLIDING SHELF HB-5450 $99
DOUBLE POINTS FOR REWARDS CARD HOLDERS ON THESE UNINTERRUPTIBLE POWER SUPPLIES*
*Valid for purchase of MP-5224, MP-5201, MP-5207 or MP-5212.
DOUBLE
POINTS
Protect your valuable setup with our value-for-money Uninterruptible Power Supplies. Keep your
systems running long enough to save critical data when the mains power fails.
MP-5224
MP-5201
MP-5207
MP-5212
Features
Line interactive,
economical model
Line interactive, desktop
model
Line interactive, smart LCD
desktop model
On-line, smart LCD rack
mountable (2U height)
Load Rating
600VA, 300W
650VA, 360W
1500VA, 900W
1000VA, 700W
Internal SLA Battery
12V/7AH x1
12V/7AH x1
12V/9AH x2
12V/7AH x3
Output Waveform
Modified Sine Wave
Modified Sine Wave
Modified Sine Wave
Pure Sine Wave
Transfer Time
<10 ms
<10 ms
<10 ms
Instant
Power Outlets
6 x AUS (3 bypass, 3
mains)
2 x AUS mains
2 x AUS mains
6 x IEC
Backup Time (Typical)
31 mins / 11 mins /
4.5 mins
25 mins / 9 mins / 5 mins
94 mins / 49 mins /
31 mins
95 mins / 47 mins /
32 mins
$
99
$
99
$
MP-5224
$
MP-5201
siliconchip.com.au
To order phone 1800 022 888 or visit www.jaycar.com.au
See terms & conditions on page 8.
449
MP-5212
299
MP-5207
April 2015 49
Page 5
REWARDS CARD OFFER
REWARDS CARD OFFER
BUY 2 FOR
BUY 2 FOR
$
159
$
QC-3834
299
Wireless Surveillance Package
REWARDS BUNDLE:
VALUED AT $328
QC-3844
SAVE $39
SAVE $39
VGA 480p
HD 720p
QC-3844
$169
QC-3834
$99
WIRELESS SURVEILLANCE SOLUTIONS
NEW
BUNDLE DEAL INCLUDES:
BASE UNIT WITH 1 CAMERA QC-3675 $219
REWARDS CARD OFFER
BUNDLE DEAL!
$
Simple to install wireless surveillance system with 7” LCD
and infrared camera for day/night recording to microSD
card (sold separately). Expandable up to 4 cameras.
249
SAVE $79
ADDITIONAL CAMERA QC-3677 $109
TECH TIP! BENEFITS OF IP CAMERAS
• Remote accessibility
• Integration with other systems
• Two way communications
....and MORE! Ask us about our full range.
Monitor Your Workspace From Your Smartphone
Create a professional monitoring system with these DIY Wi-Fi IP cameras. Features pan/tilt and
infrared LEDs for maximum visibility day or night. View live feed with your smartphone using free to
download App, broadband required.
UHF CB RADIOS
AC-1730
$
REWARDS CARD OFFER
REWARDS BUNDLE:
VALUED OVER $228
$
HDMI Extenders Over Cat5e/6
BUNDLE DEAL!
$
FROM
6495
199
Extend your HDMI signal using Cat5e/6 cable.
Use your remote in either location with the built-in
infrared transmitter.
30M* with 2 x Cat5e/6. AC-1730 $64.95
50M* with 1 x Cat5e/6. AC-1732 $139
SAVE $29.95
BUNDLE DEAL INCLUDES:
* Depending on cable used and resolution.
See website for details.
5W UNDER-DASH UHF DC-1120 $149
HIGH GAIN ANTENNA to suit DC-1120. UHF 5dBi with 5m cable.
3W Floating UHF
REWARDS CARD OFFER
DC-1074 $119
A robust floating 80-channel
transceiver with transmission range
up to 10km line of-sight*.
Featuring CTCSS function,
Hi/Lo power output, auto
squelch function and low
battery display. Includes a
Li-ion rechargeable battery,
AC adaptor and charging
cradle.
• IP67 rated
BUY 2 FOR
$
199
SAVE $39
DOUBLE
POINTS
$
Composite AV Extender
Balun over Cat5 QC-3681
Transmit crystal-clear audio and video
signals over long distances via economical
Cat5 cable. Ideal for extending the range
of your remote control. The signals can be
transmitted up to 300 metres on UTP.
AR-1819 $19.95
DOUBLE
POINTS
NEW
FROM
$
4995
MP-3332
VGA Extender
over Cat5 AC-1671
Transmits VGA and audio signals
across a standard CAT5 cable
for distances up to 300 metres.
Suitable for VGA cable runs
through existing wiring in a wall
or ceiling. Sender and receiver
pair with plugpacks included.
• Supports up to 1920x1200
resolution
NEW
5995
Keep Your Laptops/USB Devices Charged! 90W Automatic Car Laptop Power Supply
Replace your lost or broken laptop charger without having to buy
the expensive branded replacements. These mains power supplies
include 1A or 2.1A USB charging ports and quick-change output
plugs. See website for specifications and compatibility.
65W FIXED-SLIM MP-3321 $49.95
90W AUTOMATIC-SLIM MP-3332 NEW $79.95
120W FIXED-SLIM MP-3329 $89.95
144W MANUAL MP-3471 $119
*Typical open field (line-of-sight), range will vary in built-up areas.
119
$
SPARE IR RECEIVER
Compact under-dash unit with long transmission range up to 20km line of
sight*. Features 80 channels, channel scan, repeater access, CTCSS, and
signal strength meter. Microphone, lead and mounting bracket included.
DC-3078 $79.95
89
MP-3323
High efficiency, ultra-slim power supply with automatic output that
connects to your car’s cigarette lighter socket. Features a 2.4A USB
port, LCD display and includes 13 interchangeable plugs to suit most
laptops. See website for compatibility.
• Input voltage: 12VDC
• Output voltages: 14-24VDC / 5VDC (USB)
• Output current: 6A / 2.4A (USB)
• 64(L) x 50(W) x 17(H)mm
DOUBLE POINTS ON THESE REPLACEMENT BATTERIES AND CHARGER FOR REWARDS CARD HOLDERS*
Valid for purchase of SB-1770, SB-1771, SB-1774, SB-1775, SB-1653, SB-1654, SB-1651, SB-1646, SB-1634, SB-1648 or MB-3563.
*
Rechargeable Cordless Telephone Batteries
Suitable for Uniden or Panasonic cordless phones, all
batteries are wrapped with suitable connectors.
DOUBLE
POINTS
FROM
1195
$
Non-Rechargeable
Computer Backup Batteries
See website for compatibility or speak to us
to find a suitable replacement battery for you.
DOUBLE
POINTS
SB-1654
FROM
DOUBLE
POINTS
1495
$
BATTERY TYPE
GP BATTERY NO.
PRICE
High capacity batteries used in many computers
to retain critical system information while the
computer is switched off.
SB-1653
2.4V 650mAh Ni-MH
65AAAH2BMS
$17.95
SB-1654
2.4V 650mAh Ni-MH
65AAAH2BMJ
$17.95
HALF AA 900mAh SB-1770 $11.95
HALF AA WITH TAGS 900mAh
SB-1651
2.4V 800mAh Ni-MH
80AAM2BMS
$17.95
SB-1646
3.6V 650mAh Ni-MH
GP65AAAH3BMS
$14.95
SB-1634
3.6V 850mAh Ni-MH
GP85AAALH3BMS
$28.95
SB-1648
3.6V 1000mAh Ni-Cd
GP100AAS3BMS
$16.95
SB-1771 $13.95
AA 2000mAh SB-1774 $16.95
AA WITH TAGS 2000mAh SB-1775 $18.95
50 Silicon Chip
Page 6
Follow us at facebook.com/jaycarelectronics
$
3495
Panasonic Ni-MH Battery Charger MB-3563
Charges both AA and AAA Ni-MH batteries. The included Eneloop
batteries are pre-charged and will last over 3 times longer than regular
rechargeable batteries.
• Includes 4 x AA Eneloop rechargeable batteries
siliconchip.com.au
Catalogue Sale 24 March - 23 April, 2015
BUILD YOUR OWN ARDUINO SERIAL ADAPTOR
NEW
FOR DATA AND TELEPHONE COMMUNICATIONS
DOUBLE POINTS FOR REWARDS CARD HOLDERS*
DOUBLE
POINTS
DOUBLE
POINTS
PS-0806
FROM
4
PCB Mount Data Connectors
Handy right-angle connectors to complete your
Arduino communication projects.
RJ45 8/8 SOCKETS PS-1478 $2.45
DB9 DATA PLUG PP-0803 $2.95
DB9 DATA SOCKET PS-0806 $2.95
6
$ 95
DOUBLE
POINTS
2295
$
USB-Serial Adaptor Module
XC-4241
Connects to the USB port on your computer and
acts as a virtual serial port, converting the USB
signals to either 5V or 3.3V logic level serial data.
Quick and simple way of making a PCB within
seconds! Though waterproof, the ink can be
washed off with metho, turps, etc.
• Line width fine approx. 0.6 mm
MAX232 RS-232 IC ZK-8824
Logic Level Converter Module
Dual receiver/transeiver IC to suit EIA/TIA-232E and XC-4238
V.28/V.24 communications interfaces.
This module easily connects different logic voltage
• +5V powered
levels together for bi-directional communication
on up to 4 channels, allowing you to use lowvoltage sensors with a 5V microcontroller.
DOUBLE
POINTS
$
Etch Resistant
Pen TM-3002
DOUBLE
POINTS
$ 95
2
$ 45
$
OLED Shield XC-4269
Use this handy shield to connect the 128x128 pixel
OLED module (XC-4270) to your Arduino projects.
Display menus on the screen, use the analogue
joystick for selection, and give audible feedback.
REWARDS ETHERMEGA BUNDLE:
VALUED OVER $184
$
Press ‘n’ Peel
PCB Film
DOUBLE
POINTS
2995
4
$ 95
Valid for purchase of PS-1478, PP-0803, PS-0806, ZK-8824, XC-4238, XC-4241, XC-4269 or XC-4270.
*
4995
OLED Display Module
2495
SAVE OVER $10
HG-9980 WAS $35
The easiest way to make PCBs from CAD software
or magazine PCB layout artwork. Simply print/copy,
iron on, peel off and etch!
• Includes 5 sheets of 215 x 280mm film
XC-4270
High resolution, full colour 128x128
pixel OLED module perfect for your
display needs.
• 28.8 x 26.8mm active display area
$
BUNDLE DEAL INCLUDES:
ETHERMEGA BOARD XC-4256 $119
The ultimate network-connected Arduino-compatible board combining
ATmega2560 MCU, onboard Ethernet, a USB-serial converter, a
microSD card slot, Power-Over-Ethernet support (use XC-4254, sold
separately), and an onboard switchmode voltage regulator.
REWARDS CARD OFFER
BUNDLE DEAL!
$
MEGA PROTOTYPING SHIELD XC-4257 $17.95
CLASS 10 32GB MICROSD CARD XC-4992 $47.95
159
SAVE OVER $25
PCB Etching Kit
1995
SAVE $8
HG-9990 WAS $27.95
An ideal kit for anyone needing to etch a circuit
board - complete with an assortment of double
sided copper boards, etchant, working bath and
tweezers. See website for contents.
ARDUINO ESSENTIALS
2
3ea
$ 95
$ 95
Stackable Header Set
HM-3207
The perfect accessory to the ProtoShields and
vero type boards when connecting to your Arduino
compatible project.
• 2 x 8 pin and 2 x 6 pin included
FROM
9
$ 95
PB-8814
Solderless Breadboards
Three sizes of breadboards to suit
all your project needs.
300 TERMINAL HOLES PB-8832 $9.95
640 TERMINAL HOLES PB-8814 $19.95
1280 TERMINAL HOLES PB-8816 $39.95
siliconchip.com.au
WC-6021
9
$ 95
Mixed 10-Piece Jumper Leads ATmega328P Microcontroller
For use in arduino projects, school experiments, or
RC and other hobbyist activities. 155mm long.
PLUG TO SOCKET/SOCKET TO SOCKET
WC-6021 $3.95
PLUG TO PLUG WC-6022 $3.95
1495
$
Resistor Pack 300-Pieces
RR-0680
This assorted pack contains 5 of virtually each value
from 10Ω to 1MΩ.
• 0.5W 1% mini size metal film
See website for full contents.
To order phone 1800 022 888 or visit www.jaycar.com.au
ZZ-8726
An Atmel AVR ATmega328P microcontroller to build
customised Arduino compatible projects. Includes
16MHz crystal oscillator.
• Pre-installed Arduino Uno bootloader
$
2495
LED Pack 100-Pieces
$
2695
4-Channel PoE
Midspan Injector XC-4254
Power up to four EtherMega’s (XC-4256) or
EtherTen’s (XC-4216) with DC from a low cost
plugpack across your home or office network
cables. It isolates and powers the correct wires
automatically.
$
3495
Light Duty Hook-up
ZD-1694
Wire Pack - 8 colours
This assorted pack contains 3mm and 5mm LEDs of WH-3009
mixed colours. Even includes 10 x 5mm mounting
Quality tinned hook-up wire on plastic spools. 8 rolls
hardware FREE! See website for full contents.
included, each roll a different colour.
• Red, green, yellow, orange LEDs
• 25m on each roll
See terms & conditions on page 8.
April 2015 51
Page 7
PERIPHERALS ON SPECIAL
NEW STOCK
LOW
PRICES
UP
TO
40%
OFF
IS LIMITED. ACT NOW TO AVOID DISAPPOINTMENT.
SAVE
SAVE
25%
UP TO
40%
AM-4073
Desktop
Multimedia Microphones
Foldable Keyboard
Ideal for voice recognition software or simply
recording voice and sound. Low noise levels
and wide frequency response.
WITH BLUETOOTH® TECHNOLOGY
OMI-DIRECTIONAL MICROPHONE
AM-4087 ORRP $12.95 NOW $9.95 SAVE $3
UNI-DIRECTIONAL GOOSENECK
MICROPHONE AM-4073
ORRP $69.95 NOW $39.95 SAVE $30
XC-5202
ORRP $39.95 NOW $29.95 SAVE $10
This full 66 key keyboard folds in half from a
285mm to a modest 133mm so it’s easy to transport
without damaging the keys. Bluetooth® wireless
technology means no annoying cables at all.
MUST HAVE TOOL KITS
SAVE
20%
30pc Electronic
Tool Kit
USB KVM &
Transfer Cable XC-4949
TD-2107 WAS $29.95
NOW $24.95 SAVE $5
An electronic tool kit with
all the essentials - cutters,
pliers, screwdrivers etc. Ideal
for servicing the computer.*
ORRP $49.95 NOW $39.95 SAVE $10
Control another computer or transfer files
between PC, Mac or even Android devices
without the hassle of a network. Plug and
play, no software needed on PC or Mac.
Free App available for Android.
TD-2113 WAS $29.95
NOW $19.95 SAVE $10
All the tools you need to
take apart your iPhone for
DIY repair jobs.*
SAVE
UP TO
40%
CW-2870
UP TO
*Special only, new lower prices
do not apply. See website for full
contents of tool kits.
35%
WC-7510
Adaptors and Cables
SAVE
30%
19pc Repair Kit
for iPhone
PA-0926
SAVE
SAVE
15%
Articulating Monitor Brackets
USB A SOCKET TO A PLUG ADAPTOR RIGHT ANGLE UP
PA-0926 ORRP $7.95 NOW $5.95 SAVE $2
5 PIN PLUG TO 6 PIN MINI DIN SOCKET ADAPTOR
PL-0940 ORRP $7.95 NOW $4.95 SAVE $3
5 PIN SOCKET TO 6 PIN MINI DIN PLUG ADAPTOR
PL-0941 ORRP $7.95 NOW $4.95 SAVE $3
RS232 EXTENSION LEAD – 3M
WC-7510 ORRP $19.95 NOW $15.95 SAVE $4
RS232 SERIAL LAPLINK CABLE – 1.8M
WC-7514 ORRP $19.95 NOW 11.95 SAVE $8
Position your monitor to the optimum viewing angle.
Tilt the monitor up 90°, down 45°, pan it 180°, and
rotate around a 360° range. Both models conform to
the standard VESA mount.
WALL MOUNT CW-2872 ORRP $99 NOW $79 SAVE $20
DESK MOUNT CW-2873 ORRP $69 NOW $59.95 SAVE $9.05
ALSO AVAILABLE FOR iMAC:
WALL MOUNT CW-2871 ORRP $79 NOW $47.95 SAVE $31.05
DESK MOUNT CW-2870 ORRP $89 NOW $59.95 SAVE $29.05
EARN A POINT FOR EVERY DOLLAR SPENT AT ANY
JAYCAR COMPANY STORE* & BE REWARDED WITH
A $25 REWARDS CASH CARD ONCE YOU REACH
500 POINTS! *Conditions apply. See website for T&Cs
REGISTER ONLINE TODAY BY VISITING:
www.jaycar.com.au/rewards
TERMS AND CONDITIONS: REWARDS CARD HOLDERS FREE GIFT, % SAVING DEALS, DOUBLE POINTS & REWARDS OFFERS requires active Jaycar Rewards Card membership at time of purchase. Refer to website for
Rewards Card T&Cs. DOUBLE POINTS FOR REWARDS CARD HOLDERS is for purchase of specified product listed on page. DOUBLE POINTS OFFER on PAGE 2 is for YN-8204, YN-8205, YN-8206, YN-8207, YN-8208,
YN-8294, YN-8295, YN-8296, YN-8297, WB-2020 or WB-2030. REWARDS CARD HOLDERS BUY 2 & SAVE DEALS on PAGE 2 are for YN-8410, YN-8077, YN-8078, YN-8326, YN-8328, YN-8348, YN-8352 or YN-8354.
REWARDS CARD HOLDERS 15% OFF on PAGE 5 is for HB-5430, HB-5432, HB-5434, YN-8046, YN-8048, HB-5420, HB-5422, HB-5424, HB-5426, HB-5450, HB-5452, HB-5454 or MS-4094. See in-store for full details.
SAVINGS OFF ORIGINAL RRP (ORRP). DOUBLE POINTS accrued during the promotion period will be allocated to the Rewards Card after the end of promotion.
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) 4625 0775
Castle Hill
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Erina
Ph (02) 4365 3433
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Ph (02) 4225 0969
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Ph (02) 9439 4799
Hornsby
Ph (02) 9476 6221
Maitland
Ph (02) 4934 4911
Newcastle
Ph (02) 4968 4722
Penrith
Ph (02) 4721 8337
Port Macquarie
Ph (02) 6581 4476
South Australia
Rydalmere
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Mermaid Beach
Ph (07) 5526 6722
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Victoria
Western Australia
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Tasmania
Northern Territory
Darwin
Ph (08) 8948 4043
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SERVICEMAN'S LOG
I hate letting anything beat me
It seems I just can’t help myself – unable to
resist a challenge, I often take on jobs that
are clearly not worth doing. I just hate letting
anything beat me and that certainly applied
to a no-name multi-tool I was recently given
to fix.
These days, having a workshop
packed with cool tools isn’t as financially crippling as it used to be. The
advent of cheap, imported but still
high-quality tools means that onceexpensive (and often hard-to-source)
workshop tools are now very affordable. What’s more, the abundance of
warehouse-style tool retailers up and
down the country means that they are
readily available to anyone who wants
to increase the capabilities of a home
and/or business workshop.
It’s no longer a matter of simply
choosing between cheap, mass-produced rubbish and expensive European, American or locally made professional-level tools. Now we have a
huge variety of very reasonable DIY or
home-handyman grade tools to choose
from but as with everything else, this
can be both a good and a bad thing.
These mid-range tools are often good
quality and with care, can sometimes
be used in a professional or commercial capacity. In most cases though,
they wouldn’t quite cut the level of
“abuse” that goes with professional
use.
Such tools generally come with a
“DIY” or “Home Handyman” warranty to reinforce this fact, meaning
that a tool will be repaired or replaced
provided it hasn’t been used to do
work it hasn’t been designed to do.
In the case of a hammer or similar
tools, this doesn’t really matter but in
other cases, it is important that tools
are used strictly for the purpose for
which they were designed. Exceeding
their capabilities could result in tool
failure and a serious case of missing
appendages!
One of the downsides to the proliferation of reasonably-priced tools
is that many of them are not worth
repairing if they fail. In fact, depending on their quality and purpose, this
happens far more often than with
those high-quality jobs from Europe
and the US.
I still have many of the tools I was
issued over 35 years ago when I was a
pimply-faced apprentice, starting my
working career at our national airline.
Many of my tools were made either in
Europe or America and the quality is
obvious as soon as you pick them up.
Those with ratchets or other moving
parts still operate like the day they
were made and will most likely be still
going strong long after I am no longer
able to use them.
The biggest disadvantage of my
original toolkit is that the majority
of those tools are based on Imperial
measurements. The reason for this is
simple – the aircraft we were working
on used good old inches and footpounds for their parts (airliners didn’t
Servicing Stories Wanted
Do you have any good servicing stories that you would like to share in The Serviceman column? If so, why not send those stories in to us?
