Shortwave
Antennas This chapter is about antennas used by amateur radio
operators. They are classified under the title of shortwave antennas. Such antennas are
designed using all the principles discussed in previous chapters; the difference is that
they span a very wide range of frequencies. The Radio Amateur Weve all heard the
term ham radio operator. Or we have seen an unusual series of numbers and
letters and the words amateur radio operator on automobile license plates.
Both namesham and amateuridentify a person whose hobby is experimenting with
radio. Amateur radio operators have been around since the birth of radio communications
nearly a century ago. In the early years, the
amateurs were assigned all of the unused frequency spectrum, which at that time was
anything above 1500 kilohertz (1.5 MHz). Recall that wavelength can be calculated from the
following equation:
300,000,000 (meters/sec) Wavelength (meters)=
Frequency (cycles/sec)
If we substitute 1.5 MHz
for the frequency as shown, then
300,000,000 Wavelength=
1,500,000 = 200 meters The wavelength is 200 meters. As a result all the frequencies above
1.5 MHz were called (and still are today) short waves because their wavelength
was shorter than 200 meters. The early amateurs using short waves achieved unheard of
long distance communications. Commercial communications, seeing this success, began
using short waves, and started crowding out the amateurs. To settle the
issue, an international conference allocated the frequencies to be used for various
activities, and reserved specific bands of frequencies for use by amateurs. Amateur Frequency Bands
Figure 9-1 shows the frequency spectrum indicating the frequency allocation to the various well known services, and indicating the common amateur frequency bands. The lowest amateur frequency is the 160-meter band. This band, just above the AM broadcast band, is subject to special frequency and power limitations which vary according to geographical location. The limitations have been established to prevent interference with LORAN (long-range navigation) stations. Table 9-1 indicates the major amateur bands by the common wavelength in meters. You will hear hams say that they are working at 15 meters or 10 meters, or 2 meters. This means they are transmitting and receiving on a frequency within the respective band.
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Types Of Shortwave Antennas Electrical Length vs Physical LengthBecause it gives the half-wave length in feet, a somewhat easier
equation for the half-wavelength of an antennas is:
492
Half-wave Length (in feet) =
Frequency (in Megahertz) However, the half-wave length that one
actually uses for the physical length is about 5% shorter than that calculated with the
above equation. The reason for this is that the electrical length of the antenna is
different than its physical length. The antenna wire is usually fastened to insulators by
making several twists or wraps at the ends. This produces what is known as end
effect. End effect, and the fact that energy travels along the antenna wire at
slightly less than its free space velocity, makes the effective electrical length about 5%
longer than the physical length. Long Wire AntennasProbably the most common type of antenna used by early radio
amateurs was a long wire antenna. This type of antenna is a horizontal wire antenna which
is at least one wavelength long, sometimes much longer. It may or may not have a
terminating resistor, as shown in Figure 9-2. When
no terminating resistor is used, it is bidirectional, with the maximum response off both
ends. If the terminating resistor is used, maximum response is off the terminated end. Zepp (or Zeppelin) A type of end-fed antenna shown in Figure 9-3 is called a Zepp antenna. They get
their name because they were first used on the German lighter-than-air dirigibles called
Zeppelins. This antenna is one-half wavelength at the lowest frequency. The impedance at the end is much higher (e.g. 1000 ohms or more)
than the -impedance at the center of a resonant dipole (75 ohms). Usually widely spaced 2-wire transmission line is used to couple to the antenna, and a
matching box must be used between the transmitter and the transmission line. Shortwave Listening
For the person interested in antennas for shortwave listening, a long wire antenna that is portable (Radio Shack catalog no. 278-1 374) and can be used for quick, temporary setups is a coiled unit that clips over a telescoping antenna and can be extended to 23 feet like a measuring tape.
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Vertical Antennas
Another very popular amateur antenna is a vertical antenna. In
Chapter 1 we showed the omnidirectional pattern of a vertical quarter-wavelength antenna.
Generally, the radiation pattern of the vertical antenna is not deflected upwards by the
ground nearly as much as the pattern of the horizontal antenna. Figure 9-4 shows how increasing the length of the
vertical antenna affects the radiation pattern, Increasing the frequency while keeping
length constant produces exactly the same result.
