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Articles in this series:
Items relevant to "Build A Single Chip Message Recorder":
Items relevant to "Light Beam Relay Extender":
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BUILDING THE DIGITAL LOGIC ANALYSER
$4.50 JULY 1993
NZ $5.50
INCL
GST
REGISTERED BY AUSTRALIA POST – PUBLICATION NO. NBP9047
SERVICING — VINTAGE RADIO — COMPUTERS — AMATEUR RADIO — PROJECTS TO BUILD
Keck: The World’s
Biggest Optical
Telescope
Build A Low-Cost
Quiz Game
Adjudicator
Antenna Tuners:
Why They’re
Useful
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Please feel free to visit the advertiser’s website:
www.altronics.com.au
Vol.6, No.7; July 1993
FEATURES
4 The Keck Optical Telescope, Pt.1 by Bob Symes
The world’s biggest optical telescope
18 Tektronix TDS 320 100MHz Digital Scope by Leo Simpson
A high performance digital scope that’s easy to use
22 Programming the Motorola 68HC705C8 by Barry Rozema
Lesson 1: programming models & flow charts
26 Data: The ISD1016 Voice Recorder IC by Darren Yates
New analog chip requires no battery backup
BASED ON A single IC, this
project records up to 16 seconds
of audio using a new sound chip
that retains the recording even
when the power is turned off –
see page 32.
PROJECTS TO BUILD
32 Build A Single Chip Message Recorder by Darren Yates
Records up to 16 seconds of audio
38 Light Beam Relay Extender by Darren Yates
It doubles the range of the Light Beam Relay
53 Build An AM Radio Trainer, Pt.2 by Marque Crozman
Construction & alignment
60 Windows-Based Digital Logic Analyser, Pt.2 by Jussi Jumppanen
Construction & software installation
70 A Low-Cost Quiz Game Adjudicator by Darren Yates
It tells you who pressed the button first
SPECIAL COLUMNS
IF YOU’VE EVER wanted to risk
all the prizes & go for the jackpot,
then this is the project for you. It’s
called the Quizmaster & it will
indicate which of four players
pressed the button first.
30 Serviceman’s Log by the TV Serviceman
When it looks easy, it often ain’t
80 Remote Control by Bob Young
Unmanned aircraft – current models in service
84 Amateur Radio by Garry Cratt
Antenna tuners: why they are useful
86 Vintage Radio by John Hill
In the good ol’ days of my childhood
DEPARTMENTS
2
4
10
16
65
Publisher’s Letter
Mailbag
Order Form
Circuit Notebook
Product Showcase
90
92
94
95
96
Back Issues
Ask Silicon Chip
Notes & Errata
Market Centre
Advertising Index
DESPITE ITS APPARENT circuit
complexity, the Digital Logic
Analyser is easy to build. In Pt.2
this month, we conclude with
details of the construction &
software installation.
July 1993 1
Publisher & Editor-in-Chief
Leo Simpson, B.Bus.
Editor
Greg Swain, B.Sc.(Hons.)
Technical Staff
John Clarke, B.E.(Elec.)
Robert Flynn
Darren Yates, B.Sc.
Reader Services
Ann Jenkinson
Sharon Macdonald
Marketing Manager
Sharon Lightner
Phone (02) 979 5644
Mobile phone (018) 28 5532
Regular Contributors
Brendan Akhurst
Garry Cratt, VK2YBX
Marque Crozman, VK2ZLZ
John Hill
Jim Lawler, MTETIA
Bryan Maher, M.E., B.Sc.
Philip Watson, MIREE, VK2ZPW
Jim Yalden, VK2YGY
Bob Young
Photography
Stuart Bryce
SILICON CHIP is published 12 times
a year by Silicon Chip Publications
Pty Ltd. A.C.N. 003 205 490. All
material copyright ©. No part of
this publication may be reproduced
without the written consent of the
publisher.
Printing: Macquarie Print, Dubbo,
NSW.
Distribution: Network Distribution
Company.
Subscription rates: $42 per year
in Australia. For overseas rates, see
the subscription page in this issue.
Editorial & advertising offices:
Unit 1a/77-79 Bassett Street, Mona
Vale, NSW 2103. Postal address:
PO Box 139, Collaroy Beach, NSW
2097. Phone (02) 979 5644. Fax
(02) 979 6503.
PUBLISHER'S LETTER
Old textbooks &
data books are
valuable
Do you have old electronics data books and reference
books that you are considering throwing out? Possibly
they are taking up space and
you haven’t referred to them
for awhile, so you now think
you should throw them out.
Think again, we say. At SILICON CHIP we have a policy of not throwing out any semiconductor data book
even though we have later editions which ostensibly render them obsolete.
The reason for not throwing the books out is that they are the only source
of data on components which are no longer made. The new data books from
manufacturers only feature devices which are currently being manufactured
at the time the book was sent to the printer. If you routinely throw data books
out, there is a strong chance you will regret it in the future when you need
to refer to data which is no longer in print.
This problem is bigger than you might think. Currently, there are about
one million semiconductors which are presently available and about half a
million which are obsolete and this latter number is probably growing faster
than the number of new devices being released. Even the most comprehensive
data services tend to keep only short form data on obsolete semiconductors
so once you throw a data book out, that’s it; it’s gone.
This tendency to throw out seemingly useless books extends to many
TAFE, university and state libraries – they are running out of space and so
they tend to throw out the older books which are now being referred to less
often. We are appalled at this policy. We think that such libraries should
regard older books as a valuable archive of technology as it was - the very
foundations on which present day technology is based. If we throw out
the older stuff, how are future generations going to know how much of
our technology came about? More important, how can new and innovative
technology be developed without a broad knowledge base, a base which is
ultimately stored in the reference libraries across the country?
What can be done about it? First, think twice about throwing out old
reference and data books – you might need them in future. Second, keep an
eye out at your local reference library for books which may be on sale for
a song. And third, indicate to your librarian that you think their policy of
throwing technical books out is ill-advised and short-sighted.
Leo Simpson
ISSN 1030-2662
WARNING!
SILICON CHIP magazine regularly describes projects which employ a mains power supply or produce high voltage. All such projects should
be considered dangerous or even lethal if not used safely. Readers are warned that high voltage wiring should be carried out according to the
instructions in the articles. When working on these projects use extreme care to ensure that you do not accidentally come into contact with
mains AC voltages or high voltage DC. If you are not confident about working with projects employing mains voltages or other high voltages,
you are advised not to attempt work on them. Silicon Chip Publications Pty Ltd disclaims any liability for damages should anyone be killed
or injured while working on a project or circuit described in any issue of SILICON CHIP magazine. Devices or circuits described in SILICON
CHIP may be covered by patents. SILICON CHIP disclaims any liability for the infringement of such patents by the manufacturing or selling of
any such equipment. SILICON CHIP also disclaims any liability for projects which are used in such a way as to infringe relevant government
regulations and by-laws.
Advertisers are warned that they are responsible for the content of all advertisements and that they must conform to the Trade Practices Act
1974 or as subsequently amended and to any governmental regulations which are applicable.
2 Silicon Chip
The Keck observatory
biggest optical telescop
Recently commissioned on the Hawaiian
island of Mauna Kea is the world’s biggest
ever optical telescope. At 10 metres in
diameter, it is a great deal larger the previous
biggest, the Russian 6-metre reflector. This is
the story of the Keck Telescope.
Part 1: By BOB SYMES
The Hawaiian Islands, a group of
eight main and about 130 smaller
volcanic islands, are spread across
approximately 2600km in the Pacific Ocean and they rise some 5,500
metres from the floor of the central
Pacific Basin. The highest shield
mountain of this chain, Mauna Kea,
rises a 4,205 metres above sea level,
thus leading to the claim that it is the
highest mountain on earth, from base
to summit.
The altitude, combined with the
islands’ remoteness from major centres
of air pollution, and the prevailing
NE trade winds, which combine to
keep the weather relatively constant
and the air clear and dry, were major
considerations in choosing the site for
an observatory complex.
A prime observing site can more
than double the efficiency of any
telescope. This is a most important
consideration for any large telescope
where returns in scientific knowledge
need to be balanced against the huge
costs involved.
After a world-wide survey of possible sites in 1963 by Gerard Kuiner,
Mauna Kea stood out as the best
place in the northern hemisphere for
nighttime observation. The dry air at
this altitude, where more than 90%
of the atmospheric moisture is below
the instruments, is critical for infrared
observations, water vapour being the
primary attenuator of radiation in this
part of the spectrum.
4 Silicon Chip
Furthermore, Hawaii has a relatively small population and industry is
minimal. This leads to low light and
industrial pollution. The island also
has strict regulations affecting light
pollution with particular emphasis
on maintaining astronomical quality
of the night sky.
The summit of Mauna Kea is usually
above the inversion layer at night. The
layer of clouds that often form below
the summit on the windward side of
the island as a result act as a further
trap for light coming from Hilo 30km
away. Gases and aerosols emanating
from the occasionally active Kilauea
volcano which can affect spec
tro
graphic investigations are simi
larly
trapped by the inversion layer.
The stability of the air above the
inversion layer provides exceptional
optical resolution. The ultimate limitation to reso
lution on earth-based
telescopes is air stability, which invari
ably reduces the theoretical resolution
of the instruments them
selves. On
Mauna Kea, sub arc-second “seeing”
is normal, and on nights of good air
stability, resolutions of better than 0.5
arc-seconds are possible.
As a result of these considerations,
the Mauna Kea Observa
t ory was
founded in 1967, in affiliation with
the University of Hawaii. It has the
distinction of being the highest observatory in the world.
While conditions at the summit
are conducive to astronomical obser-
y – the world’s
pe
Taken under starlight, this
photograph of the Keck Observatory,
shows the enormous scale of the
mosaic telescope which has 36
hexagonal mirror segments kept in
alignment by computer control. Note
the man standing at one side of the
dome opening. Each mirror segment
weighs 400 kilograms, giving a total
mass of glass of 14.4 tonnes. The total
moving mass of the telescope is 270
tonnes.
vations, they are not quite so good to
the astronomers and technicians who
operate the facilities. At times the
weather can be severe, it is always
cold, and oxygen deficiency may be
a serious problem for some. For this
reason, people intending to work at
the summit need to acclimatise at a
mid-level facility at Hale Pohaku (9300
feet – 2800m) which was constructed
in 1982.
The University of Hawaii’s Institute
for Astronomy at the Manoa Campus in
Honolulu leases the land above 12000
feet (3650m) from the state of Hawaii,
and has dedicated it as a Science Reserve. In turn, the university provides
site facilities for other observatories
who wish to erect telescopes on the
summit.
Currently, there are eight telescopes
in operation on Mauna Kea plus one
in the commissioning phase – the W.
M. Keck telescope, the subject of this
article.
Neglecting the atmospheric restrictions referred to above, the angular
resolution of a telescope mirror (or
lens) depends solely on its diameter
and the wavelength being investigated. When the angular separation of
two stars is very small, it might be
imagined that by merely using enough
magnification, the stars would resolve
into two distinct images. Because of
diffraction effects within the optics
however, the image of each object
is not a point source, but a so-called
“Airy disc” whose diameter is 1.1 λ/D
radians, or 2.27 x 105λ/D arc-seconds
(D being the diameter of the objective
lens/mirror in centimetres).
If the two discs substantially overlap, any increase in magnification
merely gives a larger blur of light, but
does not result in separation of the
images. The stars will be just resolved,
however, when their Airy discs touch;
July 1993 5
light that we see left that object so
much earlier in the history of the universe. But at those vast distances, the
light reaching the earth is extremely
feeble and the apparent size of the
object is extremely small. So unless
an instrument can be built that can
gather as much of the available light
as possible, and of sufficient angular
resolution to show details of structure
etc, little information can be gleaned
from these objects.
Mirror problems
This model of the Keck telescope again shows the enormous size of the main
mirror. It is much larger than most domestic swimming pools and with a focal
ratio of f/1.75 (focal length divided by the diameter) it is deeply concave.
ie, when the centre to centre distance
is equal to the diameter of the disc.
Since D is the denominator, by increasing the diameter of the primary mirror/
lens, the diameter of the Airy disc will
be proportionately smaller, hence the
resolution will increase.
Last century, the noted British
amateur astronomer W. R. Dawes,
working with close double stars, gave
an empirical limit for the resolution of
a telescope in arc-seconds as 11.5/D
(the “Dawes Limit”). Strictly speaking,
this figure is wavelength dependent,
and refers to visible light of 5 x 105cm. Since it is a rule of thumb rather
than an exact physical formula, the
difference across the visible spectrum
is marginal, and can be neglected.
6 Silicon Chip
Wavelength does become important
however, when calculating the resolution in the infrared spectrum.
It follows therefore, where resolution is a factor, that the bigger a lens
or mirror can be made, the better. The
same goes for light gathering, although
in this case it is surface area that is important rather than diameter. The two
are not necessarily related. Doubling
the diameter of a circular mirror gives
four times the light-gathering power,
and a doubling in resolution.
Since researchers are forever trying to look further back in time, this
increase in light-gathering power
becomes of great importance. The
further away an object is, the further
back in time we can look, since the
The simple solution is to make bigger monolithic mirrors or lenses. But
the problems associated with them
ultimately become insurmountable.
Lenses supported only around their
circumferences sag under their own
weight. Once the sag becomes apprec
i
able, image-quality deteriorates to
a point where it becomes unusable.
Thus it is unlikely that large lenses
will ever again be used for astronomical work, although the existing ones
still perform admirably. The largest
of them, the 40-inch (1m) telescope at
Yerkes Observatory at William Bay in
Wisconsin, built by that most famous
of telescope builders, Alvin Clark,
and dedicated in 1897, is likely to remain forever the greatest of refracting
telescopes.
Larger mirrors are easier to design
and build, since they can be supported
from the rear, and since only one critical surface has to be figured to high
accuracy, as opposed to the four (or
sometimes six) surfaces that need to
be ground and polished for an achromatic objective lens. In addition, flaws
such as bubbles, inclusions and striae
in the glass of a mirror are acceptable,
whereas they would be intolerable in
a lens system.
Nevertheless, massive engineering
problems remain. The larger a mirror
becomes, the thicker it needs to be to
avoid flexure and hence the heavier
it becomes. The mounting becomes
bigger and heavier, along with the
cost, and finally there is reached a
point at which further gains are no
longer feasible. There is the additional
problem that the more mass of glass
there is, the longer it takes to reach
thermal equilibrium, and during this
time, image quality suffers due to local
distortions in the mirror.
As new materials and techniques
became available, the boundary of
what was feasible was pushed further
8MM VIDEO CASSETES
These 120-minute 8mm metal oxide video cassettes
were recorded on once for a commercial application
and then bulk erased. They are in new condition but
don’t have the record protect tabs fitted. The hole
in the upper right corner will have to be taped over.
$9 Ea. or 5 for $38
LARGE NIGHT VIEWERS
One of a kind! A very large complete viewer for
long range observation. Based on a 3-stage fibre
optically coupled 40mm first generation image
intensifier, with a low light 200mm objective mirror
lens. Designed for tripod mounting. Probably the
highest gain-resolution night viewer ever made.
ONE ONLY at an incredible price of:
$3990
BINOCULAR EHT POWER SUPPLY
This low current EHT power supply was originally
used to power the IR binoculars advertised elsewhere in this listing. It is powered by a single 1.5V
“C” cell and produces a negative voltage output
of approximately 12kV. Can be used for powering
prefocussed IR tubes etc.
$20
IR BINOCULARS
High quality helmet mount, ex-military binocular
viewer. Self-powered by one 1.5V “C” size battery.
Focus adjustable from 1 metre to infinity. Requires
IR illumination. Original carry case provided. Limited
stocks, ON SPECIAL AT:
$500
IR FILTERS
A high quality military grade, deep infrared filter.
Used to filter the IR spectrum from medium-high
powered spotlights. Its glass construction makes
it capable of withstanding high temperatures.
Approx. 130mm diameter and 6mm thick. For use
with IR viewers and IR responsive CCD cameras:
ON SPECIAL
$45
12V OPERATED LASERS WITH KIT
SUPPLY
Save by making your own laser inverter kit. This
combination includes a new HeNe visible red laser
tube and one of our 12V Universal Laser Power
Supply MkIII kits. This inverter is easy to construct
as the transformer is assembled. The supply powers
HeNe tubes with powers of 0.2-15mW.
$130 with 1mW TUBE
$180 with 5mW TUBE
$280 with 10mW TUBE
MAINS OPERATED LASER
Supplied with a new visible red HeNe laser tube with
its matching encapsulated (240V) supply.
$179 with 1mW TUBE
$240 with 5mW TUBE
$390 with 10mW TUBE
GREEN LASER HEADS
We have a limited quantity of some brand new
2mW+ laser heads that produce a brillant green
output beam. Because of the relative response of the
human eye, these appear about as bright as 5-8mW
red helium neon tubes. Approximately 500mm long
by 40mm diameter, with very low divergence. Priced
at a small fraction of their real value
$599
A 12V universal laser inverter kit is provided for
free with each head.
ARGON HEADS
These low-voltage air-cooled Argon lon Laser Heads
are priced according to their hours of operation.
They produce a bright BLUE BEAM (488nm) and
a power output in the 10-100mW range. Depends
on the tube current. The head includes power meter
circuitry, and starting circuitry. We provide a simple
circuit for the supply and can provide some of the
major components for this supply. Limited supplies
at a fraction of their real cost.
$450-$800
ARGON OPTIC SETS
If you intend to make an Argon laser tube, the
most expensive parts you will need are the two
mirrors contained in this ARGON LASER OPTIC
SET. Includes one high reflector and one output
coupler at a fraction of their real value. LIMITED
SUPPLY
$200 for the two Argon LASER mirrors.
LASER POINTER
Improve and enhance all your presentations. Not
a kit but a complete commercial 5mW/670nm pen
sized pointer at ONLY:
$149
LARGE LENSES
Two pairs of these new precision ground AR coated
lenses were originally used to make up one large
symmetrical lens for use in IBM equipment. Made
in Japan by TOMINON. The larger lens has a
diameter of 80mm and weighs 0.5kg. Experimenters
delight at only:
$15 for the pair.
EHT GENERATOR KIT
A low cost EHT generator kit for experimenting
with HT-EHT voltages: DANGER – HIGH VOLTAGE! The kit also doubles as a very inexpensive
power supply for laser tubes: See EL-CHEAPO
LASER. Powered from a 12V DC supply, the EHT
generator delivers a pulsed DC output with peak
output voltage of approximately 11kV. By adding
a capacitor (.001uF/15kV $4), the kit will deliver
an 11kV DC output. By using two of the lower
voltage taps available on the transformer, it is
possible to obtain other voltages: 400V and 1300V
by simply adding a suitable diode and a capacitor:
200mA - 3kV diode and 0.01uF 5kV capacitor: $3
extra for the pair.
Possible uses include EHT experiments, replacement supplies in servicing (Old radios/CRO’s),
plasma balls etc. The EHT generator kit now includes
the PCB and is priced at a low:
$23
LED DISPLAYS
National Seminconductor 7-segment common
cathode 12 digit multiplexed LED displays with 12
decimal points. Overall size is 60 x 18mm and pinout
diagram is provided.
2.50 Ea. or 5 for $10
BATTERIES
Brand new industrial grade PANASONIC 12V-6.5AHr
sealed gel batteries at a reduced price.Yes, 6.5 AHr
batteries for use in alarms, solar lighting systems,
etc. Dimensions: 100 x 954 x 65mm. Weight of one
battery is 2.2kG. The SPECIAL price?
$38
PIR DETECTORS
What are the expensive parts in a passive movement dector as per EA May 89? A high quality dual
element PIR sensor, plus a fresnel lens, plus a white
filter. We include these and a copy of PIR movement
detector circuit diagram for:
$9
MASTHEAD AMPLIFIER KIT
Based on an IC with 20dB of gain, a bandwidth of
2GHz and a noise figure of 2.8dB, this amplifier kit
outperforms most other similar ICs and is priced
at a fraction of their cost. The cost of the complete
kit of parts for the masthead amplifier PCB and
components and the power and signal combiner
PCB and components is AN INCREDIBLE:
$18
For more information see a novel and extremely
popular antenna design which employs this amplifier: MIRACLE TV ANTENNA - EA May 1992: Box,
balun, and wire for this antenna: $5 extra
SODIUM VAPOUR LAMPS
Brand new 140W low pressure sodium vapour
lamps. Overall length 520mm, 65mm diameter, GEC
type SO1/H. We supply data for a very similar lamp
(135W). CLEARANCE AT:
lenses: two plastic and one glass. The basis of
a high quality magnifier, or projection system?
Experimenters’ delight!
$30
CRYSTAL OSCILLATOR MODULES
These small TTL Quartz Crystal Oscillators are hermetically sealed. Similar to units used in computers.
Operate from 5V and draw approximately 30mA.
TTL logic level clock output. Available in 4MHz,
4.032MHz, 5.0688MHz, 20MHz, 20.2752MHz,
24.74MHz, 40MHz and 50MHz.
$7 Ea. or 5 for $25
FLUORESCENT BACKLIGHT
These are new units supplied in their original
packing. They were an option for backlighting Citizen
LCD colour TVs. The screen glows a brilliant white
colour when the unit is powered by a 6V battery.
Draws approximately 50mA. The screen and the
inverter PCB can be separated. Effective screen
size is 38 x 50mm.
$12
MAINS FILTER BARGAIN
For two displays - one yellow green and one
silver grey.
SOME DIFFERENT COMPONENTS
1000pF/15kV disc ceramic capacitors ..............$5
20kV PIV - 5mA Av/1A Pk fast diodes .........$1.50
3kV PIV - 300mA / 30A Pk fast diodes ........... 60c
0.01uF /5kV disc ceramic capacitors ...........$1.80
680pF / 3kV disc ceramic capacitors .............. 30c
Who said that power MOSFETS are expensive??
MTP3055 N-channel MOSFETS as used in many
SC projects ............................$2 Ea. or 10 for $15
MTP2955 P-channel MOSFETS (complementary
to MTP3055) ..........................$2 Ea. or 10 for $15
BUZ11 N-channel MOSFETS $3 Ea. or 10 for $25
Brief DATA and application sheet for above MOSFETS free with any of their purchases (ask)
Flexible DECIMAL KEYPADS with PCB connectors
to suit ...........................................................$1.50
1-inch CRO TUBES with basic X-Y monitor circuit
CLEARANCE <at>..............................................$20
Schottky Barrier diodes 30V PIV - 1A/25A Pk. 45c
100 LED BARGRAPH DISPLAY
Note that we also have some IEC extension leads
that are two metres long at $4 Ea.
Yes 100 LEDs plus IC control circuitry, all surface
mounted on a long strip of PCB. SIMPLE - a 4-bit
binary code selects which one out of the 10 LED
groups will be on, whilst another 4-bit binary code
selects which one of each group of 10 LEDs will
be ON. Latching inputs are also provided. We
include a circuit and a connecting diagram. VERY
LIMITED QUANTITY
WEATHER TRANSMITTERS
FM TRANSMITTER KIT - MKll
A complete mains filter employing two inductors
and three capacitors fitted in a shielded metal IEC
socket. We include a 40 joule varistor with each filter.
$5
These brand new units were originally intended
to monitor weather conditions at high altitudes:
attached to balloons. Contain a transmitter (12GHz?) humidity sensor, temperature sensor,
barometric altitude sensor, and a 24V battery which
is activated by submersing in water. The precision
all mechanical altitude sensor appears similar
to a barometer and has a mechanical encoder
and is supplied with calibration chart. Great for
experimentation.
$16 Ea.
SOLAR CHARGER
Use it to charge and or maintain batteries on BOATS,
for solar LIGHTING, solar powered ELECTRIC
FENCES etc. Make your own 12V 4 Watt solar
panel. We provide four 6V 1-Watt solar panels with
terminating clips, and a PCB and components
kit for a 12V battery charging regulator and a
three LED charging indicator: see March 93 SC.
Incredible value!
$42
6.5Ahr. PANASONIC gel Battery $35, ELECTRIC
FENCE PCB and all onboard components kit $40.
See SC April 93.
$7Ea.
This low cost FM transmitter features pre-emphasis, high audio sensitivity as it can easily pick
up normal conversation in a large room, a range
of well over 100 metres, etc. It also has excellent
frequency stability. The resultant frequency shift
due to waving the antenna away and close to a
human body and/or changing the supply voltage
by +/-1V at 9V will not produce more than 30kHz
deviation at 100MHz! That represents a frequency
deviation of less than 0.03%, which simply means
that the frequency stays within the tuned position
on the receiver.
Specifications: tuning range: 88-101MHz, supply
voltage 6-12V, current consumption <at>9V 3.5mA,
pre-emphasis 50µs or 75µs, frequency response
40Hz to greater than 15kHz, S/N ratio greater than
60dB, sensitivity for full deviation 20mV, frequency
stability (see notes) 0.03%, PCB dimensions
1-inch x 1.7inch.
Construction is easy and no coil winding is necessary. The coil is preassembled in a shielded metal
can. The double sided, solder masked and screened
PCB also makes for easy construction. The kit
includes a PCB and all the on-board components,
an electret microphone, and a 9V battery clip:
$11 Ea. or 3 for $30
LARGE LCD DISPLAY MODULE - HITACHI
These are Hitachi LM215XB, 400 x 128 dot displays.
Some are silver grey and some are yellow green
reflective types. These were removed from unused
laptop computers. We sold out of similar displays that
were brand new at $39 each but are offering these
units at about half price. VERY LIMITED STOCK.
$40
OATLEY ELECTRONICS
$15 Ea.
PO Box 89, Oatley, NSW 2223
STEPPER MOTORS
Phone (02) 579 4985. Fax (02) 570 7910
$12
MAJOR CARDS ACCEPTED WITH
PHONE & FAX ORDERS
These are brand new units. Main body has a diameter of 58mm and a height of 25mm. Will operate
from 5V, has 7.5deg. steps, coil resistance of 6.6
ohms, and it is a 2-phase type. Six wires. ONLY:
PROJECTION LENS
Brand new large precison projection lens which
was originally intended for big screen TV projection systems. Will project images at close proximity
onto walls and screens and it has adjustable
focussing. Main body has a diameter of 117mm
and is 107mm long. The whole assembly can
be easily unscrewed to obtain three very large
P & P FOR MOST MIXED ORDERS
AUSTRALIA: $6; NZ (Air Mail): $10
July 1993 7
and further back. The 200-inch (5m)
Hale telescope on Mount Palomar in
southern California would not have
been possible without the development of Pyrex, a low expansion glass
which allowed the 14.5-tonne mirror
to reach thermal equilibrium in time
for the astronomers to still have some
dark hours in which to do their work!
The development of air-conditioning and efficient insulating materials
also helped by keeping the inside of
the dome and hence the mirror at a
constant average night-time temperature; ie, cold. Nevertheless, Mount
Palomar seems to be about the largest
size telescope that can be made using
conventional mirrors and equatorial
mountings.
Continuing the development of new
techniques, the 6-metre BTA (Bolshoi
Teleskop Azimutal’ny = Large Alta
zimuth Telescope) on Mount Pastuk
hov in southern Russia was the first
large telescope to use an altazimuth
mount instead of an equatorial, since
the equatorial would have been too
massive to control accurately, and too
costly to build.
But the advent of the altazimuth
mount had to await computers with
sufficient power to control the continually changing position of the
telescope, since the calculations to
move each axis are far more complex
than the requirements of an equatorial
mount, where (more or less) the drive
has only to be able to rotate the polar
axis at the sidereal rate.
Altazimuth telescopes have the
additional complexity of field rotation
8 Silicon Chip
during ob
serva
tion, a problem not
encountered with equatorial mounts.
Further computing and mechanical
complexity is involved in resolving
this problem.
The type of glass used in a tele
scope mirror has a great bearing on
the ultimate size that can be produced.
Ordinary borosilicate glass is easy to
cast in large sizes and to stress relieve
after casting, but thermal expansion is
so great that it is unusable in this role.
The development of Pyrex, in reducing thermal expansion to tolerable
limits, enabled much larger mirrors
to be contemplated, but casting an
homogenous blank was far more difficult, and it had a tendency to crack
when being stress-relieved, a process
that often took months or even years
of slow cooling. Fused quartz has been
used successfully but the extreme
difficulty of making large blanks has
limited its use on very large telescopes,
as has the development of new and
better materials.
As each new glass was developed,
the rewards in temperature stability
were greater, but so were the problems of manufacture. Cervit and its
Soviet counterpart SITAL (used in the
replacement mirror for the 6-metre
telescope) were the first successful
attempts to make a complex ceramic-glass mixture, where the coefficient
of expansion of the ceramic almost
exactly countered the opposite coefficient of expansion of the glass.
This was taken a step further with
the development of Zerodur by Schott
of Mainz, Germany. After initial cast-
ing, careful control of the subsequent
stabilising/stress-relieving thermal
cycle results in a glass in which half
of the mass is cryptocrystalline and
half is a supercooled liquid – the socalled “ceramization” process. Again,
the coefficients of expansion of the
two phases are equal but opposite and
closely cancel each other out.
The worst example of thermal
problems in a large telescope came
with the original 42-tonne pyrex-like
primary of the BTA, where a change
of no more than 20°C per day in glass
temperature could be tolerated and
still maintain a useable figure during
night-time observing runs.
The next development was that of
thin-mirror telescopes. Usually, the
thickness:diameter ratio of the glass
blank is between 1:6 to 1:8. As mentioned before, these larger mirrors become inordinately heavy and need to
be supported by inordinately massive
mounts, and the problem of pointing
finesse and controllability as well as
thermal equilibrium considerations
again dictate limits.
Thus was born experimentation
and success
ful implementation of
thin-mirror technology, with thickness:diameter ratios of 1:10 to 1:25.
These were made possible by the rigidity of the newly developed glasses,
and by casting the blanks so that they
tapered in thickness from the centre
out, as well as having anti-flexure webs
incorporated on the rear of the mirror.
This went a great way to reducing the
problems associated with weight, flexure and thermal equilibrium.
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As each of the above problems of
large mirror making were more or
less, successfully solved, even larger
mirrors became feasible. But there
remained one difficulty that couldn’t
be reduced easily – that of the actual
figuring and final polishing of the
reflecting surface itself. It is generally
agreed amongst optical engineers that
doubling the diameter of a mirror
makes it 10 times more difficult more
difficult to grind.
The amount of material to be removed is significantly greater, and the
final zonal corrections are fraught with
time-consuming difficulty. If one zone
is high, it only has to be polished down
to specification, but if it is low, the
entire surface has to be polished down
to accommodate the low spot. Even
though we are speaking of microns,
the work involved in polishing down
a large mirror is massive. And always
bearing in mind that not only does the
final figure have to be good, but the
focal point cannot be changed by any
corrections or re-figuring, as by this
abolise or hyperbolise the surface by
deepening the centre with a sub-diameter polishing lap.
The first new technique is a computer controlled polishing engine, usually
combined with a laser profilometer
feeding back to the controller. It has
the advantage of good accuracy and
is much quicker and less labour intensive than manual polishing. Since
large mirrors are so seldom made, the
computer polisher is usually made as
a one-off special for that particular
mirror and this adds substantially to
the cost, speed of execution notwith
standing.
The second new technique is known
as spin-casting. Glass is melted in an
electrically heated mould and held for
a time to soak so as to remove as many
bubbles and other imperfections and
inclusions as possible, and then spun
whilst cooling to produce the required
paraboloidal shape. The mould also
incorporates a honeycomb base which
creates a lightweight blank. The resulting curved blank dramatically reduces
All this had to come together at the top of a
windswept mountain where the air is so thin
that the engineers & construction workers
had to contend with dizziness, headaches,
forgetfulness & dehydration.
time the structural engineering side
would be well on the way to designing
and building the mounting, which by
now cannot be changed.
There is also a trend to design large
telescopes with very fast optics, often
less than f/2. Firstly, this gives the
observer a much brighter image to
work with, albeit at a reduced image
scale. Also, the supporting structure
can be much lighter because of the
shorter tube involved and significant
savings can be made in the design and
construction of the dome.