We pay for all contributions published but please note that your material must
be original. Send your contribution by email to: editor<at>siliconchip.com.au
Please be sure to include your full name and address details.
siliconchip.com.au
Dave Thompson*
Items Covered This Month
•
•
•
•
Faulty multi-tool motor
Reorganising a Howard organ
PA amplifier repair
DSE Q1418 multimeter
*Dave Thompson runs PC Anytime
in Christchurch, NZ.
Website: www.pcanytime.co.nz
Email: dave<at>pcanytime.co.nz
go metric until relatively recently).
Of course, those tools were fantastic
when I owned British-made cars and
motorbikes but they became all but
useless when I started buying betterequipped (and better-engineered) Jap
anese vehicles.
That’s why I now have two distinct
sets of tools: my high-quality aircraftengineer era tools in one set and the
tools I’ve purchased since then in the
other. The latter are, I have to admit,
not quite as top-end as the others.
This is down purely to economics.
Where possible, I invest in the best
tools available (much to the distress
of my significant other) but while my
philosophy is that buying good tools
is never a waste of money, there is a
limit to that approach. Some tools are
ridiculously expensive and it makes
no sense spending hard-earned money
on them when there are alternatives
available that are “just-as-good-forwhat-I’m-doing” for a whole lot less.
That said, I did like the culture of
“nothing but the best” during my work
with the airline (which set me up to
strive for nothing but the best in the
rest of my endeavours). Of course,
“nothing but the best” is great when
someone else is picking up the bill for
all the nice tools!
Most older readers can probably
relate to the following scenario: many
years ago, you bought a screwdriver
set at a tool sale and the very first time
you tried to use one, the tip twisted or
was stripped when you tried to undo a
screw. The rest of the set then ended up
April 2015 53
Serviceman’s Log – continued
gathering dust under the workbench
because they simply weren’t up to
the job. These days though, quality
tools are so much more affordable and
available that this type of scenario now
rarely happens.
Even so, with tools you usually get
what you pay for. For example, a few
years ago, I invested in one of those
rotary engraver type tools that usually
come in a moulded plastic case with
a gazillion different cutting, grinding
and drilling attachments. Dad had a
Dremel-branded model and I coveted
that tool for years but to buy one back
then was still prohibitively expensive
until the low-cost generic models hit
the market.
While the Dremel tools did come
down in price a little, you could buy
a no-brand multi-tool for much less
money and, by and large, it would do
exactly the same job as the big-name
models. Mine even came with a flexible shaft and a very handy hangertype arrangement so it became almost
like a dentist’s drill, useful for carving,
shaping, drilling and all sorts of jobs.
What’s more, it got a lot of work. As
part of my computer repair workshop,
it did everything from drilling holes to
chopping and channelling cases using
the cutting discs. It was also used for
54 Silicon Chip
shaping polymer fillers with the sanding attachments.
The tool even came with a new set
of brushes but they are still sitting unused in their little plastic bag. In fact,
they are not likely to be used now as I
eventually inherited Dad’s Dremel and
that now graces my workbench. The
only real difference – and I suppose
this is where the money comes into it
– is the quality of the speed controller.
The controller on the Dremel is much
smoother and easier to adjust than on
my no-name model.
Of course, I could use one of the
excellent SILICON CHIP designed speed
controllers on the old no-name model.
However, it now sits unused and will
remain that way while the Dremel is
still going strong. And that’s after many
years of use.
Multi-tool sob-story
So what’s all this leading up to?
Well, a good friend of mine turned
up the other day with a very familiarlooking plastic case and a sob-story
to go with it. It turns out that he had
seen my original multi-tool in my
workshop a few years back and had
decided then and there that he should
also have one. He builds houses for a
living so I’m not entirely sure what
he wanted it for but nonetheless, he
went out and purchased one exactly
the same and here it was, a couple of
years later, sitting on my workbench.
I opened the case and it still sparkled with that brand-new look that
tools have when they’ve never been
used. My friend said that after originally buying it, he took it home, plugged
it in and tested it before putting it back
in its case, ready for use when the time
came. When that day arrived, he took
it out of the case, plugged it in and . . .
nothing; it didn’t work.
At the time, he did all the usual
checks. He checked the brushes, tried
another wall socket and did whatever
else he could think of before deciding it was dead. Unfortunately, by
then, he’d lost the receipt and since
it had been quite a few months since
he’d purchased it and because he’d
bought it on sale from one of those
big hardware chain stores, he figured
it unlikely they’d consider taking it
back without proof of purchase.
He told me that the price was pretty
low anyway and it wasn’t worth the
grief of going through the motions to
return it. In the end, he simply put it
back in its case and stashed it away,
forgetting all about it until he was
recently having one of those “oncein-five-years” spring clean-outs. That’s
when he rediscovered it and so he
brought it around to my workshop,
thinking that I might be able to do
something with it.
He didn’t want to waste my time
and any more of his money on it so
he said that if I could get it going, I
could have it. He’d long since resigned
himself to the fact that it was dead and
if I couldn’t get the handset/motor
going, then at least I could use all the
cutters, drills and grinding wheels that
came with it.
Never one to look a gift horse in
the mouth, I accepted his challenge
knowing full-well it would be unlikely
I’d get this thing going. Most of these
units have potted electronics and it
was likely I’d open it up, take one look
and throw it in the bin (after scrounging any reusable bits and pieces). As
it turned out, I was to be pleasantly
surprised.
Opening it up was simple as it didn’t
use any of those horrible “security”
fasteners (the ones with a weirdshaped hole and sometimes a raised
dot in the middle that requires a specially-formed, hollow screwdriver tip
siliconchip.com.au
to undo). Instead, six ordinary PK-style
screws held the two plastic halves of
the case together and while they were
very tight, I soon had them out.
The fit of the parts was actually
very good compared to some tools I’ve
pulled apart in the past. The top half
of the case came away easily, leaving
the internals sitting in the bottom half.
The armature was mounted on two
sealed bearings – one at the front near
the chuck and one at the rear supporting the very end of the armature. The
brush holders sat at the three and nine
o’clock positions and were part of the
bottom half of the case.
Next, I undid the two plastic grubtype screws and removed the brushes
before going any further. By lifting
everything up a few centimetres, I
could slide the armature out towards
the front and it came out easily with
the bearings attached. This left the
fields, speed controller board and wiring, along with the mains cord which
was terminated in a couple of screwterminals on the controller board after
passing through a strain-relief clamp
at the very end of the case. That clamp
was held in place with two short PK
screws, as was the speed controller
board, and after removing them the
whole caboodle could be removed
from the case.
With the plastic parts placed aside,
I set about inspecting the electrics
and other components. Surprisingly,
the controller board was made up of
discrete components that even had
the values clearly marked on them, an
unusual find when the manufacturers
of many similar units do everything
possible to obfuscate the parts used
and the way they’re wired in. That’s
usually done by sanding the surfaces
of any ICs in the board to obliterate
type numbers and by using potting
materials to coat and cover the entire
circuit board.
However, regardless of the fact
that nothing had been obscured, I
hoped that I didn’t have to dig too far
into the electronics side of the thing.
Mains power and fiddling about with
unfamiliar circuits don’t go hand in
hand, particularly as this whole circuit
operated at mains potential!
Nothing obvious
There was nothing obvious on the
board to explain why the unit had
suddenly stopped working; no burnt
patches, no melted wires and no acrid smells to indicate anything had
become too hot or had let the magic
smoke out. I could always just replace
components until it started working
again but my instincts told me that
the board was OK so I’d have to look
further afield (no pun intended!).
The wound stator fields had been
tied with waxed string and dipped in
varnish, making them one solid lump
of wound copper wire and metal laminates. I checked where the controller
wires and brush holder leads joined
onto the fields (a common location for
faults) and the connections seemed to
be OK.
I then decided to check for continuity across the fields and brush connectors with my multimeter, so I it set
to a low ohms range, and applied the
meter’s probes to the relevant connections. I got a satisfying beep between
one brush connector and one output
lead of the speed controller board and
an indication of few ohms. However, I
wasn’t particularly interested in figures
at this stage because I didn’t know what
it was supposed to measure anyway;
the fact that I got some measurement
at all was enough.
Conversely, I got nothing on the
other side, which explained why the
motor didn’t work. I triple-checked
that I was measuring the right connections but that’s where the fault lay. It
was in the fields somewhere and at that
point I felt even less confident I’d have
a fix up my sleeve. I turned everything
off and went inside – I’d had enough
for the night.
The next afternoon, I went back to
it for a closer look. Before I got under
way, I mounted and wired in my “new”
10W LED work light, a project I’d built
up some time ago from a SILICON CHIP
article and had been meaning to rig
up for ages. This lamp throws out an
enormous amount of light and amply
covers my work area. This job would
be an ideal acid test for it to see if I
could visually discover why this coil
didn’t have continuity from one end
to the other.
Under the light and with my magnifying headset on, I carefully inspected
the whole assembly and a slight flaw
in the coils at the top inside edge of
the stator soon caught my attention.
It looked as if something had hit the
coils with a sharp edge (or it had been
dropped onto something) and this had
left a definite dent and barely-visible
line across a few of the windings.
The varnish was holding it all together so I soaked the area with a few
drops of “turps” and got stuck in with
my dentist’s pick, carefully cleaning
the area of varnish which had softened
and could now be easily scraped off. It
was a painstaking job but suddenly a
wire popped free, indicating the location of the break.
With one meter probe clipped to the
brush holder, I touched the end of the
broken wire with the other probe and
got a satisfying “beep”. A bit more turps
and digging then revealed the other end
of the wire and again with great care I
ualiEco
Circuits Pty Ltd.
siliconchip.com.au
April 2015 55
Serviceman’s Log – continued
coaxed it free of the coil. I was then able
to measure continuity between this
wire and the speed controller board so
all I had to do was join the two wires
and I was away.
To keep things tidy, I brought the
ends of the wires out to the upper edge
of the fields and used a similarly-sized
piece of wire to make up the resulting gap. Once soldered, I put a piece
of insulation tape under the join and
moulded the joined wire into the shape
of the fields before coating it all in two
coats of nail varnish.
I could then measure continuity
from both brush holders to both ends
of the speed controller board and
after reassembling the tool, it worked
perfectly. Since I didn’t need another
one, I returned it to my friend who was
impressed and surprised I’d gone to so
much trouble.
I told him what any servicemen
would say: “I don’t like letting anything beat me”!
PA amplifier repair
R. W. of Christchurch, NZ recently
parted with coin of the realm for an
old PA amplifier. It came complete
with several faults which he managed
to track down . . .
This is a short tale about a PA ampli-
56 Silicon Chip
fier I bought for $30 at the Christchurch
City Council recycling shed. It was an
Inkel 2500D rated at 120W and featured a 100V line output, two balanced
mic inputs, one unbalanced mic input
and two auxiliary inputs.
When I got it home, all the inputs
worked fine so I tested it into a dummy
load at 100V. The power transformer
buzzed like crazy so clearly it had a
serious fault somewhere.
I soon found that the power transformer had a cooked secondary. I
removed it, dismantled the core and
made a new (non-standard) bobbin.
A friend then rewound the primary
and secondary windings after which I
reassembled the transformer for a test
but found only 20V on the secondary
instead of the 29V required. As a result,
I dismantled it again and returned bobbin to my friend who said he had mistakenly put 44 turns on instead of 64.
He added the extra 20 turns and
I again reassembled and tested the
transformer. This time, there was only
10V on the secondary so back to my
friend it went who confirmed that the
primary winding was OK at 2.22 turns
per volt. However, he had added the
extra winding turns in anti-phase (ie,
buck, not boost), which was the same
conclusion I had come to!
He rewound the added turns yet
again and this time the result was
29V – success at last!
I then reinstalled the clamps and
the copper shield, etc, only to find a
leftover core “I” piece on the workshop floor. That meant that I had to
dismantle the clamps again and
install the “I” piece properly. This
was becoming tedious!
Next, I tried to refit the
rectangular hollow steel
shield around the transformer
only to find that this
has to be done before
the clamps are fitted.
And so I removed the
clamps again, fitted the
shield, then fitted the
clamps yet again and
reinstalled the transformer in amplifier.
The transformer
voltage was correct
and the amplifier’s
output measured
OK but the sound was absolutely horrible during a low-level music test.
I applied an 800Hz test tone and
observed massive crossover distortion
on the scope. I then discovered that the
first transistors in the power amplifier
chain had 1.55V of forward bias on
them. This came from a regulated 17V
supply via an 8.2kΩ dropper resistor
and a 1kΩ shunt resistor to ground,
plus a 100µF electrolytic capacitor
across the shunt.
I soon discovered that this 100µF
electro was leaky but there was more –
someone unknown had tacked an extra
15kΩ resistor across the 1kΩ resistor.
The capacitor was replaced and the
extra resistor removed, after which
the bias voltage increased to 1.6V. And
that eliminated the crossover distortion – it was no longer audible and
what’s more, it was no longer visible
on the scope.
Here’s hoping it stays that way!
DSE Q1418 multimeter repair
Regular contributor B. P. of Dundathu, Qld likes snapping up bargains
on eBay but not all secondhand gear
works properly. Here’s how he recently
saved an old DSE multimeter from
landfill . . .
In amongst a bundled lot I recently
bought on eBay was a DSE Q1418
multimeter. This unit arrived without
the battery (due to postage regulations)
and I noticed that one of the screws
holding the back cover on was missing.
These DMMs are quite handy as
general-purpose meters. I already have
a couple of Digitor Q1467 multimeters
and this DSE multimeter appears to
have been made by the same manufacturer as they are virtually identical.
After fitting a replacement battery,
I turned the unit on but nothing happened. I was sure that the battery was
good but I used one of my other multimeters to check it, just to make sure.
Sure enough, it tested good at 9.5V so
there was obviously a fault in the unit
somewhere.
With the unit switched on, my first
step was to check the supply voltage
where the battery leads connected to
the PCB. Strangely, the voltage here
was well under 7V but it still gave a
reading of 9.5V at the battery terminals.
That meant that the fault had to be
somewhere between the battery and
the PCB.
When I was replacing the battery,
I’d noticed some slight corrosion on
siliconchip.com.au
Reorganising A Howard Organ
Here’s something completely different: a Howard Skyline 100 electronic organ. B. B of Little Mountain,
Qld recently took on the repair . . .
The Howard Skyline 100 electronic organ is quite a nice unit with a
dual manual keyboard and foot pedals. This one was completely dead
but I felt that it shouldn’t be all that
difficult to get it going again, despite
the fact that there is nothing about
this unit on the internet.
Removing some clips allowed
the back panel to be removed, after
which a collection of PCB assemblies
was observed. Removing two screws
then allowed the filter switch panel
to be hinged out of the way, while removing two more screws made everything else accessible. This looked
like an American product from the
early 1970s and it was designed to
be repaired!
The main reason the organ produced no sound was that a diode had
died in the power supply and had
taken out the fuse. That was easily
fixed. Now there was sound but a few
notes sounded decidedly sick. This
fault was traced to a tone generator IC
which was apparently very popular
in the early 1970s. The keyboards
worked but the rhythm section was
also faulty and did not work.
One board had a number of CMOS
logic gates, some of which oscillated
at around 14MHz. If this was the
rhythm section, it would be difficult
to hear any sound as the drum frequencies would be 1000 times higher
than our hearing range! Another IC
generated sawtooth waves at around
40kHz.
After prodding around for some
time, I eventually concluded that
the 40kHz IC had something to do
with the rhythm section, as one of
its pins was connected to the rhythm
the battery snap terminals but hadn’t
thought it significant at the time. Nevertheless, it was a clue. I cut the battery
cables near the PCB, bared the ends and
temporarily connected a spare battery
snap to the cut wires. I then switched
the unit on again and presto . . . it now
worked.
Further investigation revealed that
the original negative battery lead had
suffered corrosion under the insulasiliconchip.com.au
speed control pot. This control pot
had a very high resistance and it was
difficult to determine just where the
wiring at the other end ran to.
The part number identification on
the rhythm IC was unreadable but
then came an internet breakthrough.
One of my many searches eventually
turned up a rhythm generator circuit
for organs. The speed control pot was
between the 40kHz pin and earth and
was designed to control the oscillation frequency.
The speed control pot was a 1960s
slide potentiometer and getting one
of these would be difficult. But this
wasn’t the time or place to give up
so I dismantled the pot and took a
look at its internal parts. This revealed that the sliding contact blade
had been dislodged and had been
crushed into the lower corner.
After bending the contact blade
back into a reasonable shape, I glued
it to the slider knob, lubricated the
tracks and had a perfectly working
pot. I then re-assembled the rhythm
panel and switched the unit on but
there was still no sound, just a blinking LED (very modern in those days).
Obviously though, the rhythm generator was now working as I could
vary the blinking rate of the LED.
At that stage, I traced out the
schematic diagram of one wildly
oscillating gate. It was very strange,
with two resistors in series between
the gate’s input and output. That
would explain the oscillation, as the
gate was forced to operate as a linear
amplifier. But why?
I then discovered two capacitors
in series between the same input
and output. A resistor then ran from
the junction between these two capacitors to the rhythm chip, while a
capacitor ran to earth from the junction between the resistors. Finally,
tion, immediately adjacent to the battery snap terminals. As a result, it had
effectively turned into a resistor which
is why only 7V was being applied to
the PCB.
Having established the cure, I soldered the new battery snap to the PCB
and checked the unit out by comparing its readings to those on my other
DMMs. It all worked as expected, so
I now have an additional multimeter
there was also a trimpot from input
to output.
It’s worth noting that the PCB was
single-sided and that these components were spread out over an area of
about 70 x 80mm. So it was a bit of a
challenge to trace the circuit out and
draw an accurate circuit diagram.
After redrawing the circuit a
number of times, I noticed that the
resistor values were all the same,
as were the capacitor values. This
looked very much like a double-T
filter and based on the RC values
used, would produce a note around
1kHz (like a snare drum?). But surely,
a logic gate is a digital element and
not a transistor?
The late 60s was an era of great
innovation and using logic gates as
amplifiers was just the “in-thing”.
Indeed, the logic gate and its accompanying RC circuit was supposed
to operate as a damped double-T
filter, with the damping level (decay)
controlled by the trimpot. That is an
inventive use of logic gates!
The problem is, this is a dicey
design that’s rather prone to wild
RF oscillations. To get around this,
the designer selected CMOS chips
with low input to output gain and
high output impedance. I replaced
the CMOS ICs with older types and
suddenly there was sound.
The newer CMOS gates are not
going to work here and that explains
why these chips were in IC sockets –
so that they could be easily changed.
Indeed, this might be the very last
organ in existence just because of this
design problem. And that’s a pity because the keyboards are of very high
quality and still work well, even after
50 years of standing around.
The bass pedals also work extremely well and the speaker is about
350mm in diameter and will shake
the floor at full power. Now, if I could
only play the thing!
in my arsenal for general purpose use.
I also found an identical screw to the
missing one and I replaced that while
I was reassembling it.
This was an easy fix that saved a
good unit from being binned – all for
the sake of a 20-cent replacement battery snap. Simple fixes like this are
always rewarding because, with very
little effort, a useful piece of test gear
is saved from going into landfill. SC
April 2015 57
By NICHOLAS VINEN
Low Frequency
Distortion Analyser
Are you concerned about the quality of your 50Hz 230VAC supply?
Would you like to measure the harmonic distortion of your loudspeaker system? This unit will measure the distortion of a 50Hz or
60Hz mains waveform (via a low-voltage isolating transformer) or
the distortion of any 3-20VAC sinewave signal in the range of 20Hz10kHz, eg, the output of a midrange or bass loudspeaker.
W
E TEND TO think of the 50Hz
AC mains supply as a 230V RMS
sinewave but if you have a look at it on
an oscilloscope (see Fig.1), it is often
quite distorted. A large proportion
of mains loads are not resistive but
reactive and since they draw current
out-of-phase or in a non-sinusoidal
manner, they generate a voltage across
the finite impedance of the mains supply network and distort the signal.
Typical “waveform distorters” are
fluorescent and gas discharge lights
and devices with transformer/rectifier-based linear power supplies or
non-PFC (Power Factor Correction)
switchmode power supplies. These all
tend to draw current only at the voltage peaks, leading to the pronounced
58 Silicon Chip
“flat-topping” you can see in Fig.1.
Does this matter? Well, most equipment will not be affected by even quite
severe levels of mains distortion but
some sensitive devices could be upset.
As an extreme example, there are plenty of devices which will not operate
correctly from square-wave inverters
and some devices won’t operate from
modified sinewave inverters either.
Having said that, the distortion
levels of such inverters are well above
the maximum allowable figure for
the mains supply which is normally
quoted as 5%. In our experience, a
typical harmonic distortion figure is
around 3% but it varies quite a bit
depending on location. Interestingly,
different power points in our office
gave quite different readings, from 2.43.2%, suggesting that they are wired
to different mains phases.
And yes, this analyser can be used
to (indirectly) check the distortion
of portable 230VAC generators and
inverters. It’s safe to use because a
small 3-20VAC plugpack is used as an
isolation transformer (ie, the plugpack
is plugged into the generator or the
mains and the plugpack’s low-voltage
AC output is fed into the signal input
of the analyser).
So how would you know whether
your mains supply is badly distorted?
Well, this simple device will tell you.