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Loops
A loop consists of one or more turns of wire wrapped around a
supporting structure that is shaped into a rectangle or a circle. Figure 9-5 shows examples of loop antennas. A loop
is quite directive and relatively compact, which makes it attractive for portable
equipment. Its small size makes it easy to rotate for either maximum sensitivity or
minimum interference. It is usually much smaller than the wavelength at which it is used.
Its characteristics can be modified by changing the antenna Q (quality factor). This is
usually done with a fixed or adjustable magnetic (ferrite) core. The radiation resistance
of small loops is so low that it is nearly impossible to match a transmitter to them, so
that loops are used primarily for receiving. Beam Antennas
An antenna is called a beam antenna when its radiation/reception pattern is a very narrow beam to make it a very directional antenna. Weve seen many examples of Yagi antennas which are beam antennas. Hams use beam antennas at all frequencies. You may have noticed very large Yagi type arrays mounted on a tower in the backyard of an amateur radio operator. In many cases, the antennas can be rotated. Beam antennas are about the only type shortwave antennas besides loops that can be rotated easily to permit efficient transmission and reception in any direction.
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Quad-Cubical Antennas
An antenna that combines directivity and loop antenna
characteristics is the quad-beam antenna shown in Figure
9-6. It is one of the more effective long range shortwave antennas. It consists of two
or more square loops of wire supported by spreaders that were often made from bamboo,
although fiberglass is more common today. The length of each side of the square is equal
to a quarter wavelength of the transmitted signal. Loops may be either driven or
parasitic. If parasitic elements are used, they have the same dimensions as the driven
element. By tuning with shorted tuning stubs, the parasitic loop may be made to function
as either a reflector or director, giving the antenna its directivity characteristics. In Figure 9-6, the parasitic element is a reflector. Collinear Arrays
A collinear array consists of two or more elements mounted in-line
along the same axis, with the current in each element in the same direction (in phase) as
all other elements. The radiation pattern is bidirectional, with maximum radiation at
right angles to the line of the elements. Although large collinear arrays may contain from
48 elements to as many as 128 elements, amateur arrays rarely contain more than 4
elements. Other Antennas
There are other less frequently used types, such as the V and rhombic antennas, and broadside and endfire arrays. Information on these types, as well as more detailed descriptions of the antennas described above can be found in The ARRL Antenna Handbook, published by the American Radio Relay League, Newington, Connecticut, an association for radio amateurs.
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Antenna Placement
Most of the predictions of antenna performance are based on
free-space behavior. Objects surrounding an antenna after it is mounted may affect its
performance significantly. The erection of new buildings, the growth of trees, adjacent
wires or towers are common environmental changes that occur to change an antennas
performance. As we have stated many times throughout this book, one of the best ways to isolate an antenna is to mount it high above other obstructions. This may be very difficult for the very large and heavy antennas used for the lower frequency amateur bands. If the antenna is not mounted high enough its radiation/reception pattern will be affected. For example, Figure 9-7 shows vertical radiation patterns of a horizontal antenna at various heights above ground. Generally the lower the antenna, the more the radiated (or received) wave is directed upwards. Consequently, the antenna position adversely affects long range communication. Also, the impedance of an antennas is dramatically reduced for heights much less than one quarter wavelength.
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Antenna
Measurements
We have found that antenna performance characteristics vary because
of a number of factors. Several that have been mentioned are: electrical length is
different than physical length, the placement of the antenna, and the impedance matching
of the antenna to its transmission line. It is necessary to have the correct
characteristics for good signal reception when using any antenna, but it is particularly
important if one is transmitting on a shortwave band. Maximum performance cannot be
obtained unless the antenna and transmitter are properly adjusted. One of the best ways to
verify that an antenna has the characteristics desired is to make several measurements
after the antenna has been installed. Grid-Dip Meters
One of the instruments that has been used for many years by ham
operators to measure radio frequencies is the grid-dip meter. With this meter, it is
possible to determine and adjust the frequency of tuned circuits, including antennas,
without applying high power from the transmitter. A typical grid-dip meter is a handheld,
battery-powered instrument containing a tunable oscillator with a scale or dial that is
calibrated in frequency. The meter has a probe or coupling loop that couples energy into
or out of the grid-dip oscillator (GDO) circuit. When the coupling loop is held near a
tuned circuit and the frequency is varied, the resonant frequency of the tuned circuit can
be detected. At resonance, the circuit absorbs the maximum power from the GDO. This causes
a meter in the oscillator circuit to drop (dip) as the GDO is tuned through a resonant
frequency of the circuit. In like fashion, when a loop is connected from the grid-dip
meter to antenna terminals, energy from the oscillator is fed to the antenna and its
resonant frequency may be determined. In other applications, the GDO does not radiate energy but is used
as an absorption wave meter to absorb energy from a live circuit. As the grid-dip
meter is tuned to the frequency of the energy in the circuit, the meter rises to a peak.