Two techniques are successfully
used today to partially overcome the
difficulty of grinding and polishing
mirrors to the required shape. Virtually all telescope mirrors have a para
boloidal or hyperboloidal cross-section and the traditional technique is
to first grind it to a spherical surface,
and then after testing for the sphere
by traditional optical means, to par-
the amount of material that has to be
removed and hence the time to attain
the final figure.
Several large astronomical mirrors
in the 6-metre to 8-metre range have
been cast successfully with this method, although at least three (8.2- metre
blanks for the European Southern Observatory’s Very Large Telescope –VLT)
have cracked and have been destroyed
in the annealing stage.
A final technique that had been
discussed theoretically for years is
that of stressed mirror polishing. In
effect, the mirror blank is deliberately
distorted to a predetermined shape
and then polished to a spherical section by conventional methods. After
final polishing, the distorting forces
are removed, and the mirror takes up
(hopefully!) the desired shape.
The greatest proponent of this new
method was Jerry Nelson of the University of California. In the late 1970s
he proposed that large astronomical
mirrors could be produced this way.
He made a further proposal, one that
was to have a great bearing on the
design and building of modern tele
scopes – that large mirrors be made
of multiple segmented smaller mirrors
rather than one large blank.
The idea of segmented mirrors to
avoid the weight problem and the increased complexity that accompanies
figuring large single mirrors is not new,
having been discussed by the third Earl
of Ross in the mid 1800s. In the late
1940s, Horn-d’Aturo in Italy actually
made a 61 hexagonal-segment mirror.
This formed a 1.8-metre f/6 telescope
that gave good images, although it was
unsteerable.
With the previously discussed years
of telescope design, glass making and
polishing technology, and adequate
computing power, the stage was set for
the development of the most ambitious
optical device ever built, the 9.82-metre W. M. Keck telescope.
The driving force behind the radical new telescope was Jerry Nelson.
He spent a great deal of time convincing the pundits that such a project
was feasible, since nothing on this
scale had ever been tried before. From
the start, the concept and design
were revolutionary. New methods
had to be devised to construct mirror segments, the warping harness,
support struc
t ure, actuators, and
the computer programs that brought
them all together.
The segmented mirror design on
such a large telescope was novel, and
there was no previous experience
at this scale to draw on. The mount
would have to be rigid enough to keep
the segments in exquisite alignment
but light enough to gain from the benefit of such a design. The electronics to
sense and correct misalignment had to
be developed from scratch. Even the
grinding and polishing of the mirror
segments themselves were to use new
and untried techniques.
In all facets, innovative thinking and
methods had to be employed. And all
this had to come together at the top
of a windswept mountain where the
air is so thin that the engineers and
construction workers had to contend
with dizziness, forget
fulness, headaches and dehydration, while solving
the engineering problems that would
be inevitable with such a massive
SC
undertaking.
July 1993 11
SILICON
CHIP
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dicksmith.com.au
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
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SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
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SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
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Please feel free to visit the advertiser’s website:
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CIRCUIT NOTEBOOK
Interesting circuit ideas which we have checked but not built and tested. Contributions from
readers are welcome and will be paid for at standard rates.
Battery charge
status monitor
This circuit gives a more reliable
battery status indicator for the SLA
battery charger described in the March
1990 issue of SILICON CHIP. Upon
investigation, it was found that the
charging mode was indicated by the
logic level of the “State Level Control”
output (pin 10) and the “Over Charge”
output (pin 1) on the UC3906.
These pins can be decoded using a
2-to-4 decoder such as a CMOS 4556
or TTL 74LS139 which then activates
the appropriate LED. Pin 10 goes
low when the UC3906 is in trickle
or main charging mode and high for
float charge. Pin 1 goes low for main
charge only. See the charge graph of
the UC3906 in the article on page 11
of the March 1990 issue for details.
The LEDs are connected to the output pins of the decoder as shown with
the “Float” LED being connected via
two 1N914 diodes to keep the LED on
Single-chip
combination lock
100
16 Silicon Chip
FLOAT
GREEN
LED1
0.1
10k
10k
UC3906
PIN6
D3
16
2
UC3906
PIN10
A
CHARGE
ORANGE
LED2
3
5
7
4
Q1
Q3
Q0
6
Q2
IC1
4556,
74LS139
B
E
1
when fully charged. The 560Ω resistor
provides current limiting for the LEDs.
As only one LED is on at a time, a single
resistor is all that is required.
IC1 is a dual decoder and the second
half is not used, so pins 13, 14 & 15
should be tied low. If a 4556 cannot
be obtained, then a 74LS139 can be
used with the following changes: (1)
delete the two 10kΩ resistors; and (2)
D4
D2
IN914
UC3906
PIN1
TRICKLE
RED
LED3
2x1N914
D1
1N914
8
13
14
15
replacehe the 1.5kΩ supply resistor
with a 78L05 voltage regulator to
provide a 5V source.
The LEDs were wired to the board
using their original wires but their
order was changed so that Red =
Trickle; Yellow = Charge; Green =
Float.
Douglas Ritson,
Ourimbah, NSW. ($20)
+5V
10k
This simple lock circuit has 109 pos-
sible combinations. Nine buttons on
the keypad are used and each button
can be wired to any of nine outputs
Q0 to Q8 of IC1. The tenth output, Q9,
is used as the output of the circuit, to
drive a relay via a transistor. Whenever
a correct button is pressed, the output
of transistor Q1 goes low, disabling the
reset pin of IC1 and discharging the
timing capacitor. When the button is
released, the collector of Q1 goes high
and this positive edge increments the
4017 counter, and the capacitor starts
to charge. There is about a 3-second
limit before the next button must be
pressed, or else the charging of the
timing capacitor will reset the counter.
This sequence is followed until a
maximum of 9 correct buttons have
been pressed. When all correct buttons have been pressed in the right
1.5k
UC3906
PIN5
1k
470k
D1
1N914
Q0
15
RST
Q1
10
Q2
Q1
BC548
14
CLK
Q3
IC1
4017
Q4
Q5
Q6
Q7
Q8
ENA
Q9
33k
1
2
33k
2
4
33k
3
7
33k
4
10
33k
5
1
33k
6
5
33k
7
6
33k
8
9
33k
9
3
11
OUTPUTS
OUTPUT
0
D1
OA90
5-15VDC
1.2k
IC
4093
82k
1
3.3
25VW
TANT
14
IC1a
3
1k
2
S1
68pF
12
82k
5
4
Q1
BC558
IC1d
8
6
IC1b
D2
OA90
7
9
Q3
BC558
1.2k
0.1
11
22k
13
68pF
Q2
BC548
1.2k
OUTPUT
Q4
BC548
3.3k
120k
1.8k
IC1c
10
1k
C2
1
25VW
600Hz
OSCILLATOR
1k
1k
C1
4.7
25VW
Pulser probe for
TTL & CMOS
This probe will generate a single
pulse or a pulse stream, depending on how long pushbutton S1 is
pressed. The circuit uses a 4093
quad 2-input Schmitt NAND gate
package. IC1c is connected as a
free-running square wave oscillator
which is enabled whenever its pin
8 input is low. This happens whenever S1 is pressed long enough to
allow C1 to charge and thus take
pin 8 high.
If S1 is pressed only briefly, the
resulting high to low transition at
pin 3 of IC1a is coupled through
IC1d which goes high at pin 11.
Pin 11 of IC1d is capacitively cou-
sequence, the Q9 output at pin 11
goes high for three seconds, as set by
the 10µF capacitor and 470kΩ resistor
at pin 15.
The keypad combination is hardwired by connecting the appropriate
keys to their respective IC pins. The
4017 outputs are connected to the
keypad in the order in which they
are required to be pressed; ie, the first
button to be pressed is connected to
the Q0 output and so on. Any number
of digits can be used for the combination, simply by taking the “unlock”
pulse from a different output. It is
also possible to re-use a digit, simply
by making two connections to the
relevant button. A few examples are
shown below:
4017 connections: 3 2 4 7 10 1 5 6 9
Low-cost piezo
screamer siren
which has its centre-tap connected
to the +9V supply. Positive feedback
is applied to the base of Q1 via 22kΩ
and 1kΩ resistors and phase shift is a
combination of the inductance of the
transformer primary and capacitor C1.
The low impedance secondary
of the transformer drivers a piezoelectric tweeter. With values ranging
between .027µF and 0.1µF, the circuit can deliver quite a high output
from the tweeter. Suitable 1kΩ:8Ω
transformers can be obtained from
suppliers such as Dick Smith Electronics (M-0216) or Jaycar Electronics
(MM-2532).
Andrew Merrick,
Northbridge, NSW. ($15)
C1
.027-0.22
AUDIO
1k- 8
22k
S1
PIEZO
1k
Q1
BC548
9V
This circuit is an oscillator based
on a small 1kΩ:8Ω audio transformer.
Transistor Q1 is connected to the high
impedance side of the transformer
pled to the output stage comprising
transistors Q1 to Q4. If pin 11 goes
high, Q2 and Q3 turn on while Q1
and Q4 are held off. This pulls the
output low. Similarly, if pin 11 goes
low, Q1 and Q4 are turned on and
Q2 and Q3 are held off. This pulls
the output high.
Greg Freeman,
Nairne, SA. ($25)
Combination 1: 1 5 9 7 2 8 4 6 3 Output from pin 11
Combination 2: 8 3 6 7 3 5 8 2 4 Output from pin 11
Combination 3: 9 4 2 6 9 5 - gnd Output from pin 5
Combination 4: 3 6 7 4 - - - gnd - - Output from pin 10
Any unused keypad digits should
be tied to ground.
Steven Merrifield,
Heidelberg, Vic. ($25)
Electronics your hobby? Taken a redundancy package or just retired early?
How does the idea of moving to the Blue
Mountains in NSW and making your
hobby your business sound? Thriving
electronics business with name brand
distribution rights available. $70,000 plus
SAV. Reply in first instance to: Sydney
(02) 833 5136 BH; (047) 39 3301 AH.
July 1993 17
Review
Tektronix TDS 320
100MHz digital scope
In the last couple of years, digital scopes have
been redefined & presented with an ease of
use undreamt of even with analog scopes. The
Tektronix TDS 320 continues this process,
combining a simplified menu of control features
with a 500 megasamples/second sampling rate
and 100MHz bandwidth.
By LEO SIMPSON
The big challenge to scope manufacturers these days is how to combine
the ever-increasing performance and
potential complexity of features in a
package that is intuitively easy to use.
No longer do users want to refer to
thick manuals to find out how to make
a measurement – they want to do it all
simply by pushing some buttons on
the front panel.
Over last 18 months or so, we have
reviewed a number of digital scopes
and they have all had a different
approach to solving the conflicting
requirements of ease of use and
flexibility of use.
For its part, Tektronix has chosen
yet another approach – one which
makes extensive use of “soft” buttons
and pictorial menus.
First impressions
First impressions of the Tektronix
TDS 320 scope are that it is quite a
bulky unit, but one which is surprisingly light for its bulk. Overall dimensions of the unit, not including its
handle, are 325mm wide, 165mm high
and 470mm deep, including knobs and
rear projections. Its mass is only 6.8kg
which means that it is easily carried
with its large handle.
The front panel is uncluttered
although it does carry quite a lot of
buttons, when you count them all up;
there are 35 buttons and six knobs.
The layout is logical though and you
can clearly identify the main
knobs for vertical sensitivity
and timebase. To the left
of the vertical sensitivity
knob are but
tons to select
channels 1 and 2 and others
which become clear as soon
as you press them: Math, Ref
1 and Ref 2. Math gives you
the choice of CH1 + CH2,
CH1 - CH2 and CH2 - CH1, all
selectable via “soft” buttons
down the side of the screen.
I should explain that many
The Tektronix TDS 320 is a
2-channel digital scope with
main & delayed timebases,
500 megasample/second
sampling rate & 100MHz
bandwidth.
18 Silicon Chip
digital scopes nowadays make use
of these “soft” buttons whereby the
functions change depending on what
control menu is being displayed on
the screen. It actually sounds more
complicated than it is to use and it is
a highly practical way of providing
lots of features without having huge
numbers of buttons.
Naturally, there is an “Autoset”
button which allows you to sit back
while the scope rapidly makes all
the appropriate internal adjustments
to give an appropriate display of signals on the screen. It is the lazy way
of doing things but it makes a lot of
sense and you can then manipulate
the sensitivity and timebase controls
to show the waveform exactly as you
want it.
One very attractive feature of a digital scope such as this is a continuously
variable vertical sensitivity which is
calibrated. To bring this feature into
use on the TDS 320, you first press
the “Vertical Menu” button and then
press the “Finescale” soft button at the
bottom of the screen. Pressing any of
the menu buttons at the bottom of the
screen brings another menu into play,
down the righthand side of the screen,
and these menu choices are activated
by pressing the appropriate soft button
at the side of the screen.
However, when the “Fine Scale” option is pressed, the topmost knob (the
General Purpose knob) on the front
panel is activated, and it is signified
by a knob symbol in the top righthand
corner of the screen. As you vary the
knob, the actual gain setting is shown
at four places on the screen which
really is a bit of overkill. Of course,
once you select some other menu option, say from the “Horizontal Menu”,
the vertical gain setting is shown only
once, next to the appropriate channel
indicator on the screen.
Hence, along the bottom of the
screen you may have readings such
as “Ch1 1.66V Ch2 50mV M2.5µs
Ch1 ~ 33.2mV”. These indicate that
the vertical sensitivity for Channel
1 is 1.66 volts/div, for channel 2 it is
50mV/div, the main timebase setting
is 2.5µs/div, the trigger source is Channel 1 and with triggering on positive
slopes and for signals above 33.2mV.
As with other digital scopes with CRT
readouts, this obviates the need for any
scales on the controls themselves since
all the relevant settings are shown on
the screen.
Coming back to the Vertical Menu,
the sensitivity can be varied by the
“Volts/Div” knob from 2mV/div to
10V/div if you are using a x1 probe
and from 20mV/div to 100V/div if
you are using a Tektronix x10 probe.
The TDS 320 will recognise whether
you are using Tektronix probes which
have a third contact inside the socket
locking ring but it will default to the
gain setting for a x1 probe.
There is no probe menu to allow
you to tell the TDS 320 the settings of
a non-Tektronix switchable probe so
you have to resort to mental arithmetic
in that case.
When using the “Volts/Div” knob
the gain is varied in a 1/2/5 sequence
while in the Fine Scale mode the
gain is continu
o usly varied with
3-digit resolution, in steps ranging
“Delayed Runs 4.13722ms After
Main”. Whichever option you pick
from the side menu is then echoed
at the bottom of the screen together
with another option for Trigger Position. Pressing this soft button gives
you three options for trigger position:
10%, 50% and 90%.
This concept may seem a little odd
until you realise that with a digital
scope you can display part of the
waveform before the nominal trigger
point. In fact, the entire record of a
trace has 1000 sample points and only
the middle section of this record is
normally displayed. You can scroll
along this record by using the horizontal position control. Hence, the 50%
trigger option is in the centre of the
trace and is indicated by a “T” symbol
The high rate of sampling means that it is tops
at catching glitches which are undetectable
on other scopes. It can detect glitches a short
as 10 nanoseconds at all timebase settings
between 25µs/div and 2.5 seconds/div.
between 0.4% and 1%. For example, if the gain is in the range from
100mV/div to 200mV/div it is varied
in 1mV steps, while in the range from
200mV/div to 500mV/div it varies
in 2mV steps. This is in line with
the 8-bit vertical resolution of the
instrument. Vertical gain accuracy
is ±2%.
Timebase
The main and delayed timebases are
not able to be varied continuously but
they are adjusted in four steps per decade; ie, a sequence of 1/2.5/5 which is
adequate for just about all foreseeable
measurement situations. When you
want to make precise measurements
on waveforms you don’t need to vary
the timebase; you either use the vertical cursors or just call up one of the
many measurement options which
we’ll come to later. The timebase accuracy is ±0.01%.
Pressing the “Horizontal Menu”
button brings up two options at the
bottom of the screen and a number
of options down the righthand side:
Main Only, Intensified, Delayed Only
and then a fourth message such as
(although again, there is an option to
turn that off).
Triggering
There is also a Trigger Menu button
and pressing this gives two broad options of either edge triggering (positive
or negative slope) or video triggering
via the in-built sync separator. This
latter option enables the scope to be
triggered on field 1 or field 2 or the
lines of a composite video signal such
as PAL or NTSC. (Note that the instrument does not have a line selector).
Measurements
There are 21 automatic measurements available with the TDS 320 and
they are brought into play by pressing
the “Measure” button. This brings
up five options along the bottom of
the screen and pressing any of the
accompanying soft buttons brings up
options down the side of the screen.
For example, pressing “Select Measurement” brings up the first four of
the 21 measurements and these can
be paged through to pick the ones you
want. Each measurement option is accompanied by a little diagram which
July 1993 19
Review: Tektronix TDS 320 100MHz digital scope
perform volts and time related measurements using moveable vertical
and horizontal cursors. You can then
measure absolute volts, delta volts,
frequency and time difference.
Performance
A typical screen display from the TDS 320. In this case, one channel is shown
together with measurements of pulse rise time, fall time, & positive & negative
duty cycles. Note that the menu at the side of the screen has been cleared so that
the measurements can be displayed without obscuring the waveform.
shows just what is being measured.
This “pictorial approach” is used
extensively on the TDS 320 and is
very useful even for those who are
very familiar with scope measurements. Seeing the little diagrams
makes the measure
ment selection
quite unambiguous and would be a
boon for anyone not so familiar with
the English language or for students
leaning about scopes.
The instrument also provides
a running commentary about the
measurements. For example, it might
accompany a measurement of rise time
with a “low resolution” comment. This
means that you should select a faster
timebase speed. All 21 measurements
will be accompanied by comments
where applicable and again, this can
be most helpful, even to experienced
users.
One problem that can arise with
on-screen measurements is that they
are superimposed over the waveforms
and this can lead to a lot of clutter. Tektronix has thought of that too. If you
push the “Clear Menu” button, all the
measurement readings are transferred
to the area down the side of the screen.
Result: no clutter.
20 Silicon Chip
One aspect which could be argued
about relates to the selection and
removal of measurements from the
screen. As presented, you can select
up to four of the 21 possible measurements on the screen. If you want to
select an additional measurement, the
TDS 320 flashes up a message which
states that only four are allowed. You
then have to clear that message, push
the “Measure” button again to bring
up the measure menu and then push
“Remove Measurement”. You then
have the option of removing any or
all of the existing four measurements
after which you can select another
measurement.
On other brands of digital scopes,
the measurements are displayed on
the screen in a FIFO (first in, first out)
scheme; ie, the first measurement in
is the first to disappear off screen as
you select more measurements. That
has the beauty of simplicity but it can
mean quite a few button presses to
display the particular set of measurements you want.
Cursors
As well as the automatic measurements noted above, you can also
All of the foregoing has focused
on the user features of the TDS 320
without really mentioning its overall
performance. It really does have quite
remarkable performance with 500
megasample/second sampling rate,
giving a true 100MHz bandwidth
even for “single shot” mode. And the
high rate of sampling means that it is
tops at catching glitches which are
undetectable on other scopes. It can
detect glitches a short as 10 nanoseconds at all timebase settings between
25µs/div and 2.5 seconds/div.
That’s pretty amazing stuff and is
indicative of a level of performance
that was unthinkable in instruments
in this price range before the TDS
320 was released just a couple of
months ago.
Excellent manuals are provided
with the TDS 320 although most
users should seldom need to refer to
them. There is a large spiral bound
instruction manual, a 4-page reference
manual showing the menu maps and
controls, a 72-page spiral bound manual entitled “Basic Concepts” which
would be an excellent source for anyone learning about scopes and finally,
a 3-ring binder programming manual
which allows you to fully exploit the
GPIB and parallel printer interfaces
of the TDS 320 if you purchase that
option.
Perhaps I should make some comments about the optional GPIB and
printer interfaces. As with most other
scope manufacturers, Tektronix makes
the TDS 320 available without any
interfaces but to my mind, buying an
instrument such as this without the
interfaces means that you are not getting the full benefit of the product. We
had only a few days with the review
instrument and it did not have any
interfaces on it as it was an advance
sample.
Another option which could be very
useful is a thermal printer mounted in
a pouch on top of the scope.
Points for improvement
Any complex product such as this
always has facets which could be
improved and, in fact, Tektronix has
Conclusion
To conclude, the Tektronix TDS 320
is high-performance scope which is
deceptively easy to use. In some ways,
its ease of use conceals the power of
the instrument. This is a paradox that
comes about because in the past high
performance instruments of any type
have generally not been easy to use.
We should also emphasise that space
limitations and the brief time we had
the sample scope meant that we have
not been able to cover the full range
of features.
The price of the Tektronix TDS 320
is $4395 plus sales tax, while Option
14 (the GPIB and Centronics printer
interface) is $774 plus tax.
For further information on the TDS
320 and other digital scopes in the
range, contact Tektronix Australia Pty
Ltd, 80 Waterloo Road, North Ryde,
NSW 2113. Phone (02) 888 7066. SC
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a policy of continuous upgrades. With
this in mind, there are some points
which could be improved. Perhaps
the most noticeable is the fan which
is quite noisy. I mentioned this to the
Tektronix sales staff and they assured
me that this aspect would definitely
be improved.
So much for the hardware. All
the other points of note relate to
the software and could probably be
easily modified. For example, when
you select the “Fine Scale” option
for vertical sensitivity, it would be
more logical if the gain was then
con
tinuously varied by the Volts/
Div knob than by the general purpose
knob at the top of the control panel.
A probe menu would be useful too,
so that non-Tektronix probes can be
used. This could be a subset of the
“Coupling” menu.
Finally, when you have selected
an option which involves the general
purpose knob, a knob symbol appears
in the top right
hand corner of the
screen, as already noted. However, as
soon as you touch the knob, the symbol disappears even though you can
still use the knob while ever the same
menu is displayed on screen. In this
reviewer’s opinion, the knob symbol
should remain on screen while ever
the facility is available.
Tektronix has a policy of continuously upgrading the internal software
of their scopes so maybe some or all
of these quibbles will be addressed in
the near future.
July 1993 21
Lesson 1
Programming the Motorola
68HC705C8 microcontroller
Following our series on the MAL-4 Microcon
troller Aid for Learning, we now present a series
of lessons on programming its central device:
the MC68HC705C8 microcontroller. If you’ve
always wanted to learn about microcontrollers,
this series will give you a good grounding.
By BARRY ROZEMA
Welcome to the fascinating world of
microprocessors and microcontrollers.
Over the next few months, we will
be showing you how to program the
Motorola MC68HC705C8 single chip
microcontroller. This microcontroller
unit (MCU) is a member of the large
6805 family and the lessons will be
based on its internal architecture and
instructions set. We will be using
the MAL-4 Microcontroller Aid for
Learning for the practical parts of the
lessons (see SILICON CHIP – Nov-Dec.
1992 & Feb. 1993).
The lessons are aimed at everyone
from keen beginners to those with
some programming experience but
who need to refresh their knowledge
of microcontrollers. However, to get
the most from the lessons, you should
at least have a reasonable grounding
in digital electronics.
Each lesson will consist of:
• Theory.
• Practical program examples.
• Things to do between lessons.
• A new program to try.
Note, however, that the lessons
Fig.1: this diagram is called
a “programming model” &
shows the various internal
registers of the 68HC705C8
microcontroller.
7
6
5
4
3
2
ACCUMULATOR
7
6
5
4
3
INDEX REGISTER
7
1
6
1
5
4
3
STACK POINTER
1
0
2
1
0
2
1
0
8 BITS
8 BITS
15
0
14
0
13
0
12
0
11
0
10
0
9
0
8
0
Hardware
6 BITS
15
0
14
0
13
0
12
11
10
9
8
7
6
5
PROGRAM COUNTER
4
3
2
1
0
4
H
3
I
2
N
1
Z
0
C
13 BITS
CONDITION CODE REGISTER
7
1
6
1
5
1
HALF CARRY (FROM BIT 3)
INTERRUPT BIT
NEGATIVE
To carry out the practical aspects of
the course, you will require a MAL-4
Microcontroller Aid for Learning with
a power supply and loudspeaker. You
should be well read with regard to the
MAL-4 operations manual and you
should be able to load programs and
run them.
Programming concepts
ZERO
CARRY (FROM BIT 7)
5 BITS
22 Silicon Chip
will be specific to the MC68HC705C8
micro
controller and its associated
hardware. It will also be necessary for
you to do some further reading after
completing each lesson.
As you are probably aware, when
it comes to electronics, you can never have too many text and reference
books. The microcontroller area is no
exception.
There have been many good text
books written about microprocessors,
most of which have been written for
specific devices. Unfortunately, I have
not seen any based on the 6805 family
to date. However, any microprocessor
text written around an 8-bit Motorola
processor or 6502 processor may suffice; eg, Microprocessors & Microcomputers, The 6800 Family or The 6502
Family, by Ronald J. Tocci & Lester P.
Laskowski (Prentice-Hall).
A good digital text book will also be
of value; eg, Digital Systems, Principles & Applications, by Ronald J. Tocci
(Prentice-Hall).
You will also need the MAL-4 Operation and Construction Manual, plus
two publications from Motorola:
(1) Microprocessor, Microcontroller &
Peripheral Data, Volumes 1 & 2.
(2) MC68HC705C8 8-Bit Micro
con
troller Unit. Technical Summary. BR
594/D Motorola.
All microprocessors and microcon
trollers, from those used in main
frames to the simplest MCUs, must
be capable of running a “program”. A
program is simply a list of instructions
that are to be carried out (executed)
in a given order. All microcontrollers
run in “machine code”, although this
is usually hidden from us by what
are called “higher level languages”.
Some typical higher level languages
include Pascal, Forth, Basic, DOS
and Windows. Even the humble word
processor can be regarded as a higher
level language.
The level of instructions in a given
application depends on the power of
the processor. For example, an adult
human can easily understand and carry out an instruction “go to the shop
and get some milk please”.
No other information would be
necessary. But if you wanted a child
to perform the same task, you would
have to give the correct change for the
milk, instruct him on how to cross the
road safely, and provide other information that would not be necessary
with an adult.
Now try to give the same task to a
robot. You would have to give every
detail of the job. For example, you
would have to tell the robot how and
when to lift its legs, how to maintain
its balance and how to get out of the
door – and that’s before you even tell
it how to successfully find its way to
the shop. In fact, the task is probably
impossible given today’s level of robot
development.
Machine code
All microcontrollers are similar
in the way they are pro
grammed.
You cannot say “go and get the milk
please”. Instead, you have to lay out
each step in machine code form.
Machine code – also called opcode (for operation code) – is issued
in binary form and is simply an instruction code for a given machine or
microprocessor. In the case of the 8-bit
MC68HC705C8 microcontroller, it
takes the form of an 8-bit binary code.
To make it easy for us, this binary code
is hidden in the form of other numbering formats, such as octal, hexadecimal
or decimal.
In most cases, the hexadecimal format is used for programming and this
also applies to the MAL-4. But what
ever the programming format used,
the processor still works in binary.
Hexadecimal numbers in these lessons
will have a “$” sign in front of them;
eg, $1234, $EA, $1FFE.
If we wanted a program larger
than say 10 bytes, it would be very
difficult to write in either binary or
hexadecimal format. That’s because
we are not very good at remembering
numbers and because we find it hard
to relate hexadecimal numbers to
events. Although the microprocessor
understands binary instructions, we
need to program in “plain” language.
For example, to load an accumulator we could use the in
struction
“Load Accumulator”, or other in1
START
structions which are then converted
into hexadecimal op-code. This code
is stored in the memory and the MCU
then “runs” the program.
Programming model
In order to program the
MC68HC705C8, we need to find out
what internal registers are available. Fig.1 shows the details for this
device. This diagram is called the
“programming model” (all microprocessors have one) and it enables the
programmer to best utilise the CPU.
A brief explanation of the registers in
the MC68HC705C8 follows.
Accumulator
2
SET
REGISTER
3
DECREMENT
REGISTER
4
ZERO?
NO
YES
5
END
Fig.2: this flowchart shows an
MCU counting down to zero.
Symbols 1 & 5 are terminators,
symbols 2 & 3 are process blocks,
& symbol 4 is a decision block.
structions like “Store Accumulator”
and “Or Accumulator”. This is how
the instructions are written for the
human side of the program, though in
a shortened form called “mnemonics”
(pronounced nu-mon-ics). The last
three instructions in mnemonic form
would look like this:
LoaD Accumulator - LDA
STore Accumulator - STA
OR Accumulator - ORA
To write a program using mnemonics, the programmer first thinks of the
instruction in plain language. He then
finds the correct mnemonic and looks
up the applicable binary machine code
(usually given in hexadecimal). The
MC68HC705C8 has 62 of these mnemonic instructions – see p.28 of the
MC68HC705C8 Technical Summary.
A typical microprocessor program
consists of a series of mnemonic in-
The accumulator is the workhorse
of the CPU. Some micropro
cessors
have more than one accumulator but
the 6805 only has one. A better name
for the accumulator would be “general purpose, do-almost-everything
register”.
Like the MCU, the accumulator
is eight bits wide. Its cont
ents can
be loaded from memory or stored in
memory. We can add, subtract and
multiply with it; perform logical functions (AND, OR, NOT & XOR) with it;
shift it right or left; rotate it right or
left; increment or decrement it; and
negate it (2s complement).
To understand how the accumulator
is used, picture yourself at the kitchen
sink washing dishes. With one hand
you grab a dirty plate and place it in
the sink. You wash it. With your other
hand, you then take the clean plate out
of the sink and place it on the dish
rack to dry.
This process is analogous to the
way in which we use the accumulator
– for example, to take data from the
input port and place it on the output
port. To do this, we must first LOAD
the accumulator from the input port,
then STORE the accumulator at the
output port.
Going back to our analogy, when
washing up, we can not send the
dirty plate directly to the dish rack –
we must handle it and wash it up. A
similar situation applies to data – it
must be “handled” by the accumulator.
The 6805 family has no instruction to
direct data around the memory; eg,
from output to input.
Index register
The index register operates in a
similar manner to the accumulator.
July 1993 23
Table 1: Noise 1 Laser/Spaceship Sound Generator Program
Address
Date
Label
Mnemonic
0030
A6 00
Start
LDA
#$00
;Set highest frequency
0032
B7 BF
STAZ
TEMP
;Store at temporary memory
0034
B6 BF
LDAZ
TEMP
;Get delay time
0036
CD 14 A1
JSR
D100US
;100us X ACC delay
0039
B6 02
LDAZ
PORTC
;Get speaker
003B
A8 80
EOR
#$80
;Complement speaker
003D
B7 02
STAZ
PORTC
;Store speaker
003F
3C BF
INCZ
TEMP
;Inc delay time
0041
B6 BF
LDAZ
TEMP
;Get delay time
0043
B1 00
CMPZ
PORTA
;Compare with Port A
0045
27 E9
BEQ
START
;Start again if equal
0047
20 EB
BRA
LOOP1
;Back to Loop 1
Loop 1
Comments
Comment: this program causes the MAL-4 to generate a laser/spaceship sound from its loudspeaker.
The program is loaded from RAM location $0030. The DIP switch on PORT A changes the sound. Be
sure to enable PORT A by turning DIP SW2 7 (E) on. Try changing location $0031 from $00 to other
values.
Like the accumulator, it is an 8-bit
register but it can not do all the
arithmetic and logic operations that
the accumulator can do. However,
the index register can perform a very
powerful form of programming called
indexed addressing, whereby it is
used to point to individual memory
locations.
START
SET DELAY
TIME
Stack pointer
This 6-bit register is used by the
CPU itself. The stack pointer points
to a RAM location where the CPU can
store or load data. The stack pointer
moves down to store new data or
moves up to load old data. In this
respect, it functions like a FILO (First
In Last Out) register. The stack pointer
memory range is $00FF-$00C0.