It can measure harmonic distortion
from below 0.1% to around 33% with
a bandwidth of a few kilohertz and
siliconchip.com.au
it’s very simple to build and operate.
Some devices which may be sensitive to mains distortion include certain
types of (mainly older) test equipment
and medical devices. Devices with
motors will still run with highly distorted mains but some may get hotter
than normal. Severe harmonics, such
as those present when mains tone
control signals are being broadcast,
can also cause transformers, motors
and fluorescent light ballasts to hum
or buzz audibly.
Some hifi enthusiasts also believe
that AC mains waveform distortion
and noise can also affect the sound
quality of amplifiers and other equipment. In our experience, while control
tones and some mains-borne interference may become audible, that tends
to be more likely in valve amplifiers.
Otherwise, typical distortion of the
50Hz (or 60Hz) mains waveform is
not likely to have any effect on audio
performance.
However, there is one exception. If
the mains waveform is severely “flat
topped” that means that its peak-topeak value will be significantly reduced with respect to an undistorted
sinewave. That in turn means that
the resulting supply voltages in the
amplifier can be less than they should
be and that can definitely affect performance, particularly if the amplifier
being driven hard.
For more information see this link:
http://www.mantenimientomundial.
com/sites/mm/notas/Harmonics.pdf
If you want to measure loudspeaker
distortion you will need a microphone
and preamplifier. The easy solution
is to use the PreChamp featured in
our article on “How To Do Your Own
Loudspeaker Measurements” in the
December 2011 issue.
Fig.1: a typical mains waveform, as measured at our office (yellow, top) with its
distortion residual (green, bottom). Not only are the peaks badly flattened but
there are visible bumps along the rising and falling edges too, especially around
the zero crossing points. It isn’t obvious from the residual but the distortion is
almost all odd-order harmonics (ie, 3rd, 5th, etc) due to the flat-topping. This is
very similar to the distortion in an audio amplifier when the output is clipping.
How it works
Traditional audio analysers use a
tunable notch filter. The filter removes
the fundamental frequency (eg, 50Hz
or 60Hz for a mains supply) and the
remaining harmonics and noise are
measured and related to the input
voltage to obtain a percentage reading.
This project idea was initially
suggested to us as a series of passive
notch filters driven by a low-voltage
transformer. The notches would be
tuned to the local mains frequency (ie,
50Hz), thus removing the fundamental. The residual signal (ie, distortion
components) could then be measured
siliconchip.com.au
Fig.2: at top is the same distorted mains waveform as in Fig.1 with a low-pass
filter applied to remove noise; below is the spectrum calculated by the scope
from this data using a Fast Fourier Transform. It is configured to use the same
Flat Top window as the microcontroller in this project. You can see that the
third, fifth, seventh and ninth harmonics are dominant at around -39dB with a
second harmonic at about -48dB. The number of harmonics shown is about the
same as the micro uses to calculate total distortion.
April 2015 59
Parts List
1 double-sided PCB, coded
04104151, 104 x 60.5mm
1 UB3 jiffy box (optional)
1 5kΩ mini horizontal trimpot
(VR1)
1 28-pin DIL IC socket (for IC1)
1 9V battery snap
1 9V battery
1 piece non-conductive foam,
approximately 65 x 40 x 8mm
1 PCB-mount DC socket (optional) (CON1)
1 2-way terminal block, 5.08mm
spacing (CON2)
1 5-pin right-angle header (CON3)
(for programming IC1)
1 2-pole 6-position rotary switch
(S1)
1 knob to suit S1
2 PCB stakes
2 chassis-mount binding posts
(optional, for use with case)
Semiconductors
1 PIC32MX170F256B-I/SP
programmed with 0410415A.
HEX (IC1)
1 78L05 100mA regulator
(REG1)
2 MCP1700-3.3/TO 3.3V lowdropout regulator (REG2)
1 yellow or orange 3mm LED
(LED1)
1 red 3mm LED (LED2)
1 1N4004 1A diode (D1)
1 1N5819 1A Schottky diode
(D2)
Capacitors
1 220µF 25V electrolytic
3 100µF 16V electrolytic
1 10µF+ 6V tantalum or SMD
ceramic
1 1µF multi-layer ceramic
3 100nF multi-layer ceramic
Resistors (0.25W, 1%)
3 100kΩ
2 470Ω
1 33kΩ
1 22Ω
3 10kΩ
1 10Ω
1 1kΩ
with a DMM and divided by the raw
transformer output voltage in order
to calculate the THD+N figure as a
percentage.
We investigated this concept but
concluded that passive filters are too
fiddly to tune and too lossy for this
purpose. Tuning is a tricky issue because such filters inevitably involve
60 Silicon Chip
capacitors which are not normally
sold in tolerances better than 5%. So
each notch stage would need at least
one trimpot and they would all need
to be tuned very close to 50Hz to get
a deep enough notch for sufficient
fundamental rejection.
However, the real show-stopper
for the passive filter idea is its inherent signal loss and its lack of notch
depth; you need a really steep notch
to remove the fundamental but have
no effect on the harmonics. A simulation of the required filter with ideal
components showed that the first few
harmonics (ie, 100Hz, 150Hz, 200Hz
etc) were severely attenuated by the
shoulders of the notch, making the
resulting reading likely to severely
underestimate the actual level of
distortion.
The third harmonic at 150Hz is normally the largest component of mains
distortion and a twin-T passive notch
filter tuned for 50Hz is still 10dB down
at this frequency. If multiple such
filters were used (and it seems likely
this would be required), the attenuation would be 20dB or more and this
is clearly unacceptable.
We did consider using active notch
filter(s) but to get the required notch
depth with sufficiently little attenuation for the second harmonic at 100Hz
would require a complex circuit. The
alternative is to use digital signal processing with a microcontroller.
DSP software to the rescue
The DSP concept is relatively simple, even if the software is not. The
output of a 9VAC or 12VAC plugpack
is attenuated to give a signal of about
3.3V peak-to-peak. This is fed to the
analog-to-digital converter (ADC)
input of a 32-bit microcontroller. The
micro digitises the signal, does some
filtering to make up for its relatively
low-performance internal ADC, then
does a spectral analysis and determines the THD from the result.
The output from the microcontroller
is a pulse width modulated (PWM)
signal which is filtered to obtain a DC
voltage that can be read with a multimeter or panel meter. So the circuit
is really quite simple even though the
software is anything but.
In fact, we use a Fast Fourier Transform (FFT) to produce a spectrum
analysis of the input signal. This tells
us the amplitudes of fundamental
frequency and all the harmonics up to
the 20th. The tallest peak will be the
50Hz fundamental and the micro can
easily search for the highest peak, so
frequency accuracy is not important.
The distortion components (ie, the
harmonics) will be at equally spaced
frequencies above this peak. These
calculations are performed in the frequency domain.
As hinted at earlier, the formula for
computing THD (in the time domain)
is to divide the RMS average of the
residual signal (ie, signal minus 50Hz
fundamental sinewave) by the RMS
average of the fundamental sinewave
itself, then take the square root of the
result. It isn’t hard to do this in the frequency domain, as the spectral peaks
correspond to the RMS voltages of
each individual sinewave component.
In theory, the answer is the same
although the time-domain method
inevitably includes any noise within
the measurement bandwidth of the
instrument while the spectral version
gives the possibility of ignoring noise
and only considering the harmonics
themselves, thus giving a THD (only)
measurement rather than THD+N.
In this case, it’s necessary because
the micro’s 10-bit ADC has a lot of
aliasing noise and this would cause a
THD+N reading to be much too high.
Also, if mains noise is going to cause
any problems, it’s most likely to be
due to RF emissions. This would not
normally contribute much to a THD+N
reading, partly because the absolute
power is low and partly due to the
typically limited bandwidth of the
measurement.
Other uses
The aforementioned distortion
measurement method is sufficiently
generic that it could be used for other
purposes. Because the unit searches
for the fundamental, the THD of any
signal in the range of 20Hz-10kHz can
be measured. However given that the
output starts to become less accurate at
lower readings (<0.1%) and the lowest
reading you’re likely to get is around
0.03%, it isn’t suitable for measuring
hifi audio amplifiers.
Having said that, it certainly should
be suitable for measuring the kind of
distortion that’s typical for . . . ahem .
. . a valve amplifier. The lowest readings the device can give are more or
less in line with the best performance
expected from a valve amplifier. And
with solid-state amplifiers, it’s good
siliconchip.com.au
CON1
22Ω
6-12V
DC
POWER
D1 1N400 4
1 ON/OFF
2
3
S1b
K
A
K
A
5
6
9V
BATTERY
OUT
IN
GND
+3.3V
GND
100 µF
220 µF
100k
REG2
MCP1700-3.3/TO
+5V
OUT
IN
4
D2 1N 5819
+
REG1 78L05
100 µF
100nF
16V
25V
16V
33k
+3.3V
10Ω
470Ω
CON2
SIGNAL
+
INPUT
(20VAC MAX.)
MMC
MMC
10k
ADJUST VR1
SENSITIVITY 5k
13
1 µF
470Ω
3
2
VDD
1 SELECT
2
3
4
S1a
6
5
K
AVDD
RA1/AN1/VREF–
SOSCO/RA4
RA0 /AN 0 /VREF+
PGED1/AN2/RB 0
AN9/RB15
11
10
9
6
AN 10 /RB1 4
SOSCI/RB4
AN11/RB13
RA3/CLKO
AN12/RB12
RA2/CLKI
PGEC2/RB11
IC1
PIC32MX170PIC3
2 MX170F256B
RB2/AN4
+3.3V
PGED2/RB10
TD0/RB9
TCK/RB8
CON3
ICSP
TDI/RB7
10k
1
1
2
14
3
15
4
AN5/RB3
MCLR
A
λ LED1
28
MODE
100k
A
100nF
100nF
100k
1k
PGEC1/AN3/RB1
12
LOW
BATTERY/
OPERATE
λ LED2
CLIP
K
4
26
25
10k
24
TP1
23
22
21
OUTPUT
VOLTAGE
100mV/%
100 µF
18
16V
17
16
7
TP2
5
LEDS
PGED3/RB5
PGEC3/RB6
5
VCAP
K
A
20
10 µF
AVSS
27
VSS
19
78L05
6.3V
TANT.
OR SMD
CERAMIC
VSS
8
GND
IN
OUT
MC P1700
SC
20 1 5
LOW FREQUENCY DISTORTION ANALYSER
D1, D2
A
K
IN
OUT
GND
Fig.2: the distortion analyser circuit. There isn’t much to it since most of the work is done in IC1’s software. The signal
is attenuated by VR1 and then biased to half-supply (1.65V) before being applied to analog input RA0. A PWM signal
from pin 24 (RB13) passes through a low-pass RC filter with the reading available between TP1 and TP2. Power comes
from a 9V battery or DC plugpack while rotary switch S1 provides both on/off switching and mode selection.
enough to at least check that an amplifier is operating correctly and so it
might be useful for servicing work.
In order to provide relatively accurate readings at higher frequencies,
the unit automatically increases its
sampling rate (by reducing the amount
of averaging done) when it detects
that the fundamental is at a higher
frequency.
Circuit description
The full circuit is shown in Fig.2.
It would normally be powered from a
siliconchip.com.au
9V battery via Schottky reverse polarity protection diode D2 but it could
be powered from a DC plugpack via
diode D1. It cannot be powered from
the same 9-12VAC plugpack which
is used to couple the 50Hz mains AC
signal into the analyser.
If a plugpack is used to power the
Low Frequency Analyser, the 9V battery is disconnected by the socket
switch, CON1. D1 provides separate
reverse-polarity protection for the
plugpack. The DC supply is connected
to the circuit via one pole of 6-position
2-pole rotary switch S1.
Two 3-terminal regulators are connected in series to provide a 3.3V supply for the microcontroller. The first is
REG1, 78L05 5V regulator which acts
as a pre-regulator for 3.3V regulator
REG2 which can only handle a maximum input voltage of 6V.
In practice, this two-regulator combination provides a regulated 3.3V rail
(important for accuracy of the output
voltage) for input voltages down to
about 5V, which would mean the 9V
battery was well and truly flat.
April 2015 61
10Ω
10k
+10 µF
–
ICSP
+
%
+
TP1
5819
Batt
1
TP2
Clip
100 µF
470Ω
1k
LED1
LED2 A
100nF
100nF
100 µF CON3
PIC32MX170F256B
IC1
9V 0V
100k
470Ω
22Ω
REG2 +
REG1
A
D1
Power/Mode
100nF
100 µF
10k
D2
220 µF
+
S1
+
9V BATTERY
Distortion Analyser
CON1
33k
CON2
100k
100k
AC in
4004
VR1 5k
C 2015
1 µF
10k
04104151
(GREY OUTLINES REPRESENT
COMPONENTS NOT USED
IN THIS PROJECT)
Fig.3: follow this PCB overlay diagram and the photo at right to build the Distortion Analyser. Note that many of the
components are left off as this PCB was designed to be used for multiple purposes. It snaps into the side rails on a UB3
jiffy box or can be housed in a larger enclosure if a panel meter is to be fitted, to display THD readings.
So that you know if the battery has
gone flat, a 100kΩ/33kΩ resistive divider allows PIC32MX17F256B microcontroller IC1 to monitor the battery
voltage at its AN1 analog input (pin
3). The 3.3V rail is used as a reference
and if the battery voltage drops below
about 5.6V, LED1 is illuminated.
The input signal is fed in via CON2
and has a 15kΩ fixed resistive load.
This minimal loading means that a
9VAC or 12VAC transformer’s output
closely tracks the mains waveform, ie,
the transformer itself causes minimal
extra distortion. The signal is then
coupled via a 1µF capacitor and DCbiased to 1.65V (half the 3.3V supply)
by a pair of 100kΩ resistors. The signal
then goes to analog input AN0 (pin 2)
of IC1 via a 470Ω protection resistor.
The chip uses its internal RC (resistor/capacitor) oscillator and PLL
(phase locked loop) to run at 24MHz,
so that its FFT calculations on the
sampled data at AN0 complete fairly
quickly. The ADC requires 13 clocks
per sample (1 for sampling, 12 for
conversion) and is run at ¼ the main
clock rate, giving a sampling rate of
24MHz ÷ 13 ÷ 4 = 460kHz.
Between 1 and 16 samples are averaged, giving an effective sampling rate
of between 28.75kHz and 460kHz. For
a 50Hz signal (eg, mains) at 28.75kHz
and a window size of 8192 samples,
this means 8192 / 28750 = 285ms
worth of data or just over 14 full cycles
is processed at a time.
Having done the THD calculation,
the micro then uses one of its internal
PWM peripherals to generate a signal
at output RB13 (pin 24). The associated timer period is set to 3300 so that
for each increment in the PWM duty
cycle value, the average output voltage
increases by 1mV. This assumes an ac-
Features & Specifications
Input signal voltage: 3-20V RMS
Input signal frequency: 20Hz-10kHz
THD measurement range: 0.03-33%
THD measurement accuracy: typical error less than 0.1% (absolute)
Modes: total distortion %, second harmonic %, third harmonic %, even harmonic %
and odd harmonic %
Power supply: 9V battery or 6-15V DC plugpack
Operating current drain: ~15mA
Low battery indicator: LED, ~5.5V threshold
62 Silicon Chip
curate 3.3V rail; the MCP1700 has an
output voltage tolerance of ±0.4% at
25°C so it should be well within ±1%
at normal room temperatures.
This PWM signal passes through a
10kΩ/100µF RC low-pass filter with a
time constant of around one second.
This gives a DC voltage to make the
meter’s job easier and also to smooth
out any jitter in the measurement due
to noise and so on. It can then be measured between TP1 and TP2.
Each time the output voltage is
updated, LED1 is flashed briefly. This
indicates that the unit is operating.
As mentioned earlier, IC1 monitors
the battery level via its AN1 input
and should the battery voltage drop
to a low level (before output accuracy
suffers), the state of LED1 is inverted.
That is, LED1 is switched on all the
time, except briefly when the output
voltage is updated when it flickers off.
Thus, if LED1 is on most of the
time, the battery is flat and should be
changed.
LED2 is used to indicate ADC
overload on input AN0. For optimum
performance, VR1 is adjusted to just
below the level where LED2 lights.
Having said that, the exact setting is
not critical as long as LED2 remains
off during operation; if VR1 is set a
little low, it doesn’t appear to affect
the readings much.
Rotary switch S1a connects either
pin 6 or one of pins 9-11 of IC1 to
ground. With S1 in position 1, power
siliconchip.com.au
the circuit are the two supply bypass
capacitors for IC1’s VDD and AVDD
rails, a 10Ω resistor to help filter its
analog supply and a 10µF capacitor
at pin 20 (VCAP) which is used by its
internal core regulator. This 10µF capacitor must be a low-ESR type (below
1Ω) which means either tantalum or
ceramic.
Construction
is disconnected so the unit is off. IC1
can determine which of the other five
positions the switch is in by enabling
its weak internal pull-up current
sources on these pins. If S1 is in position 2, none of these pins (6 or 9-11)
is pulled low whereas positions 3-6
each pull a different pin low.
IC1 checks the state of S1 immediately after it updates its output and
performs a slightly different measurement at the next update, depending on
its state. In position 2, the normal THD
calculation is made. In position 3, only
the THD contribution from the second
harmonic is read out. Similarly, position 4 reads the third harmonic only,
position 5 gives the THD contribution
of all even harmonics (2nd, 4th, 6th,
etc) and position 6 reads only odd
harmonics.
CON3, the ICSP header, is used to
program IC1 and is not required if
you are using a pre-programmed chip.
The only remaining components in
Building this unit is straightforward
with most of the parts mounted on a
PCB coded 04104151. Note that there
are a number of blank component locations, as this PCB was designed for
other uses as well.
Fig.3 shows the parts layout on the
PCB. Start by checking the resistor
values with a DMM and fit them where
shown. Follow with diodes D1 and D2;
these are different types and are both
orientated with their cathode stripes
facing the bottom edge of the PCB.
Next, fit the IC socket with its
notched end towards the top of the
board. Check that it’s sitting flat after
soldering two diagonally opposite
pins, then make the rest of the joints.
Follow with the ceramic capacitors,
trimpot VR1 and then the two regulators. Don’t get the latter mixed up and
note that you will probably need to
crank their leads out with small pliers
before mounting them so that they fit
the pads.
If fitting the DC socket, do so now.
Similarly, you can install pin header
CON3 but note that it isn’t required
if you have a pre-programmed chip.
Now fit the two PCB stakes at lower
right, followed by the tantalum and
electrolytic capacitors. These capacitors are all polarised, with the longer
(positive) leads all going towards the
top of the board. If fitting CON3, lay the
adjacent 100μF electrolytic capacitor
over, otherwise you will have trouble
plugging the PICkit programmer in.
CON2 can now go in, making sure
Table 1: Resistor Colour Codes
o
o
o
o
o
o
o
o
siliconchip.com.au
No.
3
1
3
1
2
1
1
Value
100kΩ
33kΩ
10kΩ
1kΩ
470Ω
22Ω
10Ω
4-Band Code (1%)
brown black yellow brown
orange orange orange brown
brown black orange brown
brown black red brown
yellow violet brown brown
red red black brown
brown black black brown
its wire entry holes go towards the
nearest edge of the board. That done,
trim about 10mm from the end of
switch S1’s shaft, leaving it 30mm long
as measured from the top of switch
body. File off any burrs and check
that the knob still fits, then mount S1
on the PCB.
Be careful with S1’s orientation as
there are two possible ways it can go
in. The plastic locating spigot must go
towards IC1 as shown in Fig.3
Once the switch is in, feed the battery snap leads through the two strain
relief holes and solder them in place.
Note that if you haven’t fitted CON1,
you will also need to solder a wire
link between its pad nearest the edge
of the board and the vertical pad immediately to its left and slightly below.
This replaces CON1’s internal switch.
Without this, the circuit won’t get any
power from the battery.
The two LEDs are fitted at almost
full lead length, with the base of their
lenses 25mm above the top of the PCB
(use a cardboard spacer). This allows
them to just poke through the lid of
the jiffy box. If you aren’t using a jiffy
box, you could just push them all
the way down onto the board. Either
way, both anodes (the longer leads) go
towards the left.
We used a red LED for the clipping
indicator (LED2, at left) and yellow
for the operation/low battery indicator
(LED1, at right) but you can change the
colours if you want. You may need to
adjust the current-limiting resistors to
suit though.
You can now plug microcontroller
IC1 into its socket, ensuring it has the
correct orientation, ie, pin 1 towards
upper left. If your chip is blank, use
Table 2: Capacitor Codes
Value µF Value IEC Code EIA Code
1µF
1µF
1u0
105
100nF 0.1µF
100n
104
5-Band Code (1%)
brown black black orange brown
orange orange black red brown
brown black black red brown
brown black black brown brown
yellow violet black black brown
red red black gold brown
brown black black gold brown
April 2015 63
Total harmonic distortion is defined as
the ratio of the RMS voltage of a signal’s
harmonics to the RMS voltage of the
signal itself (the signal normally being
a sinewave). The traditional method for
measuring the THD of a sinewave is to
align a deep, adjustable notch filter with
the fundamental frequency, measure the
RMS voltage of the residual, then divide
this by the RMS voltage of the signal.