With a transmitter on and the grid-dip meter probe close to the antenna, the frequency of
the transmitter is determined by tuning the grid-dip meter for a maximum reading. Or the
grid-dip meter tuning can be set on the desired transmitter frequency, and the
transmitter tuned until the meter reads maximum. SWR
A very useful measurement to make on the transmission line from the
transmitter to the antenna is the standing wave ratio (SWR). Recall that if there is a
mismatch of impedances along the circuit including the transmitter, transmission line,
and antenna, there will be an inefficient transfer of energy. Not all the energy will
flow forward from transmitter to the antenna. Some of it will be reflected and set up a
standing wave on the transmission line. A standing wave ratio meter is shown in Figure 9-8. It has cable connections so that it
can be inserted into the transmission line and the standing wave ratio measured. By
placing the meter selector switch in the CALIBRATION position, the forward energy
measured by the meter is set at a calibration point (full-scale); in the SWR position,
the meter measures the reflected energy and allows the SWR to be read directly. A properly
matched circuit will have an SWR below 1.5 (about 4% reflected energy). To properly match the antenna to the transmission line, or vice
versa, the meter is inserted between the transmission line and the antenna, and the
antenna or transmission line impedance changed until the minimum reflected energy is
obtained. This is a much easier and much more effective measurement than trying to
measure the antenna impedance directly. SHORTWAVE ANTENNA PROJECTSNow
that we know the type of antenna used for various applications, lets look at a
number of antenna project that you can build for your particular frequency application.
We have chosen antennas that will be particularly useful for people that listen on shortwave, listen to scanner radios, are active ham operators, or that have business and mobile radio applications. Diagrams with dimensions, parts lists and construction details are included in order to make it easy for you to build useful antennas.The only equations we will
use will be those needed to calculate antenna element lengths, which are derived from the
basic equation for wavelength given in Chapter 9 and repeated here.
x, wavelength in meters =
300 (meter/sec) Frequency (In megahertz) Since a meter equals 3.28 feet, x, wavelength in feet =
984 (feet/sec) Frequency (In megahertz)
Thus, a half-wavelength in feet,
=
492
2 Frequency (in
Mhz) In thin conductors there are self-inductance effects that make the
physical length 5% shorter than the theoretical or Free Space length.
Therefore, we use the following equation for one-half wavelength antennas, Dipole length in feet, x =
468
2
Frequency (in Mhz) And for a one-quarter wavelength antenna, Element length in feet, x =
234
4 Frequency
(in Mhz) SHORTWAVE LISTENING
Project No.1 Long Wire Antennas The oldest antenna used by Shortwave Listeners (SWLers) has been the long wire. We talked about long wire antennas in Chapter 9 and showed the radiation pattern of a long wire. Antennas have reciprocality. This means that the receive pattern is identical to the transmit pattern. However, when receiving shortwave signals, it is not as important to match the feed line. Just run a wire 20 to 150 feet to some nearby support. Trees work well, other
buildings, or even a pole put up for this purpose. It is good to get the antenna as high
off ground as practical, but keep your long wire antenna away from electrical wires! Not
only for safety, but also because noise can be coupled from power lines. On the lower frequencies, a long wire will favor signals off the sides. As you go up in frequency it will tend to favor signals off the ends. If you have enough room, run long wire antennas in different directions to favor different parts of the world. However, if you do, you should use a video switch like the one in Project No. 4 to isolate each antenna. Figure 11-1 shows a typical installation.
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Parts List for Long Wire Antenna
QtY. Description
Catalog No.