Program counter
The program counter is a 13-bit
register that keeps track of a program’s
location in memory. When we start
a program from a given memory location, the program counter must be
loaded with the start location. As the
program progresses through memory,
the program counter keeps track of
the location. If the program has to
jump or branch to another memory
location, this is achieved by changing
the program counter. The 13 bits of
the register give an addressing range
of 8Kb ($0000-$1FFF).
Condition code register
The condition code register (some24 Silicon Chip
DELAY
100us X
ACC
Flowcharts
The old saying “a picture is worth
a thousand words” is very true, especially when we are programming
MCUs. The “picture” that programmers use is called a flow chart. A flow
chart con
sists of symbols “strung”
together, usually stacked vertically
from top to bottom. Each symbol indicates a particular function, either
carrying out an instruction or making
a decision.
For example, the flowchart in Fig.2
shows an MCU counting down to zero.
This could be used to give a time delay.
Symbols 1 and 5 are terminators – they
indicate the start and finish of a program (or part of a program). Symbols 2
and 3 are process blocks and indicate
a process or operation.
Symbol 4 is a decision symbol. It
has one input and two outputs. One
output is for a result that is true,
while the other is for a result that is
untrue. The result from a decision
is bi
nary; ie, true/false, yes/no or
zero/one.
The best way to study a flow chart
is to follow it with your finger in
the direction of the arrows until you
come out at the end. Although there
are many flow chart symbols, we will
only use five basic types during this
course.
Subjects to study
COMPLEMENT
SPEAKER
INCREMENT
DELAY
EQUAL TO
PORT A?
decide if it should branch. A detailed
look at each instruction will show how
and which flag is affected.
YES
NO
Fig.3: this is the flowchart for the
laser/spaceship sound program
listed in Table 1.
times called the flag register) is a 5-bit
register. This register tells us what
happened in the ALU (arithmetic logic
unit) on the previous instruction(s).
If we use conditional branching, the
CPU looks at the flags in this register to
Following is a list of things to study
before next month’s lesson, listed in
order of importance:
(1.) Microprocessor fundamentals: basic operation; block diagrams; central
processing unit (CPU)
(2.) Numbering systems: binary to
hexadecimal to decimal
(3.) Motorola MC68HC705C8 8-Bit
MCU Technical Summary; pages 1-11,
28-31.
Sample program
Finally, Table 1 list a simple program that generates laser/spaceship
sounds using the MAL-4. Try entering the program as set out in the
instruction manual and be sure to
enable PORT A by turning DIP SW2
7 (E) on.
The program is loaded from RAM
location $0030 and the DIP switch on
SC
PORT A changes the sound.
THE ISD1016
VOICE RECORDER IC
IC Data
Using new techniques, Information Storage
Devices in the US has designed a 16-second
voice recorder on a single chip. It stores an
analog signal directly in an internal EEPROM,
making battery back-up redundant.
can forget about long battery life in
portable devices. Second, the memory
is volatile – if the power is removed,
the recording is lost.
The EEPROM advantage
By DARREN YATES
During the last few years, quite a lot
has happened to the way we record
and store sound. In addition to the
new hifi digital tape formats, digital
recorder ICs have also slowly begun to
take off as their advantages in certain
applications are recognised.
The obvious advantage is that
digital recorder ICs have no moving
parts. The motors, gears, heads and
tape of the conven
tional machines
are replaced with clock oscillators,
A/D converters and dynamic RAM
(DRAM). Result – greater reliability
and much reduced power consumption.
However, at this stage, solid state
recorders cannot compete with tape
machines (either analog or digital) in
terms of sound quality or recording
length. For example, it would require
one 256K x 8 DRAM chip for every
second of CD quality stereo sound.
INTERNAL
CLOCK
ANA OUT
MIC
MIC REF
AGC
AMP
The digital storage technique uses
A/D converters to sample the audio
waveform and the resulting binary
numbers, representing the sampled
values, are then stored away in
DRAMs. Similar A/D converter techniques are used in CDs and digital
audio tape recorders, except of course
the storage medium differs.
When the audio is to be recovered,
the binary numbers are fed into a
digital-to-analog converter (DAC)
and the output filtered to recover the
original waveform. But although dynamic RAMs are cheap, fast and easily
available, they do have a few bugbears.
First, they are power hungry so you
Block diagram
ANALOG
TRANSCEIVERS
ANTIALIASING
FILTER
PREAMP
Digital storage
SAMPLING
CLOCK
TIMING
DECODERS
ANA IN
That said, the solid state devices
have real benefits in applications
where you only need voice quality
recordings.
SMOOTHING
FILTER
SP+
MUX
AMP
128K CELL
NONVOLATILE
ANALOG STORAGE
ARRAY
SP-
AGC
POWER
CONDITIONING
VCCA
+5V
VCCD
+5V
ADDRESS BUFFERS
DEVICE CONTROL
A0 A1 A2 A3 A4 A5 A6 A7 TEST
(CLK)
PD P/R CE EOM
AUX
IN
Fig.1: block diagram of the ISD1000A chip family. The devices store the audio
signal in an internal EEPROM that retains memory when the power is switched
off. Other features include cascading & multiple message address options.
26 Silicon Chip
That’s where we come to the ISD1016A Single Chip Voice Record/
Playback device from Information
Storage Devices. Released in early
1992, this IC differs from other solid-state devices in that it stores the
sampled waveform in analog form.
And in
stead of storing the data in
volatile dynamic RAM, it stores it in
a non-volatile EEPROM (Electrically
Erasable Programmable Read-Only
Memory) that’s built right into the
chip.
The main advantages of this technique are better sound quality and
the fact that the recording is retained
in memory even when the power is
turned off. And because the information is stored in the EEPROM in analog
form, there’s no need for A/D and D/A
converters.
Actually, the ISD1016A is just one
of three voice recorder chips from Information Storage Devices. The other
two devices are the ISD1012A and the
ISD1020A and these have recording/
playback durations of 12 seconds and
20 seconds respectively.
Let’s take a closer look at how the ISD1016A IC works – see Fig.1. This device combines both digital and analog
electronics on the one chip, as well as
a 128,000-cell EEPROM array – enough
for 16 seconds of telephone-quality
audio. It comes in a 28-pin DIL or PLCC
package and runs off a 5V rail.
Starting at the input, audio can be
fed in from either a dynamic or electret
microphone to a preamplifier stage, or
it can come from a line level output;
eg, from a CD player or tape deck. The
gain of the microphone preamplifier
is controlled by an automat
ic gain
control (AGC) circuit. This makes
recording an easy task, as there are no
recording levels to set.
The preamplifier output is coupled
into the main input amplifier (via the
ANA OUT & ANA IN terminals) and
this in turn drives an anti-aliasing
filter. This filter is a hefty 5th order
Chebychev design which cuts all frequencies above approximately 40% of
the sampling frequency. This is done to
eliminate any mixing effects between
the input frequency and the sampling
frequency.
In this IC, the sampling rate is 8kHz
and the audio frequency cutoff point is
3.4kHz. Following the filter, the audio
signal is sampled and stored in the
128K cell EEPROM. This is where the
new technology is involved.
Because analog techniques are used,
the information storage density is eight
times that of a conventional digital
system. This eliminates the need to use
data compression or fancy algorithms
to get the physical size down.
What happens is that each cell forms
part of a closed loop which includes
a comparator. A sample-and-hold
circuit applies the analog voltage to be
stored to one input of the comparator.
The other input is connected to the
cell itself. The cell is then “pumped
up” using programming pulses until
its voltage is the same as the analog
voltage from the sample-and-hold
circuit. When the two voltages are
equal, the comparator shuts down the
programming pulses.
The magnitude of these programming pulses sets the resolution and
hence the clarity of the recording. In
the ISD1016A, there are approximately
256 levels and this translates into 8-bit
resolution.
In operation, it takes a fair amount of
time to store a sample in the EEPROM
array – about 10 milliseconds, in fact.
And since we are taking a sample every
125 microseconds, we must either lose
some information or find some way of
temporarily storing it.
To overcome this problem, the ISD1016A has two rows of 80 sample
and hold circuits. One row records
the input in real time in serial mode,
while the other row is connected in
parallel to program multiple cells in
the EEPROM simultaneously. By using
this arrangement, the IC can sample
every 125µs and still take 10ms to
program the multiple EEPROM cells
without losing data.
TABLE 1: PIN FUNCTIONS
Pin
Pin No.
Function
A0-A5
1-6
Address
A6-A7
9,10
Address
VCCD
28
VCC Digital Power
Supply
VCCA
16
VCC Analog Power
Supply
VSSD
12
VSS Digital Ground
VSSA
13
VSS Analog Ground
SP+
14
Speaker Output +
SP-
15
Speaker Output -
Test (CLK)
26
Test – Must Be Tied
Low
Aux In
11
Auxiliary Input
Ana Out
21
Analog Output
Ana In
20
Analog Input
AGC
19
Automatic Gain Control
Mic
17
Microphone Input
Mic Ref
18
Microphone Reference
PD
24
Power Diwb
P/R
27
Playback/Record
EOM
25
End-of-Message
CE
23
Chip Enable
The 128,000 cells in the EEPROM
are arranged into 160 rows of 800,
each row corresponding to 0.1s of
storage. Each row can be individually
addressed as a starting point, allowing
the device to broken up into 160 separate “phrases”.
The starting address of a recording
is set by applying an 8-bit code to
external address pins A0-A7. When
the recording is stopped, an End-OfMessage (EOM) marker is inserted
to mark the end of the message.
Playback can then be initiated from
the relevant addressed location and
continues until the EOM marker is
encountered.
In practice, this means that several short messages (or even single
words) could be stored in the chip
and accessed at will. The device could
therefore be used to play back single
word instructions in response to user
inputs, or even to construct entire
phrases under software control.
For example, the device could be
used to provide voice annotation in
test equipment, microwave ovens,
vending machines and toys, to name
just a few applications.
Longer recordings
An internal clock provides the timing signals for the sample and hold
circuits. This clock is accurate to ±2%
over the specified temperature and
voltage range to ensure good speech
fidelity. If greater accuracy is required,
the chip can be externally clocked via
its test (CLK) pin.
Playback
During playback, the signal is
clocked out of the EEPROM array and
passed through a smoothing filter. This
filter removes the sampling frequency
content of the signal and drives a
multiplexer stage, which selects either
the output from the EEPROM array or
signal fed in from an auxiliary input.
From there, the signal is fed to an audio
amplifier which can provide 50mW
into a 16-ohm load. An 8-ohm loudspeaker can also be used, provided a
10Ω resistor is installed in series with
one of the output leads.
Multiple message options
One useful feature of the chip is its
ability to play back one of many individual message stored in the EEPROM,
or to repeat a message continuously or
at set intervals.
One problem with DRAM designs
is that the main sound chip can only
address so much RAM – usually 1MB
at most – and this severely limits the
maximum recording time. However,
unlike its digital counterparts, the ISD10XX series overcomes this problem
by providing a simple cascading facility to obtain longer recording times.
Cascading four ISD1016 devices, for
example, will give up to 64 seconds
of speech, while 10 devices will provide a recording time of 2 minutes 40
seconds.
Finally, the ISD1016 also has a number of control inputs which can be programmed using external switches or
logic circuitry (eg, a microcontroller).
These include chip enable (CE-bar),
playback/record (P/R-bar) and power
down (PD). Pulling the PD pin high
when the unit is not recording or
playing back switches the unit into a
low-power standby mode to reduce the
operating current from 25mA <at> 5VDC
to less than 1µA.
Further information on the ISD
1016A voice recorder IC is available
from R & D Electronics, PO Box 179,
Springvale, 3171. Phone (03) 558 0444
SC
or (02) 712 3855.
July 1993 27
SILICON
CHIP
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SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Please feel free to visit the advertiser’s website:
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SILICON
CHIP
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more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Please feel free to visit the advertiser’s website:
www.altronics.com.au
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July 1993 31
Build this
single chip
MESSAGE
RECORDER
By DARREN YATES
Throw away those old messages on
the fridge. This project records up to
16 seconds of audio using a new sound
chip that retains the recording even
when the power is turned off.
It happens in just about every
household every day. One family
member has to rush out and go somewhere but needs to leave a message
for someone else in the family to take
the chops out of the fridge or bring
the clothes in, etc.
The tried and true technique is
the paper message stuck to the fridge
using a rubberised magnet – if you
can find paper and pen, that is. How
much time has been wasted searching
for those two items in your household? And even if you do have a
message pad, it’s always completely
used up when it’s your turn to write
something.
If that’s a common scenario in your
house, then this solid-state Message
Recorder is just what the doctor ordered. It can record up to 16 seconds
of speech (or music) and, unlike
earlier designs, is based on a single
32 Silicon Chip
chip that doesn’t require a back-up
battery or external memory devices
or controllers.
The project fits inside a small plastic case and is operat
ed using just
two pushbutton controls. To record
a message, you simply hold down
the RECORD button and speak into the
microphone. The message can then be
replayed at any time by holding down
the PLAYBACK button.
Unlike a tape recorder, you don’t
have to worry about “rewinding”
the unit at the end of the message.
That’s because the message is stored
in memory inside the IC. Each time
you press the PLAYBACK button, the
message automatically starts from the
beginning.
When you want to record a new
message, you simply record over
the top of the old one – just as you
would with an ordinary cassette tape.
This eliminates the need for an erase
control.
There’s no need for a power switch
on the unit either. When not in use,
the IC automatically powers down into
a stand-by mode and typically draws
less than 1µA.
The frequency response of the recorder is about 80-3400Hz, which is
about the same as telephone quality.
It has a total harmonic distortion of
typically 2% at 1kHz and the operating
current is 25mA <at> 5V.
Of course, there are other applications for the device apart from its
obvious role as a message recorder.
For example, by using the Playback
button as a bell-push, it could be
used as a doorbell. Alternatively,
it could be built into an answering
machine, or into machinery and used
to deliver instructions in response to
user inputs.
Single chip design
The new IC used in the Message
Recorder is designated ISD1016A
and comes from Information Storage
Devices in the USA. It uses analog
rather than digital technology and
includes a microphone preamplifier,
128K cell EEPROM and an audio output amplifier which can directly drive
a loudspeaker.
Fig.1: the circuit is
based on IC1 – an
ISD1016A single
chip message
recorder. When the
RECORD button is
pressed, signals
picked up by the
microphone are fed
into IC1 & stored in
an internal EEPROM.
Pressing the PLAY
button switches the
chip to playback
mode.
D1
1N4004
OUT
2.2k
0.1
47k
47k
16
0.22
2
MIC 1
D2
1N914
17
0.22
1
18
20
47k
RECORD
S2
28
VCCA
MIC
VCCB
SP+
1
C
B
21
P/R
8
250mW
IC1
ISD1016AP
ANA IN
SPVSSD
ANA OUT
VSSA
TEST
23
0.1
MIC
B
C
I G O
VIEWED FROM BELOW
12
470k
15
12
13
26
A0 A1 A2 A3 A4 A5 A6 A7
CE AGC
47k
E
0.1
14
MIC REF
24
Q1
BC548
9-12VDC
300mA
PLUG-PACK
10
16VW
10
3
27
E
GND
IN
10
16VW
10k
PLAY
S1
10
16VW
0.1
78L05
19
1
2
3
4
5
6
9
10
4.7
16VW
3
SINGLE CHIP MESSAGE RECORDER
POWER
Let’s now take a look at the circuit
diagram of the Message Recorder –
see Fig.1. As you can see, there’s not
much to it – just the IC, a microphone,
a loudspeaker, and a handful of minor
parts.
As soon as power is applied to the
circuit, IC1 goes into “power down”
mode. This occurs because the POWER
DOWN pin (pin 24) is pulled high by
a 47kΩ resistor. The current drawn
from the supply is then just the current
D1
10uF
78L05
SPEAKER
10uF
10uF
4.7uF
10k
2.2k
MIC
470k
1uF
47k
0.22
0.1
1
47k
Q1
S2
47k
D2
S1
10
47k
0.1
IC1
ISD1016AP
0.22
0.1
Circuit details
required to run the 78L05 5V regulator
– about 4mA.
When the RECORD button is pressed,
the PLAY/REC pin (pin 27) is pulled
low, while the POWER DOWN pin
(pin 24) is pulled low via diode D2.
The CHIP ENABLE pin (pin 23) is also
pulled low – via a 47kΩ resistor and
D2 – so that the IC can now accept an
audio input.
Finally, pressing the RECORD button
also turns the electret microphone on.
This now picks up sound and feeds an
audio signal into a preamplifier stage
inside the IC at pin 17.
The 470kΩ resistor and 4.7µF capacitor on pin 19 set the AGC time
constant for the microphone preamplifier. The aim here is to achieve the
highest level of audio possible without
clipping, to keep the signal-to-noise
ratio as high as possible.
The 1µF capacitor between pins 21
& 20 couples the audio signal from
the preamplifier to an internal amplifier block. From there, the signal
passes via an anti-aliasing filter and
is clocked into the 128K cell analog
storage array.
All clock and timing functions are
carried out automatically inside the
chip, so no external clock components
are required.
The chip continues to record the
0.1
During recording, this device samples the incoming audio signal and
stores these samples as analog voltages
in the EEPROM. This technique is
more efficient than digital storage and
provides the added bonus of 10-year
zero-power data retention.
If necessary, individual devices
can be cascaded to obtain longer
recording times. The chip also has
a message addressing facility so that
individual messages can be repeated
or different messages played back.
We haven’t used these features here
though, to keep the circuit as simple
as possible.
For detailed information on the
ISD1016AP IC, take a look at the feature article on this chip elsewhere in
this issue.
TO
SPEAKER
Fig.2: note the orientation of
switches S1 & S2 when installing
them on the PC board. The flat
side of each switch body faces
towards IC1.
signal on its pin 17 input until either
the RECORD button is released or the
device runs out of memory.
July 1993 33
When the PLAYBACK button (S1)
is pressed, Q1 turns on and pulls
the POWER DOWN pin (pin 24) low
to bring the chip back “on line”. At
the same time, D2 prevents the PLAY/
REC pin from being pulled low again
since this diode is now reversed bias
PARTS LIST
1 PC board, code 01104931,
100 x 55mm
1 green snap action pushbutton
switch (S1)
1 red snap action pushbutton
switch (S2)
1 plastic zippy case, 130 x 67 x
42mm
1 57mm 8Ω loudspeaker
1 electret microphone insert
4 15mm-long x 3mm tapped
spacers
8 6mm-long x 3mm machine
screws
4 3mm nuts
8 PC stakes
Semiconductors
1 ISD1016AP sound recorder IC
(IC1)
1 78L05 5V regulator
1 BC548 NPN transistor (Q1)
1 1N4004 silicon diode (D1)
1 1N914 signal diode (D2)
Capacitors
3 10µF 16VW electrolytic
1 4.7µF 25VW electrolytic
1 1.0µF 63VW MKT polyester
2 0.22µF 63VW MKT polyester
4 0.1µF 63VW MKT polyester
Resistors (1%, 0.25W)
1 470kΩ
1 2.2kΩ
4 47kΩ
1 10Ω
1 10kΩ
Miscellaneous
Light-duty hook-up wire, tinned
copper wire (for links), epoxy
resin.
ed. This means that the internal
recording circuitry remains
disabled.
The recorder now replays the
message stored in its memory. If
the PLAYBACK button is released
during playback, the mess
age
stops. If the button is then pressed
again, the message restarts from
the beginning.
The audio output signal appears across pins 14 & 15 (SP+
and SP-). These are complementary outputs which provide
50mW of power into a 16Ω load.
Since we are using an 8Ω loudspeaker, a 10Ω resistor is installed
in series with the output to provide the correct load.
In order to keep digital “noise”
to a minimum, the analog and
digital sections of the circuitry
have been isolated by providing
separate ground return rails on
the PC layout. This helps prevent
digital noise from finding its way
into the low-level audio sections,
such as the preamplifier and the
AGC circuitry.
The circuit requires a 5V
supply and this is derived via
reverse polarity protection diode
D1 and a 78L05 3-terminal regulator. Power is derived from the
mains via either a 9V or 12V DC
plugpack.
MIC
MESSAGE RECORDER
HOLD KEYS DOWN
RECORD PLAYBACK
Fig.3: this full-size artwork can be used
as a drilling template for the front panel.
Construction
All the parts for the Message Recorder – including the loudspeaker –are
installed on a small PC board. This
board is coded 01104931 and measures
100 x 55mm.
Before starting construction, check
the PC board for etching defects by
comparing it with the published
pattern. If you find any, correct the
problem immediately. Fortunately,
etching defects are fairly uncommon
but it’s always wise to make sure.
When you’re sure that everything
is OK, you can begin by installing
the five wire links – see Fig.2. Make
sure that the link wires are straight
so that they don’t short against other
components and note that one link
runs under IC1.
CAPACITOR CODES
❏
❏
❏
❏
Value
1.0µF
0.22µF
0.1µF
IEC Code
1u0
220n
100n
EIA Code
105
224
104
RESISTOR COLOUR CODES
❏
❏
❏
❏
❏
❏
No.
1
4
1
1
1
34 Silicon Chip
Value
470kΩ
47kΩ
10kΩ
2.2kΩ
10Ω
4-Band Code (1%)
yellow violet yellow brown
yellow violet orange brown
brown black orange brown
red red red brown
brown black black brown
5-Band Code (1%)
yellow violet black orange brown
yellow violet black red brown
brown black black red brown
red red black brown brown
brown black black gold brown
Once the links are in, install PC
pins at each of the switch mounting
pads and at the microphone mounting pad nearest the edge of the board
(note: not needed for a 2-terminal
microphone). This done, the resistors,
capacitors and semiconductors can
all be installed on the board. The accompanying table shows the resistor
colour codes but it’s also a good idea
to check each resistor with your multimeter before installing it, as it can
be difficult to distinguish the colours
on some brands.
Pay particular attention to the orientation of the polarised components.
These include the electrolytic capacitors and the semiconductors. Pin 1 of
the IC is adjacent to a small notch in
one end of the plastic body.
The two pushbutton switches (red
for RECORD, green for PLAYBACK) can
now be soldered to the tops of the PC
stakes (see photo). To do this, first
lightly tin the PC stakes and switch
pins, then position the switches on
the PC stakes and heat the contact
points with a soldering iron to re-melt
the solder.
Note that the switches must be oriented exactly as shown on Fig.2 – ie,
with the flat side of each switch body
towards IC1.
The electret microphone insert is
mounted with its top surface about
16mm above the PC board. If it is a
3-terminal device, it should be oriented so that its outer shield connection
is soldered to the PC stake previously
installed. If it is a 2-terminal device,
ignore the outer shield connection. In
both cases, the positive terminal goes
Make sure that all polarised parts are correctly oriented when installing them
on the PC board. The loudspeaker is mounted using double-sided tape or epoxy
resin, while the microphone is mounted with its top surface about 16mm above
the PC board – see photo below.
July 1993 35
to the centre of the three pads.
Finally, complete the PC board by
installing four mounting spacers (each
consisting of a 15mm spacer and a nut)
and then mounting the loudspeaker
in position. The loudspeaker can be
affixed to the board using double-side
tape or epoxy resin.
Use light-duty hook-up wire to connect the output terminals on the PC
board to the loudspeaker terminals.
Similarly, connect two 120mm-long
flying leads to the power supply terminals – these will later be wired to
the DC power socket.
doesn’t foul the PC board.
After that, it’s simply a matter of
attaching the board to the lid and
connecting the supply leads to the DC
input socket. Before doing this though,
connect the plugpack supply and use
your multimeter to identify the positive and negative terminals on the back
of the socket. The supply can then be
disconnected and the leads soldered
to their respective terminals.
Testing
Final assembly
The completed board assembly
can now be installed in the specified
plastic case. To do this, first attach the
adhesive label and use it as a drilling
template for the front panel. You will
have drill four mounting holes for
the PC board, two clearance holes for
the switches and access holes for the
loudspeaker and microphone.
In addition, you will have to drill
mounting holes in one end of the case
to accept the DC power socket. This
hole should be positioned near the
bottom of the case, so that the socket
Fig.4: check your PC board for etching
defects by comparing it against this
full-size pattern before mounting any
of the parts. In particular, check the
tracks that run between IC pads.
To test the unit, apply power and
hold down the RECORD button while
you speak into the microphone. Now
check that the message replays when
you press the PLAYBACK button.
If it doesn’t work, first check for
+5V at the output of the 3-terminal
regulator. Check also that this voltage
appears on pins 16 & 28 of the IC. If
these checks prove OK, check that
pin 24 switches from +5V to almost
0V when the PLAYBACK button is
pressed. If it doesn’t, check the circuit
around Q1.
Finally, if your microphone is a
2-terminal device, check that it is
correctly oriented, with the positive
terminal going to the centre pad. SC
CEBus AUSTRALIA KITS
CEBus Australia has opened the Circuit Cellar door to bring you a range
of high quality, educational electronics kits. There are three types of kit
available: an Experimenter’s Kit which includes the PCBs, manuals, any
key components that are hard to find and the basic software required
by the finished product. Then there is the Complete Kit which includes
everything above plus the additional components required to complete
the kit. Finally, there is the complete kit with Case & Power Supply.
Regardless of which kit you purchase you get the same high quality
solder masked and silk screened PCB and the same prime grade
components.
Our range of kits includes:
HAL-4 4 Ch, EEG Monitor, Complete kit only ................... $356.00
Experimenter’s Kits:
SmartSpooler, 256K print spooler ..................................... $214.00
IC Tester, Tests 74xx00 family ICs .................................... $233.00
Serial EPROM Programmer, For 27xxx devices ............... $214.00
Ultrasonic Ranger Board with Transducer.......................... $194.00
NB: The above prices DO NOT include sales tax.
Don’t forget we also have the HCS II, Home Control System, available,
Its features include: Expandible Network, Digital & Analog 1/O, X-10
Interface, Trainable IR Interface and Remote Displays.
Call fax or write to us today for more information.
Bankcard, Mastercard & Visa accepted.
CEBus AUSTRALIA.
Ph (03) 467 7194. Fax (03) 467 8422.
PO Box 178, Greensborough, Vic 3087.
36 Silicon Chip
LED BRAKE LIGHT INDICATOR
This “brilliant” brake light indicator employs 60
high intensity LEDs (550-1000mCd) to produce
a display that is highly visible, even in bright
sunlight. The intensity produced is equal to or
better than the LED brake indicators which are
now included in some late model “upmarket”
vehicles. The LED displays used in most of
these cars simply make all the LEDs turn on
every time the brakes are applied. The circuit
used in this unit can perform in this manner
and, for non-automotive applications, it can be
customised to produce a number of sweeps (110) starting at the centre of the display and with a
variable sweep rate. It not only looks spectacular
but also attracts more attention.
All the necessary “electronics” is assempled
on two identical PCBs and the resulting overall
length of the twin bargraph display is 460mm.
It’s simple to install into a car since only two
connections are required: Earth and the brake
LASER SCANNER ASSEMBLIES
These are complete laser scanners as used in
laser printers. Include IR laser diode optics and
a very useful polygon scanner ( motor-mirror).
Produces a “fan” of light (approx. 30 deg) in one
plane from any laser beam. We provide information on polygon scanner only. Clearance:
$60
400 x 128 LCD DISPLAY MODULE –
HITACHI
These are silver grey Hitachi LM215XB dot
matrix displays. They are installed in an attractive housing and a connector is provided.
Data for the display is provided. BRAND NEW
units at a low:
$40
LASER OPTICS
The collimating lens set is used to improve the
beam (focus) divergence. The 1/4-wave plate
and the beam splitter are used in holography
and experimentation. All are priced at a fraction
of their real value:
1/4 wave plate (633nM) ..............................$20
Collimating lens sets ..................................$45
Polarizing cube beam splitters ....................$65
GREEN LASER TUBES
We have a limited supply of some 0.5mW
GREEN ( 560nm) HeNe laser tubes. Because
of the relative response of the human eye,
these appear as bright as about a 2mW red
tube: Very bright. We will supply this tube and
a suitable 12V laser power supply kit for a low:
$299
CCD ELEMENT
BRAND NEW high sensitivity monolythic single
line 2048 element image sensors as used in
fax machines, optical charachter recognition
and other high resolution imaging applications:
Fairchild CCD122. Have usable response in
the visible and IR spectrum. Supplied with 21
pages of data and a typical application circuit.
$30
INFRARED TUBE AND SUPPLY
These are the key components needed for
making an INFRARED NIGHT VIEWER. The
tubes will convert infrared light into visible light
on the phosphor screen. These are prefocussed
tubes similar to type 6929. They do not require
a focus voltage. Very small: 34mm diameter,
68mm long. All that is needed to make the tube
light connecting wire. The case for the prototype
unit which would be suitable for mounting on
the rear parcel shelf, was mainly made from
two aluminium “L” brackets that were screwed
together to make a “U” section. A metal rod and
its matching holders (commonly available from
hardware shops) are used for the supporting leg.
$60
for both the PCBs, all the onboard components &
instructions: the 60 LEDs are included! We also
have available a similar kit that does not have
the sweeping feature. It produces similar results
to the commercial units installed in cars: all the
LEDs light up when power is applied.
$40
for both the PCBs and all the onboard components. This kit is also supplied with the 60 LEDs
and it uses different PCBs, that have identical
dimensions to the ones supplied in the above
mentioned kit.
operational is a low current EHT power supply,
which we provide ready made or in kit form:
powered by a 9V battery and typically draws
20mA. INCREDIBLE PRICING:
$90
For the image converter tube and an EHT
power supply kit!
All that is needed to make a complete IR night
viewer is a lens an eyeiece and a case: See
EA May and Sept. 1990.
ALUMINIUM TORCHES – INFRARED
LIGHTS
These are high quality heavy-duty black anodised aluminium torches that are powered by
four “D” cells. Their focussing is adjustable from
a spot to a flood. They are water resistant and
shock proof. Powered by a krypton bulb – spare
bulb included in cap.
$42
Note that we have available a very high quality
INFRARED FILTER and a RUBBER lens cover
that would convert this torch to a good source
of IR: $15 extra for the pair.
PASSIVE NIGHT VIEWER BARGAIN
This kit is based on an BRAND NEW passive
night vision scope, which is completely assembled and has an EHT coaxial cable connected.
This assembly employs a high gain passive
tube which is made in Russia. It has a very
high luminous gain and the resultant viewer
will produce useful pictures in sub-moonlight
illumination. The viewer can also be assisted
with infrared illumination in more difficult situations. It needs an EHT power supply to make
it functional and we supply a suitable supply
and its casing in kit form. This would probably
represent the best value passive night viewer
that we ever offered!
BECAUSE OF A SPECIAL PURCHASE OF
THE RUSSIAN-MADE SCOPES, WE HAVE
REDUCED THE PRICE OF THIS PREVIOUSLY ADVERTISED ITEM FROM $550 TO
A RIDICULOUS:
$399
This combination will be soon published as a
project in EA. NOTE THE REDUCED PRICE:
LIMITED SUPPLY. Previous purchasers of the
above kit please contact us.
24VDC TO MAINS VOLTAGE INVERTERS
In the form of UNINTERRUPTABLE POWER
SUPPLIES (UPS’s).These units contain a
300W, 24V DC to 240V 50Hz mains inverter.
Can be used in solar power systems etc. or
for their original intended purpose as UPS’s.
THESE ARE VERY COMPACT, HIGH QUALITY UPS’s. They feature a 300W - 450W (50Hz)
SINEWAVE INVERTER. The inverter is powered by two series 12V 6.5Ahr (24V). batteries
that are built into the unit. There is only one
catch: because these NEW units have been
in storage for a while, we can not guarantee
the two batteries for any period of time but we
will guarantee that the batteries will perform
in the UPS’s when these are supplied. We will
provide a 3-month warranty on the UPS’s but
not the batteries. A circuit will also be provided.