However, this calculation can also be
done based on a spectral analysis of
the signal. Spectral analysis breaks the
signal down into a series of sinewaves
with various frequencies, amplitudes and
phases. When these sinewave components are summed, the original signal is
reconstructed.
We can find the fundamental by looking for the sinewave component with
the largest amplitude and we can then
find its harmonics at integer multiples of
the fundamental frequency. The ratio of
the sum of harmonic amplitudes to the
fundamental amplitude then gives us
the THD figure.
Note that this is not THD+N since
we’re only looking at the harmonic
amplitudes and not the wideband noise
(which would also be at frequencies
below the fundamental and between the
fundamental and harmonics).
That all sounds relatively easy but
there are quite a few tricks to it. First,
we need to discuss the use of the Fast
Fourier Transform method which is used
to convert the sampled time-domain data
to frequency-domain (ie, spectral data).
The input to a Fourier Transform is
typically a buffer with a power-of-two
number of sample values, encoded
as complex numbers. Normally the
complex numbers would initially have
a zero imaginary portion, ie, they are
real numbers nominally in the range of
-1 to 1 (we’re using some tricks here to
get extra performance but we’ll explain
them later; for now, assume that’s true).
The Fourier Transform converts these
complex numbers into another set of
numbers of identical size, the magnitude
of which indicate the amplitude of the
component sinewaves at a set of evenly
spaced frequencies. For example, say
we have a 4096-entry buffer (212) and
the sampling rate is 8192Hz.
The magnitude of the resulting complex number at index #1 indicates the
amplitude of the sinewave component
at 1Hz, index #2 at 2Hz and so on, up
to 2047Hz (ie, half the Nyquist limit).
The complex “angle” of these values
indicates the relative phase of the constituent sinewaves but we aren’t really
interested in that.
So you might expect that if you performed an FFT transformation on a pure
sinewave at say 100Hz, you would be
able to read out its amplitude at index
#100 and all the other values would be
zero, indicating the lack of any other
frequencies in the signal. However, with
the naive implementation of the FFT, as
well as getting a positive magnitude at
index #100, you also get lesser values
at index #101, index #102, etc with decreasing values. The result is similar at
lower indexes, ie, #99, #98, etc.
In fact, you will get a non-zero value
in every single “bin”. That’s because of
the fact that in the 4096-sample window,
the signal abruptly starts at sample #0
and ends at sample #4095. These sudden start and end transitions cause this
“blurring” of the data.
This problem is mitigated to a large
extent by the practice known as “windowing” the data. This is akin to a piece
of music which fades in at the start and
fades out at the end – you lose the abrupt
transitions at these points. There are
infinitely different ways to do this (which
vary by the rates of “fade-in” and “fadeout”) and depending on which windowing
method you use, the result has different
properties.
Basically, different methods provide
different compromises as to how much
the “blurring” is reduced versus how
much the magnitudes are altered. Popular windowing methods include Hann
(also known as Hanning), Hamming,
Blackman-Harris and Flat Top. If no
such function is applied, this is known
as a “Rectangular Window”. These is an
excellent description of these methods at
the following URL: http://en.wikipedia.
org/wiki/Window_function
The behaviour of some common windows is shown here, in images taken from
that article. In each case, the left panel
shows the function by which the input
time-domain samples are multiplied. On
the right is the sample output of an FFT
for a pure sinewave with this windowing
function applied. Note how slowly the
function falls off from the peak with a rectangular window compared to the others.
For the task at hand, we decided to
use Flat Top because this makes measuring the exact amplitude at a given
frequency easy. Basically, it guarantees
that even for frequencies which fall
between two “bins”, one of the bins will
contain the correct value. The other will
contain a similar or lesser value. This
means we don’t have to do any complex
summing to determine fundamental or
harmonic amplitudes. For an explanation, see: http://www.dsprelated.com/
showarticle/155.php
Flat Top has worse frequency resolution than most other windowing methods
however since the harmonics are spaced
apart nicely (by the fundamental frequency in fact), it isn’t really an issue.
But there is another, more subtle (and
less discussed) issue with windowing
and this is that it also causes the resulting
amplitudes to fall off at higher frequencies. Failure to compensate for this will
cause under-estimation of distortion
an in-circuit programmer to flash it
now, via CON3. You can power the
chip from the programmer if it has
that capability (the PICkit3 does) – if
not, apply DC power to CON1 or the
battery snap.
First, turn trimpot VR1 fully anticlockwise and apply the triangle-wave
to CON2 with a peak-to-peak voltage
close to 5V if possible. That done, apply power, switch S1 to position 2 and
turn VR1 clockwise until either LED2
lights or you reach the end-stop. If
LED2 lights, turn VR1 anti-clockwise
until it just turns off.
Now measure between TP1 and TP2.
It may take a little while to settle but
it should give a reading close to 1.2V
(representing 12% distortion) and
stay there. However, it may be slightly
higher if your triangle-wave source is
badly distorted. LED1 should flash at
a few hertz, depending on the signal
frequency (anywhere in the range of
20Hz-10kHz should be OK).
If you don’t have a suitable signal
Calculating Distortion Using A Fourier Transform
Testing
If you have a triangle-wave generator, you can test the unit quite easily.
64 Silicon Chip
Windowing
siliconchip.com.au
due to apparently reduced harmonic
amplitudes.
Our simple solution to this problem
was to run a Flat Top-windowed FFT
on a series of sinewaves of equal amplitude, each of which was at a frequency
centred on a bin, measure the resulting
peak value and store its inverse in a
correction table. By then multiplying the
output of the FFT by this correction table,
we cancel out the frequency-dependent
windowing attenuation.
Having sampled the data, applied
the windowing function, performed the
FFT and determined the fundamental
frequency, we then look for the second
harmonic at twice the fundamental
frequency. We handle cases where the
fundamental falls between bins using an
estimation function. Normally, there will
be a small but definite second harmonic
spike and we then look at a 50% higher
frequency for the third harmonic and so
on. Each harmonic spike that is found
improves the accuracy of the guess for
the location of the next harmonic.
It’s then just a matter of summing the
squares of the resulting amplitudes,
then dividing this by the amplitude of the
fundamental and performing a square
root to give the THD result.
generator, you can use the same procedure with the signal fed in from a
9-12VAC plugpack instead. Expect a
reading of around 300mV, ie 3%.
If LED1 doesn’t flicker or the reading
seems wrong, switch off and check for
circuit faults. Assuming it’s all OK,
you can optionally do a further test if
you have a sinewave generator. Apply its signal to CON2 using the same
procedure as above and you should
get a low voltage reading at TP1 of
around 30-100mV, representing the
lower limit of the distortion measurement – 0.03-0.1%, depending on how
pure the sinewave is.
Note that if the unit can’t find a
signal at all, the output voltage goes to
0V. This will be the case if the input
signal amplitude is too low, given the
siliconchip.com.au
Improving efficiency
We said above that the input to an FFT
is normally a set of complex numbers
with zero imaginary components. Our
FFT algorithm is a 32-bit fixed-point inplace calculation with a 4096 window
size. This means the input is 4096 x 32
x 2 bits (two 32-bit numbers for the real
and imaginary part of each complex
number), for a total of 32KB storage
required. Our micro has 64KB RAM,
leaving half for other stuff.
Here the advantage of the in-place
FFT becomes apparent; because the
same buffer is used as the input and
output and no temporary storage is
required, we can have a larger window
size than would otherwise be possible.
But it’s actually possible to double the
effective window size to 8192 samples
without using any extra RAM. How you
ask? Well, have a look at this explanation
from Texas Instruments: http://processors.wiki.ti.com/index.php/Efficient_
FFT_Computation_of_Real_Input
To start off, what you do is you take
your 8192 samples and create 4096
complex numbers where the real and
imaginary part of each consists of
alternating sample values. Thus, the
imaginary portions aren’t “wasted” by
being filled with zeros. You then perform
a normal FFT computation.
Normally, half of the FFT output is
“wasted” as the second half is identical
to the first half (but reversed in order).
With this method, the extra data is no
longer duplicated and by convolving it
with some sinewave coefficients, using
the formulae provided by TI, we recover
the full set of result vectors that we would
have gotten with a twice-as-large window
with a regular FFT.
Don’t worry too much about understanding the mathematics behind this – it
certainly works!
setting of VR1. If a signal is detected
but it is grossly distorted (eg, a square
wave), then the output will peg at 3.3V.
Putting it in a box
If you’re planning on building the
unit into the recommended UB3 jiffy
box, it will snap into the integral ribs.
All that’s required is three holes in the
lid for S1 and the two LEDs, plus some
April 2015 65
This is the view inside the completed instrument. The PCB snaps into integral plastic ribs inside the case,
while the battery is sandwiched between a piece of foam and the case lid as shown.
holes in the base for the signal input
and output.
For the lid, copy the front-panel label
shown in Fig.4 and use this as a drilling
template. You can then download the
label in PDF format from the SILICON
CHIP website, print it out, laminate it
and glue it to the lid. The holes can
be cut out using a sharp hobby knife.
For the signal input, we drilled a
hole adjacent to the location of CON2
and fitted a small rubber grommet. We
then cut away a section of the grommet
on the inside of the case so that the PCB
would still fit properly (you probably
don’t need a grommet; we just wanted
to make sure the leads don’t fray from
rubbing on the edges of the hole).
For the output, we drilled two holes
19mm (0.75-inch) apart at the right-
Using it
There isn’t much to it, simply connect a 3-20VAC signal source (eg, an
SILICON
CHIP
Sensitivity
Signal Input:
20VAC Max.
hand end of the box (centred on that
end). We then fitted binding posts and
soldered two strands of ribbon cable to
the binding post lugs. The other ends
of these leads were then soldered to
TP1 & TP2.
After passing the signal cable
through the grommet and screwing
it firmly into CON2, we dropped the
board in the box, placing some nonconductive foam next to S1 (either
side will do), connected the 9V battery
and sat the battery on top of the foam.
The lid was then attached which holds
the battery in place and the knob the
secured to S1’s shaft.
3rd Harmonic
2 Harmonic
Even Harmonics
nd
Odd Harmonics
THD
Off
Clip
66 Silicon Chip
AC plugpack) to the signal input leads
and turn S1 to its first stop, for the
full THD measurement. Use a small
flat-bladed screwdriver to readjust the
sensitivity control if necessary, then
connect the outputs to a DMM and
calculate the distortion by dividing the
voltage reading by 10 to get the percent
figure. For example, a reading of 0.28V
indicates 2.8% distortion.
If you want to use the device for
measuring audio signals, you may
wish to reduce the 10kΩ resistor value
at the top of VR1 however it should
not go below 470Ω (higher if you will
be probing signals above 20V peak).
This is to protect IC1 from excessive
current flow. In this case, you may
wish to connect some sort of probe or
SC
clip leads to CON2.
Fig.4: top lid label for the UB3
jiffy box. To make a reading,
connect the signal up and
simply rotate the knob to the
required position. The output
voltage will stabilise after a
few seconds, once the unit
has adjusted for the signal
frequency and the output
filter capacitor has finished
charging.
Operate/Low Battery
siliconchip.com.au
PRODUCT SHOWCASE
Near HiFi Quality USB Recording Module with almost unlimited capacity
The LT1955 voice recording/playback
chip from KitStop features a 20Hz-20kHz
±0.5dB stereo recording/playback bandwidth and up to 256 different messages,
music passages or a combination of both,
the length of which is limited only by the
capacity of the USB memory stick used.
Applications for the LT1955 include
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elevator cues, point-of-sale prompters,
personal recording machines, background
music, call-on-hold phone storage and speech laboratories.
The LT1955 chip is also available installed onto a populated USB-compatible development board.
The development board features:
•
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•
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•
Signals (mono only) may be recorded
through the inbuilt microphone or direct via
line-in ports for mono and stereo inputs
The
LT1955 Evaluation Contact:
Board and the LT1955 Perrin, Wright & Associates
IC are available for via PO Box 5422, Clayton, Vic 3168
Tel: (0432) 502 755
the KitStop website.
Website: www.kitstop.com.au
New Raspberry
Pi 2 Model
B from
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OKW’s new iPad
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GST.
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I INTERFACE-TERMINAL housing.
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The front panels are available in matt anodised aluminium or
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For further details
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visit the website.
siliconchip.com.au
April 2015 67
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H 8168
$69.95
47-84”
H 8169
$99.95
$42
$54
$79
A 3834
89.95
$
HANDY!
NEW!
A 2620
H 8181A
25
49
$
$
Swing Arm LCD Monitor Bracket
Extends up to 335mm from the mounting surface. Ultra
slimline design. 20° ball joint for tilt adjustment. Suits all
100x100mm VESA monitors. Max weight 15kg.
Mount your TV just like a
picture on the wall.
Features reinforced wall
mounts, steel cabling &
TV support for easy
cable connection.
32-55” TVs, 50kg max.
14.95
$
HALF PRICE
$
H 8140
70 Silicon Chip
BUILD IT YOURSELF ELECTRONICS CENTRE
SAVE $20
NEW
79
SAVE 12%
USB Background Music Player
Simply plug in a USB stick, connect the RCA output to your
amplifier & press play! It even automatically loops. Requires
M 9272B 12VDC plugpack $17.95.
5.8GHz Wireless
AV Sender
99
$
SAVE $30
79
$
Great for wireless CCTV!
• Transmit stereo audio &
composite video without
cables from room to room •
30m range • IR sender built
in • Includes transmitter,
receiver & plugpacks.
SAVE $20
S 9359
Digital ready amplified
TV antenna for
great reception
on the road!
Easy to install,
includes cabling &
power supply.
L 2002
Also great
for boats!
99.95
$
NEW!
PRICE
DROP!
Wireless sound
anywhere you want it!
This wireless speaker uses
the latest Bluetooth 4.0
standard with quick NFC
device pairing with your
smartphone or tablet. 40mm
compact speaker and tuned
enclosure • Hands-free
phone functionality.
D 2037
Great for beginners and
mobile DJs requiring a robust
lightweight mixer. Two pairs of
switchable phono and line
inputs, plus stereo record and
amp outputs. Bass, treble and
gain adjustments. Cue
crossfader makes it easy to
cue upcoming tracks. Includes
power supply.
A 2544
Compact
Caravan Aerial
$
H 8150
Great for smaller TV’s
up to 32”. 200mm
VESA mount. With
locking bar. Max 35kg.
35
Powered by 9V battery or plugpack (M 9237A $17.95) this
tiny mixer is perfect for karaoke or small productions. It mixes
four 6.35mm mics. Robust steel case.
A 2710
Compact Small
Screen Wall
Bracket
SAVE 30%
Portable Mini Mixer
SAVE 24%
Great for cafes
and shops
“Picture Hanging”
TV Bracket
299
$
Lightweight, Compact
2 Ch DJ Mixer
9V battery
powered!
SAVE 18%
SAVE $80
C 8867C Handheld Pack
C 8868C Beltpack Pack
Scale up 1080p to
4K resolution
Plus, extract digital audio
from your HDMI signal
along the way. A handy
adaptor for 4K TV owners
looking to upscale HD
sources. S/PDIF audio out.
Includes power supply.
New 520MHz models work throughout Australia!
A complete wireless mic system with
your choice of handheld or beltpack
mic. • Plugs into existing PA systems
• Crisp vocal reproduction
• Ideal for clubs, restaurants
& wedding ceremonies.
Up to 70m range.
319
$
A 2384
119
$
Extend your sound system with ease!
19
$
.95
VALUE!
SAVE $30
Connect up to two additional pairs of speakers to your stereo amplifier
without risk of damage or overloading. Each speaker “zone” has
volume control and ON/OFF switch. 50W RMS per channel. Suitable
for 4 or 8Ω speakers.
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» Auburn NSW: 15 Short St » Perth WA: 174 Roe St » Balcatta WA: 7/58siliconchip.com.au
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Educational Electronics
In our opinion
these sound
just as good as
famous US
brands costing
3-4 times the
price.
Resellers
21.95
$
NEW!
K 1132
Age
8+
K 1126
158
$
The Ultimate In Live Sound By Redback®
Delivers punchy, powerful & clean sound. Titanium
diaphragm compression tweeter. Perfect for large
venues, halls, pubs, function centres, clubs etc. Ideal for
stand mounting on C 0521A. Wall mount with H 8055
($49ea). See page 107 of the catalogue for more info.
All models feature: • Titanium diaphragm tweeters
• Neodymium magnets for high power handling
Model
RRP
Per Pair
8” 80W
C 0996A
$250pr
12” 200W
C 1004A
$698pr
15” 250W
C 1008A
$798pr
$200
$560
$640
Size
Age
21
.95
$
SAVE UP TO
8+
NEW!
Motorised
4 in 1 Robotics Kit
6 in 1 Solar Recycler Kit
Assemble 4 different robot designs
which teach kids about geared
movements in a practical and fun
way! Requires 1xAA battery. No
soldering required.
Uses common household items like soft
drink cans and old CDs to create fun and
interesting solar powered designs. Build a
robot, steam roller, CD racer, bottle yacht
and more! No soldering required.
Age
Age
8+
8+
39
$
K 1123
.95
FUN KIT!
19.95
$
K 2204
NEW!
A great starter option for the kids
169
A 4198
$
30 in 1 Electronics Lab
Contains everything you need to
build a range of electronic projects
to encourage learning about
essential principles. Requires
2 x AA batteries.
SAVE $50
T4 4 in 1 Solar Robot Kit
Build a robot, t-rex dinosaur, drill vehicle
and rhino beetle. Performs different
movements when placed in the sun.
A great intro to solar power and
electronics. No soldering required.
Four stereo 30W
amps in one!
4 Zone 30W Amplifier
159
$
Ideal for multi-zone audio distribution. Offers 30W RMS
per zone (15W per/ch) all from a unit measuring just
200mm wide! Individual volume controls. Headphone
output. RCA input. Includes power supply.
SAVE $20
K 2222
Age
60
$
SAVE 24%
A 2630
10+
300 fun
projects in
the one unit!
300 in 1 Spring Terminal Electronics Lab Kit
4 Channel Headphone Amplifier
Ideal for audio monitoring in bands, music production,
connects four headphones with individual level control.
Stereo RCA, 3.5mm and 6.35mm TRS inputs. Includes
power supply. 113x73x40mm.
The ‘Rolls-Royce’ model with all the bells and whistles. Teaches you about electronics
from A to Z. You will learn about electronic parts, how to read schematics, and wiring
diagrams. All this, while building up to 300 projects. Provides many hours of tinkering
- a great way to gradually build on your knowledge. Requires 6 x AA batteries.
39.95
$
SAVE 20%
Age
8+
K 1115
189
$
SAVE $40
29
$
2x15W RMS
class-D amp.
A 1113
SAVE 17%
‘Follow Me’ Robot Kit
Simply hook up a pair of speakers and stream audio
from your Bluetooth® smartphone or tablet up to 10m
away. Infra-red remote volume, bass & treble
adjustment. Includes remote control, IR target &
power supply.
Uses four inbuilt microphones to
detect sound (such as a hand
clap) and moves toward it. No
soldering required. Requires 4 x
AAA batteries (not included).
B 0092
Sale Ends April 30th 2015
Altronics Phone 1300 797 007 Fax 1300 789 777
siliconchip.com.au
12+
Robotic Arm & Claw Kit
Wireless 30W Bluetooth Amplifier
®
Age
K 1107
A great introduction to basic robotics.
Includes five motors allowing base
rotation, shoulder, elbow and wrist motion,
plus claw for picking up objects (up to
100g). Includes wired controller.
Please Note: Resellers have to pay the cost of freight and
insurance and therefore the range of stocked products & prices
charged by individual resellers may vary from our catalogue.
Mail Orders: C/- P.O. Box 8350 Perth Business Centre, W.A. 6849
© Altronics 2015. E&OE. Prices stated herein are only valid for the current month or until stocks run out. All prices include GST and exclude freight and
insurance. See latest catalogue for freight rates. All major credit cards accepted.
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NEW ZEALAND
Christchurch Riccarton Global PC +64 3 3434475
April
2015 71
Christchurch Shirley
Global
PC +64 3 3543333
Part 2 of our quality Weather Station based on
System designed
by Armindo Caneira*
Built and written
by Trevor Robinson
*www.meteocercal.info
Starting to build it:
the ‘TX’
board
L
ast month, we told you how we obtained many of the
specialised parts from ebay sellers – in fact, quite a
number came from just a couple of them.
If you’re considering building your own weather station,
we’ll assume you’re well on the way to obtaining these
parts, along with the PCBs which come from the designer
in Portugal (www.meteocercal.info).
In this second instalment, we list all the parts, conveniently broken down into individual lists for each component
(ie, the transmitter, receiver etc) and then we move on to
building the first module – the TX (transmit) Unit.
As you can see, apart from the specialised parts, most
are “garden variety” components available at virtually any
electronics retailer. We understand that some of these retailers may also attempt to obtain stock of the more specialised
components as well.
Building the TX unit
If you’re familiar with building projects you can skip
this part as it’s all common practice and common sense.
If not, though, there are a few tips to keep in mind:
The soldering iron
Keep your soldering iron tip clean. Use a wet sponge
(often incorporated into soldering iron stands) or a copper
or brass woolly pad to regularly drag the tip over.
