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AMATEUR RADIO
BY GARRY CRATT, VK2YBX
How glass mount antennas work
One of the status symbols on cars today is a
small antenna mounted on the rear window for
a mobile \elephone. These antennas have the
advantage that they can be installed without the
need to drill holes for cables but are they as
effective as conventional body mounted
antennas? This article gives the answer.
One of the dilemmas facing today's
amateur is how to mount mobile antennas without permanently marking
or modifying the exterior of a motor
vehicle. In the past, tradition has dictated that a 1/4-wavelength whip antenna mounted in the centre of a vehicle roof provides optimum performance.
.These days, people are far more
reluctant to drill a hole in the centre
of the roof of a brand new motor vehicle for the sake of antenna performance, particularly when they are informed that the performance of a suit-
ably sited glass mount antenna can be
just as good.
Glass mount antennas are available
for a wide range of frequencies, including the now more commonly used
cellular bands (830-890MHz). This
kind of mounting system has considerable appeal to operators using rental
or company vehicles where any modification to the exterior of the vehicle
would be out of the question.
Many communications retailers
now stock glass mount antennas for
VHF, UHF and other radio bands. This
type of antenna is unobtrusive, easily
This photograph shows a typical glass-mount antenna coupling box that has
been modified to form a test probe. The centre conductor of the coaxial feedline
is connected to a conductive plate whose area is the same as that of the
mounting foot of the antenna on the other side of the glass.
78
SILICON CHIP
removed, weatherproof, broadband,
and an ideal alternative to bumper or
boot mounted systems which cannot
provide a good omnidirectional radiation pattern.
If an antenna is to be used without
a groundplane, then theory dictates
that it must be a 1/2-wave antenna
rather than a shorter 1/4-wave whip
which requires a groundplane to form
the symmetrical half of the antenna.
Another consideration when designing a glass mount antenna is the mechanical "foot" that must be used to
mount the radiator. This must be mechanically stable and easily affixed to
any window of a motor vehicle.
Ideally, it should also allow some
adjustment of the angle of elevation
of the antenna to compensate for the
slope of the window, ensuring that
the antenna remains vertical in all
mounting situations.
How they work
To analyse the theory of glass mount
antennas, it is best to consider the
external radiator first. The whip section and the mounting foot comprise
a 1/2-wave resonant radiator. However, due to the loading capacity
caused by the mounting foot and the
dielectric loading resulting from
mounting the foot on glass, the physical length of the radiator will be somewhat shorter than the theoretical
value. However, the radiator will still
be presented as an electrical 1/2-wavelength with voltage loops occurring at
both ends.
The foot can be mechanically
mounted onto the windscreen or rear
window in the motor vehicle using a
suitable adhesive. This has negligible
effect on the performance of the antenna. The impedance of the exterior
radiator is around 2-3kQ. As the patent theory of coupling through glass
is much the same as that of an interstage coupling capacitor, and since
the coupling is done at a high impedance point, very little loss occurs, and
only a small amount of capacitance is
needed for efficient coupling through
the glass.
Fig.1 shows the equivalent circuit
of a glass-mount antenna. In most
modern applications, a 2-element colinear radiator has been chosen which
provides some gain over a standard
1/4-wave whip , and also radiates a
fairly omnidirectional pattern.
Theoretically, two 1/2-wave radiators spaced approximately 0.7 of a
wavelength between centres produce
some gain above that of a 1/4-wave
radiator if they can'1be kept in phase.
Practical experience has shown that
the airwound phasing coil is the best
trade off between the electrical requirement and mechanical robustness.
Most designs use a 5/8-wavelength
upper radiator and a quarter wavelength lower radiator, separated by an
airwound phasing coil. This design is
known as a "3dB" gain antenna.
By stacking and correctly phasing
these two elements, the radiation pattern is compressed, resulting in a
lower angle of radiation. The major
lobe of a 1/4-wavelength antenna is
approximately 30° above the horizon,
while a "3dB " antenna has an angle of
radiation of 8°. Under test conditions ,
it has been shown that a properly
sited "3dB " glass mount antenna can
be made to perform ldB better than a
roof mounted quarter wavelength antenna and, at the same time , provide a
radiation pattern with relatively low
distortion.
Interestingly, one of the design criteria is that a glass-mounted antenna
should be able to survive going
through a car washing system.
The RF energy is coupled through
the glass by placing a coupling box
cl
I SOURCEl
I
GENERAWR
I
I
L-
A---------,.1---]l
.
iJI,
_ _ _j
inside the window and then affixing
the mounting foot precisely over the
same area on the outside of the window. The coupling box contains a tunable LC network, with a high-Q air
dielectric capacitor, formed from a
piece of brass sheet, providing the
means for varying the resonant frequency. A non-conductive screw is
adjusted to distort the brass sheeting,
thereby varying the capacitance. The
bottom end of this sheet connects to
the coaxial cable braid. The centre
conductor of the coaxial feedline is
connected to a conductive plate whose
area is the same as that of the mounting foot on the other side of the glass.