PRICED AT A FRACTION OF THEIR REAL
VALUE: BE QUICK! LIMITED STOCK!
$239
ATTENTION ALL MOTOROLA
MICROPROCESSOR PROGRAMMERS
We have advanced information about two
new STATE OF THE ART microprocessors
to be released by Motorola: 68C705K1 and
68HC705J1. The chips are fully functional
micros containing EPROM/OTPROM and RAM.
Some of the features of these new LOW COST
chips include:
*16 pin DIL for the 68HC705K1 chip * 20 pin
DIL for the 68HC705J1 chip * 10 fully programmable bi-directional I/O lines * EPROM
and RAM on chip * Fully static operation
with over 4MHz operating speed.
These two chips should become very popular.
We have put together a SPECIAL PACKAGE
that includes a number of components that
enable “playing” with the abovementioned
new chips, and also some of the older chips.
IN THIS PACKAGE YOU WILL GET:
* One very large (330 x 220mm) PCB for the
Computer/Trainer published in EA Sept. 93; one
16x2 LCD character display to suit; and one
adaptor PCB to suit the 68HC705C8.
* One small adaptor PCB that mates the
programmer in EA Mar. 93 to the “J” chip,
plus circuit.
* One standalone programmer PCB for programming the “K” chip plus the circuit and a
special transformer to suit.
THE ABOVE PACKAGE IS ON SPECIAL AT
A RIDICULOUS PRICE OF:
$99
Note that the four PCBs supplied are all silk
screened and solder masked, and have plated
through holes. Their value alone would be in
excess of $200! A demonstration disc for the
COMPUTER/TRAINER is available for $10.
No additional software is currently available.
Previous purchasers of the COMPUTER/
TRAINER PCB can get a special credit towards
the purchase of the rest of the above package.
PLASMA BALL KIT
This kit will produce a fascinating colourful
changing high voltage discharge in a standard
domestic light bulb. The EHT circuit is powered
from a 12V supply and draws a low 0.7A. We
provide a solder masked and screened PCB, all
the onboard components (flyback transformer
included), and the instructions at a SPECIAL
introductory price of:
$ 25
We do not supply the standard light bulb or
any casing. The prototype supply was housed
in a large coffee jar, with the lamp mounted
on the lid – a very attractive low-cost housing!
Diagrams included.
LASER DIODE KIT – 5mW/670nm
Our best visible laser diode kit ever! This one is
supplied with a 5mW 670nm diode and the lens,
already mounted in a small brass assembly,
which has the three connecting wires attached.
The lens used is the most efficient we have
seen and its focus can be adjusted. We also
provide a PCB and all on-board components
for a driver kit that features Automatic Power
Control (APC). Head has a diameter of 11mm
and is 22mm long, APC driver PCB is 20 X
23mm, 4.5-12V operation at approx 80mA.
$85
PRECISION STEPPER MOTORS
This precision 4-wire Japanese stepper motor
has 1.8 degree steps – that is 200 steps per
revolution! 56mm diameter, 40mm high, drive
shaft has a diameter of 6mm and is 20mm long,
7.2V 0.6A DC. We have a good but LIMITED
supply of these brand new motors:
$20
HIGH INTENSITY LEDs
Narrow angle 5mm red LED’s in a clear housing.
Have a luminous power output of 550-1000mCd
<at> 20mA. That’s about 1000 times brighter
than normal red LED’s. Similar in brightness
SPECIAL REDUCED PRICE: 50c Ea or 10
for $4, or 100 for $30.
IR VIEWER “TANK SET”
ON SPECIAL is a set of components that can
be used to make a complete first generation
infrared night viewer. These matching lenses, tubes and eyepieces were removed from
working tank viewers, and we also supply a
suitable EHT power supply for the particular
tube supplied. The power supply may be ready
made or in kit form: basic instructions provided.
The resultant viewer requires IR illumination.
$180
We can also supply the complete monocular
“Tank Viewer” for the same price, or a binocular
viewer for $280: Ring.
MINI EL-CHEAPO LASER
A very small kit inverter that employs a switchmode power supply: Very efficient! Will power a
1mW tube from a 12V battery whilst consuming
about 600 mA! Excellent for high-brightness
laser sights, laser pointers, etc. Comes with
a compact 1mW laser tube with a maximum
dimension of 25mm diameter and an overall
length of 150mm. The power supply will have
overall dimensions of 40 x 40 x 140mm, making
for a very compact combination.
$59
For a used 1mW tube plus the kit inverter.
OATLEY ELECTRONICS
PO Box 89, Oatley, NSW 2223
Phone (02) 579 4985. Fax (02) 570 7910
MAJOR CARDS ACCEPTED WITH
PHONE & FAX ORDERS
P & P FOR MOST MIXED ORDERS
AUSTRALIA: $6; NZ (Air Mail): $10
July 1993 37
Build this light beam
relay extender
This simple infrared transmitter circuit is
designed to go with the Light Beam Relay project
published in the December 1991 issue. It’s based
on a 555 timer IC & will more than double the
effective range.
By DARREN YATES
The Light Beam Relay published in
our December 1991 issue has proven
to be a popular project. In most applications, it is used to monitor a path
or a doorway (eg, to a shop) using an
invisible infrared light beam. When
someone walks through the beam, it
briefly sounds an alarm.
To simplify construction, the original project housed the transmitter and
receiver circuits in the one case. This
meant that the infrared light from the
transmitter had to be reflected back
to the detector in the receiver using a
mirror mounted on the opposite side
of the doorway.
But what if you want greater range,
or a unit that can be moved to another
location and quickly set up without
critical alignment? The answer is to
disable the internal transmitter circuit and use this external transmitter
circuit (or Light Beam Relay Extender)
instead. It uses a 555 timer IC and a
transistor to pulse two IR LEDs at a
frequency of about 2kHz.
This external circuit increases the
working range to about five metres
–2.5 times that of the original. That’s
mainly because the light no longer
travels over a double path length and
because scattering losses at the mirror
are eliminated (since the mirror is no
longer required).
Further improvements in the range
are derived from increasing the gain of
the receiver and by moving the detector diode (D2) right up to its viewing
hole in the side of the case. These last
two modifications must not be applied
to the original project however, as this
would cause false triggering due to the
close proximity of the IR LEDs and
the detector.
Refer now to Fig.1 for the circuit
details. IC1 is a 555 timer and is
connected as an astable oscillator. Its
frequency of oscillation is about 2kHz,
while the duty cycle of the output
waveform at pin 3 is about 100:1.
The output signal at pin 3 drives
transistor Q1 via a 100Ω current limit
ing resistor. Since Q1 is a PNP type,
it only turns on during the narrow
low-going pulses from pin 3 (ie, its
duty cycle is about 1%). Each time
Q1 turns on, about 200mA is pulsed
through the two IR LEDs to turn them
hard on. Although this may seem a
very high current, the LEDs are only
on for about 1% of the total time and
so the current averages out to about
2mA which is well within their rating.
Power for the circuit is derived from
the same source that’s used to power
the receiver (ie, a 12V DC plugpack).
Diode D1 provides reverse polarity
protection, while the 10µF capacitor
provides supply line decoupling.
Construction
All the parts for the Light Beam Relay Extender are installed on a small
PC board coded 03106931. Fig.2 shows
the parts layout.
No particular order need be followed when installing the parts but
take care to ensure that all polarised
parts are correctly oriented. These
D1
1N4004
68k
4
7
3.3k
IC1
555
6
2
3 100
A
IRLED1
B
E
C
VIEWED FROM
BELOW
10uF
+12V
C
D1
.01
1
0.1
K
IRLED2
IRLED1
100
Q1
A
2xCQY89
A
LIGHT BEAM RELAY EXTENDER
38 Silicon Chip
0V
Q1
BC327 E
B
1
.01
47
3.3k
0.1
8
IC1
555
10
16VW
68k
12V
K
IRLED2
K
47W
Fig.1 (left): the circuit uses astable oscillator IC1 (555) to
pulse two IR LEDs on & off via driver stage Q1. Fig.2 (above)
shows how the parts are installed on the PC board. Make
sure that the LEDs are correctly oriented.
K
ALEX
The UV People
ETCH TANKS
● Bubble Etch ● Circulating
LIGHT BOXES
● Portuvee 4 ● Portuvee 6
● Dual Level
TRIMMER
● Ideal
PCB DRILL
● Toyo HiSpeed
MATERIALS
The PC board fits inside a small plastic utility case, with the two IR LEDs
protruding through holes drilled in one end.
● PC Board: Riston, Dynachem
● 3M Label/Panel Stock
● Dynamark: Metal, Plastic
✸ AUSTRALIA’S NO.1 STOCKIST ✸
PARTS LIST
1 PC board, code 03106931,
56 x 41mm.
1 plastic case, 83 x 54 x 30mm
Fig.3: the full-size etching pattern for
the PC board.
include the two IR lEDS, the semiconductors and the 10µF electrolytic
capacitor. Mount the two LEDs at full
lead length so that they can later be
bent to protrude through one end of
the case.
A small plastic utility case is used
to house the transmitter circuit. Drill
two holes in one end for the LEDs plus
four mounting holes in the base, then
secure the PC board using machine
screws and nuts.
Power for the transmitter circuit
can be obtained by run
ning a long
lead back to the DC socket inside the
receiver. This lead can be hidden by
running it over the top of a doorway,
for example. Alternatively, you can
power the transmitter from a separate
plugpack supply.
Receiver modifications
In order for the extender circuit
to do its job, you need to disable the
transmitter in the original project.
This is done by removing the 100kΩ
Semiconductors
1 NE555 timer IC (IC1)
1 BC327 PNP transistor (Q1)
1 1N4004 silicon diode (D1)
2 CQY89A infrared LEDs
(IRLED1, IRLED2)
K
ALEX
40 Wallis Ave, East Ivanhoe 3079.
Phone (03) 9497 3422, Fax (03) 9499 2381
Silicon Chip Binders
Capacitors
1 10µF 16VW electrolytic
1 0.1µF MKT polyester
1 .01µF MKT polyester
Resistors (1%, 0.25W)
1 68kΩ
1 100Ω
1 3.3kΩ
1 47Ω
Miscellaneous
Hook-up cable for power leads,
machine screws & nuts.
resistor between the +12V supply rail
and pin 2 of IC1. If you are building
the project from scratch, just leave out
the transmitter components around
IC1a. You should also connect pin 2
of IC1 to ground and connect pins 1
& 3 together.
The gain of the receiver circuit is increased by reducing the 10kΩ resistor
on pin 9 of IC1c to 1kΩ. Note that you
can save a few dollars by transferring
the IR LEDs to the external transmitter
SC
circuit.
These beautifully-made binders will
protect your copies of SILICON CHIP.
They are made from a distinctive
2-tone green vinyl & will look great
on your bookshelf.
Price: $A14.95 (incl. postage in
Australia). NZ & PNG orders add
$5 each for postage. Not available
elsewhere. Send your order to:
Silicon Chip Publications
PO Box 139
Collaroy Beach 2097.
Or fax (02) 979 6503; or ring (02)
979 5644 & quote your credit card
number.
July 1993 39
SERVICEMAN'S LOG
When it looks easy, it often ain’t
Yes, it did look easy. There it was; an obviously
damaged component clearly visible. All I had to
do was find out why it was damaged. Although
this would involve some searching, it turned out
to be a much bigger search than anyone could
have imagined.
One of the most elementary methods of servicing has always been
visual observation. Way back in the
very early days of radio, when bright
emitter valves were the norm, the
first thing one looked for in a dead
set was whether all the valves were
alight. In fact, there were those who
bemoaned the advent of the dull
emitter valves, significantly more
economical though they were, because they no longer provided this
visual clue.
Much has changed since then of
course, but the visual clue remains
a valuable one, even with today’s
technology. The burn marks on a PC
board, the bulging capacitor, the blackened fuse, the burnt resistor; they all
pinpoint a fault area. And while they
don’t necessarily pinpoint the fault
itself, they can show one where to
start looking.
All of which is leading up to a
particularly frustrating problem I
encountered recently; the more so
because at first glance – literally –
there was a typical visual clue which
should have put me straight on the
right track.
It all started when the customer
turned up with a Samsung colour set,
model CB-5012Z. This is a 51cm set
using a P/58SC type chassis and was
about three years old. The complaint
was straightforward enough; the set
was completely dead, having simply
failed in the middle of a program.
So, at the first opportunity, I put
it up on the bench. I didn’t bother to
switch it on but simply pulled the back
off and looked for any obvious clues.
This was relatively easy because all the
parts are on a single PC board, the only
reservation being that the components
in the power supply section are very
tightly packed.
Two things were immediately obvious: (1) the mains fuse, F801 (3.5A),
was blown; and (2) resistor R809
(270kΩ, 1W) was badly blackened.
This resistor runs from the positive
side of the bridge rectifier, at about
300V, to pin 4 of the switchmode power supply control IC, IC801 (TDA4601).
And, as I subsequently dis
covered,
safety resistor R801 (5.6Ω 7W) in the
mains input line, just after the fuse,
had also been sacrificed.
cial about all that. Fairly obviously,
there was a short that involved all
three components and, as such, I
didn’t think that it would be hard
to find. Anyway, the first thing to do
was to replace the faulty resistors and
I did this without even testing them.
This done, I replaced the fuse and
switched on with everything under
close scrutiny.
Splat! There was a flash of flame, a
puff of black smoke, and I had another
blackened resistor. Fortunately, a fast
reflex action by my switch finger saved
the fuse and the safety resistor.
My initial thought was simply along
the lines that a short at the IC end of
R809 could produce such symptoms. I
even went so far as to check for a short
circuit between pin 4 of the IC and
chassis; it was almost a reflex action.
But then, on reflection, I realised that
this didn’t make sense. Even putting
a 270kΩ resistor directly across 300V
would dissipate only about one third
of a watt.
So what was destroying the resistor?
All I could think of was that a much
higher voltage, from somewhere else
in the power supply, was finding its
way to this resistor. But from where
and by what means remained a mystery.
I went over the circuit around pin
4 of IC801 and resistor R809 but drew
a complete blank. Finally, and somewhat against my better judgement, I
decided that it must be a faulty IC. In
any case, replacing it would prove the
point, one way or the other.
The only snag was that I didn’t have
this particular IC in stock, so one had
to be ordered. When it arrived a couple
of days later, I lost no time in fitting it.
This proved to be a somewhat tricky
exercise due to the rather cramped
conditions on this part of the board
and the fact that the IC is mounted on
a heatsink.
Splat No.1
Splat No.2
Well, there was nothing very spe40 Silicon Chip
Eventually, the job was completed
Fig.1: the power supply circuit for the Samsung CB-5012Z. Fuse F801 is at
extreme left, safety resistor R801 to the right, & the bridge rectifier to the
right again. R809 is below the lower left corner of IC801 at top right, while
C816 is mid-way up the right-hand edge of the diagram.
and I made ready for another test. A
new 270kΩ resistor had been fitted and
I hoped all would go well this time.
I pressed the power switch. Splat!
Another flash of flame, another puff of
smoke, and another blackened resistor.
I gave up!
Well, almost but I certainly felt like
it. Unfortunately, I had no choice but
to keep at it and so, for want of a better
ap
proach, I simply began checking
every component around the IC, either
measuring then in-situ or removing
them from the board for testing where
necessary.
I had checked a dozen or more components in this way, without result,
and was beginning to question the
wisdom of this approach when I found
myself in the vicinity of transistor
Q801, the power supply switching
transistor. This was removed and tested but also proved to be OK.
The next component was C816, a
222pF 1000V ceramic capacitor connected between Q801’s collector and
chassis. This component is obviously
a spike suppressing device. Because
of the associated circuitry around it,
I decided that this it would also have
to be removed for testing.
In fact, pulling it out was all the testing needed. It was mounted so close
to other components that I could see
only one side of it. But when I pulled it
out and the other side became visible, I
realised that I had struck oil. The case
had split open to reveal a great black
gaping crack.
So at last I’d found the real culprit.
But what, you may ask, did it have to
do with resistor R809, which appears
to be in no way connected with this
part of the circuit. And if you are thinking of way-out explanations involving
spikes in Q801’s collector circuit, forget it. Maybe there were some spikes
but that isn’t the explanation.
In fact, it was much more mundane
than that and simply hinges on the
proximity of C816 to R809. They were
sitting side by side, virtually touching,
with C816 lying slightly over the top
of R809.
So the smoke and flame I had
observed had come from C816, not
R809. And the blackening of R809?
This was almost certainly a burn – not
from internal heat but from external
heat generated by C816. Remember, I
mentioned earlier that I had not even
bothered to check the “damaged” resistors. That was a fatal mistake.
Had I done so, I would almost
certainly have adopted a dif
ferent
approach. When I eventually checked
all three of these resistors, they were
spot on in value. There was nothing
wrong with any of them. The damage
was purely cosmetic and I had been
well and truly conned.
Rubbing in the salt
But there was still some salt to be
rubbed into the wound. I replaced
C816, fitted a new resistor for R809
purely for appearance, and switched
on. And up came a perfect picture; the
only thing that had ever been wrong
with the set was C816. And it had
carried a perfect visual clue but one
which was impossible to see.
Had I been able to see it, I would
have simply replaced the capacitor
and the set would have been back in
operation in a matter of minutes. As
it was, I wasted hours on the job and,
financially, it was a total disaster;
something which had to be written
off to experience.
In that sense, it wasn’t a complete
loss. Apart from the obvious lessons,
one other point emerged. I realised
that there was a failure pattern
emerging concerning the C816 type
capacitor.
Quite recently, I had also serviced a
couple of Samsung chassis which carried the Akai label. Both suffered from
the same fault – failure of a capacitor
across the horizontal output transistor.
And it was an identical capacitor: blue
ceramic, 222pF, 1000V. In both cases,
July 1993 41
SERVICEMAN'S LOG – CTD
But my customer knew where; onto
the power mains connected to his TV
set. After that, the TV set didn’t go any
more. I wonder if the Greek gods know
about TV sets?
OK, enough! But it was classic case
of a mains lightning strike and this
customer wasn’t the only one affected.
When I pulled the back off the set, the
damage was plain to see.
The most obvious was the mains
fuse, F801, 4A. The inside of the glass
was totally blackened, suggesting a
pretty violent strike, and I had no
doubt that I would find more subtle
damage as I went along.
The other visual clue involved a line
filter, L801, in the mains lead immediately following the fuse. The filter
coils themselves were undamaged but
the white plastic case which enclosed
them had been blown to pieces. Since
it was still working, I decided to leave
it until later.
The fuse was replaced and I moved
on to the next item down the line:
the bridge rectifier involving diodes
D801-804. Two of these four diodes
had snuffed it and these were replaced.
Switch-on
they had simply developed a dead
short and shut the set down without
any fireworks. But from now on, I’m
keeping my eye out for any faults
which might involve this particular
capacitor. It could well be less reliable
than one expects from this type in
general service.
Further to that observation, I have
been able to secure another make of
capacitor which I hope will be less
troublesome than the originals. When
I needed replacement capacitors for
the Akai sets, it was more convenient
to order them from an independent
supplier rather than from Samsung.
These not only carry a different brand
but, more importantly, are rated at
2000V.
These new capacitors were fitted to
the Akai sets, as well as to the Samsung set which was the subject of this
month’s story. Here’s hoping that I
have struck a blow for my customers.
hardly the set’s fault. No, the blame
really lies with the great god Jupiter.
In a fit of pique, “he hurled a thunderbolt into the air, which fell to earth
he knew not where” (as they say in
the classics).
Jupiter strikes
Fig.2: parts layout for the power
supply in the Samsung CB-5012Z.
R809 (circled) is situated between
transistor Q801 on the right & C816
on the left. Note that, in practice, the
board layout is much more crowded
than this diagram indicates.
My next story is also about a Sam
sung set – a model CB-518F fitted
with a P50HA chassis – and it also
in
volves visual clues. But I must
hasten to add that this problem was
42 Silicon Chip
OK, time for a switch-on test. This
left no doubt that there was more
trouble ahead. There were loud
protestations from the switchmode
section of the power supply, suggesting a serious overload. I immediately
checked the HT rail for any suggestion of a short to chassis but could
find nothing wrong.
On this basis, and because all the
faults so far had been at the input to
the power supply, it seemed likely
that the fault was still in this area.
There are several more diodes in this
section and I checked all these but
found nothing wrong.
The next suspect was the regulator
IC, Q801 (STR50103A). But before
taking a final step in this direction, I
made a few more checks. I was able
to measure some HT rail voltage –
about 68V as compared to the 103V
shown on the circuit (pin 2 IC Q801
and TP103) – and I also checked the
horizontal output transistor (Q404,
2SD-1555) but this appeared to be OK.
At that stage, I felt that I had gone as
far afield as was reasonable for a strike
of this kind, so I returned to the regu
lator IC. This is a small device, having
only five pins, and I had one in stock
so it was a simple matter to replace it.
ing circuit, caused the two coils to be
pushed apart slightly, due to magnetic
repulsion. They sat only loosely on the
ferrite core.
The movement wasn’t very great,
and would not have caused any
damage in the normal way. But with
the massive surge that destroyed the
bridge diodes and the fuse, the movement had obviously been much great
er; enough to break the flimsy plastic
cover. So that solved that particular
mystery.
Unanswered questions
This photo clearly shows the crack in the back of C816. Also shown in the
blackened fuse (F801) and one of the replacement resistors used for R809.
But all that did was establish that
there was nothing wrong with the
original IC; the new one made no
difference.
I made a few more checks and found
that the 12V rail was down in about
the same proportion as the HT rail
loss. This 12V rail is derived from a
16.5V tap (pin 2) on the horizontal
output transformer via diode D408
and resistor R225 (47Ω, 2W).
But there is also a 12V rail derived
from the chopper transformer via diode D820, which is used as a starting
supply to get the horizontal system
running. And at this point I couldn’t
be sure which of these two supplies
was powering the system, to the extent
that it was working at all.
I also realised that, while all this
analysis of the circuit was very interesting, it wasn’t really revealing
anything that might help solve the
problem. It was time to change tactics.
let-down after all the chasing around
the circuit.
And what about the line filter I
mentioned earlier? While the coils
were undamaged in any way, the white
plastic cover was scattered in pieces
around the inside of the cabinet. How
come?
I found the answer quite by chance.
The filter consists of two fine wire
coils (or chokes) wound on small flat
plastic bobbins, about the diameter of
a 5-cent piece, but somewhat thicker.
These in turn are mounted side by
side on the centre leg of a rectangular
ferrite core.
And I noticed, when switching the
set on after it was repaired, that the
switch-on surge, due to the degauss-
But that still leaves other questions
unanswered. Why did such a massive
surge, having destroyed the bridge
diodes in that part of the circuit, skip
over the regulator IC and the horizontal
driver stage, to pick on the horizontal
output stage? And why didn’t it spread
further via the supply rails and do a
lot more damage?
More importantly, from a practical
point of view, why did Q404 test OK
when it wasn’t?
I don’t have any answers for the
first two questions. I doubt whether
anybody has – except Jupiter perhaps
and he’s not telling.
I don’t have a complete answer to
the third question eith
er, but there
seems little doubt that the protective
devices in these transistors (ie, the
diode between collector and emitter
and the resistor between base and
emitter) make them difficult to test
reliably. The resistor, in particular
(normally 35-40Ω), makes it difficult
Transistors cheat
Speculating on likely component
failures, my thoughts came back to the
horizontal output tran
sistor, Q804.
Granted, I had run the meter over it
and decided that it was OK. But it
wouldn’t be the first time that such
a transistor had cheated the testing
procedure.
As always, and as they used to say
in the old valve days, the ultimate test
of a suspect device is to replace it.
Which was what I did, it not being a
particularly difficult procedure.
And that was it. The set was up and
running in all its original glory. Which
was both a relief and something of a
July 1993 43
SERVICEMAN'S LOG – CTD
Fig.3: the power supply circuit for the Samsung CB-518F. The mains on/off
switch is at the bottom left of the diagram. Fuse F801 follows, then the line
filter L801, the degauss circuit L802, and bridge rectifier D801-804. Next in
line is chopper transformer T801 then and switching IC Q801. The horizontal
deflection circuit is at the top of the diagram.
to determine the condition of the
base-emitter junction.
On the other hand, they don’t always confuse the issue; sometimes
faults are quite readily detected. It all
depends on the nature of the failure.
So the rule seems to be if it tests faulty,
then it is faulty; if it tests OK, it might
44 Silicon Chip
be faulty, or it might not.
Must try not to get caught like that
again.
Circuit diagrams
One final comment. Unfortunately,
the quality of the diagrams in many
manuals leaves a lot to be desired,
and the diagrams for the Samsung sets
just discussed fall into this category.
The main problem stems from the
large size needed for many original
drawings, followed by over reduction
in an effort to accommodate them in a
typical manual.
This can create major problems
when trying to trace a circuit, while
tracking down a difficult fault. Component values are often hard to read,
particularly where figures 6, 8, 9 and
even 0 (zero) are concerned. In a blurr
ed reproduction, one can easily be
mistaken for the other.
Even more confusion can occur
where circuit lines cross. While the
concept of using small circular blob
to denote a con
nection, or no blob
to denote a non-connective crossing,
has the advantage of draughting simplicity, it falls down badly where the
reproduction is poor.
A certain amount of image spread
can occur where lines cross, creating
the impression of a blob where none
exists, or giving rise to doubts as to
whether a genuine blob is really only
a blur. And take my word for it; it can
waste a lot of time.
Personally, I much prefer the more
conservative drawing convention,
which uses a loop to denote a non-connective crossing. The stated objection,
of course, is that this requires more
work and is therefore more costly.
Well maybe it used to be but these
days, with Computer Aided Drawing
(CAD) programs, I doubt whether the
difference is all that great.
Anyway, for my money, the differSC
ence is worth any extra cost.
SILICON
CHIP
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Please feel free to visit the advertiser’s website:
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CHIP
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CHIP
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SILICON
CHIP
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SILICON
CHIP
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SILICON
CHIP
If you are seeing a blank page here, it is
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SILICON
CHIP
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SILICON
CHIP
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has requested that the page be removed to
prevent misunderstandings.
Please feel free to visit the advertiser’s website:
www.jaycar.com.au
BUILD THIS AM
RADIO TRAINER; PT.2
In this second & last article on the AM Radio
Trainer, we show you how to assemble &
align it for best performance. You won’t need
an RF signal generator for this task, as we
describe a simple alignment oscillator at the
end of this article.
By MARQUE CROZMAN & LEO SIMPSON
The big attraction of the AM Radio
Trainer, apart from giving you the
opportunity to build a classic circuit, is the fact that the PC board is
over-printed with the circuit diagram.
This is instead of the more usual component overlay diagram and should
enable the novice to better come to
grips with the functions of the various
components.
There are also a number of test
points on the circuit board and these
can be used for voltage measurements
or to provide waveforms which can
be displayed on an oscilloscope. We
will feature some typical waveforms
in this article, so you will know what
to expect.
Another point to note about the
board is the large area of copper in
the pattern. Most of this copper is
all connected to the 0V rail from the
battery and forms a “ground plane”
for the circuit. This helps isolate the
various sections of the circuit from
each other and thereby ensures a good
level of performance.
Before you start assembly of the
board, there are a number of checks
you should do. First of all, check that
there are no shorts between tracks
or breaks in tracks. These should be
repaired before you go any further.
Second, make sure that the board is
suitably drilled for all the components. In particular, make sure that
the IF transformers can be inserted
and that there are holes drilled for
the volume control potentiometer, for
the mounting screws and shaft of the
tuning gang, the 3.5mm headphone
socket, the power switch and the
battery holder.
There should also be a pattern of
small holes in the large circular region where the loudspeaker is to be
mounted – otherwise the sound will
be muffled.
The resistors should be inserted
first. You can check the colour code
for each resistor value by referring to
the table of resistor values accompanying this article. However, whether
or not you are familiar with the resistor colour code, we strongly suggest
that you check each resistor value
with a digital multimeter (switched
to the appropriate “Ohms” ranges)
before it is inserted and soldered
into place.
The resistors can be inserted either
way into the board but it is a good
idea to install them so that their colour
codes all run in the same direction.
This makes it so much easier to check
their values later on. Besides, it looks
better.
Trimpot VR2 for the audio amplifier
output biasing can also be installed at
this stage. Note that its value should
be 100Ω, not 200Ω as specified on the
circuit last month.
July 1993 53
This close-up view shows the mounting details for the on/off switch, the
headphone socket, the loudspeaker & the volume control. The loudspeaker is
secured using three small solder lugs which are soldered to the groundplane.
Next, you can install all the capacitors with a value under 10µF, which
means all the non-electrolytic capacitors. These are specified as monolithic
or ceramic disc types.
In practice, you are most likely to
be supplied with small rectangular
capacitors which have leads 5mm
apart, to match the hole spacing on the
board. These will have their capacitance marked in one of two possible
codes, EIA or IEC, as shown in the
capacitor code table accompanying
this article.
Having inserted the ceramic capacitors, the electrolytics are next.
These have a black stripe down one
side to indicate the negative lead.
The electrolytic capacitors must be
installed the correct way around otherwise they will be reverse-polarised
and they will become leaky (in the
electrical sense).
Next, install diodes D1 and D2.
Don’t swap them around otherwise
the circuit won’t work well at all. The
OA91 germanium diode (D1) will have
a larger glass body than the 1N4148
silicon diode (D2). Diodes are also
polarised so be sure that the coloured
band for the cathode is at the right end.
Note: on the circuit, the cathode end
of the diode is the end to which the
arrow is pointing. The arrow also indicates the direction in which current
can flow. Normally, diode symbols on
our circuits are marked with A and K
to designate the anode and cathode.
54 Silicon Chip
Both diodes should be installed
with a stress relief loop at one end so
that they are less likely to be fractured
if the board is stressed; ie, flexed or
bent.
A trap for young players
The transistors go in next. Be sure
to check that you get them around the
right way. All the transistors specified
come in plastic TO-92 encapsulation
and the three leads from the underside
are in a triangle configuration. This is
shown on the pinout diagram on the
circuit.
But there is a big trap for young (and
old) players in assembling this board.
Because we have printed the circuit
on top of the board and arranged the
circuit pattern to match it, it has been
necessary to take liberties with the
leads of most of the transistors. For Q1,
Q2, Q3, Q4 and Q6, it is necessary to
push the base lead between the emitter
and collector leads, so that their leads
match the circuit.
If you don’t do this, the circuit
won’t work. And make sure you put
the correct transistor in each position.
IF transformers
Now you can install the oscillator
coil and IF transform
ers. These all
look the same except for the colour
of the slug at the top. The colours are
as follows: oscillator coil (L2), red;
1st IF transformer (T1), yellow; 2nd
IF transformer (T2), white; third IF
transformer (T3), black (ie, no colour).
One point we did not cover in last
month’s circuit description concerns
the capacitors which are connected
in parallel with the primary winding
of each of these transformers and the
oscillator coil. Have a look now and
note these capacitors. However, if you
have a look on the PC board, you will
find that there is no place to put the capacitors. That is because the capacitor
for each unit is actually inside the can
and is wired internally. So you don’t
have to worry about it.
Having capacitors inside the cans
of resonant coils is common practice
in radios, transceivers and TV sets. It
ensures manufacturing consistency,
minimises wiring and saves board
space.
By the way, you should resist the
temptation to twiddle the slugs of the
IF transformers and oscillator coil
by using a small screwdriver. Don’t
do it. You should buy a set of plastic
alignment tools and use one which
has a blade with a neat fit in the slot
of the slug.
If you can’t purchase a suitable
alignment tool, you can make one out
of a plastic styling comb. Cut off the
long thin portion of the handle of the
comb and then shape one end so that
it is like a small screwdriver blade.
You can easily do this with a sharp
utility knife.
There are several reasons not to use
a small screwdriver to adjust the slugs.
First, it is all too easy to damage the
slots in the slugs. Second, the blades
of screwdrivers are often magnetised
and this can affect the magnetic characteristics of the slugs. Third, when
you are going through the actual
alignment of the radio, the steel blade
of the screwdriver will badly affect the
resonance of the coil and you will get
quite misleading results.