If you’re not using the iron, turn it off – nothing kills a
72 Silicon Chip
soldering iron tip faster than leaving it heated. And if you
don’t already have one, a temperature-controlled soldering
station is a really good investment (particularly if you build
more projects, repair devices and so on).
Beware of static
Quite a few of the components in this project can be damaged by static electricity. This can build up on you and on
your tools (including the soldering iron) simply by using
them – and usually you don’t know about it!
If a component is supplied to you on foam, in foil or
in an anti-static tube, take anti-static precautions such as
earthing the workspace and yourself, making sure any tools
you use are discharged and so on. It also pays to leave the
component in the anti-static material until you are ready
to use it.
You’ll find a lot of helpful tips on the internet, courtesy
of Dr Google.
Populating the PCB
These are double-sided boards so the first thing to do is
work out which is the “normal” (or top) component side
and which is the reverse side. Use our component overlay
diagrams for this.
It’s normal practice to insert the lowest height components first – obviously, resistors fall into this category.
Capacitors are usually soldered in next, remembering
siliconchip.com.au
that electrolytic types are polarised and must be inserted
into the PCB so that the “-” on the side of the component
matches the “-” symbol on the PCB.
Leave diodes and other semiconductors until later, with
“hardware” the last to go on.
Soldering
When soldering the components in, make sure you don’t
use too much heat but you need enough heat to make sure
the component leads are properly soldered to the pads on
both sides of the board, where appropriate.
If soldering a heat-sensitive component such as a transistor, it’s better to leave as much leg length as possible
because this will tend to minimise the heat getting to the
transistor itself. You can also use a small clip-on heatsink
(or even a crocodile clip) on each lead as you solder to
further protect the device.
Also make sure you don’t use too much solder and form
bridges between pads – most particularly when pads are
very close together. Good soldering comes with practice,
practice and more practice.
Inspection
When complete, give your PCB the once-over – twice!
First check your component placement, including polari-
ties where required, against the
overlay diagram. If there are
any blank component positions,
check that they are supposed to
be – blank, that is!
If you’re happy with what
you’ve done, then use a loupe
or magnifying glass to carefully
inspect the soldering. Where possible, check both top and bottom The miniature 433MHz
joints and if in doubt, use a con- transmitter module
solders into the TX PCB.
tinuity tester (or a multimeter)
to check for shorts between pins or pads. If a joint looks
doubtful now, re-solder it and avoid problems later!
Notes about the PCB and components
Normally, you won’t need to install resistors labelled R5
and R6 (10kΩ, 0.25W) on the PCB, as they are for optional
I2C devices that don’t have internal pull-up resistors.
After installing the 20kΩ preset potentiometer, set it
to its mid-point (ie, 10kΩ). This is a fine adjustment for
the wind vane but once set to 10kΩ, it’s unlikely to need
further adjustment.
The 7809 regulator and the IRLZ44N MOSFET both
come in “TO-220” packages so are easy to mix up. Refer to
SCL
OUT
+BAT
2
IN
12V
1
GND
100nF
4
3
REG1 7809
+9V
100nF
GND
POWER
3
SDA
2
+5V
1
1
GND
3.0k
2
2
IC
A0
A1
SDA
SCL
GND
+5V
3
1
4
2
5
3
6
4
7
5
8
6
9
10
UV-SOL
4.7k
4.7k
11
12
+5V
13
14
15
V+
OUT
IC1
TMP36
D12
D11
3.3V
D10
A0
D9
A1
D8
A2
D7
A3
D6
ARDUINO
NANO
A4
A5
D5
D4
A6
D3
A7
D2
5V
GND
30
5
29
4
28
3
27
2
26
1
25
D10
+5V
GND
EXP
24
3
23
DATA
2
22
20
100nF
19
LED2
FAN
K
+9V
1
K
A
21
GND
RF_TX
D1
1N4004 A
1
18
+9V
2
17
GND
D12
D11
D
100
–V
FAN
16
Vin
G
VR1
20k
GND
10k
10k
S
Q2
IRLZ44N
1
TEMPERATURE
SENSOR
2
+5V
2N7000
LM35DZ
3
4
GND
V+
D
OUT
G
D
D
IN
S
S
K
K
D
S
G
10k
100nF
4
3
2
1
100nF
RAIN
CLK
4
3
2
1
WIND
K
A
ARDUINO WEATHER STATION TX MODULE
siliconchip.com.au
DAT
+5V
DHT22
390
LEDS
OUT
1N4004
Q1
2N7000
GND
GND
A
A
TX LED1
1k
7809
IRLZ44N
G
+9V
GND
Fig.1: the circuit diagram for the first WeatherDuino
module to be built, the TX (Transmitter) Module.
April 2015 73
Parts List – TX Unit
Parts List – RX Unit
1 WeatherDuino Pro2 TX V4.0 PCB
(Notes)
1 Arduino Nano v3.0 microprocessor module
(H)
1 SHT10 digital temperature and humidity sensor module
1 FS100A 433MHz TX module
(I)
1 433MHz antenna
(D)
1 SMA female panel connector, with pigtail
(C)
1 TMP36 temperature sensor (#)
(G)
1 case to suit
(E)
1 heatsink to suit 7809 (#)
1 12V DC fan (optional – used only with a Stevenson Screen)
1 power supply, 12VDC <at> 1A or higher if fan used
Connectors (both plug and socket required #)
1 3-pin polarised header (power & battery voltage sensing)
1 2-pin polarised header (“Stevenson Screen” fan)
2 4-pin RJ-12 4P4C sockets (for temperature sensors)
1 6-pin polarised header (UV solar interface)
1 5-pin header (for expansion port; optional – unused but may
be used for later expansion)
Semiconductors
1 IRLZ44N N-channel MOSFET (Q2)
1 2N7000 N-channel MOSFET (Q1)
1 7809 9V positive voltage regulator (REG1)
1 1N4004 rectifier diode (D1)
1 3mm red LED (LED1)
1 3mm green LED (LED2)
(G)
Capacitors
1 100nF ceramic
Resistors (0.25W, 5% or better)
3 10kΩ 2 4.7kΩ (J) 1 3kΩ 1 1kΩ
1 20kΩ horizontal trimpot
1 390Ω
1 100Ω
(#) – See text for more information
their labels and the screen printing on the PCB to get them
correct! In both cases, the metal heatsink of both of these
devices goes towards the edge of the PCB.
To connect the SMA pigtail GND, you have to carefully remove some of green solder-mask on the FS1000A
module’s PCB, near the ANT hole. Then solder the centre
conductor to the “ANT” and the shielding braid to the
4004
Most constructors will power the TX unit with a 12V DC
IC1
LM35
100nF 100nF
10k
4.7k
4.7k
GND
Vin
A7
5V
3.0k
UV–SOL
WIND
1k
390
DAT
5V
CLK
GND
SCL
GND
5V
A0
A1
SDA
12V
D1
100
SDA
5V
GND
Power connection
VR1
20k 100nF
D3
D2
GND
D7
D6
D5
D4
A0
A1
A2
A3
A4
A5
A6
REG1 7809
10k
WeatherDuino Pro2 TX v2.50
By Werk_AG www.meteocercal.info
SCL
where you removed the varnish.
When installing the Arduino Nano, stagger the soldering
of the pins to avoid heat build-up. Even better, use a 30-pin
socket and plug the Nano in later.
GND
Q2 IRLZ44N
+Bat
10k
GND
Q1
2N7000
Arduino Nano
3.3V
Resistors (0.25W, 5% or better)
2 10kΩ
1 360Ω
1 120Ω (use 100nF ceramic capacitor instead if your Arduino
Nano has a CH340 chipset)
POWER
100nF
D12
D11
D10
D9
D8
EXP
Data
Vcc
RF_TX
SHT21/I2C
Connectors (both plug and socket required #)
1 3-pin polarised header (power & battery voltage sensing)
1 2-pin header (for screen mode pushbutton switch)
1 2-pin header (for SPST switch used for
program/run mode selection)
1 4-pin polarised header (for temperature sensor)
4 4-pin polarised headers (for TFT screen and backlight)
1 jumper shunt (for pressure sensor)
Semiconductors
1 2N7000 N-channel MOSFET (Q3)
1 3mm red LED (LED2)
Capacitors
5 100nF multi-layer ceramic
GND
5V
D10
D11
D12
(Notes)
1 WeatherDuino Pro2 RX PCB
(M)
1 Arduino Nano v3.0 microprocessor module
(H)
1 DS3231 real-time-clock Arduino module
(A)
1 3V lithium battery (coin cell) for RTC
1 DHT22 temperature/humidity sensor
(A)
1 BX-RM06 ASK OOK RF receiver
(B) (K)
1 BMP180 (or BMP085) barometric pressure module
(A)
1 SMA female board connector
1 Jumper (sets BMP module voltage)
1 momentary pushbutton switch, NO
(E)
1 SPST pushbutton on/off switch
(E)
1 display: either ST7735 1.8” TFT, OR 20 x 4 alphanumeric
LCD, OR 16 x 2 alphanumeric LCD
(A)
1 433MHz antenna
(D)
1 case to suit
(E)
+9V–
DHT22/SHT1X FAN
FANLED
A
100nF
TXLED RAIN
A
Fig.2 (left): the WeatherDuino Pro TX PCB component overlay shown at 1:1 scale, with the blank PCB alongside. There are
minor dfferences between the prototype boards and the final production boards.
74 Silicon Chip
siliconchip.com.au
Parts List – Wireless Display Unit
1 WeatherDuino Pro2 wireless display PCB
(includes all SMD parts already soldered on)
1 5V DC power supply, fitted with mini-B USB plug
1 pushbutton switch, momentary, NO
1 SMA female PCB connector
(Notes)
(M)
(E)
(C)
Semiconductors
1 Arduino Nano
(H)
1 DHT22 temperature/humidity sensor
(A)
1 BX-RM06 ASK OOK 433MHz RF receiver module
(B)
1 3mm red LED (LED4)
1 display – one of: ST7735 1.8” TFT,
or ILI0341 2.2” 20 x 4 alphanumeric LCD,
or ILI934 2.4” 320 x 240 alphanumeric LCD
or 20x4 LCD module OR 16 x 2 with I2C
module (#)
Capacitors
1 10µF/16V tantalum
3 100nF ceramic
Optional components for Rx Unit
(Highly recommended, needed if you want to relay data to a
wireless display).
1 KXD-10036 433MHz transmitter module
1 433MHz antenna
1 2.5mm DC power socket
1 2N7000 MOSFET
1 3mm green LED
1 7809 9V positive voltage regulator
1 heatsink to suit 7809
Capacitors
1 10µF 16V tantalum
Resistors (0.25W, 1% metal film)
7 10kΩ
1 180Ω
Notes Table
(#) See text for more detail
Connectors (recommended, as it makes it a lot easier to
connect and remove the PCB from its housing for later
firmware updates, troubleshooting, etc).
1 5-pin polarised header (for touch screen interface)
1 SMA female board connector
1 4-pin header (for inside temperature sensor)
Resistors (0.25W, 1% metal film)
1 10kΩ
1 470Ω (required for V4.03 PCB only)
– please refer to listings last month for ebay item numbers
A All these came from same ebay seller.
B From supplier nominated, both pieces come together as a pair. These can be brought separately elsewhere but must match the
picture as these types work best!
C All these came from same ebay seller.
D All these came from same ebay seller.
E Up to the end user to choose the best for the application/ and desired look.
F Also requires 12VDC power pack to suit (positive centre)
G All these came from same ebay seller.
H All these came from same ebay seller.
I This came from the same seller as A (above).
Please don’t use the included Receiver module in this pair. It’s not good (but the transmitter is good!).
J Only required if you are using the I2C connector with a device that doesn’t have internal pull-up resistors on the SDA and SCL lines.
K Can be omitted if you buy the KXD-10036 RF Transmitter/Receiver modules for the optional data relay as this part is included in the
kit.
M From www.meteocercal.info/forum/index.php
plugpack. But if it’s not close to mains power, you could
use a solar panel and 12V battery. The TX unit allows remote monitoring of the battery voltage so if using a battery,
connect the +BAT terminal to the 12V battery (+) and the
12V terminal to the output of your solar charger controller.
If you’re using a plugpack, simply connect the +BAT and
12V terminals together.
Your TX unit should now be complete and ready for
connection of the External Temperature Sensor. But first
you need to attach it to a cable.
Temperature Sensor
As discussed last month, we opted for the SHT10 Temperature Sensor as we feel it offers the best “bang for buck”.
Others might be more accurate but are also significantly
more expensive. The SHT1x and the DHT22 use a serial
protocol to pass information to the Arduino microprocessor.
siliconchip.com.au
SHT1X
FRONT
VIEW
SHT1X
REAR
VIEW
DH22
FRONT
VIEW
PCB
designation
Schematic
Pin
SHT1x
pins
DHT 22
pins
GND
1 (GND)
-
3 or 4
DAT
2 (D6)
D
2
5V
3 (5V)
+
1
CLK
4 (D9)
S
April 2015 75
ARDUINO LINGO:
In Arduino-speak, software is known as “sketches”.
And the add-on boards which plug into the Arduino are known as “shields”.
The datasheet for these SHT1x sensors can be found
here: www.sensirion.com/fileadmin/user_upload/customers/sensirion/Dokumente/Humidity/Sensirion_Humidity_SHT1x_Datasheet_V5.pdf
The WeatherDuino TX board also supports the SHT1X
(and the SHT2X using the I2C port), so if your budget allows
it, feel free to upgrade. However, if you go with the SHT2x
module, you will need to visit the Meteocercal forum for
the details required to use it.
The ebay reference number we gave last month will take
you directly to the SHT10 which has the senor already
attached to a breakout board, making it easier to connect
to the TX Unit.
Sensor cable
Make up a temperature sensor cable using a 4-pin connector (eg, Jaycar HM3404) and a length of good quality
4-core cable (maximum length 5 metres). Carefully solder
the pins and heatshrink the other end of the cable to the
sensor pins (or use a suitable plug to connect but remember,
this needs to be protected as it is out in the open).
Case Temperature sensor
The TMP26 temperature sensor gives a voltage output
proportional to the temperature.
This is used only to monitor the temperature inside the
TX unit case. However, it isn’t essential so if you want to
save a little money, this can be omitted.
Programming the Arduino Nano
Programming is done by connecting the Nano to a PC
USB port and running suitable software.
While all this looks quite complex at first, in reality it’s
fairly easy, especially for the TX unit. Once you’ve done
these steps once, you shouldn’t need these instructions
again.
Ok, lets get started on some software fun.
Finding the COM Port
To program the Nano, you need to see what COM port is
created when the Nano is connected to the host PC’s USB port.
Before plugging in the Nano, open the Device Manager
on the PC (Control Panel>Device Manager) and expand the
“Ports (COM & LPT)” item by double clicking it.
Now plug in the Nano and you should see a COM port
created like that shown below left.
If the icon beside it has an exclamation mark then you
will need to install the driver.
If you purchased the Nano from the ebay supplier listed
last month, the required driver for the CH340G serial adaptor is called CH341SER.zip.
You can download it from that seller’s site or from this
thread at the Meteocercal forum www.meteocercal.info/
forum/Thread-Arduino-Nano-USB-Driver
By the way, the Serial/USB converter onboard the Nano
dictates which method of reset pullup we use later on the
RX/WD boards, but we will cover that in the next part of
the series.
Keep the Nano plugged in and move on to the next step.
Installing and configuring the Arduino IDE
Download the Arduino integrated development environment (IDE) software from the Arduino.cc site.
You will need the Arduino 1.5.8 BETA IDE as the code
needs the extra optimisation that this beta release of the
IDE gives, otherwise the code will not fit in the Nano’s
32KB flash memory.
You can download the Arduino IDE here: http://arduino.
cc/en/Main/Software#toc3
I’d recommend selecting and downloading the Windows
Installer option from the above link (if, of course you are
running Windows on this PC). Run the installer and give
it a little while to install as it’s quite a large program with
all the built in libraries.
Once it’s installed open it. Then:
1. Click File then Preferences. Take note of the Sketchbook
location. The path will have the name of the current logged in
user.
This is where we’ll extract the WeatherDuino software folders
to.
2. While in Preferences, we recommend checking the
76 Silicon Chip
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*For a free monthly mailer please contact us* Email: salesdept<at>rockby.com.au
2015 77
“Display line numbers” and “Automatically associate .ino files with
Arduino” check boxes. Then click OK.
3. Next click Tools, then Board. Find and Select Arduino Nano.
4. Click Tools again, and then Processor. Select ATmega328.
5. Once again click Tools, then Port and then select the COM port
that you saw in the step above.
All good? Close the Arduino IDE and move to the next
step.
WeatherDuino software
Now you need to download the WeatherDuino software
(also called a sketch in the Arduino circles) from the
Meteocercal forum site.
Here is the link to the thread for the RX and TX unit:
www.meteocercal.info/forum/Thread-WeatherDuinoPro2-RX-TX-Software-Latest-Release
Save the .zip file to wherever is convenient.
Now extract the .zip file to the location found in step 1
above. Choose OK to merge or replace the files.
If the libraries are not in the right location the IDE will
throw errors when you go to compile and upload the software to the Nano.
You can manually ask the IDE to import the Libraries
(menu/sketch/Import libraries) tho it’s easier just to put
them where the IDE is expecting to find them.
Browse to the WeatherDuino_Pro2_vXXX_XXXXXXXX
in the location in step 1 above (The “x”’s will change depending on the version).
Inside there should be three folders. Open the WeatherDuino_TX_vXXX_bXXX and inside that folder should be
WeatherDuino_TX_vXXX_bXXX.ino, double click that and
it should open in the Arduino IDE.
Make sure it’s the file with TX in the filename.
Configuring the WeatherDuino Pro TX options
Now you should be looking a window that looks like this:
articles, nothing needs to be changed here in the TX config (shown below) unless you need to alter the Stevenson
Radiation Screen fan hysteresis (if used), or if you decided
against going with the SHT10 temperature sensor, then you
would need to alter this line to suit:
#define ID1 0 // Temp / Hum data - 0 for SHT1x sensor,
1 for DHT22 sensor
for say, a DHT22 temp sensor
#define ID1 1 // Temp / Hum data - 0 for SHT1x sensor,
1 for DHT22 sensor
An example of WeatherDuino TX user options section
of the code:
// ----------------------------------------------------------------------------// User configurable options start here.
// ------------------------------------------------------------------------------byte StationID = 0xA1; // Must be equal to your RX Unit
(Value from 0x00 to 0xFF)
byte UnitID = 0; // If you use only one TX unit define it as UnitID = 0
// For a second TX unit, define it as UnitID = 1
// ---------------- Let’s define the data we want to send ----------------//#define ID0
// SHT21 Sensor
#define ID1 0
// Temp / Hum data - 0 for SHT1x sensor,
1 for DHT22 sensor
#define ID2
// Wind data
#define ID3
// Rain data
//#define ID4
// UV / SolRad data
#define ID5
// Hardware Status - System Temp, Battery
Voltage etc
byte fanOn_HiTemp = 32; // RS Fan turn on when outside temperature
is >= than this value (°C)
byte fanOn_LowTemp = 1; // RS Fan turn on when outside temperature is <= than this value (°C)
byte fanOn_LowWind = 2; // RS Fan turn on when Wind Average is
<= than this value (m/s)
//------------------------------------------------------------------------------
Uploading the software to the
WeatherDuino TX_unit
You can read the comments which always start with “//”
(the // tells the device not to run the code), doing so should
make it fairly self explanatory what that line of code does.
We will attempt to explain main config lines, where
needed, that you need to change to get a working Weather
Station suited to you location and set up.
Any queries regarding changes to settings besides the
usual basic configuration discussed in these articles, should
be asked in the Metocercal forum (www.meteocercal.info/
forum).
For this Weather Station we’re building in this series of
78 Silicon Chip
If you have made changes, we would recommend saving
them with a descriptive name (file/save as).
Then it’s as easy as clicking the right arrow in the IDE
to compile and upload the sketch.
Normally it will work without error if configured correctly. But there’s two problems that can happen:
1. The IDE will give an error that the sketch won’t fit.
That’s usually caused by not using the latest beta version
of the IDE.
2. The IDE will give an error if it can’t find the libraries required. Check the location of the libraries or use the
manual import function in the IDE (Sketch/Import Library).
At this point you can disconnect the TX unit from the
Host computer and when you power it up from a 12VDC
power pack, you should have an operating TX unit sending
data packets out over 433MHz.
The green transmission LED should also blink when it
does.
The sensors and instruments
Also at this point, it would be a good idea to read up
on sensor and instrument placement. There are quite a
siliconchip.com.au
few “rules” on where specific sensors need to go to obtain
correct readings.
For example, the rain sensor needs to be located away
from buildings so that any rain which falls into it is not
subject to amplifying or shielding; the temperature sensor
should ideally be located in a “Stevenson’s Screen”; wind
sensors cannot be located in either a wind shadow or wind
funnel and so on.
The location will also govern where you would locate
your TX unit and its sensor suite – and of course the cable
run lengths required.