2
Insulators Stand-off screw mount
15-853
(choose type)
Stand-off masonry
15-820
Stand-off strap mount
15-823
Mini-egg
278-1335 As required Antenna wire 70
roll 14-gauge stranded copper
278-1329
1
Ground wire 40 8-gauge aluminum
15-035
1
Ground rod 8 copper-plated
15-529 Project No. 2
Vertical Wires Another very simple antenna
for listeners to shortwave radio is the vertical antenna. We showed the radiation pattern
of a vertical antenna in Figure 9-4. A vertical antenna is very
simple to make, just run 8 to 15 feet of wire straight up from your radio. Your vertical
will be omni-directional and pick up signals equally well from all directions. Your
vertical will also pick up less manmade noise. Thats because most man-made noise
is horizontally polarized. Any kind of wire will do, speaker wire, power cord wire, magnet wire and the like, as long as it is stiff enough to stand alone. Or you can secure the top end of it to hold it as long as you do not short it out. Just strip the insulation off the bottom end and attach to your radios antenna connection. Figure 11-2 shows the simple installation.
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Project No.3
Fan Dipole
The fan dipole is a time
honored antenna among shortwave listeners. Each wire in
the fan is a dipole antenna cut for a shortwave band. Every SWLer has their favorite
bands. Listed are the dipole lengths for the common shortwave broadcasting bands. The
lengths are calculated for the top frequency in the band.
SW Band (Meters)
Length (In feet)
49M
75ft
41M
63ft
31M
47ft
25M
38ft
21M
34ft
19M
30ft
16M
24ft
13M
21ft Your author has used as many as 5 dipoles on one antenna. It is necessary to keep the ends of the individual dipoles at least a foot apart to prevent interaction between dipoles. A typical installation is shown in Figure 11-3.
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Choose the end insulator
that will work best for your installation. Use
the nylon rope to tie the other end of the
insulator to a tree or pole. Each dipole will have a different length. Make sure that you
solder all wires together at the Dogbone insulator. Poor solder joints will
produce unreliable and noisy connections. You may have to use an adapter to match the
RG-59U coax connector to your receiver. Parts List for Fan Dipole Antenna
Qty.
Description
Catalog No. As required
Antenna wire 70 roll 14-gauge
stranded
copper
278-1329
1
Dogbone insulator
278-1336 2 per dipole
End insulators Screw mount
15-853 (choose type) Masonry
mount
15-820
Strap mount
15-823 As required
RG-59U coax
278-1315
1
Cable tie
278-1622
or 278-1652 As required
Light nylon rope or heavy duty fishing line
RF adapter connector
To match receiver Project No.4 The Complete SWL Station Here is an installation for
the avid listener to shortwave radio. With various skip angles and reflections from other
metal objects around your station, it is hard to predict which antenna will work best. And
the best antenna will change with the time of day and the station you are
listening to. In this installation, there are several antennas and a video switch as shown
in Figure 11-4a. By having several antennas, you can switch around until the
signal is clearest. The high isolation and low loss of a video switch is ideal in this
application. Your long wire and vertical antennas can be easily converted to F connectors for use with the video switch. Just cut in half a 75-ohm coax patch cable with F connectors on each end, available at Radio Shack. Solder the center conductor of the coax to your antenna wire, as shown in Figure 11-4b. This makes a compatible connector to the video switch. The other half of the cable can be used between the switch and the receiver. However, you may have to use an adapter at the receiver depending on the receiver input connections. If you use the fan dipole antenna, you may need an adapter connector to match the RG-59U connector of the antenna to the video switch. Radio Shack has many adapters available. Choose the video switch with the number of inputs equal to the number of antennas you want to use. The parts list only includes the additional parts required for the switching. The parts for each antenna are listed previously with the antenna.
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Parts List for SWL Station
Switching
Oty.
Description
Catalog No.
1
Video switch 2 inputs
15-1247
(choose type)
3 inputs
15-1248
2 inputs, high-isolation 15-1249
As required
Ant. patch cable 4 ft.
15-1533
RF adapter connector
To match receiver The section, shortwave antennas was written by Alvis J. Evans and the section, shortwave antenna projects was written by Kent E. Britain. These selected sections are only two from a book called ANTENNAS Forth Edition and is available at Radio Shack (part #62-1083B). The information here is a small part of what is covered within the book mentioned. The information contained here is provided free and for educational purposes only.
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