Ferrite rod antenna
When installing the ferrite rod antenna, you will need to solder the coil
connections first and then secure the
ferrite rod itself in place with a small
plastic cable tie through the board.
This is a temporary mounting method
and there is a particular reason for doing it this way at this stage. The coil has
four coloured cotton-covered wires
and these should not be shortened
back since they are already pre-tinned.
The circuit board holes for the antenna connections are labelled with the
Rear view of the assembled project. Bend the tags of the volume control & tuning
capacitor so that they touch their respective pads on the board & solder them in
place. The on/off switch, loudspeaker & headphone socket are connected to the
PC board via wire links.
colours; ie, white (WHT), black (BLK),
red (RED) and green (GRN).
The plastic dielectric tuning capacitor is secured to the PC board by two
small countersunk screws. After these
are inserted and tightened, the three
tags need to be bent at right angles
to make contact with the relevant
pads on the PC pattern; they are then
soldered.
Secure the volume control potent
iometer to the board with its washer
and nut. Bend the tags so that they
touch the pads on the board and solder
them in place.
The battery holder and on/off switch
are next to be mounted. The battery
holder is mounted on the component
side of the board and is held in place
with two 8BA screws and nuts.
Use short lengths of hook-up
wire to connect its terminals to the
relevant spots on the PC board. The
on/off switch is mounted through
the board and secured with a nut
and washer. The terminals are then
connected to the board with short
lengths of wire.
Speaker mounting
Three small solder lugs hold the
speaker in place, as shown in the
photo. The lugs are soldered to the
ground plane, equally spaced around
the rim of the speaker.
Mount the headphone socket next
to the on/off switch. The tab closest
to the board is soldered to the ground
plane. The other two connections must
be made in such a way that when the
headphone (or earphone) jack is in-
serted, it disconnects the speaker and
connects the headphone. This means
that the tag which makes contact with
the tip of the jack when it is inserted
must connect to the negative side of
the 100µF 16VW capacitor. The other
tag is connected to one side of the
speaker. You can check the switching
operation of the socket by using your
multimeter.
The other terminal of the speaker
is connected to the ground plane of
the board via a short length of hookup wire.
To finish off the construction,
four 25mm tapped metal spacers are
secured to the board with machine
screws, one in each corner. This allows
the board to sit on a flat surface and
provides clearance for the volume pot,
tuning gang and loudspeaker.
Now check all your work very carefully and you will be ready for the next
stage which is alignment.
Aligning your radio
The major difference between
this project and any other that you
may assemble from the pages of this
magazine is the need for alignment.
Even if you have assembled the radio
precisely as we have described so far,
there is little chance that it will work
satisfactorily when you first turn it on.
This is because all the slugs in the IF
transformers need to be adjusted to
give the best gain.
At the same time, you will need to
adjust the slug in the oscillator coil
and the trimmer capacitors associated
with the tuning gang to give the best
“tracking”. These latter adjustments
ensure that the resonant circuit of the
oscillator coil “tracks” with the input
resonant circuit across the whole of the
broadcast band. If this is not done, the
sensitivity will vary quite markedly
across the broadcast band.
Before you start the alignment process though, rotate trimpot VR2 fully
anticlockwise. This will set the quiescent current in the output stage transistors, Q6 and Q7, to zero. Rotate the
volume control pot fully anticlockwise
and the tuning knob fully clockwise
or anticlockwise. This done, connect
a 9V battery or DC power supply set to
9V and then measure voltages around
the circuit. Connect the negative probe
of your multimeter to a point on the
ground plane and then measure the
following voltages:
Emitter of Q1 .......................... +0.95V
Emitter of Q2 ............................ +0.5V
Emitter of Q3 ...............................+1.1
Emitter of Q4 ............................ +4.7V
Base of Q7 ................................. +4.0V
TP8 ............................................ +4.6V
In each case, the voltage should
be within about ±10% of the value
noted above. It will depend on the
precise value of the supply voltage,
the resistor tolerances and the individual gains of the transistors. If the
voltages are quite different from the
values listed above, then you should
investigate why.
By the way, these voltages are “no
signal” voltages, because little or no
signal should be picked up by the
input stage and the volume control is
turned down so that there is no signal
going through the amplifier stages.
Naturally, the presence of signals
will alter the voltages, although not
greatly.
July 1993 55
Note that if you take the trouble
to calculate the expected base bias
for each transistor and then subtract
0.65V to get the emitter voltage, you
will find an odd result for the base
bias voltage of Q2. This is because
a major factor in its bias condition
is the detector diode D1. This has a
static forward voltage of 0.2V and this
effectively “loads down” the voltage
at the emitter to about 0.5V.
You can also measure the current
drain now. This can be done by connecting your multimeter (switched to
a low current range) across the on/
off switch. If your multimeter has
automatic polarity switching, you
don’t have to worry about how this
connection is done. If your meter
doesn’t have auto polari
ty, connect
the positive probe to the battery side
of the switch and the negative probe
to the other side. With the switch set
to OFF, the current through the meter
should be less than 10 milliamps. If
the current is substantially more, you
probably have a fault.
Note that there is a risk in this
procedure of connecting your multimeter across the on/off switch. If
one side of the multimeter shorts to
the groundplane, you could damage
your meter or, at the very least, blow
its internal fuse.
A safer way of monitoring the current drain is to connect a 1Ω resistor
in series with the positive lead to the
battery holder. This done, use your
multimeter to monitor the voltage
Fig.3: this diagram shows the
locations of the antenna & oscillator
trimmer adjustments on the tuning
gang.
across the resistor. For example, if the
voltage reading is 9mV, (9 millivolts)
then by Ohm’s Law, the current will
be 9mA (9 milliamps)
Aligning the IF stages requires the
injection of a 455kHz signal into the
front end of the circuit. Connect an
RF oscillator, set to 455kHz, through a
.001µF ceramic capacitor to test point
TP1. If you build the test oscillator
described later in this article, you
will not need the .001µF capacitor.
Ideally, you should disable the local
oscillator by connecting a short lead
between the collector of Q1 and test
point TP2 but in practice, it doesn’t
seem to matter.
Connect your multimeter (set to
read DC volts) between test point
TP3 and ground. Set the generator
to give an RF signal output of about
1mV. Now the idea is to adjust each
of the slugs in the IF transformers in
turn for a minimum voltage on test
point TP3. What happens is that as
you adjust the slugs, the gain of the
IF stages improves and the signal fed
to the detector diode (D1) increases.
The detector diode rectifies the IF
signal and so as the signal increases,
the negative voltage produced by the
detector increases. Hence, the voltage
at test point TP3 decreases.
If you want to look at it another
way, you will be adjusting the slugs
for a null voltage at TP3. If you have
an analog multimeter, you will find
it more suitable for this task than a
digital meter since you can judge the
centre of the null more easily by the
way the pointer swings back and forth
as you tweak each slug.
Oscilloscope method
If you have access to an oscilloscope, you can connect it to TP5 and
observe the IF signal directly. Now, as
you adjust the slugs, you will see the
CAPACITOR CODES
❏
❏
❏
❏
Value
IEC Code
.022µF 22n
.01µF 10n
.0047µF 4n7
EIA Code
223
103
472
RESISTOR COLOUR CODE
❏
❏
❏
❏
❏
❏
❏
❏
❏
❏
❏
❏
❏
❏
❏
❏
No.
1
1
1
1
1
1
1
1
1
1
2
2
2
1
2
56 Silicon Chip
Value
1.2MΩ
1MΩ
820kΩ
56kΩ
47kΩ
39kΩ
27kΩ
12kΩ
10kΩ
4.7kΩ
3.3kΩ
2.2kΩ
1kΩ
470Ω
100Ω
4-Band Code (1%)
brown red green brown
brown black green brown
grey red yellow brown
green blue orange brown
yellow violet orange brown
orange white orange brown
red violet orange brown
brown red orange brown
brown black orange brown
yellow violet red brown
orange orange red brown
red red red brown
brown black red brown
yellow violet brown brown
brown black brown brown
5-Band Code (1%)
brown red black yellow brown
brown black black yellow brown
grey red black orange brown
green blue black red brown
yellow violet black red brown
orange white black red brown
red violet black red brown
brown red black red brown
brown black black red brown
yellow violet black brown brown
orange orange black brown brown
red red black brown brown
brown black black brown brown
yellow violet black black brown
brown black black black brown
Setting the tuning range without an RF generator
In the accompanying procedure
for setting oscillator and antenna
tracking we assumed that you had
access to an RF signal generator.
For many constructors, this won’t be
the case and they will have to rely
on broadcast signals at the top and
bottom of the broadcast band.
However, this poses something
of a “chicken & egg” situation. How
do you do the tracking adjustments
if you cannot receive the signals?
In most cases, you should be able
to readily receive a signal at or
near the bottom of the broadcast
band, especially at night. However,
picking up a signal at the top end
of the band might not be anywhere
near as easy.
A solution to this problem is available if you have another AM radio.
How’s that again? Well, as you now
know, every superhet radio has a
signal increase or decrease. Adjust the
slugs for the best possible signal amplitude. Note that if there is a tendency
for clipping of the signal at TP5, just
reduce the signal input from your RF
oscillator.
local oscillator and for an AM broadcast receiver this oscillator will be
455kHz above the tuned frequency.
There
fore, you can use the local
oscillator in your other AM radio to
set the tracking adjustments at the
top of the band.
The method to follow is this: place
the ferrite rod of the AM Radio Trainer
near the antenna rod of your other
AM radio (this will usually be at the
top of the case). Rotate the tuning
knob of the AM Radio Trainer fully
clockwise to tune to the top of the
band. Tune your other AM radio to
1165kHz or as close to this figure
as you can.
As you do so, you should be able
to hear a faint heterodyne whistle
from the speaker of the AM radio.
Now proceed to peak the antenna
and oscillator circuits as described
in the article.
These adjustments ensure that
the RF input circuit and the local
oscillator cover the correct range of
frequencies so that you can tune over
the broadcast band. Ideally, you need
an RF signal generator to do this task.
If you don’t have access to one, you
will have to rely on tuning stations
at the top and bottom of the band. In
Australia, the broadcast band is specified as 531-1602kHz, so to be sure
of covering this band, it is normal to
make a radio tune slightly more, say
525-1620kHz.
Let’s first proceed on the basis that
you have an RF signal generator. Set
it to 525kHz and rotate the tuning
knob fully anticlockwise. This sets the
plates of the tuning gang “in mesh”
which is the maximum capacitance
condition, for the low frequency end
of the band. Now adjust the slug in the
oscillator coil for maximum loudness
of the signal via the speaker, or for
maximum signal amplitude at TP5, if
you have an oscilloscope.
Fig.4: this is the waveform that will
appear at test point TP5 during
alignment if you are using a signal
generator modulated at 400Hz.
Fig.5: this 1kHz sinewave shows the
crossover distortion nicks which will
be present when the quiescent current
in the audio output stage is zero.
Tracking adjustments
Now rotate the tuning knob so that it
is fully clockwise. Set your RF signal
generator to 1620kHz. Tune the adjustment screw on the back of the tuning
gang labelled “oscillator trimmer” (see
Fig.3) for maximum signal amplitude,
as before.
Rotate the tuning knob fully anticlockwise and redo the oscillator coil
slug adjustment again at 525kHz. This
done, go back to the top of the band
at 1620kHz and adjust the oscillator
trimmer again. These adjustments
need to be done a number of times as
the top adjustment affects the bottom
adjustment and vice versa.
You have now adjusted the oscillator range so that the broadcast band
can be tuned in. As a point of interest,
the oscillator will now be tuned over
the range 980-2075kHz.
Now you need to adjust the ferrite
rod coil and antenna trimmer (on
the back of the tuning gang). Set the
tuning knob fully anticlockwise and
set the RF signal generator to 525kHz,
then move the coil along on the ferrite rod until the signal amplitude is
at a peak. Now set the RF generator
to 1620kHz and turn the adjustment
screw on the back of the tuning gang
labelled “antenna trimmer” (see
Fig.3) until you peak the incoming
signal again.
You should now repeat these adjustments for the optimum response.
When this is done, the ferrite rod coil
should be fixed in place by melting a
little candle wax over one end.
That completes the alignment of the
AM Radio Trainer.
Quiescent current
All that remains to be done is to
set the quiescent current by means
of trimpot VR2. By selecting a value
Fig.6: this is the waveform from the
calibration oscillator shown in Fig.7.
The hash on the waveform is the
residual 3.58MHz harmonic content.
July 1993 57
A Crystal Controlled IF Generator
4.7k
1.5k
4.7M
+9V
If you can’t lay your hands
0.1
on an RF signal generator to
0.1
do the alignment for your
16
AM Radio Trainer, then you
4011
14
12
.001
can build this crystal con4.7k
4.7k
IC2
6 4.7k
11 10
5
8
1
3
4
10
4040
IC1d
trolled IF generator board. It
IC1a
IC1b
IC1c
ö8
13
OUTPUT
6
9
2
is based on a standard Amer470pF
470pF
470pF
7
1.5k
11
8
ican 3.579545MHz colour
4.7M
burst crystal. When divided
by 8, you end up with a freX1
3.579MHz
quency of 447.4kHz. This is
within 2% of 455kHz and is
22pF
22pF
probably more accurate than
CALIBRATION OSCILLATOR
you would obtain by setting
a typical RF generator to
Fig.7: the circuit divides the output from a 3.58MHz crystal oscillator by
455kHz.
eight & then filters it to provide a sinewave at 447.4kHz.
Three CMOS gates of a 4011
OUTPUT
quad gate package are connected
in series and the 3.58MHz crystal
0.1 470pF .001
0.1
9V
GND
connected between input and
IC2
IC1
output via a 1.5kΩ resistor. The
4040
4011
gates are biased into the linear re1
1
22pF
4.7k
gion with the 4.7MΩ resistor and
470pF
X1
the output is a square wave. This
22pF
4.7k
470pF
is buffered by the fourth gate of
the 4011 which then drives IC2, a
4040 12-stage binary counter. The Fig.8: the parts are all mounted on a small PC board coded 06107931.
divide-by-8 pin of the 4040 is then
used as the output.
strip. The final output is a sinewave
followed by the capacitors and ICs.
A third order low-pass RC filter
with an amplitude of about 35mV
Next mount the crystal and the
then removes the harmonics and
peak-to-peak into a 10kΩ load.
PC stakes. Lastly, the battery clip
reduces the amplitude to a level
leads can be soldered in.
Construction
suitable for injecting into the IF
In operation, this oscillator needs
Check the board carefully for
to run from a fresh 9V battery, as
shorts and breaks in the tracks.
it drops in frequency below about
This done, install the resistors first,
8.5V or so.
PARTS LIST
1 PC board, code 06107931,
88 x 30mm
1 9V battery clip
1 9V alkaline battery
2 alligator clips
Semiconductors
1 4011 quad 2-input NAND
gate (IC1)
1 4040 12-stage binary ripple
counter (IC2)
Capacitors
2 0.1µF 63VW metallised
polyesters
1 .001µF ceramic
3 470pF ceramic
2 22pF ceramic
Resistors (0.25W, 1%)
1 4.7MΩ
1 1.5kΩ
3 4.7kΩ
58 Silicon Chip
This view shows the fully-assembled alignment oscillator. Note that it should
be powered from a fresh 9V battery, as it drops in frequency below about 8.5V.
Connections to the AM radio are made via alligator clips.
Acknowledgement: our thanks
to Bob Barnes of RCS Radio Pty
Ltd for producing the prototype
screen printed boards. RCS Radio
can supply the board in two versions: a standard phenolic board
with the circuit screen-printed in
black on the topside, or the deluxe
board which is screen printed in
two colours (white cir
cuit on a
deep blue background). The code
number is 06106931. The standard board is available for $19.90
and the deluxe board is $24.90.
Post & packing is $2.00. Contact
RCS Radio Pty Ltd, at 651 Forest
Road, Bexley, NSW 2207. Phone
(02) 587 3491.
The sensitivity of the receiver can be improved by mounting the ferrite rod up
off the board using a plastic bracket. The reason for doing this is that the copper
pattern on the board substantially de-sensitises the antenna.
of 100Ω for this trimpot, we have
deliberately restricted the range of
adjustment. This has been done for
safety’s sake because if the range of
adjustment was larger, it would be
possible to destroy one or both of the
output transistors, because of excessive quiescent current.
The best way to adjust the quiescent
current is to feed a sinewave modulated signal into the front end of the
radio from an RF signal generator.
Connect an oscilloscope to the output
at test point TP8 and adjust the volume
control for a signal amplitude across
the speaker of about 2V or 3V peak to
peak. At this stage, VR2 should still
be fully anticlockwise
If you now have a look at the signal
on the scope screen, you will see the
classic sinewave with crossover distortion – notches in the waveform at
the crossover point (see Fig.5). Now
if you rotate VR2 you will see the
crossover nicks disappear from the
waveform and, at the same time, the
sound will become cleaner. Rotating
VR2 to reduce the crossover distortion will not increase the current by
much, by no more than a milliamp,
but it will make a big difference to
the sound quality.
By the way, you should measure the
current drain of the radio while you
are adjusting the quiescent current
with trimpot VR2.
Typically, the current drain of the
radio at 9V should be less than 10
milliamps when the volume control
is at minimum setting (ie, no signal
through the audio amplifier stages).
With the volume control well advanced to make the radio quite loud,
the current drain may be 40 milliamps
or more.
You can also easily measure the
current drain of the radio without the
audio stage. Just plug an open-circuit
3.5mm jack into the headphone socket.
This disconnects the loudspeaker and
causes the amplifier to latch up and
thus draw negligible current. Under
Fig.9: this is
the full-size
PC pattern for
the calibration
oscillator.
these conditions, the rest of the radio
circuit will draw around 4mA or less.
Mounting the ferrite rod
By now, you will have tried out
the radio and possibly found that its
performance leaves something to be
desired, even though you should be
able to tune in stations right across
the broadcast band. You will find lots
more stations at night, provided you
are not attempting to listen to your
radio close to a TV set or computer.
Both cause loud whistles across the
dial.
There is a further step you should
take to get the best out of your radio
and that is to mount the ferrite rod
antenna up off the board by at about
25mm. The reason for doing this is
that the copper pattern of the PC board
substantially de-sensitises the antenna
– in fact, any metal will do this.
To mount the antenna rod off the
board by the requisite amount, we
made up a rightangle bracket out of
scrap plastic. This was secured to the
PC board with two screws and nuts,
while the rod was secured to the brack
et with two small plastic cable ties.
Mounting the antenna rod in this
way will make a substantial difference
to the sensitivity. You should repeat
the peaking procedure for the ferrite
rod coil and antenna trimmer.
Notes & Errata
The trimpot specified for VR2 in the
audio amplifier output stage should
be 100Ω, not 200Ω as specified in the
SC
first article.
July 1993 59
Last month, we
introduced the Digital
Logic Analyser &
gave the circuit
details. This month,
we describe the
construction & the
software installation.
Windows-based
digital logic analyser; Pt.2
By JUSSI JUMPPANEN
Despite the apparent circuit complexity, this project is very easy to
build. All the circuitry is contained on
the two double-sided PC boards and
these feature plated-through holes,
component overlays and solder masks.
The main thing to watch out for is that
all parts are correctly installed the first
time. Once you have soldered a part
into a plated-through board, it is quite
difficult to remove.
60 Silicon Chip
The easier of the two boards is the
internal XT bus card which uses just
five ICs plus a few other parts. None
of these ICs require sockets so the first
step in the construction is to solder
them all in place. Make sure that each
IC is correctly positioned and that it
is aligned as shown in the overlay
diagram – see Fig.7.
Once the ICs have been soldered
into place, the 8-bit DIP switch, resis-
tors and decoupling capacitors can
be added. Finally, the female DB37
connector can be soldered into place
and the slot bracket attached to the
card – see photo in Pt.1.
Make sure that the DB37 connector
used is a female type and that it is a
long version so that it protrudes the
correct amount beyond the end of the
board. If a short DB37 connector is
used, the socket will not be flush with
1
1
0.1
U1 74LS688
U4 74LS245
J2
DB37/F
A8
A9
A10
A11
A12
A13
A14
A15
ON
S1 SW-DIP8
0.1
0.1
U3 74LS04
0.1
Logic analyser board
1
U5 74LS244
0.1
The external logic analyser card is
a little more complicated to build as
it uses some 29 ICs in total. The first
step is to install IC sockets for IC1,
IC2, IC10, IC13 & IC22 – see Fig.9. Do
not use sockets for the remaining ICs
however, as they will only add to the
expense of the project.
Once the sockets have been installed, the remaining ICs can be
installed by soldering them directly
to the PC board. As before, take care
to ensure that each IC is placed in
its correct location and is oriented
correctly. This done, the remaining
components can be installed. These
include the resistors, capacitors and
crystal. A 16-pin IDC socket will also
have to be soldered into the IDC16
location.
A point to note here is that although
the PLL (IC13) is a 74HC4046, not all
74HC4046s are the same. A Philips
device will be supplied with the kit
but a National Semiconductor device
can also be made to work simply by
changing a few component values –
see Table 4.
At this point, the DB37 expansion
port connectors can be added. A male
connector is used for the input socket,
while a female connector is used as the
output socket.
The final stage in the construction
involves the wiring of the channel
inputs and the external clock. The
channel inputs are very simple to wire
because IDC connectors are used. The
external clock wiring (to the input
socket and switch) is slightly more
difficult because each lead has to be
soldered independently, but fortunately there are only six connections
to make.
The external board can now be
mounted in the instrument case. To
do this, the front and rear panels need
to be drilled to match the supplied
templates. The rear panel is then fastened to the DB37 connectors, while
the DB15 channel input connector,
external clock input RCA jack and
internal/external clock switch are
attached to the front panel.
All that remains now is to wire the
nine probe clips (eight input channels
plus ground) to the matching DB15
plug connector. Be sure to connect
each input to the pin number des-
1
1
U2 74LS02
1k
1k
1k
1k
1k
1k
1k
1k
the PC case when the card is installed
in the bus slot.
J1 IBM XT BUS
Fig.7: parts layout for the internal bus card. DIP switch S1
(top, left) is used to partially set the hardware address.
Fig.8: the hardware address entered in the software must match the address set
by the DIP switches on the internal & external cards – just click Edit/Hardware
to bring up the above display. The default is 0F30; change this only if necessary.
ignated on the circuit diagram and
use a black probe clip for the ground
connection.
Hardware installation
The first step in the installation is
to set the DIP switches on the two PC
boards to match the required I/O address. During testing, the I/O location
0F30 was used successfully on a machine with two serial ports, a printer
port, a games port and a fax card. It
is recommended that this location be
used for your initial tests.
Table 5 shows the DIP switch settings on the two boards for various
I/O addresses. Note that, because of
the inverting nature of the circuit, a
logic 0 is set by turning the DIP switch
on, while a logic 1 is set by turning the
DIP switch off.
Thus, to set an address of 0F30,
turn DIP switches A15-A12 ON and
A11-A8 OFF on the internal card; and
July 1993 61
OUTPUT
INPUT
1
1
IC8 74LS193
IC9 74LS193
IC19 74LS193
33pF
IC7 74LS193
1
0.1
0.1
0.1
0.1
0.1
0.1
XTAL
33k
1
IC18 74LS125
0.1
1
1
0.1
1k
GND
IC12 74LS74
IC20 74LS193
1
0.1
0.1
EXT
CLOCK
120
0.1
U103 74LS245
0.1
U104 74LS245
0.1
1
IC13 74HC4046
1
U102 74LS138
1k
U101 74LS138
1k
1
U100 74LS85
A4
A5
A6
A7
ON
1
1
IC15 74LS04
1
1k
470
1k
S100
SW-DIP4
470
1
0.1
S1
4.7uF
1
IC17 74LS374
IC4 74LS374
IC16 74LS374
IC11 74LS245
IC10
6116
0.1
0.1
0.1
0.1
0.1
1
1
IC22 74HC4040
1
IC24 74LS08
1
IC14 74LS32
0.1
1
0.1
IC23 74LS08
IC6 74LS85
0.1
0.1
IC5 74LS08
IC21 74LS193
1
1
0.1
0.1
0.1
0.1
0.1
Fig.9: parts layout for the external PC board. Install IC sockets for IC1, IC2,
IC10, IC13 & IC22 but not for the other ICs. A male DB-37 connector is used for
the input socket, while a female connector is used for the output socket.
turn A7-A6 ON and A5-A4 OFF on the
external card. The remaining address
locations (A3-A0) are fixed – see
Table 5.
The internal card can be inserted
into any spare XT or AT bus slot (make
sure that the power is off). At this
point, the computer can be powered
up and checked to ensure that it boots
as normal. If the machine starts but
locks up, the card is probably using
an I/O location required by another
device. If so, turn the machine off,
change the I/O address to another
location (eg, to 1030, 0E30 or 0D30)
and try again.
IC2 74LS14
1
1
SENSORS
IDC16
1
1
IC1 74LS14
1
1
IC3 74LS374
1
0.1
into a directory called dla (you have
the option of changing this to another name) and create the relevant
program group. After that, the program can be run by double clicking
TABLE 4
Software installation
An installation program on the disc
supplied with the kit makes this job
a breeze. This program must be run
from within Windows.
To install the software, insert the
disc into drive A:, then choose the
FILE RUN menu option and type A:\
install. This will install the software
IC13
Philips 74HC/
GCT4046
NS 74HC4046
C200
2200pF
33pF
C201
0.47µF
4.7µF
R200
10kW
1kW
R202
100W
120W
R203
10kW
33kW
Table 2
Address
Internal XT Card
External Card
Fixed
A15
A14
A13
A12
A11
A10
A9
A8
A7
A6
A5
A4
A3
A2
A1
A0
1030H
0
0
0
1
0
0
0
0
0
0
1
1
0
x
x
x
0F30H
0
0
0
0
1
1
1
1
0
0
1
1
0
x
x
x
0E30H
0
0
0
0
1
1
1
0
0
0
1
1
0
x
x
x
0D30H
0
0
0
0
1
1
0
1
0
0
1
1
0
x
x
x
Note 1: 0 = DIP Switch ON; 1 = DIP Switch OFF due to the inverting nature of the circuitry.
Note 2: an "x" means software controlled addressing.
62 Silicon Chip
Above: the IDC socket on the external
board is wired to a DB15/F connector
on the front panel via a ribbon cable.
The front panel also carries the DPDT
clock source switch & an RCA socket
for the external clock input.
on the Digital Logic Analyser icon.
With the software running, click the
Edit/Hardware menu option to set the
hardware address to match the address
previously set by the DIP switches (the
default is 0F30; change this only if
necessary). The hardware addressing
can then be easily checked by toggling
the external/internal clock switch on
the front panel.
As the switch is toggled, the clock
status field at the bottom right of the
screen should also toggle to match
the switch setting. If the status does
not change, this probably means that
the actual hardware address does not
match the software hardware address.
If this fails to fix the problem, check
the switch wiring. The voltage on
pin 9 of IC18 should change from 0V
to 5V as the switch is toggled. If no
voltage change is observed it means
The nine probe clips (eight input channels plus ground) are wired to a DB15
plug connector that matches the socket on the front panel. Be sure to connect
each input to the pin number designated on the circuit diagram.
that the switch is wired incorrectly.
If the voltage changes but is not registered by the software, the address
must be wrong.
When the internal/external clock is
correctly registered by the software,
the system is correctly configured and
the setting will not need to be changed
again. The project can now be tested
for correct operation by first connecting the various channel probes to
any suitable TTL clock circuit (don’t
forget to connect the ground probe).
Fig.12 shows a suitable test circuit.
July 1993 63
Where to buy the kit
Fig.10: the frequency & period of a waveform can be measured by clicking the
right mouse button at the start of a cycle & by holding down the SHIFT key &
clicking the right mouse button at the end of the cycle.
Fig.11: the Search Level Selection dialog box lets you search for particular data
samples & trigger levels. A channel can be marked high, low or don’t care. All
individual channel search criteria must be met for the search to succeed.
The next step is to program the
triggering options and the sample
frequency. To program the triggering
options, simply select the Edit/Trigger
menu to bring up the Trigger Selection
menu (or double click the left mouse
button in the display area). The sample frequency can be set anywhere
between 100kHz and 6MHz (in 100kHz
steps) by clicking on the UP & DOWN
buttons located towards the bottom
left of the display.
After that, it’s simply a matter of
clicking on the Start button. If the
sample is not completed within one
second, click on the Abort button,
reprogram the trigger value and try
again. If all is OK, the screen should
64 Silicon Chip
+5V
16
7
5
11
27k
2.7k
4
6
10
IC1
4060
14
33pF
13
9
15
CLOCK
FREQUENCY
200kHz
1
12
Q4
Q5
Q6
Q7
Q8
Q9
Q10
Q12
8
Fig.12: this simple test circuit
generates eight spot frequencies
ranging from 12.5kHz to 48.8kHz.
The kit is offered in three formats:
(1). A complete kit consisting of all
the parts as listed – price $215.00
plus $10.00 p&p.
(2). A complete kit of all parts except
for the case – price $185.00 plus
$5.00 p&p.
(3). Two double-sided PC boards
(with screened overlays) plus software – price $90.00 plus $5.00 p&p.
To order, send cheque or money
order to Jussi Jumppanen, PO
Box 697, Lane Cove 2066, NSW.
Phone (02) 428 3927. Please specify
whether a 5¼-inch or 3½-inch disc
is required.
Note: copyright of the two PC boards
for this project is retained by the
author.
refresh and the results of the sample
will be displayed.
A context-sensitive help system is
provided and this can be accessed
at any time by clicking on the Help
menu option. For example, if the
Help button is clicked in the Trigger
selection menu, an explanation of the
Edit Trigger Command will be given.
Once you have sample waveforms
displayed, you can try out some of
the other features of the software. For
example, you can examine the effects
of changing the trigger selections and
the timebase option. The software
also lets you search for particular data
samples and trigger levels. And if you
don’t like the display colours or the
line thickness, you can edit these to
suit your requirements.
You can also make accurate frequency and period measurements
on individual waveforms. To do this,
place the cursor at the beginning of
a waveform cycle and click the right
mouse button, then move the cursor to
the end of the cycle and click the right
mouse button while holding down the
SHIFT key. The frequency and period
of the waveform can now be read from
the data bar.
Finally, readers should note that the
4MHz crystal was left off the main circuit diagram (Fig.4). This crystal goes
between pin 13 of IC15f & pin 10 of
IC15e. Several pin numbers were also
left off: the input of IC15d is pin 9; the
input of IC15e is pin 11; and the input
SC
of IC15f is pin 13.
PRODUCT SHOWCASE
Panasonic GPS
receiver
12VDC to 240VAC
inverter
This compact 12V to 240VAC inverter will operate most low powered
electrical equipment such as VCRs, TV
sets, fans, computers, small kitchen
appliances and in fact, almost any
mains-powered appliance with a
power consumption of up to 160 watts.
No-load power consumption is a
mere 1.2W while the output surge
capability is 400W. Weight is 1.1kg
and dimensions are 180 x 105 x 60mm.
The inverter is available from all
Dick Smith Electronics stores at $249
(Cat. M-5010). Also available is a 600
watt model at $399 (Cat. M-5000).
Dynalink dish
alignment meter
This dish alignment
meter covers the frequency
range from 900-2050MHz
and it contains a nicad
battery pack, allowing the
LNB (low noise block) of
the dish to be powered directly. The instrument has
a 2-stage MMIC (monolithic microwave IC) amplifier
and internal integrator to
average all signals in the LNB output band and then drive an analog
signal strength meter. It has an
adjustable sensitivity control and
an audio indicator which increases
in pitch as the dish alignment is
improved.
For anyone contemplating dish
installations for either the present
or future pay TV transmissions,
this is an indispensable tool. The
unit comes complete with a 2-metre length of RG-6/U cable with
F connectors, wall charger and
carry case with should
er strap.