There’s plenty of great information on the internet regarding this subject. A fairly good summary can be found
here: www.wunderground.com/weatherstation/installationguide.asp
Connecting the “Fine Offset” sensors:
As mentioned in the first part of this series, the TX unit
supports the Fine Offset weather station sensors. These
look like this:
The Anemometer
The Wind Vane
The Rain Gauge
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Usually with the Fine Offset sensors, the Anemometer
connects to the Wind vane via the common old flat 4-core
telephone cable, using one pair. Then the Anemometer
connects to the TX unit using the same cable.
The Wind vane data goes via one pair to pins 1 & 2 and
the Anemometer goes via the other pair to pins 3 & 4. The
board has screen printed designations showing which RJ11
socket is which.
If your sensors don’t usually connect in this fashion,
then you will need to make or buy a splitter of sorts.
Check the schematic – it shouldn’t be too difficult. You
may even be able to use a phone line splitter (though not
a ADSL splitter).
Wind and Rain sensors are available via ebay and some
online stores.
Tip: By using multiple TX units, you can mount more
than one sensor, in various locations. This is handy. for
example, if your anemometer needs to be higher than the
cable allows, or, another example, when you need to move
the temperature sensor to a better or shadier position.
To use more than one sensor, you need to alter this code
and upload it to the second TX unit (the system supports
a maximum of three TX units). A third unit can only be
used with temperature/humidity and solar/UV sensors,
not with rain or wind sensors.
byte UnitID = 0; // If you use only one TX unit define it as UnitID = 0
// For a second TX unit, define it as UnitID = 1
So this part of the series was fairly easy. huh? Good, as it was
bit of a warm-up as the next part gets a little more involved
with the configuration of the RX unit.
And at the end of the next part you will have a fully operational weather station that’s capable of sending data to the
Internet! See you then.
SC
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April 2015 79
CIRCUIT NOTEBOOK
Interesting circuit ideas which we have checked but not built and tested. Contributions will be
paid for at standard rates. All submissions should include full name, address & phone number.
REG1 LM2936Z-5
LM2936Z
OUT
+9V
IN
GND
IN
OUT
GND
13
VBB
10
10k
FC
VCP
CP1
+5V
4.7k
100 µF
4
SPEED
VR1
5k
MOTOR
SPEED
OUTPUT
1
Vdd
MCLR
2
4
2
100nF
8
100nF
100nF
FG
CP2
IC1
A4941
9
GP5
TEST
OUT1
3
W1
15
W2
OUT2
100 µF
16
100nF
W3
7
6
AN0
AN1
5
IC2
PIC 12F6 83 CCP1
GP4/AN3
7
20kHz
OUT3
PWM
3
CTAP
Vss
8
6
SENSE
SLEW
GND
5
1
MOTOR
12
14
GND
* 0.4Ω
11
0V
FC SET FOR 50ms STARTUP
* SET MAXIMUM MOTOR CURRENT
Hard drive brushless motor
controller with speed control
Most of us will have an old hard
disk drive in our junk boxes. If you
dismantle these you will find that
they contain a very high precision
3-pole brushless motor without Hall
effect sensors. If you wish to run
these motors then this simple circuit
is for you.
More complex brushless motors
contain three Hall effect sensors
that tell the circuit exactly where
the motor poles are in relationship
to the permanent magnets. Allegro
make the A4941 3-phase sensorless fan driver (available from RS
Components) that senses the back-
co nt ri bu ti on
MAY THE BEST MAN WIN!
As you can see, we pay $$$ for contributions to Circuit Notebook.
Each month the BEST contribution (at the sole discretion of the editor)
receives a $150 gift voucher from Hare&Forbes Machineryhouse.
That’s yours to spend at Hare&Forbes Machineryhouse as you see fit
- buy some tools you’ve always wanted, or put it towards that big
purchase you’ve never been able to afford!
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80 Silicon Chip
Contribute NOW and WIN!
Email your contribution now to:
editor<at>siliconchip.com.au
or post to PO Box 139, Collaroy NSW
EMF from the un-energised winding
produced when the motor rotates.
This reduces the cost of the brushless motor as the Hall effect sensors
can be omitted. The only problem
is that the motor has to be rotating
before the back-EMF can be sensed.
To start the motor, commutations
are provided by an on-board oscillator. These commutations are part
of the start-up scheme, to step the
motor to generate back-EMF until
legitimate back-EMF zero crossings
are detected and normal back-EMF
sensing commutation is achieved. A
complete description of the sensing
technique can be found in the A4941
data sheet.
Typical hard disk drive motors
will have three or four pins for the
connections to the windings. The
windings are connected in a star (Y)
arrangement as shown in the circuit.
The motors with three pins have the
start of the windings connected to
them and the ones with four pins
also have the common connection
run out to the additional pin.
siliconchip.com.au
siliconchip.com.au
A
CELL #1
14.4V
REGULATED
CHARGER
λ LED1
D1
K
B
A
K
E
B
K
A
10k
E
CELL #2
10k
4 x IDENTICAL CIRCUITS (ONE PER CELL)
A
Q8
2N3055
C
Q7
BD139
E
K
B
K
E
B
λ LED4
D7
D8
C
CELL #4
–
C
Q1
BD139
CELL #3
+
D2
C
Q2
2N3055
4 x 3.6V LITHIUM CELL BATTERY PACK
To determine the motor pin-out,
measure the resistance between the
various pins. When you have the
common terminal, the resistance
from it to each of the three others
should be the same. Those motors
with three wires will still work as the
IC will generate its own null point if
the common is not connected.
By the way, to reverse the direction of the motor, swap over the connections to any two of the windings.
The maximum motor current is set
by the 0.4Ω resistor on pin 14 of IC1.
The value of this resistor is equal to
200mV divided by the maximum
motor current. The motor current
is 9V divided by the resistance of
two motor windings added together.
Two 100nF charge pump capacitors at pins 2, 3 & 4 of IC1 provide
the high voltage for the output stage
drivers. The FG output at pin 8 of
IC1 gives a frequency signal related
to the speed of the motor.
IC1’s FC (force commutation) pin
(pin 10) sets the start-up time. The
time is 50ms when connected to
+9V, 100ms when connected to 0V
and 200ms when left open (no connection). Try different settings if you
find that the motor is hard to start.
The slew input, pin 6, enables or
disables soft switching. It is enabled
when connected to 0V and disable
when left open.
To vary the speed of rotation,
PIC12F683 microcontroller IC2
is programmed to convert the DC
voltage from 5kΩ potentiometer
VR1 at pin 7 to a 20kHz pulse width
modulated (PWM) signal on pin 5.
This is fed to the PWM input, pin 7,
of the A4941 (IC1). The PWM duty
cycle can be varied between zero
and 100%, depending on the setting
of the VR1.
If you can’t make your own PCB
you will need a 16-pin TSSOP breakout board (available from RS Components) to mount the A4941. The
IC has an exposed thermal pad on
its base that needs to be soldered to
an earth plane of at least one square
inch to dissipate the heat generated.
To achieve this, when using the
breakout board, I soldered a piece of
copper foil onto the IC’s base before
soldering the device in place. This
foil was then soldered to a larger
piece of foil on the PCB containing
A
K
A
10k
10k
2N3055
BD13 9
LEDS
D1– D8: 1N4148
A
K
K
A
Lithium battery
cell equaliser
While lithium batteries of all
types have big capacity advantages
over other rechargeables, it is most
important that each cell in a battery stack is charged up to the same
voltage. So every lithium cell needs
an equaliser and while these are
usually incorporated into lithium
battery charger controllers, if you
are making up a battery from individual cells and charging them with
a simple circuit, you need a separate
equaliser for each cell, as shown in
the accompanying circuit.
In effect, the equaliser is just a
brute-force shunt regulator. So in
this case, the battery is charged to
14.4V and each cell has an accompanying shunt regulator which limits
the cell voltage to a maximum of
about 3.6V.
Each equaliser comprises a Darlington-connected transistor pair,
two silicon diodes and a red LED. It
works like a rugged zener diode, with
the limit voltage set by the total of
the forward voltages of the red LED,
the rest of the components.
The software, PWMMotorControl.
hex, is available for download from
B
E
B
C
E
C
the two diodes and the two baseemitter junctions of the transistors.
Note that the forward voltages of both
the diodes and the transistors will
be lower than normal (ie, less than
0.6V) because they operating at quite
a low current, to give a total of about
3.6V. If you have lithium cells which
require a higher end-point voltage,
add another series silicon diode.
So to sum up, as the cells begin
charging, each cell equaliser/shunt
regulator will have negligible effect
but as it approaches the limiting
voltage for its associated cell, the
equaliser will progressively bypass
more current around the cell, until
negligible current is actually going
into the cell. This shunting action
will mean that transistor Q2 will
dissipate a significant amount of
power, depending the current output
of the charger. Hence, Q2 may need
a substantial heatsink.
For example, if the charger delivers 2A, the dissipation in Q2 will
be 7.2W and four equalisers will
dissipate around 30W.
David Francis,
Kilburn, SA. ($45)
the SILICON CHIP website.
Les Kerr,
Ashby, NSW. ($75)
April 2015 81
Circuit Notebook – Continued
+5V
+5V
100nF
100nF
1k
KEYPAD
(E.G., JAYCAR AB-3462)
2
(4V)
1
ROW1
2
1
+V
B4
3
C0
1k
7
(3V)
4
ROW2
5
C1
6
LK1
1k
6
(2V)
7
ROW3
8
4
9
4
*
0
#
COL1 3
COL2 1
COL3 5
ROW4
17
19
1k
22k
ICSP
HEADER
S1
A
T1
B7
SER.OUT
B0
SER.IN
DISP2
7
9
6
8
4
7
2
6
1
5
9
3
10
6
a
f
DISP1
7
b
g
e
c
a
4
f
2
9
d
b
g
e
1
d
Vcc
3,8
13
DATA
1k
12
1k
11
170mm
LONG
ANTENNA
c
10
3,8
433MHz
TX
MODULE
C
B
B
Q2
+
E
C
Q1
E
PIEZO
BUZZER
REG1 7805
K
IN
16V
+5V
OUT
433MHz Tx MODULE
10 µF
GND
ANT
Vcc
DATA
GND
16V
TAG
0V
D2 1N4004
A
PICAXE-based next
number display system
This system is for business owners
and displays numbers matching the
last two digits on numbered tickets
or dockets, to determine the order
clients or customers will be served.
This system is suitable for use in
waiting rooms, service counters and
in fast-food outlets.
The design is in two parts: (1) a
wall-mounted “display unit” with
multi-tone alarm and jumbo LED
display; and (2) a desk-mounted
control unit with a keypad and
small LED display. Ticket numbers
between (00) and (99) are supported
by using 2-digit 7-segment displays.
Both parts are based on a PICAXE20M2 microcontroller (IC1 & IC2)
K
ANT
GND
18
0V
20
2200 µF
E
82 Silicon Chip
B3
7x 100Ω
10
0V
6V
N
B6
B2
D1 1N4004
6V
230V AC
MAINS
2
B5
B1
10k
18k
POWER
A
C4
C7
IC1
PICAXE 20 M 2
16
18k
C6
C5
15
18k
C3
TONES
1k
(1V)
C2
14
7805
Q1, Q2: BC 33 7
1N4004
A
K
and they operate in the UHF band using pre-assembled 433MHz wireless
modules. The numbers are transmitted using eight bytes of Manchester
encoded data, containing both a
5-byte “security code” and a 3-byte
“control code”. The data is transmitted using the “rfout” command and
received using the “rfin” command.
The units may be placed up to 20
metres apart and do not require any
interconnecting cable. The program
notes give more details, in particular
for changing the default “security
code”.
The control unit employs IC1 and
a ZW-3100 (TX) transmitter module.
The small 7-segment display is multiplexed using transistors Q1 & Q2
to sink the common cathode pins,
while seven 100Ω current-limiting
B
E
GND
IN
C
GND
OUT
resistors diIan Robe
rtson
rectly drive
is this m
onth’s w
the anode
inner
of a $15
0 gift vo
ucher fro
pins.
m
Hare & F
orbes
The keypad connects to
the analog input pins
15-17 of IC1. The program is able
to detect individual keys using the
voltage levels present on the resistor
divider feeding the keypad. Fitting
a jumper on LK1 will increase the
number of alarm tones played from
two to four.
There are two ways to change
the displayed numbers. First, you
can add “one” to the existing number by pressing the * key (step)
followed by the # key (send).
Alternatively, to select any other
number, you simply press two
siliconchip.com.au
+5V
TENS
DISP4
170mm
LONG
ANTENNA
7
JUMBO
a
f
b
g
e
c
d
100nF
Vcc
ANT
433MHz
RX
MODULE
7 x 100Ω
10
6
9
4
8
3
7
2
6
9
5
10
3
1,5
DATA
UNITS
1
4
19
2
GND
+V
C0
B0
C1
B1
C2
B2
C3
B3
C4
B4
C5
C7
18
6
16
4
15
3
13
JUMBO
2
13
9
11
IC2
B7
PICAXE 20 M 2
10
f
e
B6
SER.IN
10
c
IC3d
d
8
9
IC3c
1,5
12
220 µF
6
5
16V
IC3b
2
1
12
11
IC3a
SER.OUT
IC3f
IC3e
b
g
C6
4
3
8Ω
SPEAKER
7
IC3: 74HC14
0V
20
10k
14
a
14
B5
DISP3
7
17
22k
ICSP
HEADER
7 x 100Ω
2x
100nF
0V
433MHz Rx MODULE
–5V
D3
A
REG2 7805
K
IN
Vcc
DATA
DATA
GND
ANT
GND
GND
Vcc
POWER
A
D4
T1
S2
230V AC
MAINS
K
16V
TAG
0V
0V
D5
6V
A
K
10 µF
2200 µF
GND
D6
K
A
IN
D3–D6: 1N4004
A
siliconchip.com.au
16V
TAG
16V
K
The Manchester encoded data is
received by the RX module and fed
to input pin 4 of IC2. The received
data has the “security code” tested
before displaying the next number
and sounding the alarm tones based
on information in the control code.
The wireless transmitter and
receiver modules will each require
a suitable antenna, the simplest being is a length of stiff plastic coated
hook-up wire 170mm long. Depending on the enclosure dimensions, the
antenna wire may be left straight or
coiled into a spiral.
The control unit and display unit
circuits each employ a transformerbased power supply, with both having a 7805 3-terminal regulator while
the display unit also has a 7905
3-terminal regulator. The jumbo display segments each have four LEDs
in series (forward voltage drop 8V)
and this requires the full rail-to-rail
voltage of 10V DC.
–5V
OUT
REG3 7905
number keys (00-99) followed by the
# key (send).
Numbers are transmitted by turning on output pin 14 of IC1 to power
the TX module’s VCC pin, then output pin13 of IC1 sends Manchester
encoded data to the TX module’s
DAT pin. Each key press is accompanied by a beep from the 3.3kHz
piezo buzzer on pin 18 of IC1.
The display unit employs IC2 and
a ZW-3102 (RX) receiver module.
The 7-segment display is driven by
14 microprocessor output pins using
100Ω current limiting resistors.
Display multiplexing was not
used as the “rfin” command monitoring the RX receiver module’s DAT
pin prevents the normal display
scanning process from running. The
alarm tones are generated in the software and sent to output pin 12 of IC2
and then to 74HC14 buffer stage IC3
which drives the capacitor-coupled
8-ohm loudspeaker.
10 µF
16V
6V
N
E
2200 µF
A
+5V
OUT
GND
7805
GND
IN
GND
7 9 05
OUT
IN
GND
IN
OUT
Note that each regulator requires
a small heatsink (Jaycar HH8502 or
similar).
The displays used on the prototype were ZD1855 (small) and
ZD1850 (Jumbo) from Jaycar. Other
types could be substituted but
the pin numbers may not be the
same. The ability to directly drive
the Jumbo displays was tested by
continually displaying “88” for
many hours while checking that the
microcontroller remained cool and
operated normally.
The microcontrollers each have
ICSP headers for programming, with
pin 2 as the serial input and pin 19
as the serial output. Use a special
PICAXE serial or USB cable and
download nxcontrol_20m2.bas to the
control unit and nxdisplay_20m2.
bas to the display unit from the
SILICON CHIP website.
Ian Robertson,
Engadine, NSW.
April 2015 83
Vintage Radio
By Ian Batty
The AWA 897P: Australia’s
first transistor radio
Designated the model 897P, Australia’s first
transistor radio was developed by AWA and
first marketed in November 1957. It uses seven
transistors, is built onto a metal chassis and
uses the same case as its valve predecessor.
W
ITH THE centenary of Amalgamated Wireless Association’s
listing on the Sydney Stock Exchange,
it seems timely to review their first
transistor radio. Formed as a result
of the rivalry between the German
Telefunken and British Marconi companies, AWA has been a pioneering
presence in radio and electronics here
in Australia and around the world.
The first chairman, Hugh Denison, eventually made way for the
better-known Ernest Fisk. Fisk’s later
knighthood and towering presence
84 Silicon Chip
eventually extended to the familiar
“Fisk Radiola” badges on many of
the company’s radios and even to the
naming of the former Imperial Wireless Chain station as “Fiskville”. For a
more complete history on this, see the
Historical Radio Society of Australia’s
Radio Waves, July 2013.
Early transistor radios
Regency (USA) marketed the first
successful all-transistor radio in 1954,
designated the TR-1 (SILICON CHIP,
April 2013). Given the stupendous en-
gineering task (a learning “cliff” rather
than a “curve”), AWA’s offering of the
897P in November 1957 is remarkable.
The initial offering used a mix of “2N”
and “OC” transistor types, the latter
echoing AWA’s early association with
German company Telefunken.
The CSIRO had begun investigating
semiconductors in 1953, initially with
the assistance of Bell Laboratories. Dr
Louis Davies had spent six weeks at
Bell Labs and came back from the US
armed with two essential precursors
to making transistors: the technologies for purifying germanium and for
growing single crystals of germanium.
A subsequent symposium attracted
the attention of industry, rather as the
original Bell Labs seminars had in the
USA. Although all the “big four” Australian companies attended, it was the
work of Ted Watt and Henry Banks that
led to AWA starting local production
in 1958. Watt and Banks had attended
an engineering “apprenticeship” at
RCA and their efforts were pivotal in
AWA’s entry to the local market.
The 897P transistor radio used an
existing valve portable case design
from the model 581PZ. Like many sets
of the era, it also used a pressed and
punched metal chassis and the parts
were all installed by hand. It’s quite
similar the RCA Victor Transistor Seven, even down to the 2-gang volume
control (the RCA set was described in
the October 1956 issue of Radio, TV
and Hobbies).
Two restorations
This article summarises two restorations, as I was very generously loaned a
number of 897 variants by the HRSA’s
Ray Gillett. And while on the subject
of variants, the original 897P used
RCA 2N219 (converter) and 2N218
transistors in the RF/IF section and
Telefunken OC602/604 types in the
audio stages. By contrast, the later
897PX/PY/PZ used all RCA types,
with 2N408 & 2N270 types now in
the audio amplifier. These are all
siliconchip.com.au
Fig.1: AWA 897P is a 7-transistor superhet design with 455kHz IF stages. Transistor VT1 is the converter stage, VT2
& VT3 are IF amplifier stages, VT4 is an audio preamplifier, VT5 an audio driver stage and VT6 & VT7 function as a
push-pull output stage.
“second generation” alloyed-junction
types.
The 897P: first look
As stated, AWA’s 897P uses a press
ed and punched metal chassis just
like the Bush TR82C (SILICON CHIP,
September 2013). It uses seven transistors, five of which are fitted into
chassis-mounted rubber grommets
with their leads then wired to adjacent
solder tags.
By contrast, the two output transistors are held in heatsink clips which
are screw-mounted on the underside of
the chassis. This differs from the later
PX, PY & PZ models which (strangely)
also have their output transistors
mounted in rubber grommets, defeating any possibility of heatsinking.
Unfortunately, the grommet-mounting technique means that the transistor leads are underneath the chassis.
This means that unless the chassis is
removed, the only circuit access, either
for measurement or signal injection, is
at the aerial coil, the volume control
and speaker terminals.
As shown in the photos, the chassis
is mounted in a substantial leather case,
with the wrap-around shell closed off
by stitched-on ends. The front dial
turns easily with a direct drive. It sits
within the front escutcheon which
siliconchip.com.au
also contains the speaker grille. The
volume/power switch is mounted on
the righthand end of the set.
897P circuit details
Fig.1 shows the circuit details of the
AWA 897P. Many of its components
were common to the valve era and
apart from the the transistors and the
low-voltage electrolytic capacitors,
they appear much the same as those
found in portable battery valve sets.
Some models use the classic Philips
tuning gang with rounded edges on its
frame, brass plates and identical aerial
and oscillator sections. The 897P and
897PY models use gangs with 445pF
per section and a 470pF padder, while
the 897PZ and 897PX models use
385pF sections and a 420pF padder.
There are also minor mechanical differences, with the 897PZ and 897PX
models using a different dial scale.
The circuit itself is a fairly conventional 7-transistor superhet design.
The RF signal is picked up by antenna
rod T1 and tuned by C3, one section of
the tuning gang. The other section, C4,
tunes the local oscillator. The tuned RF
signal is then fed to the base of PNP
transistor VT1 via coil T2.