These two parallel 9onductive
plates, together with the glass of the
window, form the capacitor which
couples energy through to the outside
antenna. Typically, the value of capacitance is about 2 to 3pF. At the
resonant frequency, the "hot" end of
the parallel LC circuit is at a high
impedance, whilst the coaxial cable
is tapped to an impedance point of
50Q. Fig.2 shows the circuit represen- ·
tation of this arrangement.
Locating the antenna
Since we know that the optimum
capacitance for good coupling of RF
energy through the glass is around 23pF, it is obvious that incorrect loca-
TRANSFORMER
I
I
I
L-=, . , J
G-_1-S-H-IE-LO-- y I-'
.,. GROUND
"'I"
Fig.1: equivalent circuit for a
glass-mount antenna. Only a
small amount of capacitance
(2-3pF) is required for efficient
coupling through the glass.
a,----,
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I
I
I
I
: :
11
11
11
50tl TRANSMISSION ·
LINE TO TRANSMITTER
AND/OR RECEIVER
Fig.2: the circuit
representation of a
glass-mount antenna.
The energy from the
antenna (A) is coupled
through the glass by
placing the mounting
foot over the coupling
box located inside the
window.
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IFOR No.1 KITS I
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SE PTEMB ER 1991
79
Amateur Radio - glass mount antennas
CHRISTIAN
BLIND
MISSH{~ ·J
Re,$totiK!
:;~~t, be1K
This view inside the coupling box
shows how the adjustment screw is
used to distort the brass plate to
change the tuning capacitance.
She is
just one of the
2.5 million blindnessthreatened people treated
every year by CBMI health
care workers and eye specialists. Millions more are
still waiting for sightsaving
treatment.
tion of either the antenna or coupling
box would severely degrade the performance of a glass mounted antenna.
In an effort to accurately determine
the optimum location for both coupling box and antenna mounting foot,
a simplified test set up has been devised. This allows the measurement
of the capacitance of the glass at any
location on the vehicle.
If the capacitance of the glass falls
within the set limits, the location is
suitable for the mounting of a glass
mount antenna. If capacitance is high,
and this can be the case if the area of
glass to be measured contains demister
wires, mesh or sun screen tinting, the
location will not be optimum.
Test set-up
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The test set up itself is made from
the coupling box of a standard glass
mount antenna. The box has been
modified so that the centre conductor
of the coaxial cable is fed directly to
the PC board coupling plate and the
braid of the coaxial cable goes to the
brass foil sheath inside the coupling
box. This box may then be connected
to a digital multimeter which measures capacitance.
Typically, the DMM should be
switched to its 200pF range, as this
will provide resolution of 0.1 pF. An
additional test lead connected to the
braid of the coaxial cable at the multimeter end and terminated with an
alligator clip at the other end may be
used as an optional vehicle earth connection. With the probe connected to
the digital capacitance meter, the meter will give a particular reading in
free space. By placing the test probe
against the glass, this reading will
increase by several pF.
Placing the probe across demister
wires or window tinting, or even close
to the chrome surround of vehicle
windows, will cause the capacitance
to be higher than optimum for good
RF performance. Hence the probe can
be used to verify that the preferred
mounting location is unaffected by
any of these factors.
If a genuine coupling box from a
glass mount antenna is unavailable,
the test probe may be made from a
zippy box with a PC board in place of
the lid.
Patent protection
Glass mount antennas are protected
in many countries of the world by
patents. The principle of coupling RF
energy through glass dates back as far
as 1929, and developments of this
technique have transpired since that
time until the 1980s. US Patent
4238799 covers a glass mount antenna
system designed for the 2 7MHz CB
bands. Since that time, other variations and improvements have been
made for virtually all radio bands utilised today. In particular, Australian
patent 535273 covers the application
of this technology for cellular use.
The information presented in this
article is for technical interest only.
Readers should be aware that any use
of the information contained in this
article on a commercial basis may
breach intellectual property rights protected by these patents. A commercial version similar to the glass mount
capacitance tester described in this
article is available from the Antennas
Specialist Company, Cliffland, Ohio,
and possibly from their representative in Australia, RF Industries Pty
Ltd - phone (02) 749 1488.
Radio Convention
Radio amateurs who will be in the
"top end" during September should
make it their business to drop in for
the 1991 Radio Convention presented
by the Townsville Amateur Radio
Club. The venue will be the James
Cook University in Townsville, on
27th, 28th and 29th of September. For
further information phone (077) 73
3487 or (077) 74 0211.
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