The meter can be looped into the
coax feed from a satellite receiver
to verify LNB power consumption
and polarity.
The Dynalink SM-01 Satmeter is
available now for $470.
For further information on this
product and other satellite TV
products, contact Av-Comm Pty
Ltd, PO Box 225, Balgowlah, NSW
2093. Phone (02) 949 7417 or fax
(02) 949 7095.
Panasonic’s KX-G5500 GPS receiver
is a compact receiver which measures
a mere 130 x 65 x 35mm and offers
all the benefits of portability and easy
operation. It’s powered by a long-lasting, rechargeable nickel metal hydride
battery or from a AA alkaline battery
pack (supplied). A lithium battery
serves as a memory backup.
The KX-G5500 comes complete
with external antenna, antenna/DC
adaptor, adjustable mount, carry
case, battery charger and AC adaptor,
and alkaline battery case. The case is
splash resistant and features a backlit
LCD panel so that it can be read in
the dark.
Note: all GPS receivers are subject
to a degradation of position of plus or
minus 100 metres as determined by
the US Department of Defence.
For further information, contact
Panasonic Australia by phoning (02)
986 7400.
Rack mounted
personal computers
Modgraph Inc, well known as a
manufacturer of Super-VGA colour
monitors, now offers a range of
personal computers in a series of
rack-mounted configurations. Intended for applications where high
July 1993 65
Music on hold
for phones
Peter Lacey
has moved
Peter Lacey has moved his
wholesale antenna and instrument
supply business to larger premises
in Frankston. According to Peter,
the company “experienced incredible growth through the aggregation
boom of last year. With a number of
new product opportunities in front
of us, we decided that the cost of
extra space was a small price to pay
to improve service. Some unique
antenna products combined with
our installation background means
we can help technicians achieve
better results from their antenna
work”.
The new address for Peter C.
Lacey Services Pty Ltd is 80 Dande
nong Rd, Frankston, Vic 3199.
Phone (03) 783 2388 or fax (03)
783 5767.
In keeping with the rack mount configuration, the system’s 89-key keyboard
can be mounted on a slide which goes
under the PC, or can be folded over the
screen and disc drives.
For further information, contact
Amtex Electronics, 13 Avon Rd, North
Ryde 2113. Phone (02) 805 0844.
This Austel approved device allows
any phone system to provide music on
hold for incoming callers or outgoing
callers. To place a call on hold you
merely press 8 on a tone or pulse dial
phone. To pick up the call again, press
8 again. The music program may be
from any source such as a tape player
or radio.
The device itself uses US modular
phone plugs and sockets but Telecom
adaptor plugs are also supplied. The
Music-On-Hold adaptor is priced at
$279 while an Austel approved line
isolation transformer is an extra $80.
For further information contact
David Reid Electronics, 127 York St,
Sydney, NSW 2000. Phone (02) 267
1385.
Rotational
speed sensor
8-channel
relay board
resolution colour and PC processing
capabilities are needed in a standard
19-inch rack format, the GX-4500
offers 800 x 600 resolution.
The GX-4500’s Sony Triniton-based
super VGA 8.5-inch diag
onal, flat
screen display is mounted with the
disc drives alongside. There is a choice
of 286, 386 or 486 processors, with two
to five expansion slots and internal
hard disc drives up to 200 megabytes.
66 Silicon Chip
The AX5008 relay and isolated
digital input board plugs directly
into any expansion slot of an IBM
PC/XT, AT or better. The eight SPDT
relays are intended for low power
switching; their contacts are rated
at 3A at 120VAC or 24VDC with a
resistive load.
The eight opto-isolated digital inputs provide 1kV channel to channel
or channel to ground isolation. Their
input impedance is 800Ω. Connections
are made via a 37-way D-type male
connector which is supplied with the
board. For more information, contact
Boston Technology Pty Ltd, PO Box
1750, North Sydney 2059. Phone (02)
955 4765.
The Philips KMI10/1 rotational
speed sensor is claimed to be the first
fully integrated contactless speed sensor to meet all the requirements of the
automotive industry. Features include
accurate measurement down to zero
rpm, an ability to operate at toothto-sensor spacings as large as 2.5mm
and at ambient temperatures as high
as 190°C. These sensors operate with a
wide variety of wheel teeth structures
while a built-in hysteresis in the signal
conditioning circuit makes it immune
to vibrations.
This combination of features suits
the KMI10/1 for use in automotive
applications such as ABS (Anti-lock
Brake Systems), ASC (Anti Slip Control) and engine management systems.
Industrial applications include the
detection of ferrous metals, proximity
detection and current flow detection.
With a very small sensor head and no
requirement for external magnets or
additional components, the KMI10/1
is small and rugged enough to be
integrated into ball-and roller-bearings. Two KMI10/1 sensors operating
together can be used to detect speed
and direction, or to make incremental
measurements.
The KMI10/1 is a 2-terminal device
which operates at fre
quencies from
0-25kHz, producing a pulsed current
output at the tooth frequency. Unlike
inductive sensors, the magnitude of
this pulsed current (7mA in the low
state and 14mA in the high state) is
frequency independent. Only one
low value resistor and capacitor are
required to turn the output current
into a TTL-compatible signal that is
suitable for microcontrollers or other
control logic.
For further information, contact
Philips Components, 34 Waterloo Rd,
North Ryde, NSW 2113. Phone (02)
805 4455.
Vivitar video fader/
audio mixer
Home control system
from Cebus
Now available from CEBus Australia is the HCS II home control
system as featured last year in the
American magazine “Steve Ciarca’s
Circuit Cellar INK”. The HCS II is
a control system which monitors
sensors and controls devices via
the AC power mains. Such systems
have been talked about for many
years as the “intelligent home
concept” but this is the first time
that a dedicated system has become
available.
Essentially, the HCS II transmits
serial data over the AC power line
via special isolating modems. You
York St, Sydney NSW 2000. Phone (02)
267 1385 or fax (02) 261 8905.
Kenwood’s luxury
L-A1 amplifier
Kenwood’s new top of the line L
Series hifi equipment is finished in a
luxurious anodised gold fascia plate
with hand-rubbed rosewood side
panels.
This compact video fader can mix
the sound from three separate sources as well as being able to provide a
smooth fade-in or fade-out of a source
such as a camcorder or VCR. The unit
comes with its own microphone and is
supplied with video and audio leads.
It runs from an external 12V DC plugpack adaptor (not supplied).
The unit retails for $199 and is available from David Reid Electronics, 127
can program the system to control
devices such as lights, heating
systems and so on. The system
uses a program language called
Express and this is supplied on
floppy discs.
Our photo shows some of the
control boards in the system. Not
shown are an LCD board (20 line
display), the appliance module and
modems, and the various cables
which are supplied.
The price is $1442 plus tax
where applicable for an assembled
and tested basic system.
For more information, contact
CEBus Australia, 26 Lambourn Rd,
Watsonia, Vic 3087. Phone (03) 435
1185 or fax (03) 432 1825.
Inside the L-A1 amplifier is a specially developed Super C4 (Super Constant Cascade Circuit) that represents
a major departure from conventional
differential amplifier design. The super C4 circuitry is claimed to reduce
the in-phase noise in much the same
way as the high CMRR (Common Mode
Rejection Ratio) of differential designs
but it produces a much cleaner signal.
continued on page 83
VIDEO
& TV
SERVICE PERSONNEL
TV & VIDEO FAULT LIBRARIES
AVAILABLE AS PRINTED MANUALS $90 EACH + $10 DELIVERY
BOTH MANUALS VIDEO & TV
$155 + $15 DELIVERY
OR AS A PROGRAM FOR IBM COMPATIBLES $155 + $10 DELIVERY
FOR MORE INFORMATION
CONTACT
TECHNICAL APPLICATIONS FAX / PHONE (07) 378 1064
PO BOX 137 KENMORE 4069
July 1993 67
Build this low-cost
quiz game adjudicator
If you’ve ever wanted to risk all the prizes
and go for the cash jackpot, then this is the
project for you. Called the Quizmaster, it
lights a LED & briefly sounds a buzzer to
indicate which of four players pressed the
button first.
By DARREN YATES
Imagine it. You’re sitting down with
two other “brains” in the local Gulargumbone Sale of the Month Championships. You’ve just got to make it
through the 60-seconds “fast money”
and all the prizes are yours –a year’s
supply of toilet paper in your choice
of pastel colours, a $100 gift voucher
at Spud Murphy’s secondhand farm
70 Silicon Chip
machinery depot, all the icecream you
can eat in a week, plus various other
(mainly useless) household supplies.
However, your eyes are firmly fixed
on the cash jackpot which grows by
$2.78 each night.
The compere, in thongs and stubbies, bellows out, “Hey, Raelene!
What’s tonight’s grand total cash bon
anza?” Raelene, regaled in the latest
fashion wear from the local opportunity shop, informs the audience, most of
whom are now asleep with excitement,
“Tonight’s bonanza is $38.75 minus
the cost of the beer. We’ll put the one
minute up on the clock and your time
starts ... now!”
Starting out $4.23 behind your opponent, you charge through the fast
money as if you knew the answers
before the questions were even asked.
It comes down to the last question. You
have to get in first and answer correctly
or you lose the lot.
“What’s the name of Bullhead Jones’
prize pig?” Knowing full well that the
answer is Beethoven, you thrust your
arm towards the heavens, expecting
to be awarded all the prizes.
D5
1N4004
470
16VW
9V
RESET
S5
4
6
100k
12
14
PLAYER 1
S1
3
PLAYER 2
S2
7
PLAYER 3
S3
11
PLAYER 4
S4
15
100k
100k
Q5
BC557
82k
16
100k
100
16VW
47k
10k
3-12V
BUZZER
E
B
5
Q6
BC337 C
B
C
S1
E
1k
S2
S3
S4
R1
IC1
4043
R2
Q2
R3
Q3
Q4
R4
100k
Q1
2
D1
1N914
D4
1N914
D3
1N914
D2
1N914
22k
Q1
BC557
E
B
9
22k
10
22k
1
22k
C
Q2
BC557
B
C
LED1
B
E
C
VIEWED FROM
BELOW
A
K
Q3
BC557
B
E
C
A
A
8
E
K
LED2
A
K
Q4
BC557
B
LED3
A
K
E
LED4
C
K
680
THE QUIZMASTER
Fig.1: the circuit is based on IC1, a 4043 quad RS latch. When one of the PLAYER
buttons (S1-S4) is pressed, the corresponding Q output of IC1 switches low &
turns on its associated PNP driver transistor (Q1-Q4) to light one of the LEDs.
Q5, Q6 & the associated 100µF capacitor are used to drive the buzzer.
Your opponent, whose arm was
broken by a freak and mysteri
ous
accident during the last round, raises
his plastered arm a full second after
your own mighty effort. However, the
compere who unbelievably loses his
glasses just after reading the question,
fails to see your arm rocket upwards
and awards the question and all of the
prizes to your opponent.
And the moral of this sorry tale?
– if the compere had been given a
Quizmaster, this would never have
happened!
Circuit diagram
Let’s take a look at the circuit diagram of the Quizmaster – see Fig.1. As
you can see, it uses a single 4043 IC
(IC1), a buzzer, and a few transistors
and LEDs.
Inside the 4043 are four tri-state
RS flipflops. The reset pins (R1-R4)
are connected to their corresponding
PLAYER buttons, while the set inputs
are tied together and connected to the
RESET button (S5). The circuit detects
which of the four PLAYER buttons is
pressed first and disables the other
three buttons until the RESET button
is pressed.
When S5 is pressed to start the game,
the four set inputs are pulled high and
so the Q1-Q4 outputs at pins 2, 9, 10
& 1 also go high. These outputs drive
PNP transistor stages Q1-Q4 via 22kΩ
current limiting resistors. Thus, when
the RESET button is pressed, transistors Q1-Q4 will all be off and none of
the LEDs will be lit.
IC1’s Q1-Q4 outputs also drive a
4-input AND gate made up of diodes
D1-D4. When all four Q outputs are
high, the output of the AND gate is
also high and thus Q5, Q6 and the
buzzer are all off. This high is also
applied to the commoned side of the
four PLAYER buttons.
Normally, the four reset inputs on
IC1 are held low by 100kΩ pull-down
resistors. However, if one of the player buttons is now pressed, the high
output from the AND gate is fed into
the corresponding reset input and
this causes the associated Q output
to go low. This low then turns on the
associated PNP driver stage to light
the correct LED.
At the same time, the output of the
diode AND gate goes low and this
prevents any of the other switches
The four PLAYER
switches are housed
in discarded 35mm
film canisters. Mount
each switch on the lid
of its canister & feed
the connecting lead
out through a hole
drilled in the bottom.
July 1993 71
10k
PARTS LIST
82k
PLAYER 4
D5
PLAYER 3
9V BATTERY
470uF
IC1
4043
Q6
1
D1
22k
22k
22k
22k
D2
D3
D4
PLAYER 1
RESET
Q1
K
100k
LED1
DC BUZZER
1k
Q2
K
LED2
100uF
Q5
47k
680
100k
100k
100k
100k
PLAYER 2
Q3
K
Q4
K
LED3
LED4
Fig.2: the parts layout on the PC board. Be sure to use the correct transistor type
at each location & take care with the orientation of polarised components. The
pin connections for the transistors & LEDs are shown on Fig.1.
from resetting its associated flipflop.
This means that the remaining player
switches are effectively disabled.
Transistors Q5 and Q6 form a simple monostable circuit which drives
the DC buzzer. It works like this.
When the output of the diode AND
gate switches low (ie, when one of
the PLAYER buttons is pressed), PNP
transistor Q5 turns on and provides
base current for Q6. This turns Q6 on
and so the buzzer sounds.
The 100µF capacitor between Q5’s
emitter and the positive supply rail
now charges via the 1kΩ collector
resistor. As it charges, the current
through Q5 tapers off and the voltage
devel
oped across the 1kΩ resistor
drops. Eventually, after about 0.2s,
it drops below 0.6V and Q6 and the
buzzer turn off.
This means that the buzzer only
gives a brief burst of sound, to indicate that one of the players has
responded. The buzzer then remains
off but the relevant indicating LED
remains on to show which player
pressed his/her button first. Pressing
the RESET button now resets IC1 and
turns the LED off again to rearm the
circuit.
Power for the Quizmaster is supplied by a 9V battery via reverse-polarity protection diode D1. The circuit
draws only a few microamps of current
while in reset mode, so there’s no need
for a power switch.
Construction
All the parts for the Quizmaster,
except for the five pushbutton switch
es, are mounted on a PC board coded
08106931 and measuring 144 x 87mm.
Fig.2 shows the parts layout on the
board.
Begin the board assembly by
installing the 10 wire links. These
should all be as straight as possible,
to avoid possible shorts to other
components. If necessary, you can
straighten the link wire by clamping
one end in a vice and then stretching
it slightly by pulling on the other end
with a pair of pliers.
The resistors, capacitors, diodes
and semiconductors can now all be
1 PC board, code 08106931,
144 x 87mm
1 3-12V DC buzzer
1 9V PC-mount battery holder
5 PC-mount 3.5mm sockets
5 3.5mm plugs
4 rubber feet
5 plastic 35mm film canisters
5 normally-open momentary
pushbutton switches
1 10-metre length of light-duty
speaker cable
1 9V battery
4 self-adhesive rubber feet
2 3 x 10mm-long machine
screws & nuts
3 8BA machine screws & nuts
Semiconductors
1 4043 quad RS latch (IC1)
5 BC557 PNP transistors
(Q1-Q5)
1 BC337 NPN transistor (Q6)
4 1N914 signal diodes (D1-D4)
1 1N4004 silicon diode (D5)
Capacitors
1 470µF 16VW electrolytic
1 100µF 16VW electrolytic
Resistors (1%, 0.25W)
5 100kΩ
1 10kΩ
1 82kΩ
1 1kΩ
1 47kΩ
1 680Ω
4 22kΩ
mount
ed on the board. Be sure to
install the correct transistor at each
location and check that the IC, transistors and capacitors are correctly
oriented. The accompanying table
shows the resistor colour codes but
it’s also a good idea to check them on
a multimeter as some of the colours
can be difficult to decipher.
RESISTOR COLOUR CODE
❏
❏
❏
❏
❏
❏
❏
❏
No.
5
1
1
4
1
1
1
72 Silicon Chip
Value
100kΩ
82kΩ
47kΩ
22kΩ
10kΩ
1kΩ
680Ω
4-Band Code (1%)
brown black yellow brown
grey red orange brown
yellow violet orange brown
red red orange brown
brown black orange brown
brown black red brown
blue grey brown brown
5-Band Code (1%)
brown black black orange brown
grey red black red brown
yellow violet black red brown
red red black red brown
brown black black red brown
brown black black brown brown
blue grey black black brown
corresponding player numbers. This
labelling can be done using transfer
lettering or a suitable marker pen.
Testing
The leads from the momentary contact pushbutton switches are terminated
with 3.5mm plugs & these go to matching 3.5mm sockets on the PC board.
Once these components have been
mounted, install the battery holder,
the buzzer and the five 3.5mm sockets. The battery holder is secured to
the PC board using three 8BA screws
and nuts, while the buzzer is secured
using two 3mm x 10mm screws and
nuts, with two additional nuts used
as spacers. You will have to drill two
mounting holes in the PC board to suit
your particular buzzer.
The five pushbutton switches are
housed in discarded 35mm film
canisters – see photo. All you have
to do is drill a hole in the lid of each
canister to accept the switch, plus an
exit hole in the base of the canister for
the switch lead.
The switch leads can each be run
using two metres of light-duty speaker cable. These leads are terminated
with 3.5mm mono plugs to match the
sockets on the PC board.
Finally, the PC board can be fitted
with four rubber feet and the input
sockets and LEDs labelled with their
To test the unit, plug in the external
switches and install a 9V battery. The
circuit should now fire up in one of
two ways – either with all the LEDs
lit or with all the LEDs off. This may
sound a bit imprecise but the initial
state of the circuit will depend on the
state of the flipflops inside IC1.
If all the LEDs are on, check that they
all go out when the RESET switch is
pressed. Now check that the buzzer
briefly sounds and that the appropriate
LED comes on when one of the PLAYER
switches is pressed. The remaining
PLAYER switches should now have
no affect on the circuit and the LED
should remain on until the RESET
switch is pressed again.
If it doesn’t work, first check that all
components are correctly positioned
and that there are no missed solder
joints or solder splashes on the copper
side of the board. This done, check that
pins 5 & 16 of IC1 are at +9V when the
battery is installed.
If one of the LEDs fails to light, check
its associated driver transistor and
check that the LED has been correctly
oriented. Similarly, if the buzzer fails
to sound, check the circuit around
transistors Q5 and Q6. In particular,
note that Q5 is a PNP type while Q6
is an NPN type so don’t get them
SC
mixed up.
Fig.3: this is the full
size pattern for the
PC board. Check
the etched board for
track defects before
mounting any of the
parts.
July 1993 73
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Rod Irving Electronics Pty Ltd
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Rod Irving Electronics Pty Ltd
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Rod Irving Electronics Pty Ltd
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Rod Irving Electronics Pty Ltd
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Rod Irving Electronics Pty Ltd
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Rod Irving Electronics Pty Ltd
REMOTE CONTROL
BY BOB YOUNG
Unmanned aircraft: current
models in service
Over the last decade, unmanned aircraft have
come into their own & this was demonstrated
to great effect in the Desert Storm campaign
in the recent Gulf War. Some of these craft are
little more than model aeroplanes but they are
extremely effective nonetheless.
In last month’s column, we looked
at the development of unmanned aircraft (UMAs) over the past 80 years
and noted the very fine line between
UMAs and primitive guided missiles.
This distinction is even closer when
the modern glide bomb (smart bomb) is
considered. With this we are virtually
back to the MISTELN concept discussed last month in which a mother
ship carries an unmanned fighter to
the target vicinity, launches the fighter
and guides it to the target.
This concept was used by the Germans in WWII with limited success.
But the smart bomb was used in the
Iraq campaign, again guided from
a mother ship, this time with great
success. Hardened aircraft shelters (or
HAS) proved totally ineffective against
these devastating weapons and once
again the shape of warfare has shifted
and moved on to the next concept.
With this blurring of lines of demarcation we are faced therefore with
the need to define what we mean by
the term RPV, the new buzzword for
UMAs. Remotely Piloted Vehicles
(RPVs), as the term suggests, covers
any vehicle capable of being controlled
The Bell Eagle Eye is a tilt-rotor UAV currently under development by the US
Department of Defence. It is to be powered by a 313kW turboshaft engine.
80 Silicon Chip
at a distance from the actual operator. My full-size remotely controlled
Volkswagen 1600TLE was strictly
speaking an RPV. Thus, the term UAV
(Unmanned Aerial Vehicle), another
modern buzzword, is probably the
more correct term for use in this series
of articles.
There is a further general agreement
on the distinction between the various
types of UAVs and these fall broadly
into aerial targets, the aerial component of a complex battlefield system
and finally, guided weapons.
As we have already noted, the days
when UAVs were of value only for
target practice have long since passed
but these still comprise a major grouping and probably the missile target is
the most sophisticated of this group.
The Australian made Jindivik is one
of the most successful of this class
of UAVs. However, it is the middle
group which forms the basis of this
month’s article.
It is the value of the UAV as a force
multiplier that has become increasingly recognised since the Vietnam
War; in other words, its value as a
component in a complex battlefield
system. This outlook was significantly enhanced as a result of the Israeli
experiences and further as a result of
the Iraq War. These events showed a
growing need for military equipment,
especially in the areas of surveillance,
electronic warfare and post-strike
damage assessment, that does not require a human crew to be exposed to
enemy weapons. Here we have a very
sophisticated class of UAVs capable
of a multitude of tasks which in many
cases have great commercial potential. One idea which has intrigued
STAND-OFF JAMMERS
RPV ON STATION
OVER TARGET AREA
OUTGOING
RPV
TANKS
SURVEILLANCE SENSOR DATA
AND HIGH RATE POSITION FIX
POSITION
FIX
RETURNING
RPV
FORWARD LINE OF OWN TROOPS
LAUNCH
AREA
INITIAL
ACQUISITION
POSITION
FIX
GROUND CONTROL STATION
(GCS)
PUMICE
GROUND DATA TERMINAL (GDT)
me for many years is the concept of a
very fast courier service using small
UAVs for cross city delivery of small
parcels. Some of the vertical take off
and landing UAVs would be ideal for
this service.
What must be remembered with this
class of UAV is that they are not independent vehicles but are merely the
aerial component in a very complex
system and thus comprise the middle
grouping of the above classification.
This system can be comprised of
fixed or mobile control and mission
planning stations, launch and recovery
equipment or vehicles, transporters
and data receiving and processing
terminals (see Fig.1).
The problems of launch and recovery are major in a combat situation
and force a further division into
sub-classes and in many instances,
they influence the design of the UAV
itself. A good example of this is the
development of the TRUS (Tilt-Rotor
study and demonstration UAV system)
program. This project is intended to
provide ship-based vertical take off
and landing UAVs for OTH (Over The
Horizon) surveillance and targeting for
USN and NATO surface vessels.
This program also provides an
excellent example of the complexity
and sophistication not only of the
UAV itself but of the business network
required to bring such a complex
unit into being. In the second half of
1991, the Bell Helicopter division put
together a design proposal for a little
Tilt Twin Rotor Vehicle much along
the lines of the much troubled Osprey
Tilt Rotor Transport aircraft.
Named the “Bell Eagle Eye”, the
span over rotors is approximately
5.9 metres and the length 4.9 metres.
Power comes from one Allison turbo
shaft rated at 313kW. The Bell team
includes Israeli Aircraft Industries,
TRW, Allison, Honeywell, Unisys,
Scaled Composites and the Stratos
Group. IAI contributes the ground
control system, data link, mission
computer and payload. TRW contributes payload trade-offs, antenna
Fig.1: this diagram shows some of the
complex infrastructure involved with
the launch, guiding and recovery of
typical UAVs. Getting them into the
air is easy but recovering them under
battle conditions can be very difficult.
simulation and interoperability,
Honeywell the AHRS and other avionics. Unisys integrates shipboard
command/control with the airborne
data link, while Stratos provides the
operational interface.
Burt Rutan (Scaled Composites Inc),
the famous designer of the around the
world lightweight aircraft, is building
two Alli
son-powered airframes and
the test flights were scheduled for the
second half of 1992. To date, I have
seen nothing of the results of this project but the above outline gives some
idea of the complexity and sophistication of the modern UAV.
Take off & landing
Vertical take off and landing is
only one approach to the launch and
recovery of UAVs. Launch is also quite
commonly by conventional take off
(ROG, rise off ground), hand launch,
air
craft launch, catapult launch or
any of several other methods. In other
words, getting the thing into the air is
easy. Recovery, however, is another
July 1993 81
Little more than a model aeroplane, the electrically powered Pointer UAV is
in service with the US Army and was used extensively for surveillance during
Operation Desert Storm, Desert Sabe and Desert Shield. It uses a CCD video
camera.
matter. Battles are rarely fought in
ideal terrain and landing conventionally is usually out of the question. The
situation for the over-the-horizon UAV
is not so bad and any suitable smooth
field within operational range will
suffice as a miniature airfield.
The smaller, shorter range UAVs
and, in particular, ship-launched units
have real problems with recovery and
thus recourse to parachute and net recovery is most common. The problems
of shipboard recovery have forced the
development of the vertical take off
strangest shaped vehicles yet seen on
planet Earth.
There are flying saucers (or more
correctly, flying dough
nuts), flying
balls, flying venturis, flying torpedoes,
flying peanuts, deltas, canards, tandem
wings, tractors, pushers, helicopters,
tilt rotors and on and on; an endless
stream of creative designs intended
to solve awkward problems. If the
aerodynamics of these vehicles ever
finds their way into manned flight
(and I believe they will), we will see
some very interesting developments
“Because the vehicles are actually
unmanned, the airframe designers have been
given virtually carte blanche in regard to
airframe & aerodynamic considerations”.
and landing UAV more than any other
factor. Try landing a speeding UAV
into a small net rigged on the heaving
deck of a ship at sea.
In fact, the recovery problem and
re
duced safety requirements have
brought about a revolution in UAV
design. Because the vehicles are
actually un
m anned, the airframe
designers have been given virtually
carte blanche in regard to airframe and
aerodynamic considerations. This
has spawned a wild profusion of the
82 Silicon Chip
in airport design in the near future.
From the modeller’s point of view
and in fact the military point of view,
possibly the most interesting modern
UAV is the Aerovironment FQM-151A
semi-expendable hand-launched mini
UAV.
Here is a sailplane straight from the
pages of Airborne or any other modern model magazine. Its wingspan is
2.74m, length 1.83m, launch weight
3.6kg, payload 910g and it is powered
by a 300W samarium cobalt electric
motor. (I wonder if they need a good
speed controller?) The electrons for
this motor are supplied by two lithium
batteries which will keep this handy
little vehicle moving for 1.25 hours at
a maximum speed of 80km/h. Cruising
speed is around 35km/h and maximum rate of climb 3.1m/s. The usual
operational altitude is in the range of
50 to 300 metres.
Every aspect of this UAV is novel
and militarily salient. The unit was
designed to be operated by one man
with a second assisting. The complete
system breaks down into two back
packs. The first contains the aircraft
and the second the shoulder-mounted
control/monitor system.
The UAV dismantles into six parts
and can be reassembled in just 2.5 minutes. It carries a fixed focus TV camera
in the nose, angled downwards at 20
degrees from the aircraft’s centreline
and giving a 22 x 30 degree field of
view. It is radio-controlled over an
8km radius and is gyro stabilised. The
Pointer is steer
able by the monitor
and is landed from the deep stall after
engine shut down.
The monitor/control system is very
interesting and appears very much
like a shoulder mounted peep show.
The monitor is mounted on shoulder
braces which place it at face height
in front of the pilot. It is completely
sealed from light and the pilot looks
into the peep window at the monitor
screen. The flight controls are mounted
on the side of the monitor housing. The
transmitter is ground based or portable. This simplicity and flexibility of
operation allows some novel uses for
the Pointer.
The UAV can move to the target
under power, which being electric is
very quiet, then glide with the motor
off to within close range of the target.
The motor is then restarted and the
UAV climbs away back to base. Being
semi-expendable it does not matter if
it is brought down by enemy fire at
this point. The data it sniffed out is
already back home, as the system is a
real-time surveillance unit.
The camera is a CCD type with
resolution of 350 x 380 lines. There
are two monitor screens, one showing
UAV heading and the other the target
information. The monitor is backed
up by a Sony 8mm cassette recorder
with stereo audio channels, replay
with freeze framing, fast slow motion
and aircraft heading.
The number of uses for this system
seems inexhaustible and has continually expanded since being adopted by
the USMC in 1988. Designed primarily
for reconnaissance, surveillance and
target spotting, the list has grown to
include evaluation of the effectiveness
of the concealment techniques of US
ground troops. Thus, any unit digging
in will launch a Pointer to check its
own camouflage from the air and to
maintain perimeter security. In the
Iraq war, it was operated by the US
Army 82nd Airborne Division, 4th M
Expeditionary Brigade and the 1st and
4th M expeditionary Force as part of
Operations Desert Shield and Desert
Storm.
Used in the above manner for the
first time, it was also used for real-time
battle damage assessment, reconnaissance, surveillance and advance
warning of enemy movements.
Another novel use for Pointer is
from a ground vehicle. In this manner, the UAV and pilot can extend the
range, depending on the terrain, to
around 50-65km, whilst maintaining
an operational field of view of up to
eight kilometres ahead of and around
the ground vehicle; very handy for
convoys and armoured columns.
However, the Pointer is not without
its drawbacks and there were reports of
launch difficulties due to high winds.
This problem of high winds and low
cruise speeds is a serious one for all
aircraft, as effective ground speeds
can very quickly drop to zero. Thus,
a Pointer cruising at 35km/h into
a 35km/h head
wind has a ground
speed of 0km/h, whereas a UAV with
a 70km/h cruise speed will still have
a ground speed of 35km/h and there
fore will be able to accomplish its
mission, albeit with a reduced range or
loiter time. When cruise speed reaches
hundreds of km/h, headwinds become
less of a problem.
Improvements
These problems aside, the Pointer
appears to have a good future and improvements are already in the system.
These include automatic heading and
altitude hold, spread spectrum transmission to minimise threat from ECM,
increased range (16km), endurance (2
hours) and flight speed. Reduction of
airframe and payload weights are also
in the pipeline, as is a twin-engined
version. All in all, this is a very handy
little unit for what is essentially a toy
aeroplane.
Pointer also has a big brother, the
HILINE, which is a high altitude long
endurance (HALE) UAV for acquisition and tracking of hot airborne
targets (launched ballistic missiles,
etc). At first glance, the figures on this
UAV appear fantastic, with a typical
mission profile as follows: carry 45kg
payload for 800km, loiter for more than
24 hours and return; range more than
4830km with an endurance of approximately 20-30 hours; range 100km from
launch at 25,000 feet; or fly for 15-20
hours at 40,000 feet.
The wingspan of this UAV is quoted
as 15.24 metres and maximum take
off weight as 341kg. It is powered by
one 31kW Ackerman OMC-200 tur
bocharged 2-cylinder engine. Whilst
on the subject of high altitude UAVs,
I have seen mission profiles calling
for altitudes in excess of 100,000 feet
from piston engined UAVs. How they
get a piston engine to breathe at that
altitude is beyond me.
However here we are again at the
end of the allocated space. Next month
we will continue with a discussion on
SC
the really exotic UAVs.
Product Showcase – ctd
from page 67
The end result is that the L-A1 boasts
one of the quietest phono stages found
in an integrated amplifier irrespective
of price.
Another outstanding feature is a
newly developed master volume control with an unusually low impedance
of only 1kΩ. Such a low impedance
design reduces thermal and other
types of noise to the order of one tenth
of traditional designs.