VT1, a 2N219, is the converter stage
(ie, a combined local oscillator and
mixer) and this uses collector-base
feedback (ie, via T3’s tuned primary
and a tapping on T2’s primary) to
maintain oscillation. While this works
reliably, it does increase the amount
of local oscillator (LO) radiation back
out through the antenna rod.
The mixer’s output feeds the primary of the first IF transformer (T3).
This uses a tapped secondary winding
to match into the low base impedance
of the first IF amplifier.
The two following IF transformers
use tapped primaries and secondaries,
with VT2 & VT3 (both 2N218 transistors) functioning as IF amplifiers.
The two IF amplifiers operate similarly to those in most other sets. AGC
action is applied to the first IF amplifier
stage (VT2) alone, reducing base bias
and thus the total collector current
on strong signals. In common with
other designs, reducing the collector
current reduces current gain and thus
the stage gain.
The applied AGC voltage (at VT2’s
base) is quite small, with the base bias
dropping by only about 70mV at full
signal. This is much less than in many
other sets and is due to the voltage
divider connected to VT2’s emitter.
Instead of allowing the emitter voltage to also drop with incoming AGC
(and thus “softening” the response
somewhat like a remote cut-off valve),
April 2015 85
This view shows the general layout of the major parts on the top of the 897P’s
chassis. Transistors VT1-VT5 were mounted by pushing them into rubber
grommets from underneath the chassis.
Unlike VT1-VT5, the two OC604 transistors used in the push-pull output stage
(VT6 & VT7) were attached to the underside of the chassis using metal clamps.
Note the point-to-point wiring technique used to assemble the circuit.
VT2’s emitter voltage is held nearly
constant. This allows the 70mV drop
in base voltage to take VT2 from its
normal forward-bias value of around
130mV down to virtual cut-off at
90mV, much like a sharp cut-off valve
characteristic. So because of the emitter voltage divider, don’t expect to
measure signal strength by the fall in
VT2’s emitter voltage.
The second IF stage operates with
fixed bias (as usual). Note that both IF
amplifiers are neutralised (using C12
& C17) to prevent instability due to
collector-base feedback.
The demodulator uses a conventional diode (MR1) and this feeds
audio to volume control R16. It also
feeds a DC voltage back into the bias
86 Silicon Chip
network for the first IF amplifier, in
common with other designs. Stronger
signals reduce the bias on the first IF,
thus controlling its gain. As with all
AGC systems, the net effect is to keep
the audio signal fairly constant with
varying RF signal strengths.
Audio stages
The 897P uses three audio stages:
preamplifier stage VT4, driver stage
VT5 and a Class-B push-pull output
stage based on VT6 & VT7. In common with the Raytheon T-2500 and
the Bush TR82 radios, the audio section uses transformer coupling. While
this adds complexity and potentially
reduces both high-frequency and lowfrequency audio response, transformer
coupling gives optimal power gain and
thus improves sensitivity.
As an aside, this design choice implies that the set’s RF/IF gain was less
than optimal and that the deficiency
was compensated for in the audio
section.
The biasing in the audio preamplifier and driver stages is similar to that
used in the IF amplifiers and works
identically. However, larger emitter
bypass capacitors are used so that they
are effective at audio frequencies.
The set is unusual in using a 2-gang
volume control and the “original”
897P model is readily identified by
this feature and the use of “OC” series
transistors in the audio section. But
why use a 2-gang volume control? The
articles in the HRSA’s Radio Waves for
July 2013 give two possible reasons:
(1) to prevent overloading and breakthrough at low volume with strong
signals and (2) to reduce the effects of
preamplifier noise.
So which of the two is correct, or
are they both correct? Well, bypassing
the second volume control pot (R22)
still resulted in effective control but
made the set noisy at low volume.
On the other hand, reinstating R22
and bypassing R16 solved the noise
problem but caused serious audio clipping and distortion on strong signals.
So the answer is that both of the possible reasons given for using a 2-gang
volume control are correct.
The output stage uses a conventional transformer-coupled Class-B
push-pull circuit based on VT6 & VT7.
As in the Bush TR82C, feedback is applied from the speaker to each output
transistor’s emitter terminal.
In addition, the output stage uses a
voltage divider to give about 160mV
of base bias to each output transistor.
In common with other Australian
designs, the lower end of this divider
includes a 130Ω NTC thermistor (ie,
its resistance falls as the temperature
increases).
The combined effect of the thermistor and transistor characteristics
ensures a fairly constant collector
current in the output stage, regardless of temperature. This arrangement
minimises crossover distortion and
protects the output transistors from
thermal runaway (due to increasing
current), thereby saving them from
damage due to overheating.
The output stage drives a large 5 x
7-inch oval speaker, which gives good
siliconchip.com.au
This internal view of Telefunken’s
OC604Spez transistor shows the metal
half-cyclinder (at top) that was used
for heatsinking.
efficiency and volume. Power came
from a single Eveready 276P 9V battery and this was capable of powering
the set for some 300-plus hours with
normal use.
The OC604Spez
The most obvious difference between the 897P and its successors
is its use of Telefunken “OC” series
audio transistors. Both the OC602
small-signal and OC604 output types
use glass encapsulation. This glass
encapsulation provides the hermetic
seal that’s vital for germanium devices
but it impedes heat dissipation.
Telefunken’s answer to this was
the OC604Spez(ial) transistor, a glassencapsulated type with internal heatsinking that allows it to deliver up to
500mW from a 6V supply. As shown in
the above photo, the heatsink consists
of a metal half-cylinder that’s attached
to the base slice (the “Germaniumplattchen”).
879PX/PY/PZ differences
By contrast, the PX/PY/PZ models
use RCA-derived 2N408 transistors for
the audio preamp and driver stages
and 2N270 types for the push-pull output stage. Despite this, these variants
perform similarly to the 897P.
Apart from that, they’re recognisable
because they also have their output
transistors mounted in grommets. The
other visible difference is the 897P’s
use of a Philips-style tuning gang with
rounded corners in its frame compared
to the more common square-cornered
types.
Restoring an 879PX
As it came to me, the 897PX set had
a “scratchy” volume control pot and
there was no audio output. A quick
check of the DC voltages revealed
siliconchip.com.au
that all was OK in this department
so the capacitors THEN came under
suspicion. I needed many millivolts
of signal at the volume control to get
even a “squeak” of output and further
checks showed that coupling capacitor
C26 (20µF) was open-circuit, as was its
companion C23.
Replacing both these capacitors immediately brought the set to life. Further checks then revealed that it had
an audio sensitivity of about 200µV for
50mW of output, which is excellent.
Audio response?
What about the audio response? In
a word, it was “rubbish” with a response of only about 190Hz to 1.3kHz.
That just had to be wrong. My chief
suspects were the two top-cut capacitors, ie, C28 (10nF) across the driver
transformer’s primary and C30 (100nF)
across the output transformer’s primary. De-soldering both dramatically
increased the high-frequency response
of the audio stages to 13kHz.
Replacing both capacitors restricted
the response to 2kHz. This was quite
acceptable, especially given the RF/IF
section’s bandwidth of about ±1.7kHz.
As an aside, removing C28 extended
the frequency response to about 6kHz
but worsened the set’s weak-signal
noise figure by over 3dB. So it appears
that the heavy “top-cut” technique was
a quick-and-dirty way to improve the
subjective performance.
One thing of note is that this set has
an unused connection on the ferrite
rod. It turned out to be an “aerial terminal” tap on the tuned winding and
provided a convenient direct signal
injection point for testing.
Now for the 897P
When I obtained the 897P, I found
an envelope containing a paper inside
the case headed “Freddy’s Hire Purchase Contract for AWA Tranny 2412-1957”. This was proof positive that
this set was indeed made in 1957. The
contract, with Industrial Acceptance
Corporation, shows a total amount
payable of £52 13s or about $105.30
before adjusting for inflation.
In today’s money, after inflation
is taken into account, that’s about
$1500 – double the cost of a high-end
smartphone. The purchaser was obligated to pay off the set over a period
of 19 months.
Cosmetically, my 897P came to me
with its leather case in poor condition.
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For a firm shipping cost send an email with APR/MAY
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Send to: branko<at>oatleyelectronics
April 2015 87
These two photos show sections of the 897PZ chassis. Unlike the 897P, this
model used 2N270 output transistors which were mounted in grommets, just
like VT1-VT5. The other visible difference is the 897PZ’s use of a “non-Philips”
tuning gang with square edges.
The leather was dull, though not badly
scratched, and the stitching on one of
the end cheeks had degraded, allowing
the end to detach.
The case would have been machinestitched during manufacture but I was
able to locate hemp cord at a local craft
shop of the same thickness as the original. After removing the original thread,
I was able to counter-stitch and restore
the case to its original appearance.
Electrically, the set was completely
dead, apart from an audible turn-on/
turn-off “click”. The reason for this
wasn’t hard to determine – audio
transformer T7 had an open-circuit
primary. This was rather odd since it’s
a low-voltage, low-power item.
Replacing this transformer with
a similar inter-stage transformer restored the set to life.
How good is it?
As noted above, the frequency response is around 190-1900Hz from
the volume control to the speaker and
around 210-1600Hz from the antenna
to the speaker. Removing that pesky
10nF top-cut capacitor (C28) from
VT5’s collector extended the response
to around 2.6kHz, and the difference
in quality was quite noticeable.
The audio performance was otherwise quite good: at 10mW output and
400 Hz, the total harmonic distortion
was just 2%, while at 50mW, the distortion was about 3.3%. This rises to
around 8% as the set just begins clipping at 220mW output and is 12% for
88 Silicon Chip
250mW. Removing the output stage’s
feedback gave a worst-case figure of
8% distortion at just 50mW output.
The Pye Jetliner transistor radio
described in the September 2014 issue
has a diode-biased output stage and
was able to maintain low distortion
down to 50% battery voltage, with
little evidence of crossover distortion.
By contrast, the 897 is unable to cope
nearly as well with falling battery
voltage because it uses voltage-divider
biasing. As a result, it gives audible
crossover distortion when the supply is down to 5V. At this voltage, it
clipped at an output of just 50mW.
The 897’s selectivity is ±13kHz at
60dB down, reflecting the presence
of three double-tuned IF transformers.
Although the 897, like the TR82C, uses
four audio stages, the 897’s design fails
to exceed the TR82C’s performance,
achieving 250µV/metre at 600 kHz and
150µV/m at 1400kHz with the volume
control adjusted for a signal-to-noise
ratio (S/N) of 20dB.
At full gain, the model 897 achieved
125µV/m at 1400kHz with an S/N of
17dB (note: all inputs are for 50mW
output and 30% modulated at 400Hz).
Given that Bush’s TR82C is a later design using alloy-diffused AF116/117
transistors in the RF/IF section, the 897
(which uses alloy-junction transistors)
performs quite well, especially as it
was AWA’s first transistor radio.
The AGC control is average and a
26dB signal increase from 60µV to
1200µV at the aerial terminal gives a
6dB increase in the audio output. The
only reservation is that this set went
into violent oscillation with a radiated
signal strength much above 30mV/m.
Graham Moore (Radio Waves, July
2013) notes the “sharp cut-off” characteristics of a transistor AGC circuit
and the 897, with its emitter tied to
about 0.47V by voltage divider R8 &
R9, certainly exhibits this.
By contrast, most sets use a single
emitter resistor to ground, allowing
something closer to a medium/remote
cut-off. With an IF stage gain of about
30dB, applying AGC only to the first IF
can’t reduce the stage gain by any more
than 30dB before the transistor is left
with virtually zero collector current.
Basically, in order to achieve greater
AGC range, the converter must also be
controlled, either by using an auxiliary
diode circuit as in the Pye Jetliner or
by applying AGC to a mixer that’s fed
by a separate local oscillator.
The 4-valve predecessor
When I dusted off a somewhat
sorry-looking 4-valve AWA 581PZ
and applied power, I was rewarded
with absolute silence. I’ll leave its
restoration details for another article.
However, when I did eventually get it
working, the 581PZ (which looks just
like the 897P) had a sensitivity of about
360µV/m at 600kHz and 250µV/m at
1400kHz.
So the 897 appears to have roughly
double the sensitivity. In practical
terms though, the two sets would
have almost identical performance
except on the lab bench. I expect that
the 581PZ’s audio performance (output power, distortion and frequency
response) will be similar to that of its
all-transistor 897 successor.
Acknowledgments
Many thanks to Ray Gillett of the
HRSA for his very generous loan of a
half-dozen variants of the 897.
Further reading
(1) For a more complete history of
AWA, see Radio Waves, July 2013.
(2) For more detail on the 897P, see
the July 2013 Radio Waves articles by
Graham Moore and Ian Malcolm.
(3) For more detail on early Australian transistor manufacture, see Mark
P. D. Burgess’ article – go to https://
sites.google.com/site/transistorhistory/
and navigate to Australian semiconSC
ductor manufacturers.
siliconchip.com.au
Keysight MSO-X 3104T
oscilloscope has
a touch screen
By Nicholas Vinen
This updated version of Keysight’s midrange scope adds a number
of new features, including a touch-screen, without a price increase.
Nor is there any need to return the unit to a service centre to
upgrade the bandwidth all the way from 100MHz to 1GHz.
A
S YOU MAY have noticed, Agilent’s test equipment division has
now been renamed to Keysight. So
this unit is the immediate successor
to the 3000A-series scope that we reviewed in the April 2011 issue. That
unit dramatically raised scope performance within the budget of advanced
hobbyists, educational institutions
and freshly minted engineers. By that
we primarily refer to its astounding
waveform update rate of one million
per second. When the 3000A-series
was launched, a typical competitor
had an update rate of around 10,000
per second.
siliconchip.com.au
The new 3000T-series has the same
specification and still leads its class,
although not by as much as the 3000A
did in 2011; its appearance forced competitors to “lift their game”, so to speak.
Even so, Keysight’s “MegaZoom IV”
ASIC (application specific integrated
circuit) technology has kept them in
the lead. So even though this is an update to a scope released three years ago,
it’s still state-of-the-art. The additional
features only serve to sweeten the deal.
Hardware upgrades
While the most obvious change with
the 3000T is the touch screen, there
are quite a few other improvements.
Sampling rate for all bandwidths is
now 5GHz compared to 4GHz for the
3000A (except for the 1GHz model)
and 4Mpoints segment memory is now
standard rather than being an extracost option.
All models come with 500MHz passive probes. This makes it easier to
upgrade the bandwidth via software
key; otherwise you would need to buy
new probes. The logic analyser cable
has also been improved, now being
thinner, lighter and more flexible, so
it’s easier to work with.
Timebase stability is now 1.6ppm
April 2015 89
Fig.1: this demonstrates the display of eight different measurements at the right
side of the screen. The touch-screen controls to drag the measurements around
and access other displays on the sidebar are visible above them. Here the new
FFT mode (now separate from “math”) is enabled.
Fig.2: thanks to the touch-screen, it’s now possible to input figures such as signal
generator frequency using an on-screen numeric keypad.
compared to 25ppm for the older
model and the calibration period is
three years rather than two.
Software improvements
There are many software improvements in the new model. Our favourite
is that you can now turn off the channel information in the sidebar, making
room for up to eight measurements at
a time. Hallelujah! See Fig.1.
Since there is now a touch-screen,
that means an alphanumeric keypad
can be used for entering values such as
waveform generator output frequency
(see Fig.2). This is a great feature. It also
allows for zone-based triggering; you
draw a box on the screen and it will
90 Silicon Chip
trigger whenever the waveform crosses
into that box. This is quite handy for
searching for occasional out-of-spec
signal glitches.
The “Advanced math” option now
comes as standard – another money
saver and quite a useful feature. Also,
the built-in counter (which can be used
for accurate frequency measurements
etc) has eight digits rather than five.
Some of the major software improvements have been made to the spectral
analysis (FFT function). This function
now has a dedicated front-panel button
and can be enabled simultaneously
with one of the “math” options, whereas before you could have only one or
the other. The FFT display is now cor-
related with the time domain, so that as
you scroll through the traces, the FFT
display updates to show the spectrum
of the data visible on the screen.
This is a feature previously seen
mainly in “Mixed Domain Oscilloscopes”. While this FFT feature does
not quite have the performance you get
with an MDO or dedicated spectrum
analyser, it is one step closer and much
more useful than the FFT function in
most scopes. Its dynamic range can
exceed 70dB, depending on how the
data is being sampled.
The FFT now has a peak search feature, akin to the cursors on a spectrum
analyser and will display a list of the
peaks with their frequency and power.
It can also do averaging on the spectral
data (a common feature in spectrum
analysers but not scopes) as well as
minimum/maximum hold.
The serial protocol decoding options
have been expanded, adding three new
automotive protocols to its already
extensive list: CAN-FD (CAN with
flexible data rate), CAN-dbc (CAN with
symbolic triggering and decoding) and
SAE J2716 SENTbus.
The scope’s user interface has been
revamped to take advantage of the
touch-screen, although you can still
perform all the functions without it if
desired (there’s even a button to disable
it). These changes include the ability
to drag various controls and displays
out to their own “window”, such as the
DVM readout, measurements, channel
summary, numeric keypad etc.
Given the relatively limited screen
space and the fact that most of it is taken up by the graticule, in our opinion
this is not that useful although there
are occasions where we would use it.
Features
Our April 2011 review was specifically on the MSO-X 2024A although
we did cover the MSO-X 3000A-series
which was launched simultaneously
and which had many similarities.
Both the MSO-X 2000A and 3000A
series (including the new 3000T) can
be had with either two or four analog
channels, with or without a logic
analyser and with bandwidths from
100MHz up to 500MHz and 1GHz
respectively. The base models (ie,
2-channel 100MHz) are quite affordable and since they can be upgraded
later, give purchasers both an attractive
starting price and an upgrade path.
The bandwidth can be upgraded at
siliconchip.com.au
any time and the cost is now just the
difference in price between the two
models. The logic analyser (ie, digital
inputs) can also be added to non-MSO
models. However, two-channel models
can not be upgraded to four channels
so that is a decision that must be made
up-front. There are also many software
options that can be added to the scope
later, including the single-channel
arbitrary waveform generator.
The main differences between the
2000-series and 3000-series are waveform update rate (50k/sec vs 1M/sec),
number of logic analyser channels (8
vs 16), sampling rate (2GS/sec vs 5GS/
sec), maximum bandwidth (500MHz
vs 1GHz) and some software options
are only available on the 3000-series.
The 3000A-series scopes are still
available but there’s no point in buying
one any more since the 3000T has all
the same features and more.
The rear panel of the demo unit, which was supplied with the optional LAN &
VGA interface module installed. Besides this, the only connectors are the mains
input, USB host & device ports and BNC external trigger inputs and outputs.
There’s also a Kensington lock and calibration access hole.
Fig.3: the new Event
Lister, at right, shows
the time stamps
of events such as
trigger locations
in the waveform
record, along with
triangles showing
their positions at the
top of the graticule.
A similar lister is
available for showing
spectral peaks when
FFT mode is enabled.
Impressions
Overall, the MSO-X 3104T is a joy
to use. Its interface is responsive and
the fast update rate is very noticeable.
This is especially true if you have averaging enabled as the fast acquisition
rate means that enough waveforms are
captured to update the average after
a change in timebase, so that it stabilises very quickly. While the screen
isn’t as large as higher-end scopes, it’s
sufficiently large that it doesn’t feel
cramped and the graduated intensity
display gives an excellent picture,
especially for smooth waveforms (ie,
with little noise).
The controls are generally intuitive,
with separate vertical controls for each
channel plus six soft buttons below the
screen to control most functions, in
combination with the dedicated mode
buttons. Overall it is an improvement
compared to earlier Agilent DSO models and is among the more logically
laid-out scope interfaces we’ve used.
The front panel button layout on the
3104T has been changed only slightly
compared to the 3000A-series, with the
Serial button function replaced by FFT,
an added illuminated “Zone” button
above the general purpose knob and
an added illuminated “Touch” button
to enable/disable the touch-screen.
If we look hard for something to
criticise, while maximum vertical
sensitivity is slightly better than average at 4mV/div (5mV/div being quite
typical), there are now low-cost DSOs
available which will do 1mV/div or
siliconchip.com.au
even 500µV/div. While this sort of
sensitivity isn’t often called for, it is
handy to have. Sometimes when we’re
probing for low level signals (eg, from
a microphone) we have to resort to
using 1:1 probes and even then, there
are times when more sensitivity would
be worthwhile.
We should point out that while this
scope does have 2mV/div and 1mV/
div settings, they are just a “software
zoom” on the 4mV/div signal. Perhaps
Keysight would have had difficulty
getting such sensitivity with the higher
bandwidths and this would have significantly increased the unit cost. But
we hope to see a larger range of input
sensitivity in future models.
Conclusion
I was so impressed with the 3000-series scopes after our 2011 review that
I subsequently purchased an MSO-X
3024A for use at home (although it
spends most of its time at our office!).
The MSO-X 3000T-series is even bet-
ter again; I wish it had been available
at the time so I could have gotten all
these extra features but I don’t regret
the purchase!
Despite the intervening four years,
the situation hasn’t changed; these
scopes still offer the best bang-foryour-buck in their segment with a
combination of ease of use, very high
performance, upgradeability, a suite
of great software options and a good
starting price. Yes, you can buy a decent mixed signal scope for well under
$1000 these days but it won’t come
close to matching the performance of
the Keysight offerings.