Power output is rated at 100 watts
RMS from a push pull parallel Darl
ington design that employs a group
of driver transistors for each power
section. All stages prior to the output
sections are class A. The power output
sections are powered by a specially
designed toroidal transformer with
extremely low mag
n etic leakage
and massive 18,000µF reservoir
capacitors that have been specially
selected for their outstanding electrical and musical properties. The main
amplifier board and phono section
boards are glass epoxy, Kenwood
claiming that this new material offers
excellent electrical characteristics
and better rigidity than phenolic resin
board.
Specifications include 100 watts
RMS per channel, with both channels
driven into 8Ω from 20Hz to 20kHz
with no more than 0.005% THD. Dynamic power is up to 420 watts into
2Ω. The frequency response is 3Hz
to 100kHz at the -3dB points, while
phono RIAA response is from 20Hz
to 20kHz within ±0.5dB.
The Kenwood L-A1 stereo amplifier
is covered by a 12-month warranty
on parts and labour and has a recommended retail price of $3999. For
further information, contact Kenwood
Electronics Australia Pty Ltd by phoning (008) 251 697.
Nifty little
magnifier
This combined
m a gn i f i e r a n d
tweezer set is very handy when you
have to examine PC boards for cold
solder joints and also to examine the
lettering on those teensy-weensy components. And even if you never touch
a PC board, it is ideal for getting splinters out of fingers. It sells for just $5.50
from All Electronic Components, 118122 Lons
dale St, Mel
bourne, 3000.
Phone (03) 662 3506.
July 1993 83
AMATEUR RADIO
BY GARRY CRATT, VK2YBX
Antenna tuners: why they are useful
If you browse through most catalogs of amateur
equipment you will find a range of antenna
tuners available for the amateur bands. Perhaps
you may have had doubts about whether these
devices are worthwhile. They are & this article
explains why.
Possibly the most commonly considered theory regarding the benefit
of antenna tuners is that they improve
antenna efficien
cy and so assist in
the effective radiation of signals by
the antenna. In fact, nothing could
be further from the truth. Anten
na
tuners do nothing to improve antenna
efficiency but there certainly are other
good reasons to use one.
These days, all modern transmitters
are designed to operate into a nominal
resonant 50Ω load. This is all very
well in theory but in practice very few
antennas present such an ideal impedance to the transmitter. In addition,
solid state transmitters are designed
so that their output power drops as
the load SWR increases, to protect
the final output stage from excessive
dissipation which would occur when
feeding a highly reactive load. So any
antenna mismatch leads to increased
SWR and therefore a subsequent reduction in radiated power.
For the VHF and UHF bands, the
scale of resonant antennas is such that
they can be made with quite manageable physical dimensions. They can
also be made to provide relatively
wide bandwidth, whilst maintaining
a reasonable Q.
We know that any piece of wire
connected to a transmitter will radiate
This heavy duty antenna tuner from Emtronics is based on the Pi network
shown in Fig.3 but it also features monitoring of forward & reflected power via
a twin needle meter to give SWR readings. It can handle HF band transmitters
with output powers rated up to 1000 watts.
84 Silicon Chip
signals to some degree, so it is logical
that there will be a considerable advantage in using a device which assists in
the matching of an HF antenna to the
transmitter output stage, maximising
the current flowing in the antenna,
and thereby resulting in improved
field strength.
A related factor to be considered
is the Q, or “quality” factor of the
antenna. Generally, RF experience
indicates that the higher the Q, the
better. However, this is not necessarily the preferred situation with HF
antennas. A high Q means a narrow
bandwidth and readjustment of the
antenna tuning unit may be necessary,
even for small changes in frequency.
For HF antennas, a low Q is preferred. As the Q of an antenna is
determined by both the radiation and
DC resistance, it may be preferable to
select an antenna tuner where capacitive reactance is added to bring the
antenna system to resonance, lowering
the Q and generally giving broader
bandwidth.
Most long wire or vertical HF
antennas are loaded against ground
and need to be only one quarter
wavelength long at the resonant
frequency. For an antenna tuner to
assist in matching this type of antenna, it is important to have a good
low impedance ground, so that equal
currents can flow in both the antenna
and ground, hence producing an antenna radiation pattern which will be
of some use. If an insufficient ground
is provided, an imbalance will exist,
and the resultant radiation pattern
will have (in the instance of a vertical)
a high angle of radiation.
Measuring antenna current
A simple antenna current indicator
can be made using a 25mm ferrite
toroid slipped over the antenna wire.
Fig.1: this circuit arrangement can be
used to monitor the current flowing in
a wire to an antenna or in the ground
return. The two capacitors are each
100pF disc ceramics while the diode
is any germanium type such as OA91.
The meter is a 1mA movement.
This photo shows the interior of the Emtron EAT-1000A antenna tuner. Note the
wide spaced variable capacitors and the large tapped inductor.
Fig.2: the simplest configuration for
an antenna tuner, used to match a low
impedance (50Ω) transmitter to a high
impedance line is either a parallel (a)
or series (b) tuned circuit, resonant at
the operating frequency.
A pick up wire, comprising several
turns around the toroid, feeds a diode
and 100pF capacitor, wired to a 0-1mA
meter which has a another 100pF
capacitor across it. Fig.1 shows the
circuit. By applying some RF energy
from the transmitter and adjusting the
antenna tuner, an increase in antenna
current can be verified. The same circuit can be used in the ground lead,
to verify current flowing.
The circuit configuration of an
antenna tuner needed to transfer maximum power from the transmitter to
the antenna depends to a large degree
on the impedance of the feed line. The
simplest configuration, used to match
a low impedance, say 50Ω, transmitter to a high impedance line is either
a series or paral
lel tuned circuit,
resonant at the operating frequency.
Fig.2 shows various configurations
of series and parallel matching
networks.
A superior arrangement,
based on the Pi network shown
in Fig.3, allows 50Ω or so to be
matched to an impedance of
up to several thousand ohms.
Both capacitors C1 and C2 are
Fig.3: based on a Pi network, this antenna
variable and, in a high power
tuner allows 50Ω or so to be matched to an
situation, must have widely
impedance of up to several thousand ohms.
spaced plates, due to the large
Both capacitors C1 & C2 are variable &
amount of energy normally
are usually ganged together. The inductor
involved at HF. The inductor
should be made from large diameter wire or
should be made from large dicopper tubing, to minimise insertion losses.
ameter wire or copper tubing,
to minimise insertion losses.
A well designed Pi network antenna
received signal performance when
tuner should also include some form
a high impedance antenna, such as
of gas discharge protection circuit, to
a long wire, is used with a low imprevent possible damage to the trans- pedance receiver. The antenna tuner
mitter equipment from atmospheric
reduces the SWR by improving the
discharge.
antenna impedance matching, resultSome lower power designs use a ing in maximum transfer of energy.
tapped inductor to ensure a “match” This is most noticeable when using a
across a wide range of impedances. receiver without an RF stage, where
In any case, the network is used to the antenna input is fed via a bandpass
correct a mismatch problem and some filter to the mixer. In receivers having
reduction in system efficiency when a high amount of RF gain in the first
compared to a correctly matched stage, the effect is not as noticeable.
antenna at the same frequency will
In summary, an antenna tuner is
be noticed. However, this can still no substitute for a properly designed
provide a major improvement over an resonant antenna, but in cases where
unmatched antenna without a tuner!
such an antenna cannot be used, they
Antenna tuners are also capable of can offer improved performance over
SC
an unmatched antenna system.
making a noticeable improvement in
July 1993 85
VINTAGE RADIO
By JOHN HILL
In the good ol’ days of my childhood
Because radio receivers were expensive in
the 1920s, many people built their own sets
and even made the batteries to run them. In
those days, it was a case of improvise or go
without. We even built our own batteries.
My interest in vintage radio started
only eight years ago and I have learnt
quite a lot in that time and enjoy my
hobby immensely. However, it is not
all new to me for there was a time in
my childhood when I built crystal
sets and often listened to these simple receivers until my callused ears
could not tolerate the pressure of the
headphones any longer.
I guess my early interest in radio
rubbed off from my father. Dad was
into radio in the early 1920s when
about the only thing one could expect
to hear was an occasional Morse signal
from a distant transmitter. In those
very early days of radio, there were
not many stations on the air to listen to
and those that were had quite limited
transmission times.
My father was but a humble gardener in the 1920s and his wages
were such that there was nothing
left over from household expenses to
spend on radios in any shape or form.
Therefore, poor old Dad had to make
his own equipment and, what’s more,
it worked.
Unfortunately, my father’s homemade radio gear has now gone. It
didn’t seem important at the time so
it all went to the tip when he died
For the best part of the author’s life, this old radio cabinet has served to remind
him of many exciting childhood activities. It sits on top of a post in the front
yard and was where the billy was left for the milkman.
86 Silicon Chip
and although it may sound unkind,
the tip was the right place for most
of it. However, with my rekindled
interest in radio today, some of Dad’s
home-made equipment would now be
nice to have, if only for sentimental
reasons.
I am convinced that few people
today have the capacity to improvise
as did those of yesteryear. Some of
the projects my father tackled were
incredible for a guy who left school
at 13. That’s another interesting thing
about my father: he caddied at the local
golf course for a year while his mother
thought he was still going to school.
God help me if I had tried that trick
when I was 13.
Crystal set
One of Dad’s first radio projects was
his crystal set. Now making a crystal
set may not seem a very daunting task
today but when my father made his,
he had to make everything including
the tuning capacitor and the crystal
detector. The only item he purchased
was a set of headphones, which gave
excellent service for many years. In
fact, I was still using them in the postwar years.
I remember the tuning capacitor
quite well for it was used in some of
my creations. I also remember that
it was a bit stiff to turn and the old
Emmco dial slipped when the shaft
became tight at one end of the travel.
I also recall that it should have had
a few more plates in it, for it lacked
sufficient capacitance to cover the full
width of the broadcast band.
The crystal detector was made up
from miscellaneous bits and pieces
mounted on a small sheet of ebonite.
However, the basic requirements were
there. The crystal cup had three setscrews to retain the piece of crystal and
the arm that held the cat’s whisker was
This Leclanche cell is similar to those
used for the front gate bell. During
the 1930s, the wet Leclanche cell was
used almost exclusively for powering
door bells.
pivoted so as to give movement across
the face of the crystal.
Home-made batteries
But those early achievements fade
into insignificance when one thinks of
Dad’s home-made “B” batteries.
When I graduated from crystal sets
to a 1-valve receiver, I was able to
obtain a discarded B battery from the
local tip. This battery kept me listening
for a month or so but there soon came
a time when it was no longer serviceable. Once again, good old Dad solved
the problem by making a rechargeable
20-volt B battery.
Now this was no ordinary battery –
in fact, few would recognise it as such.
It consisted of a wooden baseboard
with 10 shallow holes bored into it.
Placed into the holes were 10 small
pill bottles – Doctor Morse’s Pink Pills
for Pale People if I remember correctly.
These formed the cells of the battery
and were three parts filled with dilute
sulphuric acid.
Strips of sheet lead were used for
the plates. These were shaped like
an inverted “U” and arranged in the
bottles so that the ends of each strip
occupied two adjoining bottles. In
other words, it was a very simple lead
acid accumulator.
When placed on the battery charger
(which used a home-made transformer
and metal oxide rectifier), the lead
plates changed colour almost immediately. The positive plates turned to
a chocolate brown, while the negative
plates went a light grey. However, because the battery charger could only
produce about 12 volts, the battery had
to be charged in two halves.
This 20-volt B supply kept the little
1-valver working quite happily, but
after a couple of days it went strangely
quiet. Reason – a flat B battery. Further
testing indicated that the battery had
almost no capacity. It could reach
full charge in a matter of minutes and
would discharge almost as rapidly. In
fact, it could supply only about one
milliamp of current for approximately
10 hours.
But although that miserable battery
often went flat in the middle of an
interesting program, it got me out of a
tight spot at the time.
Making a rechargeable battery was
nothing new to my father because he
had made one once before. It lived
under the house in a wooden crate
and had been a source of mystery to
me for many years. Apparently it was
used way back in the days when part
of Bendigo had a DC power supply
(most likely from the tramway depot)
and the battery was recharged by
plugging it into the DC mains. During
recharging, a globe was connected in
series with the battery to provide the
correct charge rate.
When my 1-valver subsequently
grew into a 2-valver, the pill-bottle B
battery was grossly inadequate; in fact,
it was never even considered. It was
time to crawl under the house and drag
out Dad’s old battery to see if it could
be recommissioned.
Refurbishing an old relic
Once again, the old disused battery was a marvel. It was capable of
supplying B voltages to the largest of
battery receivers and was an impressive sight.
My father’s perseverance never
failed to amaze me. His B battery was
entirely home-made, including the
glass containers which housed each
cell. These were made from small flat
sided medicine bottles. The tops of
the bottles had been cut off using the
hot wire and quench method of glass
cutting. It must have taken quite some
time just to collect all the bottles and
cut them to size!
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KITS & PCBs
2.5 Watt 88-108MHz FM
Transmitter Kit $49
This is the highest powered transmitter kit
available. With line of sight, distances of
up to 100 miles can be achieved. Requires
high-level input from tape or CD player.
Runs from 12-28 volt supply. Coming soon
XTAL controlled PLL stereo version.
Note: It is illegal to use this transmitter
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MAX I/O board for PCs
7 Relays, ADC, DAC, 8 TTL inputs, Relay/
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PCB/Disc/manual $39.
DIGI-125 Amplifier Kits
One of the nicest amplifier kits to build for
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$14. 125W kit $19. Now available 200 watt
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AEM 35 watt single chip amp
35 watts RMS from a TO220 chip on a
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36 Regent St, Kensington.
S.A. Phone (08) 332 6513
July 1993 87
VINTAGE RADIO – In the days of my childhood
The plates were also time consuming to make – no lead strips in this
battery.
Each plate had been hand-cast in a
special mould which shaped the plate
with an open grid structure similar to
that of a car battery plate. The respective lead compounds (red lead oxide
for the positive plates and yellow
lead oxide for the negative) were then
hand-hammered into the plates.
The plates were installed two to a
cell with a separator in between and
held in place at the top with bees
wax. The wax seal had a vent hole
which also served as a top-up hole
for distilled water or for checking the
electrolyte with a hydrometer.
All things considered, a “helluva”
lot of effort had gone into the making
88 Silicon Chip
of this battery. However, the question at
the time was could it
be recommissioned to
work my little 2-valve
receiver?
Unfortunately, a
quarter of a century
spent in limbo under
the house hadn’t done
the old battery much
good. The electrolyte
had not been drained
before storage and the
plates had sulphurat
ed and were all white
and horrible looking.
What’s more, many of
the plates were starting to fall apart.
But it was not all
bad news. After dismantling the whole
battery, there seemed
to be enough good
plates to make up a
reasonable size unit.
And when the sulph
ura te d plates were
scrubb
ed up with a
wire brush, the prospect of a “new” battery actually looked
quite promising.
To cut a long story short, there were
enough servicea ble
plates to make up a
40 volt B battery, with
the leftover-plates being used to build
a rechargeable A battery.
Battery charger
As previously mentioned, my
father’s battery charger could only
charge at 12 volts, which made recharging a 40-volt battery a bit awkward. But good old Dad soon solved
that problem.
A special switch was made consisting of a rotating drum with numerous
brass contacts on it. The battery was
wired to this switch in four 10-volt
banks and the switch connected these
banks either in series or parallel. This
ingenious switch took the best part of
a weekend to make and install.
The rechargeable batteries were a
complete success and were used for
several years. The B battery was put on
charge every three months, while the
A battery required attention at about
3-weekly intervals.
Leclanche battery
There were other special batteries
used at home back in those distant
days of my childhood. One of them
was a wet cell Leclanche battery and it
too lived under the house in a wooden
box. This 3-cell battery powered the
front gate bell and what a set up that
was.
On the front gate was a home-made
gate closer and combined switch.
This switch closed its contacts when
the gate was opened about six inches
(sorry, but we didn’t have millimetres
back then). The switch was connected
to the battery by underground cables
which were laid before the front lawn
was planted more than 60 years ago.
The cable then ran from the battery to
an electric bell in the kitchen.
When the gate was opened, the bell
gave a short ring and then another
short ring when it closed. This switching arrange
ment prevented the bell
from ringing continuously if someone
held the gate open for a prolonged
period. For reasons unknown, the bell
was later changed to a buzzer.
The bell always gave a warning
when someone came through the
front gate and by looking into the
strategically placed mirror outside the
dining room window, the “intruder”
could be observed walking down the
garden path. Now I ask you – who
needs expensive modern electronic
surveillance equipment? Just consider
the small cost and effectiveness of this
old style system.
I’m sure that my father was never
involved in any underhand activities
but he sure had a suspicious nature,
particularly where strangers were
concerned.
Actually, the gate bell did detect
the presence of a few undesirables. In
those days, stealing milk money was
commonplace and several would-be
milk money snatchers were met halfway across the front lawn. As Dad
was a fairly good boxer in his day,
the trespasser usually got a straight
right to the jaw if he didn’t beat a
hasty retreat.
This gate bell early warning system
also had its problems, such as on those
occasions when Dad had forgotten
that I had gone out to a picture show.
We had several confrontations in the
middle of the front lawn at midnight!
The problem was solved by developing a special gate opening
technique. If the gate was zapped
open quickly and then zapped closed
again, the old bell didn’t have time
to get into the swing of things and I
was able to sneak in (or out) at any
hour –undetected.
A horsey story
Still another battery was used at
home for a while and this one was
installed in the workshed. At the time,
my older brother was interested in
electroplating and he required a DC
supply for his experiments, hence
the need for still another battery. In
this case, it was a 3-cell potassium
bi-chromate battery.
This battery was bought in kit form
from Selbys and when assembled
used large glass jars to hold the potassium bi-chromate and sulphuric
acid electrolyte. When not in use,
the plates (zinc and carbon) had to
be lifted out of the solution to protect
the zinc plates.
As I recall, the electroplating experiments were far from successful.
However, it was not the fault of the
battery. Electroplating is a specialised
process which requires special tech
niques. Unfortunately, these were
never learnt.
The bi-chromate battery did find
another use, however. Its 6-volt output
was used to drive an old T-model Ford
ignition coil (the trembler type). The
most spectacular experiment with this
equipment by far involved the electrification of the back fence.
Our neighbour at the back had a
horse which kept scratching itself on
the fence and, in the process, had just
about flattened the rickety structure.
The fence was re-erected and steel
wire was woven throughout the weather-beaten palings to help hold things
together. The final touch to the fence
repair was to connect the old Ford
coil to the wire reinforcement (with an
earth return) and wait for the horse to
come back for another scratch.
The electric fence equipment was
installed in the shed, complete with
a peep hole drilled in the rear wall for
observation purposes. The primary of
the Ford coil was wired to the battery
via a Morse key switch.
Eventually the horse returned for
a rub up along the fence and Dad
gave him a quick zap. Neddy must
have backed away at the crucial
moment and only got a bit of tickle.
But the second time around he had
his nose on the wire when the switch
was closed. He never went near that
fence again.
Part of the potassium bi-chromate
battery still survives. One and a half
zinc plates still remain and I solder
odd pieces of these plates to my car
radiator cap as sacrificial anodes. The
zinc protects the aluminium cylinder
head and other alloy components.
The only other thing that remains
to remind me of all this childhood
excitement is an old 1920s battery
radio cabinet. It stands on a wooden
post beside the garden path where it
has stood for the last 40 years or so.
However, the reason for the old cabinet’s strange and elevated position is
no longer apparent. It was where the
billy was left out for the milkman who
once called in the early hours of the
morning. Remember the days of free
home deliveries?
No doubt, lack of funds was one of
the reasons my father made so many of
the things he couldn’t afford to buy. He
grew up in difficult times and worked
hard all of his life. Nevertheless, he
still found time and a little money
to follow his hobbies and special
interests.
Radio and electronics have developed to such a degree today that
everything has become too “high-tech”
for the average person to handle.
Whereas my father and those like him
used to build their own equipment, the
situation now is entirely different. In
my opinion, all the fun has gone out
of electronics and the hobbyist has
been reduced to assembling kits if he
is inclined to do so.
That’s one of the reasons I like
vintage radio restoration for it is still
a hands-on, do-it-yourself activity
that appeals to me in particular. The
almost total lack of vintage components encourages one to improvise
and scrounge. Such a pastime can be
a lot of fun.
My current interest in old radios
helps to remind me of a time when the
style of life and the activities people
pursued were a good deal different
from the lifestyles of today. I am also
glad that I spent my childhood during
those times and if I had to choose
again, I’m sure I would follow the
SC
same path.
Send Postage Stamp For List Of Other Items Including Valves
L.E. CHAPMAN
TAPE DECK OR RADIO POWER
LEADS
Plugs and Sockets
$1.50
Test prods and leads
$1.50
TOUCH MICRO SWITCHES
as used on TV sets. 4 for $1
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plug & lead 4 for $2
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4 pos 50c
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7000 to 15/Ohm 5W
$10
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$10
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$10
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1/2 Meg dual
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INLINE FUSE HOLDERS 4
FOR $1
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3.5 to 3.5
$1
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4 for $1
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$1.50
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$2.00
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$1.50
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$1.00
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Includes cartridge and stylus.
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$15
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5 for $2.50 Special
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2 gang covers
all Aust. AM
bands. $10.
P&P $1.80 for
one or two.
CAPACITORS
6N8 150V
1000uF 16V
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0.0039uF 1500V
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47uF 63V
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470uF 16V
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0.1uF 250V
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0.027 250V
10uF 25V
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SPECIAL Dual
VU Meters $4.
P&P $1.80 for
one or two
$1.50
$1
$4.50
200 MIXED SCREWS
self-tappers, bolts, nuts etc.
200 for $2
CAR RADIO SUPPRESSORS
4 for $2
OXTAL VALVE SOCKETS
$1 each
Stick Rectifiers TV20SC $2
Transistors
AD61-62 pair $3
AD 149 $2 each
Chrome 1/4" push on knobs
RRP 1.20 EA 10 for $1
Mixed capacitors fresh stock
100 for $2
Mixed resistors all handy
values
100 for $2
Slide pot knobs 10 for $1
1F 455kHz for valve radios
$2 ea
Telsco Microphone Ceramic
$2 pp $1
SPECIAL: CELLULAR
HORN TWEETER
Mounting specification
12.5cm x 7.1cm. Frequency
range 2000-20,000Hz.
Sensitivity 105dB. Maximum
power 30 Watts. Impedance 8
ohms. $12.
TV CRYSTALS
4.43619kHz 03061 NDK;
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July 1993 89
Silicon Chip
Fluid Level Detector; Simple DTMF Encoder;
Studio Series 20-Band Stereo Equaliser, Pt.2;
Auto-Zero Module for Audio Amplifiers (Uses
LMC669).
BACK ISSUES
September 1988: Hands-Free Speakerphone;
Electronic Fish Bite Detector; High Performance
AC Millivoltmeter, Pt.2; Build The Vader Voice;
Motorola MC34018 Speakerphone IC Data; What
Is Negative Feedback, Pt.4.
Graphic Equaliser, Pt.1; Stereo Compressor For
CD Players; Amateur VHF FM Monitor, Pt.2; Signetics NE572 Compandor IC Data; Map reader
For Trip Calculations; Electronics For Everyone
–Resistors.
November 1988: 120W PA Amplifier Module
(Uses Mosfets); Poor Man’s Plasma Display;
Automotive Night Safety Light; Adding A Headset
To The Speakerphone; How To Quieten The Fan
In Your Computer; Screws & Screwdrivers, What
You Need To Know; Diesel Electric Locomotives.
April 1989: Auxiliary Brake Light Flasher; Electronics For Everyone: What You Need to Know
About Capacitors; Telephone Bell Monitor/ Transmitter; 32-Band Graphic Equaliser, Pt.2; LED
Message Board, Pt.2.
December 1988: 120W PA Amplifier (With Balanced Inputs), Pt.1; Diesel Sound Generator;
Car Antenna/Demister Adaptor; SSB Adaptor For
Shortwave Receivers; Why Diesel Electrics Killed
Off Steam; Index to Volume 1.
January 1989: Line Filter For Computers; Ultrasonic Proximity Detector For Cars; 120W PA Amplifier (With Balanced Inputs) Pt.1; How To Service
Car Cassette Players; Massive Diesel Electrics In
The USA; Marantz LD50 Loudspeakers.
February 1989: Transistor Beta Tester; Minstrel
2-30 Loudspeaker System; LED Flasher For Model
Railways; Build A Simple VHF FM Monitor (uses
MC3362), Pt.1; Lightning & Electronic Appliances;
Using Comparators to Detect & Measure.
March 1989: LED Message Board, Pt.1; 32-Band
May 1989: Electronic Pools/Lotto Selector; Build
A Synthesised Tom-Tom; Biofeedback Monitor For
Your PC; Simple Stub Filter For Suppressing TV
Interference; LED Message Board, Pt.3; All About
Electrolytic Capacitors.
October 1989: Introducing Remote Control; FM
Radio Intercom For Motorbikes Pt.1; GaAsFet
Preamplifier For Amateur TV; 1Mb Printer Buffer;
2-Chip Portable AM Stereo Radio, Pt.2; Installing
A Hard Disc In The PC.
November 1989: Radfax Decoder For Your PC
(Displays Fax, RTTY & Morse); Sensitive FM
Wireless Microphone; FM Radio Intercom For Motorbikes, Pt.2; 2-Chip Portable AM Stereo Radio,
Pt.3; Floppy Disc Drive Formats & Options; The
Pilbara Iron Ore Railways.
December 1989: Digital Voice Board (Records
Up To Four Separate Messages); UHF Remote
Switch; Balanced Input & Output Stages; Data For
The LM831 Low Voltage Amplifier IC; Installing A
Clock Card In Your Computer; Index to Volume 2.
January 1990: High Quality Sine/Square Oscillator; Service Tips For Your VCR; Speeding Up
Your PC; Phone Patch For Radio Amateurs; Active
Antenna Kit; Speed Controller For Ceiling Fans;
Designing UHF Transmitter Stages.
June 1989: Touch-Lamp Dimmer (uses Siemens
SLB0586); Passive Loop Antenna For AM Radios;
Universal Temperature Controller; Understanding
CRO Probes; LED Message Board, Pt.4.
February 1990: 16-Channel Mixing Desk; High
Quality Audio Oscillator, Pt.2; The Incredible Hot
Canaries; Random Wire Antenna Tuner For 6
Metres; Phone Patch For Radio Amateurs, Pt.2;
PC Program Calculates Great Circle Bearings.
July 1989: Exhaust Gas Monitor (Uses TGS812
Gas Sensor); Extension For The Touch-Lamp
Dimmer; Experimental Mains Hum Sniffers; Compact Ultrasonic Car Alarm; NSW 86 Class Electric
Locomotives.
March 1990: 6/12V Charger For Sealed Lead-Acid
Batteries; Delay Unit For Automatic Antennas;
Workout Timer For Aerobics Classes; 16-Channel
Mixing Desk, Pt.2; Using The UC3906 SLA Battery
Charger IC.
September 1989: 2-Chip Portable AM Stereo
Radio (Uses MC13024 and TX7376P) Pt.1;
Alarm-Triggered Telephone Dialler; High Or Low
April 1990: Dual Tracking ±50V Power Supply;
VOX With Delayed Audio; Relative Field Strength
Meter; 16-Channel Mixing Desk, Pt.3; Active CW
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90 Silicon Chip
✂
Card No.
Filter For Weak Signal Reception; How To Find
Vintage Radio Receivers From The 1920s.
May 1990: Build A 4-Digit Capacitance Meter;
High Energy Ignition For Cars With Reluctor Distributors; The Mozzie CW Transceiver; Waveform
Generation Using A PC, Pt.3; 16-Channel Mixing
Desk, Pt.4.
June 1990: Multi-Sector Home Burglar Alarm;
Low-Noise Universal Stereo Preamplifier; Load
Protection Switch For Power Supplies; A Speed
Alarm For Your Car; Design Factors For Model
Aircraft; Fitting A Fax Card To A Computer.
July 1990: Digital Sine/Square Generator, Pt.1
(Covers 0-500kHz); Burglar Alarm Keypad & Combination Lock; Simple Electronic Die; Low-Cost
Dual Power Supply; Inside A Coal Burning Power
Station; Weather Fax Frequencies.
August 1990: High Stability UHF Remote
Transmitter; Universal Safety Timer For Mains
Appliances (9 Minutes); Horace The Electronic
Cricket; Digital Sine/Square Wave Generator, Pt.2.
September 1990: Music On Hold For Your Telephone; Remote Control Extender For VCRs; Power
Supply For Burglar Alarms; Low-Cost 3-Digit
Counter Module; Simple Shortwave Converter For
The 2-Metre Band.
October 1990: Low-Cost Siren For Burglar
Alarms; Dimming Controls For The Discolight;
Surfsound Simulator; DC Offset For DMMs; The
Dangers of Polychlorinated Biphenyls; Using The
NE602 In Home-Brew Converter Circuits.
November 1990: How To Connect Two TV Sets To
One VCR; A Really Snazzy Egg Timer; Low-Cost
Model Train Controller; Battery Powered Laser
Pointer; 1.5V To 9V DC Converter; Introduction
To Digital Electronics; Simple 6-Metre Amateur
Transmitter.
December 1990: DC-DC Converter For Car
Amplifiers; The Big Escape – A Game Of Skill;
Wiper Pulser For Rear Windows; Versatile 4-Digit
Combination Lock; 5W Power Amplifier For The
6-Metre Amateur Transmitter; Index To Volume 3.
January 1991: Fast Charger For Nicad Batteries,
Pt.1; The Fruit Machine; Two-Tone Alarm Module;
Laser Power Supply; LCD Readout For The Capacitance Meter; How Quartz Crystals Work; The
Dangers When Servicing Microwave Ovens.
February 1991: Synthesised Stereo AM Tuner,
Pt.1; Three Inverters For Fluorescent Lights; LowCost Sinewave Oscillator; Fast Charger For Nicad
Batteries, Pt.2; How To Design Amplifier Output
Stages; Tasmania's Hydroelectric Power System.
March 1991: Remote Controller For Garage
Doors, Pt.1; Transistor Beta Tester Mk.2; Synthesised AM Stereo Tuner, Pt.2; Multi-Purpose I/O
Board For PC-Compatibles; Universal Wideband
RF Preamplifier For Amateurs & TV.
April 1991: Steam Sound Simulator For Model
Railroads; Remote Controller For Garage Doors,
Pt.2; Simple 12/24V Light Chaser; Synthesised
AM Stereo Tuner, Pt.3; A Practical Approach To
Amplifier Design, Pt.2; Playing With The Ansi.Sys
File; FSK Indicator For HF Transmissions.
May 1991: Build A DTMF Decoder; 13.5V 25A
Power Supply For Transceivers; Stereo Audio
Expander; Fluorescent Light Simulator For Model
Railways; How To Install Multiple TV Outlets, Pt.1;
Setting Screen Colours On Your PC.
June 1991: A Corner Reflector Antenna For
UHF TV; 4-Channel Lighting Desk, Pt.1; 13.5V
25A Power Supply For Transceivers; Active Filter
For CW Reception; Electric Vehicle Transmission
Options; Tuning In To Satellite TV, Pt.1.
July 1991: Battery Discharge Pacer For Electric
Vehicles; Loudspeaker Protector For Stereo Amplifiers; 4-Channel Lighting Desk, Pt.2; How To Install
Multiple TV Outlets, Pt.2; Tuning In To Satellite TV,
Pt.2; PEP Monitor For Transceivers.
August 1991: Build A Digital Tachometer;
Masthead Amplifier For TV & FM; PC Voice Recorder; Tuning In To Satellite TV, Pt.3; Installing
Windows On Your PC; Step-By-Step Vintage
Radio Repairs.
September 1991: Studio 3-55L 3-Way Loudspeaker System; Digital Altimeter For Gliders
& Ultralights, Pt.1; Build A Fax/Modem For Your
Computer; The Basics Of A/D & D/A Conversion;
Windows 3 Swapfiles, Program Groups & Icons.
October 1991: Build A Talking Voltmeter For Your
PC, Pt.1; SteamSound Simulator Mk.II; Magnetic
Field Strength Meter; Digital Altimeter For Gliders
& Ultralights, Pt.2; Getting To Know The Windows
PIF Editor.
November 1991: Colour TV Pattern Generator,
Pt.1; Battery Charger For Solar Panels; Flashing
Alarm Light For Cars; Digital Altimeter For Gliders
& Ultralights, Pt.3; Build A Talking Voltmeter For
Your PC, Pt.2; Error Analyser For CD Players Pt.3;
Modifying The Windows INI Files.
December 1991: TV Transmitter For VCRs With
UHF Modulators; Infrared Light Beam Relay;
Solid-State Laser Pointer; Colour TV Pattern
Generator, Pt.2; Windows 3 & The Dreaded Un
recoverable Application Error; Index To Volume 4.
January 1992: 4-Channel Guitar Mixer; Adjustable
0-45V 8A Power Supply, Pt.1; Baby Room Monitor/FM Transmitter; Automatic Controller For Car
Headlights; Experiments For Your Games Card;
Restoring An AWA Radiolette Receiver.
February 1992: Compact Digital Voice Recorder;
50-Watt/Channel Stereo Power Amplifier; 12VDC/240VAC 40-Watt Inverter; Adjustable 0-45V 8A
Power Supply, Pt.2; Designing A Speed Controller
For Electric Models.
March 1992: TV Transmitter For VHF VCRs; Studio Twin Fifty Stereo Amplifier, Pt.1; Thermostatic
Switch For Car Radiator Fans; Telephone Call
Timer; Coping With Damaged Computer Direct
ories; Valve Substitution In Vintage Radios.
April 1992: Infrared Remote Control For Model
Railroads; Differential Input Buffer For CROs; Studio Twin Fifty Stereo Amplifier, Pt.2; Understanding
Computer Memory; Switching Frequencies in
Model Speed Controllers; Aligning Vintage Radio
Receivers, Pt.1.
May 1992: Build A Telephone Intercom; LowCost Electronic Doorbell; Battery Eliminator For
Personal Players; Infrared Remote Control For
Model Railroads, Pt.2; A Look At Large Screen
High Resolution Monitors; OS2 Is Really Here;
Aligning Vintage Radio Receivers, Pt.2.
June 1992: Multi-Station Headset Intercom, Pt.1;
Video Switcher For Camcorders & VCRs; Infrared
Remote Control For Model Railroads, Pt.3; 15-Watt
12-240V Inverter; What’s New In Oscilloscopes?;
A Look At Hard Disc Drives.
July 1992: Build A Nicad Battery Discharger;
8-Station Automatic Sprinkler Timer; Portable
12V SLA Battery Charger; Off-Hook Timer For
Telephones; Multi-Station Headset Intercom, Pt.2;
Understanding The World Of CB Radio.
August 1992: Build An Automatic SLA Battery
Charger; Miniature 1.5V To 9V DC Converter;
Dummy Load Box For Large Audio Amplifiers;
Internal Combustion Engines For Model Aircraft;
Troubleshooting Vintage Radio Receivers.
September 1992: Multi-Sector Home Burglar
Alarm; The Interphone Digital Telephone Exchange, Pt.2; General-Purpose 3½-Digit LCD
Panel Meter; Track Tester For Model Railroads;
Build A Relative Field Strength Meter.
October 1992: 2kW 24VDC To 240VAC Sinewave
Inverter; Multi-Sector Home Burglar Alarm, Pt.2;
Mini Amplifier For Personal Stereos; Electronically
Regulated Battery Charger (Charges 6V, 12V &
24V Lead-Acid Batteries).
November 1992: MAL-4 Microcontroller Board,
Pt.1; Simple FM Radio Receiver; Infrared Night
Viewer; Speed Controller For Electric Models, Pt.1;
2kW 24VDC To 240VAC Sinewave Inverter, Pt.2;
Automatic Nicad Battery Discharger; Modifications
To The Drill Speed Controller.
December 1992: Diesel Sound Simulator For
Model Railroads; Easy-To-Build UHF Remote
Switch; MAL-4 Microcontroller Board, Pt.2; Speed
Controller For Electric Models, Pt.2; 2kW 24VDC
To 240VAC Sine
wave Inverter, Pt.3; Index To
Volume 5.
January 1993: Peerless PSK60/2 2-Way Hifi
Loudspeakers; Flea-Power AM Radio Transmitter;
High Intensity LED Flasher For Bicycles; 2kW
24VDC To 240VAC Sinewave Inverter, Pt.4; Speed
Controller For Electric Models, Pt.3; Restoring A
1920s Kit Radio
February 1993: Three Simple Projects For Model
Railroads; A Low Fuel Indicator For Your Car;
Audio Level/VU Meter With LED Readout; Build
An Electronic Cockroach; MAL-4 Microcontroller
Board, Pt.3; 2kW 24VDC To 240VAC Sinewave
Inverter, Pt.5; File Backups With LHA & PKZIP.
March 1993: Build A Solar Charger For 12V
Batteries; An Alarm-Triggered Security Camera;
Low-Cost Audio Mixer for Camcorders; Test Yourself On The Reaction Trainer; A 24-Hour Sidereal
Clock For Astronomers.
April 1993: Solar-Powered Electric Fence; Build
An Audio Power Meter; Three-Function Home
Weather Station; 12VDC To 70VDC Step-Up Voltage Converter; Digital Clock With Battery Back-Up;
A Look At The Digital Compact Cassette.
May 1993: Nicad Cell Discharger; Build The
Woofer Stopper; Remote Volume Control For Hifi
Systems, Pt.1; Alphanumeric LCD Demonstration
Board; Low-Cost Mini Gas Laser; The Microsoft
Windows Sound System.
June 1993: Windows-Based Digital Logic Analyser; Build An AM Radio Trainer; Remote Control For
The Woofer Stopper; A Digital Voltmeter For Your
Car; Remote Volume Control For Hifi Systems,
Pt.2; Double Your Disc Space With DOS 6.
PLEASE NOTE: all issues from November 1987
to August 1988, plus the October 1988 & August
1989 issues, are now sold out. All other issues
are presently in stock, although stocks are low for
older issues. For readers wanting articles from
sold-out issues, we can supply photostat copies (or
tearsheets) at $6.00 per article (incl. p&p). When
supplying photostat articles or back copies, we
automatically supply any relevant notes & errata
at no extra charge.
July 1993 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. Write to: Ask Silicon Chip, PO Box 139, Collaroy Beach, NSW 2097.
Suggestions for the
2kW inverter
This letter is a collection of ideas for
projects that came to me after seeing
John Clarke’s excellent project on the
2kW Sinewave Inverter. This is one of
the best and most interesting projects
I have seen for some time.
No doubt you have had plenty of
people suggesting an auto-start facility on this inverter (essential for a
normal size stand-alone system), so I
would like to add that a 500VA unit
would probably attract even more
interest.
First project idea – a circuit board
which contains the essential components of a universal switchmode DCDC converter; ie, if one wants to go
from 12-32 VDC to the same kind of
range on the output, one puts the appropriate size chokes, capacitors and
other components in the appropriate
place on the board.
Second idea – there are countless
thousands of square-wave output inverters in place around Australia, so
is there some way say, of rectifying the
output of same and then converting
this DC to sine wave. Possible?
Finally, how about a design for a
system to convert 12/24V to 110V DC
High voltage, high
current meter wanted
I have a small problem in that I
have been unsuccessful in finding
simple digital volt meters that are
capable of measuring from 0V-20V
and 0V-2kV, with more emphasis
on the first range. I have also been
unsuccessful in finding digital
current meters that will cover the
range (1) 0A-100A and (2) 0A-2kA,
again with more emphasis on the
first. I wish to run both volt and
amp meters at the same time, so
switching from one to the other
would be inappropriate. (D. C.,
Dunedin, NZ).
92 Silicon Chip
and back down again? The reason for
this is that there are a lot of stand-alone
12/24V systems which need to supply
power over some distance. A typical
situation is where solar panels need
to be located some distance from the
storage batteries. Converting to 110V
and then back down again would
save on transmission losses and, in
many cases, the cost saving in copper
wire would outweigh the cost of the
electronics.
Needless to say, my house runs off
low voltage DC (24V).
In the February 1991 issue, you
had an inverter design for fluorescent
lamps. Would it be possible to give
more information on using these
inverters with the new hybrid fluorescent tubes as they are definitely
more efficient? And how about some
suggestions for reducing RFI, a big
problem for DC power fluoros? (D. A.,
Kyogle, NSW).
• In general, we don’t think a 500VA
version of the 2kW sinewave inverter
would be really practical since its
overall cost is not likely to be substantially less than the 2kW design.
You really do need the grunt of the
big design in order to reliably start
such appliances as refrigerators and
power tools.
• We published a 3½-digit LCD
panel meter in the September 1992
issue of SILICON CHIP. As present
ed, this could be made to read up
to 200V DC and 2A DC.
It could also be made to measure to 2kV, provided the voltage
multiplier string of resistors had
a sufficiently high voltage rating.
However, it would not be practical
to make it read up to 100 amps or
2,000 amps because the necessary
shunts would have vanishingly
low resistance.
The only practical way to measure such high currents is to use a
DC clamp meter. These are readily
available but they are not cheap.
We’re not sure what point there
would be in a universal DC converter
as you suggest. If it was truly universal, it would not need any component
changes and you would merely change
the feed
back to select the output
voltage. But again, what would be its
purpose?
All those square wave inverters
could be rectified as you say and the
resulting DC converted to AC. How
ever, the resulting efficiency would be
poor. Let’s face it, for many applications, a square-wave 240VAC inverter
is quite adequate. Why go for a more
complicated circuit to get no working
improvement?
Finally, and we seem to be knocking all your suggestions, the idea for
stepping up 12V or 24V to 110VAC
and then back down again to reduce
cable costs and losses is problematic.
You would have to take into account
the cost of electronic components at
both ends plus the transformers. There
would inevitably be a significant reduction in efficiency.
One method to reduce the cost of
cable would be to use the Earth as one
side of the circuit. There is nothing
new about this and it is still used in
DC systems. You just have an earthed
metal stake at either end of the system
and just run one cable for the positive
lead. The only drawback is the risk of
corrosion in the earth connections at
either end.
It is doubtful whether the new
hybrid fluorescent lamps with solid-state ballasts are appreciably more
efficient than conventional fluorescent
lamps and they certainly don’t have
the same life expectancy. However,
if a conventional fluorescent tube is
run with an electronic ballast, there
is an improvement in efficiency. The
inverters described in our February
1991 issue will drive the new compact
fluorescent tubes, without the solid
state ballasts (ie, the circuitry in the
lamp base) being necessary. However,
you will get more light out of a conventional tube of equivalent power
rating. It will be cheaper too.
Suppressing the RFI (radio frequency interference) from fluorescent
tubes is very difficult whether or not
they are driven by inverters. The
problem is that the gas discharge
inside the fluorescent tube itself is
the source of the electrical noise.
Connecting a small high voltage ceramic capacitor (say 0.0047µF 3kV)
directly across the tube can help but
you really need to surround the tube
itself with a grounded metal mesh
to make any useful reduction in the
radiated interference.
Combating interference
in hifi systems
Do you have a circuit diagram for a
mains filter and high voltage protection device solely for stereo hifi? The
only kit I could find is the “Mains
Muzzler” (published in January 1989)
which is intended for computers. With
hifi, more care should be taken about
which frequencies are suppressed.
There are mains filter/protectors available for hifi but they are extremely
expensive for some reason. A hardwired device would be preferable to
one using a circuit board. Hoping you
can assist. (P. W., Paraburdoo, WA).
• The only project we have published
along these lines is the “Mains Muzzler”. While it was promoted as being
suitable for computers, it could also
be used for hifi systems. However, in
our experience, mains filters for hifi
systems seldom have much effect. This
is because the interference usually
comes in via the signal leads or the
loudspeaker leads, not via the mains
supply.
The most likely source for the
interference is via the loudspeaker
leads. This can easily be confirmed
by disconnecting the loudspeaker
leads and listening to your system
on headphones. If the system is free
of interference in this mode, then the
interference is definitely coming in via
the speaker leads. The easy solution in
this case is to wind both sets of speaker
leads at least five times through a large
diameter iron dust toroid (available
at outlets like Jaycar and Dick Smith
Electronics).
On the other hand, if the interference is entering via the signal leads,
there is seldom anything you can
do short of modi
fying the internal
circuitry of the offending piece of
equipment. Most people are unable or
Increasing the output of a 3-terminal regulator
Q1
I want to know
MJ2955
+V IN
about the possibility of parallel3. 3
1W
ing two TIP2955s
OUT
IN
LM340
+V OUT
as pass transistors
GND 0.1
1
with a 3-terminal
regulator to in(a)
crease the available current to
above 4A. Could
Q2
0.1
you please tell me
what approximate
2xMJ2955
current this arQ1
0.1
+V IN
rangement would
3. 3
achieve if prop1W
erly heatsunk?
IN
OUT
+V OUT
LM340
Would both tranGND
1
0.1
sistors share the
(b)
same 3.3Ω feed resistor, if its rating Fig.1(a) allows a standard 3-terminal regulator
is increased from to deliver up to 5A, while Fig.1(b) allows two
1W to 2W? What transistors to deliver a total of 8-9A.
other resistors or
components would be required to
of current flowing in the Active
parallel them so that they equally and Neutral wires of the mains
share the current?
supply in a circuit. The Active
and Neutral wires are both wound
Finally, could you explain the
several times through a toroidal
working principle of electric earth
leakage units that are used for pro- core. If both currents are exact, as
tection against electrocution? (L. they normally will be, there will
be no magnetic flux set up in the
B., Tin Can Bay, Qld).
core. If there is a slight imbalance
• If you want more current from a
3-terminal regulator, the standard between the Active and Neutral
booster circuit shown in Fig.1(a) currents, as would happen if there
can deliver 5A. If you want to was a leakage current to earth, then
use two MJ2955s for even more the resulting magnetic flux in the
current, say up to 8A or 9A, the toroidal core generates a voltage in
circuit of Fig.1(b) shows you how. a third winding and this is used to
Note that you don’t need another trip a circuit breaker.
Earth leakage circuit breakers of
3.3Ω resistor but you do need a
this type are sometimes referred to
0.1Ω resistor for each transistor, to
as “core balance relays” and as you
make sure they share the current
can see from the above description,
equally.
this latter name better describes
Earth leakage circuit breakers
their mode of operation.
work by comparing the amount
unwilling to do this and, therefore, it
is a problem that many people have
to live with.
Resistor burn-out in
power amplifier
I have a problem with the 120W
PA Amplifier featured in the issues of
November, December 1988 and January 1989. Basically, my problem is
that the three 12Ω 1W resistors in the
output burn out. It does not happen
immediately upon switch on but after
about two hours of operation, they go
up in smoke. Also the amplifier does
not appear to have its full 120W of
output when compared to another
60W amplifier.
I have measured all the voltages
and they appear to be spot on. I have
changed the output transistors, thinking that this may cure the problem but
to no avail. When the resistors burn
July 1993 93
Life, lawns & the
Woofer Stopper
Your Woofer Stopper in the May
1993 issue gives me renewed hope
and I certainly intend obtaining
one. However, my main trou
ble
with “mutts” and “moggies” is
their nocturnal fouling of lawns
and gardens.
Some time ago I installed a passive IR floodlight unit primarily
as a safety device, but find that it
readily detects and to some extent
scares animals bent on messing up
the place. This in combination with
a slightly modified Woofer Stopper
should completely overcome the
problem.
My thoughts are: (1) since the
flood unit has an adjustable timer
(a few seconds to 15 minutes), it
should be possible to delete the
out, the amplifier has been loaded
with a total of about 60W in speakers
(to the 100V line outputs).
Something that seems odd with
the design in that you say the amplifier output should be loaded with an
output transformer that presents a 4Ω
load, but on checking the data in the
Altronics catalog, the wiring configuration you suggest gives a 16Ω load.
Could this be the problem? (D. W., East
Gresford, NSW).
• We think the most likely reason
why the output resistors are burning out is that the 4.3µH inductor in
parallel with those resistors is open
circuit. That would explain why it
takes an hour or two for the resistors
to fail and also why your amplifier
does not appear to be delivering full
power.
You can easily check whether the
inductor is open circuit (or not properly soldered into circuit) by measuring across the three paralleled 12Ω
resistors with your multimeter. The
reading should be zero ohms but if it
reads four ohms, then the inductor is
open circuit.
You are not the first person to be
confused by the data in the Altronics
catalog. The data is incorrect. The
transformer should be connected as
indicated in the circuit on page 28
of the December 1988 issue; ie, with
94 Silicon Chip
Woofer Stopper timing function
and switch it on/off with the
floodlights; (2) Power a small PSU
from the 240V at the lamps (easily
accessible) to provide a suitable
common DC supply for the modified circuitry. The flood unit is
rated 300W maximum – I use two
100W lamps.
There must be many garden
enthusiasts who would appreciate
such a gadget. Would you please
consider publishing a modified
circuit and description of such a
unit? (A. B., Chittaway Bay, NSW).
• There is no reason why the system would not work (technically)
but whether it would stop dogs
defacing your lawn we do not
know. If the idea receives sufficient reader interest, we shall
consider a version along the lines
you suggest.
primary windings in series and the
secondary windings in series. That
connection “reflects” a load of close
to 4Ω to the amplifier’s output and
allows it to deliver maximum power.
Building the FM
subcarrier adaptor
I wish to build the FM Radio Receiver described in the November
1992 issue of SILICON CHIP. In doing
so, I wish to add on a subcarrier adaptor circuit detailed recently in another
electronics magazine. This will allow
me to receive the increasing number
of ACS (known as SCA in the USA)
transmissions being piggy-backed
onto the FM broadcasts in our capital cities, in the subcarrier range of
67-92kHz.
However, I have a slight problem in
that the adaptor circuit I have states
that it should be connected to the FM
receiver’s detector output, straight after the discriminator but before any filtering and obviously before the stereo
decoder. The article further suggests
that this point could be found (in the
event that you lack a circuit diagram
for the radio) by looking for audio
signals in the high frequency range
around 50kHz near the discriminator
IC or coil, with a level of around a
100mV or so.
It doesn’t seem to matter whether
this signal has some DC present as it is
AC coupled at the input of the adaptor.
This sounds fine if you happen to have
a CRO but I don’t and I also don’t want
to go out and buy your circuit and the
adaptor only to find that it will not
work. Can you suggest the ideal point
to get these signals for the adaptor on
the FM Receiver you described in the
November article?
Having described my problem, you
might like to know that the adaptor
in question requires a fair amount of
basic construction and I am not aware
of any kit resellers that intend to sell
this kit complete. This brings up another point. Would SILICON CHIP be
interested in producing a full ACS
FM receiver in a future issue? An
FM receiver along the lines of the
November 1992 circuit, modified so
that it could receive ACS or normal
FM broadcasts at the flick of a switch,
would be great. What would the readers think of this?
I believe that you produced a sub
carrier adaptor back in January 1988
but I don’t have the article and besides
no-one that I am aware of produces the
kits. I’ve also heard that it requires a
slight modification to its twin-T filter
circuit capacitors in order to receive
signals such as the BBC, etc. Wouldn’t
it be great to combine an FM receiver
and the adaptor all in one? (P. F., Camberwell, Vic).
• The FM Receiver described in our
November 1992 can be used as a
source for the SCA adaptor, as you
suggest. Just take the output directly
from pin 2 of IC1. The SCA adaptor
we described in January 1988 is no
longer available in kit form but the
parts are readily available, including
the PC board.
It is quite simple to modify it to suit
the BBC signals. All you have to do is
change the capacitors in the twin-T
filter from 0.0022µF to 0.0015µF. No
other changes to the circuit should be
necessary.
Notes & errata
Nicad Cell Discharger, May 1993:
transistor Q2 is incorrectly labelled on
the circuit diagram (Fig.1) as a BC328.
It should be a BC338 NPN type, as
shown in the parts list. The parts list
should also be amended to show 1 x
2.7kΩ resistor and 2 x 1.5kΩ (not 1 x
SC
1.5kΩ) resistors.
MARKET CENTRE
Cash in your surplus gear. Advertise it here in Silicon Chip.
ANTIQUE RADIO
ANTIQUE RADIO RESTORATIONS:
specialist restoration service provided
for vintage radios, test equipment &
sales. Service includes chassis rewiring, recondensering, valve testing &
mechanical refurbishment. Rejuvenation of wooden, bakelite & metal cabinets. Plenty of parts – require details
for mail order. About 1200 radios within
16,000 square feet. Two-year warranty
on full restoration. Open Saturday
10am-4.30pm; Sunday 12.30-4.30pm.
109 Cann St, Bass Hill, NSW 2197
Phone (02) 645 3173 BH or (02) 726
1613 AH.
FOR SALE
WEATHER FAX programs for IBM XT/
ATs *** “RADFAX2” $35 is a high resolution, shortwave fax, Morse & RTTY
receiving program. Suitable for CGA,
EGA, VGA and Hercules cards (state
which). Needs SSB HF radio & Radfax
decoder. *** “SATFAX” $45 is a NOAA,
Meteor & GMS weather satellite picture
receiving program. Needs EGA or VGA
plus “WEATHER FAX” PC card. ***
“MAXISAT” $75 is similar to SATFAX
but needs 2Mb expanded memory
(EMS 3.6 or 4.0) and 1024 x 768 SVGA
card. All programs are on 5.25-inch or
3.5-inch disks (state which) & include
documentation. Add $3 postage. Only
from M. Delahunty, 42 Villiers St, New
Farm, Qld 4005. Phone (07) 358 2785.
$13.00 ea; 11-100 = $12.00 ea. P&P
$2.00. Michael Zenere, 7 Hayfield Rd,
My Waverley, Vic 3144. Phone (03)
803 1831.
THE HOMEBUILT DYNAMO: (plans)
brushless, 1000 watt at 740 revs. $A85
postpaid airmail from Al Forbes, PO
Box 3919 - SC, Auckland, NZ. Phone
Auckland (09) 818 8967 any time.
PAY TV & SATELLITE Scrambling News
Monthly, with the latest on descrambling
techniques & addresses, where to buy
the latest descramblers. Send stamp for
info. John Papp, Box 37885 Winnellie,
N.T. 0821.
BURGLAR ALARM KIT: control panel
(no case) $180.00; Remote Keypad
$45.00; P&P $16.00. Michael Zenere,
7 Hayfield Rd, My Waverley, Vic 3144.
Phone (03) 803 1831.
SINGLE CHIP MICROCONTROLLER 68705P3S: 1.8K Eprom. 1-10 =
CLASSIFIED ADVERTISING RATES
Advertising rates for this page: Classified ads: $10.00 for up to 12 words plus 50
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To run your classified ad, print it clearly on a separate sheet of paper, fill out the
form below & send both with your cheque or credit card details to: Silicon Chip
Classifieds, PO Box 139, Collaroy Beach, NSW 2097. Or fax the details to (02)
979 6503.
UNUSUAL BOOKS: electronic devices,
fireworks, locksmithing, radar invisibility,
surveillance, self-protection, unusual
chemistry and more. For a complete
catalog send 95c in stamps to: Vector
Press, Dept S, PO Box 434, Brighton
SA 5048.
VINTAGE RADIO PARTS: numerous
new and used valves, knobs and sundry
parts. For price list, write to: Airwave
Radio Restoration, PO Box 333, North
Hobart, Tas. 7002.
FAX DECODER for satellite and HF
signals. Designed for JV FAX program
offers superb picture resolution and
zoom capability – PCB $29, kit $89;
wideband VHF APT satellite receiver
TRANSFORMER REWINDS
ALL TYPES OF TRANSFORMER REWINDS
TRANSFORMER REWINDS
Reply Paid No.2, PO Box 438, Singleton, NSW
2330. Ph: (065) 76 1291. Fax: (065) 76 1003.
❏ Bankcard ❏ Visa Card ❏ Master Card
Card No.
✂
Enclosed is my cheque/money order for $__________ or please debit my
RCS RADIO PTY LTD
Signature__________________________ Card expiry date______/______
Name ______________________________________________________
Street ______________________________________________________
Suburb/town ___________________________ Postcode______________
RCS Radio Pty Ltd is the only company that manufactures and sells every
PC board and front panel published
in SILICON CHIP, ETI and EA.
RCS Radio Pty Ltd,
651 Forest Rd, Bexley 2207.
Phone (02) 587 3491
July 1993 95
COMPONENTS, COMPUTERS, ELECTRON TUBES
SOME STOCK QTYS LIMITED
ZSI IDE HARD DISKS
RESISTORS
ZM3140 125MB $399
MOST VALUES AVAIL.
DOS 6
$95
1/4W M/FILM
$3/100
2N3440
$1
1/3W CARBON
$2/100
2SC2240
$0.60
1/2W CARBON
$4/100
2SD571
$0.80
1W CARBON
$5/100
MJE243
$0.80
2W CARBON
$8/100
74122
$0.50
5W WIREWOUND
$0.30
747DIL
$0.50
10W RESISTORS
$0.60
8250 $6 8251 $3
8259 $3 6809 $10
KEYTRONICS KB 327OPC KEYBOARDS
$220.00
1620
$8
4042
$10
VALVES
QQV07/50 $30
1B3GT
$4
417A
$8
ECF80
$6
182
$3
5651
$6
12AU7
$6
IT4
$6
5651A
$6
12AU7A $7
CV553
$3
4-400A
$80
12AU7WA $9
2C39A
$50
5651WA $7
12AX7
$8
2C40A
$40
5933S
$30
12BY7A
$10
5933WA $32
3A4
$8
12AV7
$4
6J6WA
$7
3A5
$8
QB3/300 (C1108) $250
150C2
$2
ONE ONLY TBL12/38 TRANSMIT TUBE $2700
PHONE OR MAIL ORDERS, CREDIT CARDS ACCEPTED FOR
ORDERS $20 & OVER, DISCOUNTS FOR QUANTITY ORDERS
SECONTRONICS
PO BOX 2215, BROOKSIDE, QLD 4053, PHONE (07) 355 1314
143 GRAYS RD, ENOGGERA, QLD 4051, FAX (07) 855 1014
SHOP OPEN SATURDAY 9AM - 4PM AH (07) 855 1880
MEMORY & DRIVES
PRICES AT JUNE 1ST, 1993
SIMM
1Mb x 9
70ns
4Mb (72-pin)
4Mb x 9
70ns
4Mb x 8
80ns
DRAM DIP
1 x 1Mb
256 x 4
41256
1Mb x 4
$59
$230
$225
$205
70ns
$6.25
70ns
$6.25
80ns
$2.50
Z or D $26.00
DRIVES
SEAG 42Mb
SEAG 89Mb
SEAG 107Mb
SEAG 130Mb
SEAG 214Mb
28ms
14ms
15ms
16ms
16ms
$205
$292
$310
$335
$470
IBM PS.2
50/55/70
70/35
90/95
2Mb
4Mb
4Mb
$145
$230
$230
TOSHIBA
T3200SX
T44/6400
T5200
T5200
4Mb
4Mb
2Mb
8Mb
$300
$245
$150
$575
MAC
2Mb SI & LC
4Mb P’Book
$104
$270
CO-PROCESSORS
387SX to 25
$110
387DX to 33
$110
Sales tax 20%. Overnight delivery. Credit cards welcome.
Ring for Latest Prices
1st Floor, 100 Yarrara Rd, PO Box 382, Pennant Hills, 2120.
Tel: (02) 980 6988
Fax: (02) 980 6991
PELHAM
EEM Electronics
Printed circuit board assembly, switchmode power supplies repaired. Design
work from start to finish.
Ring anytime 9am-9pm Mon-Sun.
(03) 4011393
PCB $19, kit $78 – includes $5 postage. Send cheque to Technocom, 187
McLarty Road, Halls Head, Mandurah
6210. Phone (09) 581 4297.
ROMLoader EPROM Emulator (EA
Jan/Feb 92) upgrade to handle 27128,
27256 EPROMs. Includes memory edit
facility. 8051 Proto-Boards (EA Feb 93)
also available. Send SAE for details.
Tantau Austra
lia PO Box 1232 Lane
Cove 2066 AH (02) 878 4715
EPROM Reader software is included
with my interface to control the outside
world from a PC parallel port. 32 bits
out. Units can be cascaded. Short form
kit $35. Relay PCB to suit. $15, or send
$2 for my 3.5-inch demo disk. Don Mc
Kenzie, 29 Ellesmere Crescent, Tulla
marine 3043. Ph (03) 338 6286
BATTERIES: 12-volt, 65A.h special Gel
suitable for solar power supplies. 12-volt
to 240-volt applications, camping $100
PH (02) 307291
BUSINESS CENTRAL WEST QLD
for sale. $40,000. Genuine enquiries.
Ph: (076) 58 1928. HF, UHF, TV, VCR
repairs and sales.
96 Silicon Chip
‘HEY LOOK’
AFFORDABLE REPAIRS
PLUS
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AND
MANUFACTURING
GIVE US A CALL NOW
HYCAL ELECTRONICS
Advertising Index
All Electronic Components..........39
Altronics ..........................IFC,28-31
Antique Radio Restorations.........95
A-One Electronics...................68,69
Av-Comm.......................................8
Boston Technology........................9
Cebus Australia...........................36
David Reid Electronics ................3
Dick Smith Electronics.....IBC,12-15
EEM Electronics..........................96
Harbuch Electronics....................36
Hycal Electronics.........................96
Instant PCBs................................96
Jaycar ................................... 45-52
Kalex............................................39
L. E. Chapman.............................89
Nilsen Instruments...................OBC
Oatley Electronics.....................7,37
PC Computers.............................96
Pelham........................................87
Peter C. Lacey Services..............40
RCS Radio ..................................95
Rod Irving Electronics .......... 74-79
Secontronics................................96
Silicon Chip Back Issues........90,91
Silicon Chip Binders....................21
Sportsound (Tandy Dealer).........17
T. A. Mowles.................................96
Tektronix......................................25
Transformer Rewinds...................95
Wombat Electronics.....................87
PH (02) 633 5477 FAX (02) 891 5640
PRINTED CIRCUIT boards for the hobbyist. For service & enquiries contact: T.
A. Mowles (08) 326 5590.
SATELLITE TV SYSTEM: Ku band,
1.8-metre dish, 0.9dB LNB, IR remote
control receiver, feed horn and polariser.
$1085.00 phone: (09) 306 3738 fax: (09)
306 3737.
FOR SALE: 59 issues of SILICON CHIP,
excellent condition, from 1987 on. The
lot $150. Phone 067 658079.
SOLVE YOUR SMALL circuit development problems quickly, try this one.
Parallax BASIC STAMP. A general purpose small circuit module, it is really a
25 x 50mm board with a computer chip
(4MHz PIC 16C56), EEPROM, 8 I/O sink
25mA or source 20mA board space includes 6 x 10 pad prototyping area. Has
216 type battery connections. Program it
on a PC with our development kit which
includes one BASIC STAMP $245 incl
p&p. Commands in
clude POT (crude
A/D), PWM (crude D/A), BUTTON ,
SERIN, SEROUT, SOUND & SLEEP.
Extra BASIC STAMP modules $66 incl
p&p. Reprogram
mable for reuse. For
more info send SAE for data sheet &
circuits. Quantity prices available. Bank
card, Master, Visa or cheque with order.
Parallax of USA products distributor &
technical support in Australia. MicroZed
Computers, PO Box 634, Armidale
2350. Fax (067) 728987.
GLOBAL ELECTRONIC SERVICES:
kits; consultancy; sales & design. Please
write/fax requirement to: Mr Lucas, PO
Box 755, Saint Helier, Jersey JE4 8ZZ,
Channel Islands (UK). Fax (0 534)
80570.
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