Prices for the DSO-X/MSO-X 3000AT series range from $3759 + GST
(DSOX3012T; 100MHz, two analog
channels) to $17281+GST (MSOX3104T; 1GHz, four analog + 16 digital
channels). For enquiries or to purchase
a scope, contact Trio Test & Measurement at sales<at>triotest.com.au, visit
www.triotest.com.au or phone 1300
SC
853 407.
April 2015 91
ASK SILICON CHIP
Got a technical problem? Can’t understand a piece of jargon or some technical principle? Drop us a line
and we’ll answer your question. Send your email to silicon<at>siliconchip.com.au
Remote volume control
project is obsolete
I bought the Remote Volume Control
for HiFi systems kit (SILICON CHIP, May
& June 1993) from Jaycar 18 years ago
and if it’s not still available I’d like to
get the notes anyway! Please advise if
the kit is still available or if any circuit
info can be found. (R. Q., via email).
• The kit is no longer available and
we suspect you’ll find it difficult to get
many of the parts. We’ve published
a more recent digital volume control
design, the Remote Volume Control &
Preamplifier Module, in the February
and March 2007 issues. It uses more
modern parts but even those are becoming difficult to get.
Our more recent volume control
projects have used motorised pots
which readers seem to prefer.
The original articles can be purchased from SILICON CHIP.
Car or boat
computer project
I would like to build the GPS Car
Computer project (S ILICON C HIP ,
January & February 2010) which was
marketed as kit K1133 by Altronics but
is now discontinued. Alternatively,
I don’t mind adopting the Boat GPS
computer (SILICON CHIP, October 2010)
which is available as kit K1143 from
Altronics but the hurdle I am facing is
the need to preset a determined speed
for alarms and for the speed to be displayed in km/h rather than knots. (P.
O., via email).
• Good idea. The circuits for the GPS
Car Computer and GPS Boat Computer
are very similar. You could build the
Boat Computer kit, make a few small
component modifications (if necessary) and reprogram the chip with the
software for the Car Computer. If you
can’t reprogram it, you can send it to us
and pay $10 to have it re-programmed
and posted back to you. Or you can
buy a new chip from us, already programmed for $15 + postage.
Phone dialler for
burglar alarms
Back in April 2003 I built the Burglar alarm dialler and it worked well.
I have now resurrected it to act as an
alarm for my wife who is an invalid
and sometimes falls from her wheelchair. I am triggering the alarm with
a remote doorbell. The pushbutton
is around her neck and the speaker
output is connected to the alarm input
with DIP switches S1/3 and S1/2 in
the closed position.
This works well and when triggered
rings my mobile phone and then there
is the problem that unless I answer the
phone the alarm does not reset, as I
understand it. Of course it only needs
to operate once and I come straight
home if I am local or get someone to
assist her, ambulance etc. Is there a
way that I can fit a switch to reset the
alarm when I want to and can you also
suggest a way to connect the doorbell
to the power supply as I am using two
batteries at the moment? I am loath to
rely on the alarm too much at present
which means that I cannot leave her
alone.
And just recently, after my wife
came home from hospital, I discovered that the unit no longer worked.
Thinking that possibly the PIC may
have lost its memory I purchased a
new programmed chip from SILICON
CHIP, fitted it and then I found that
Windows 7 did not have the Hyperterminal program installed. According to
Microsoft, Vista or XP were the last to
have it, therefore I could not program
the new PIC chip or check the old
PIC chip. I have tried the Hilgraeve
Hyperterminal for Windows 7 but I
could not get it to work.
Furby Motor Is Conventional Permanent Magnet Type
I’m curious to know if the motor
in the classic Furby from 1998 to
2000 is a magnetic one. I can’t find
any information on the sprung copper leaves that transfer power to the
commutator. If the parts are springloaded, perhaps the copper leaves
come in contact with it in the same
way brushes do.
Also, it’s interesting that the conductive grease used makes the classic
Furby smell “electrical” (he smells
of wires). I learned that this “wiry”
odour is known as an “electric motor” smell which occurs if the toy
has been operating continuously
for awhile. Perhaps this conductive
92 Silicon Chip
grease gets sticky over time which
might explain why older Furbys have
trouble starting up.
Once a Furby of mine smelled
of a chemical plastic odour from a
prolonged jam caused by the eye
mechanisms freezing. Luckily, he
only got slightly warm around the
motor and nothing was damaged. Is
this what happens in all jams with
a hum? (B. C., via email).
• All electric motors work by the
interaction of magnetic fields. And
yes, a Furby has an electric motor.
It has a permanent magnet field and
brushes and a commutator to feed
the current to the rotating armature.
We published an article entitled
“Inside a Furby” in our May 2000
issue. Most small electric motors will
give an “electric motor” smell which
is partly due to the sparking between
the brushes and commutator. This
sparking generates some ozone and
also causes carbonisation of any lubricant close the commutator.
Also, heat in the motor coils causes
the wiring insulation (varnish) to
contribute to the electric motor
smell. When a motor is stalled, it will
hum (due to the magnetic field) and
if the stalling continues, the motor
often burns out, the wiring varnish is
vaporised and it certainly does stink.
siliconchip.com.au
Is there any other way I can program
this PIC? Or can you assist me in any
way to get this device up and running
again as I can’t leave my wife alone at
present in case a problem arises? (N.
B., via email).
• The PIC16F84 is a very old micro
and does seem to lose its EEPROM
memory so you are right in first reprogramming the settings via the terminal.
This hyperterminal client is supposed
to work on Windows 7 and it has details on how to install it. See http://
digitizor.com/2009/08/29/how-to-install-the-winxp-hyperterminal-clienton-windows-vista-or-windows-7-free/
There does not appear to be any
way to reset the alarm without ringing
back. Neither automatic nor manual
modes allow for this. However, it
should be possible to have a power
switch that you can add to power off
the alarm (ie, switch off the 5V to IC1
for a second or so and then re-power
it so that the alarm is reset due to a
power-up reset. Alternatively, you can
momentarily connect pin 4 of IC1 to
ground to reset it.
With respect to powering the doorbell, since it runs on about 3V, you
could run it from the 5V supply by
using a string of three diodes in series
to drop the 5V down to about 3V.
Hiccup in understanding
Burp Charger
I have just built the Burp Charger
from the March 2014 edition using a kit
from Jaycar. Having just read through
the article again, it does not detail how
you turn the burp function on. Is DIP
switch 4 to be turned ON for the Burp
function? There are some setup tables
in the Jaycar printout at the end which
seem to indicate that DIP switch 4 is
the Burp function. (F. W., via email).
• Yes, it is DIP switch S4 that needs
to be on (closed) for Burp charging.
Refer to the table for switch S2 in the
circuit and also in the specifications
section under Burp discharge.
Temperature switch
has drift
I have built up the High Range Adjustable Temperature Switch with LCD
(SILICON CHIP, May 2012) but I find it
drifts overnight by 6-8°C. I am using it
in an oven on a boat that we are living
on full time.
You may think, so how is the drift
siliconchip.com.au
Victa Electronic Ignition Module
I would like to enquire about one
of my passions – the restoration of
“golden era” Victa 2-stroke motor
mowers. I realise this may not be
very well received judging by some
of the letters and Publisher’s Letters
of late, but here goes. The golden
era of Australia’s own Victa mowers extends, in my opinion, from
the mid-1960s to the end of the full
crank series 70/80 engines in 1984
when Victa introduced the half
crank Power Torque engines.
Most of those early engines used
the normal points/condenser/ignition coil flywheel magneto system
that has proven very reliable over
the years. Towards the end of this
era, some models were fitted with
a 2-terminal “electronic ignition
module” that replaced the points
and condenser completely but retained the same coil and flywheel
magnets. The module has only two
terminals, one going to earth (the
metal case) with one side of the coil
primary winding and the other going
to the “live” side of the coil primary
winding. The “kill” switch wire is
also connected here and shorts it to
earth to stop the engine.
It would be interesting to know
what this device is and how it knows
what the timing is without the points
to trigger/break the primary circuit
at the correct time etc. These devices
are available to buy from spare parts
stockists but it would be interesting
to know what the device is and if it
is a stock standard electronic part,
only encapsulated in a metal case.
It is possible to convert an engine
going to affect baking? Well, it will not
in the scheme of things but when the
oven is not used the readout should
reflect the actual cold temperature
(of the oven). So overnight as the air
temperature drops, the readout goes
up. I have tried a wire short across
the input to read the ambient so as to
eliminate the thermocouple and we
still get this change, though it is not
as great. (I. N., via email).
• Check that REF1 and REF2 give the
required 2.49V (measured between TP
GND and TP2 for REF2 and between
TP2 and TP1 for REF1). Also note
that if using the LED display module,
with points and condenser to this
system by rewiring and removing the
condenser and points completely,
making it, arguably, more reliable
still? Any information will be gladly
received. (P. C., via email).
• As far as we are aware, the electronic module acts as a direct points
replacement. Instead of the points
being opened via a cam, the module
would be triggered by the flywheel
magnets to drive probably a transistor that would be conducting unless
triggered to cause the transistor to
momentarily switch off (go open as
in points). The magneto generates a
high voltage to charge the coil and
fires when the transistor (or original
points) open.
Whether the module will work
correctly or at the right firing point
may depend on the magneto’s magnet positioning and trigger polarity
required for the module (ie, whether
triggered on a north or south magnet
pole).
The kill switch when closed shorts
the live side of the coil’s primary
to ground, preventing the magneto
charging the coil. That is the same
as having the points or module
transistor remaining in conduction
or closed.
Inside the electronic module
would be some form of magnetic trigger (Hall Effect device) or coil. That
signal would be used to momentarily
open the conducting transistor by
pulling its base to ground – see www.
mowersgalore.com.au/spare-parts/
mower-parts/electrical/coils-andaccessories/victa/
the temperature from the regulator
will be read by IC1, the cold junction
compensation component. The LCD
module draws much less current and
so this will not cause REG1 to run hot.
Frequency switch for a
one-cylinder engine
I have built the Frequency Switch
project (SILICON CHIP, June 2007) and
I want to use it to switch at a predetermined RPM on a single-cylinder
engine with a CDI unit. What is the
recommended way to obtain the pulse
signal for a system like this?
April 2015 93
Substitute For Currawong Power Transformer
I have almost completed the Currawong Valve Stereo Amplifier but I
am having a problem obtaing the Altronics MC5337 toroidal transformer. This is disappointing as I have
already spent over $250 with another
$200 in two weeks for the valves.
Is there an alternative? I found one
on the internet from NSW Photonage – 160VA, 37 + 37 + 15 + 15 + 12
+ 12V. Could this be used in lieu of
the two toroidals as it has the 12V
included? (R. W., via email).
• Unfortunately, the Chinese supplier of this transformer has discontinued it which is inconvenient
for everyone concerned with this
popular project. In essence, you have
three options:
(1) Use a 300VA toroidal transformer
but the plinth will have to be made
taller. A suitable transformer would
be Altronics MC5545 with the two
45V and two 15V windings conThe engine is a Honda Rancher ATV
and there is no tachometer. There is a
pulse signal driven off the flywheel
that triggers the CDI and the CDI is
separate to the coil which has a supply
side and a ground side and the high
tension spark side. (P. J., via email).
• The input to the Frequency Switch
would connect to the pulse signal
that is present at the CDI input. If the
Frequency Switch does not trigger off
this, change the 3.3kΩ resistor at pin
11 of IC1 to a smaller value. A value
of 1kΩ should increase sensitivity to
672mV rather than the original 1.8V
with the 3.3kΩ resistor.
Switch function query
on remote control switch
I have completed building the UHF
Remote Controlled Mains Switch
as published in your February 2008
issue. What I would like to know is
what switch S4 does. I would like to
change the time from the switched
time by adjusting S3, leave it, and run
continuous mode by switching outside
the case using the push of the button.
Can this be done? Does S4 do this? (R.
M., via email).
• S4 is a manual on/off switch. If
you do not want the timer to operate,
set S3 to position 0. This causes the
94 Silicon Chip
nected in series. This would allow
for a total output of 120V which
would give a slight improvement in
output power.
(2) Use the 160VA Altronics M5345
in combination with a separate
smaller transformer (15-18V) in series. The smaller transformer would
need to be able to handle the full load
current though of at least 1A. This
might be a bit of a squeeze although
the 18V transformer could be quite
small (eg, a 30VA toroid).
(3) Use one of these 160VA transformers from element14:
http://au.element14.com/multicomp/
mcta160-55/transformer-toroidal2-x-55v-160va/dp/9530703 and
http://au.element14.com/multicomp/vtx-146-160-155/transformer160va-2x-55v/dp/1675081
No extra windings are necessary as
the two secondaries combined produce ~110VAC which is sufficient.
mains to switch on continuously and
off continuously with each alternate
pressing of S4. Presumably, this is just
what you are wanting it to do.
LM386 power
output confusion
One of my customers raised the question of the output power of the LM386
used in the Champ project (SILICON
CHIP, February 1994). The text states
that it is a maximum of 500mW at 9V.
Fig.3 shows various supply voltages,
output power and dissipation.
I cannot make out the chip used
in the published article and the current TI data sheet states: LM386N-1
6V/8R/325mW typical, LM386N-3
9V/8R/700mW typical. Can you please
advise? (J. B., via email).
• The power output graphs for an
8-ohm load are shown in Fig.3 of
the Champ article. They show the
maximum power output as 325mW
for 6V and 700mW for 9V at the 10%
distortion level. The article quotes it as
500mW at 9V into 8-ohms and this is
a more realistic power estimate where
distortion is less than 3% and it is expected that this power can be delivered
into 8-ohms with a 9V supply with a
-1 or -3 device under music signals.
Given that the -3 version is now
cheaper than the -1 version, this would
be the preferred option. The -1 version was used in the original Champ
prototype.
Regarding the different power output ratings, these are for a continuous
sinewave signal: LM386N-1 6V/8R/
325mW typical; LM386N-3 9V/8R/
700mW typical.
Note that the 325mW rating for the
-1 device and the 700mW rating for the
-3 device are for different supply voltages and so are not easily compared.
Search for power
controller circuit
I have lost an old issue of SILICON
CHIP which described a 240VAC universal motor controller for power tools.
This design used a TL494 PWM chip
and a BUP50 IGBT to make a very simple and good power controller. Could
you tell me which issue this was this?
(L. G., via email).
• We have searched through our issues that describe 240VAC universal
motor speed controls and cannot find
one that used the TL494 and BUP50.
Actually, we don’t think that BUP50
is a valid IGBT type number.
The closest is the November 1997
full-wave speed controller that used a
BUP213 IGBT but did not use a TL494.
The other is the May 2009 version that
used a FGA25N120 IGBT. Our latest
controller and the one we recommend
is from February 2014.
We have described 12/24VDC motor controllers that use the TL494 and
a Mosfet (but not an IGBT) but these
don’t fit the 240VAC universal motor
requirement.
Garbage bin reminder
is confused
I have had my Garbage Bin Reminder (SILICON CHIP, January 2013)
working for some time and I noticed
that things did not seem correct when I
finished it. Unfortunately, I didn’t have
the time to play with it then.
Recently, I had to change the battery
and I noticed that the programming
steps don’t work the way you have
stated, eg, do you keep the Clear All/
Program button pressed all the time if
you want to exclude a LED and press
that LED button?
I have noticed that the LEDs don’t
flash once when I hold the Clear All/
Program button but do so when I
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press the Clear All/Program for more
than six seconds and then release it.
If I then press the LED button to be
excluded, after a few seconds it will
flash and go off.
The other query is are the LEDs supposed to flash differently for weekly
and alternate week/fortnightly reminders? And what is the Clear/Prgm
siliconchip.com.au
button on the front panel used for as it
not mentioned anywhere in the notes?
Finally, has the firmware been updated
from 1911112A? (R. S., via email).
• The actual way the reminders are
set is complicated due to the fact that
the set-up is just with switches and
LED indication, rather than via a more
expensive alphanumerical display that
would make schedule programming
easier.
The steps detailed on pages 60 and
61 of the January 2013 issue do detail
the schedule programming procedure.
Both weekly and fortnightly settings
have the LED flash once. The Clear
All/Program button is held for 6s with
continued page 96
April 2015 95
Notes & Errata
6-Digit Retro Nixie Clock Mk2,
February-March 2015: the articles
stated that GPS modules with RS-232
output levels were not suitable for
use. However, we have now managed to incorporate support for such
modules into the final software.
Note that a resistor of around
4.7-10kΩ must be placed in series
with the GPS module’s TX line (ie,
the wire to pin 3 of CON7, marked
“TX” on the PCB) to avoid damaging
the microcontroller. The micro will
auto-detect inversion state and baud
rate (4800 or 9600).
Ask SILICON CHIP
. . . continued from page 95
the LEDs then each flashing once in
sequence.
Continue to hold the Clear All/Program switch when you need to disable
an indicator and press its corresponding Clear/Prgm button as detailed in
step 2. Note that there is not just a
single Clear/Prgm button but one associated with each indicator LED. In
other words, the Clear/Prgm buttons
are located with each LED and are used
to enable or disable an indicator LED.
The Clear All/Program switch, when
briefly pressed for under 6s, is used to
clear the flashing “bin-out” LEDs once
you put these bins out for collection.
There are no software updates for
this design.
1.5V power
supply wanted
I have a voltage sensitive transmitter
Note also that there is no pull-up
resistor on the MCLR pin (pin 1) of
IC1; while the data sheet suggests one
may be necessary, we have found it
works fine without. If you want to
add one, it can be soldered between
pins 1 & 2 of CON3.
Currawong 2 x 10W Stereo Valve
Amplifier (November 2014-January
2015): in the November 2014 issue on
page 32, circuit diagram Fig.2 shows
T1’s secondary voltages incorrectly.
The two bottom windings should be
shown as 15VAC, not 37VAC.
that is powered by a single AA battery.
As the battery ages the transmitter
becomes unstable.
I want to use the Tx in my car and
run it from the vehicle battery. Have
you ever produced a stable 12V to
1.5V supply that I could use? I have
been looking at a simple circuit using
a voltage regulator but find that voltage regulators only go down to 5V.
The required current consumption is
negligible. (K. J., via email).
• You can use an LM317 to provide
a 1.25V supply directly or slightly increase this using a couple of resistors.
The Adjust-to-Out terminal resistor
value should be 120Ω or 100Ω to ensure sufficient minimum current for
the regulator.
Alternatively, a shunt regulator consisting of a resistor connected in series
with three 1N4148 or 1N4004 diodes
across the 12V rail will give a nominal
1.5V supply across the diodes. If the
transmitter’s current drain is minimal
(less than 5mA), then a 1kΩ 0.5W resisSC
tor can be used.
Advertising Index
Altronics.................................. 68-71
BCS International Pty Ltd............. 13
Clarke & Severn Electronics.......... 7
Control Devices Group................. 11
Element14 Pty Ltd.......................... 5
Embedded Logic Solutions.......... 14
Emona Instruments...................... 10
Front Panel Express..................... 79
Hare & Forbes.......................... OBC
High Profile Communications....... 95
Icom Australia.............................. 12
Jaycar .............................. IFC,45-52
KCS Trade Pty Ltd........................ 29
Keith Rippon ................................ 95
Keysight Technology..................... 15
KitStop.......................................... 79
LD Electronics.............................. 95
LEDsales...................................... 95
Master Instruments........................ 3
Mastercut Technologies.................. 9
Mikroelektronika......................... IBC
National Instruments...................... 6
Oatley Electronics........................ 87
Ocean Controls.............................. 6
Qualieco....................................... 55
Questronix.................................... 95
Rockby Electronics....................... 77
Rolec OKW................................. 7,9
Sesame Electronics..................... 95
Silicon Chip Binders..................... 39
Silicon Chip PCBs........................ 95
Silvertone Electronics.................. 41
Tronixlabs..................................... 95
Virtins Technology.......................... 8
Wiltronics........................................ 4
Worldwide Elect. Components..... 95
X-ON Electronic Services............ 95
WARNING!
SILICON CHIP magazine regularly describes projects which employ a mains power supply or produce high voltage. All such
projects should be considered dangerous or even lethal if not used safely.
Readers are warned that high voltage wiring should be carried out according to the instructions in the articles. When working on these projects use extreme care to ensure that you do not accidentally come into contact with mains AC voltages or
high voltage DC. If you are not confident about working with projects employing mains voltages or other high voltages, you
are advised not to attempt work on them. Silicon Chip Publications Pty Ltd disclaims any liability for damages should anyone
be killed or injured while working on a project or circuit described in any issue of SILICON CHIP magazine.
Devices or circuits described in SILICON CHIP may be covered by patents. SILICON CHIP disclaims any liability for the infringement of such patents by the manufacturing or selling of any such equipment. SILICON CHIP also disclaims any liability
for projects which are used in such a way as to infringe relevant government regulations and by-laws.
Advertisers are warned that they are responsible for the content of all advertisements and that they must conform to the
Competition & Consumer Act 2010 or as subsequently amended and to any governmental regulations which are applicable.
96 Silicon Chip
siliconchip.com.au
siliconchip.com.au
April 2015 97
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