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Antenna
Materials and
Accessories
Chapter
20
This chapter contains information on materials
amateurs use to construct antennas—what types of material
to look for in a particular application, tips on working with
and using various materials. Chapter 21 contains information
on where to purchase these materials.
Basically, antennas for MF, HF, VHF and the
lower UHF range consist simply of one or more
conductors that radiate (or receive) electromagnetic waves.
However, an antenna system must also include some
means to support those conductors and maintain their
relative positions—the boom for a Yagi antenna and the
halyards for a wire dipole, for example. In this chapter we’ll
look at materials for those applications, too. Structural
supports, such as towers, masts and poles, are discussed in
Chapter 22 .
There are two main types of material used for
antenna conductors, wire and tubing. Wire antennas are
generally simple and therefore easier to construct, although
some arrays of wire elements can become rather complex.
When tubing is required, aluminum tubing is used most often
because of its light weight. Aluminum tubing is discussed
in a subsequent section of this chapter.
Wire Antennas
Although wire antennas are relatively simple, they can
constitute a potential hazard unless properly constructed.
Antennas should never be run under or over public utility
(telephone or power) lines. Several amateurs have lost their
lives by failing to observe this precaution.
The National Electric Code ® of the National Fire
Protection Association contains a section on amateur stations
in which a number of recommendations are made concerning
minimum size of antenna wire and the manner of bringing
the transmission line into the station. Chapter 1 contains
more information about this code. The code in itself does
not have the force of law, but it is frequently made a part of
local building regulations, which are enforceable. The
provisions of the code may also be written into, or referred
to, in fire and liability insurance documents.
The RF resistance of copper wire increases as the size
of the wire decreases. However, in most types of antennas
that are commonly constructed of wire (even quite small
wire), the radiation resistance will be much higher than the
RF resistance, and the efficiency of the antenna will still be
adequate. Wire sizes as small as #30, or even smaller, have
been used quite successfully in the construction of
“invisible” antennas in areas where more conventional
antennas cannot be erected. In most cases, the selection of
wire for an antenna will be based primarily on the physical
properties of the wire, since the suspension of wire from
elevated supports places a strain on the wire.
WIRE TYPES
Wire having an enamel coating is preferable to bare
wire, since the coating resists oxidation and corrosion.
Several types of wire having this type of coating are
available, depending on the strength needed. “Soft-drawn”
or annealed copper wire is easiest to handle; unfortunately,
it stretches considerably under stress. Soft-drawn wire should
be avoided, except for applications where the wire will be
under little or no tension, or where some change in length
can be tolerated. (For example, the length of a horizontal
antenna fed at the center with open-wire line is not critical,
although a change in length may require some readjustment
of coupling to the transmitter.)
“Hard-drawn” copper wire or copper-clad steel wire
(also known as Copperweld TM ) is harder to handle, because
it has a tendency to spiral when it is unrolled. These types
of wire are ideal for applications where significant stretch
cannot be tolerated. Care should be exercised in using this
wire to make sure that kinks do not develop—the wire will
have a far greater tendency to break at a kink. After the coil
has been unwound, suspend the wire a few feet above ground
for a day or two before using it. The wire should not be
recoiled before it is installed.
Several factors influence the choice of wire type and
size. Most important to consider are the length of the
unsupported span, the amount of sag that can be tolerated,
the stability of the supports under wind pressure, and whether
Antenna Materials and Accessories
20-1
1361082838.070.png
or not an unsupported transmission line is to be suspended
from the span. Table 1 shows the wire diameter, current-
carrying capacity and resistance of various sizes of copper
wire. Table 2 shows the maximum rated working tensions of
hard-drawn and copper-clad steel wire of various sizes. These
two tables can be used to select the appropriate wire size for
an antenna.
3) Choose an operating tension level (in pounds) consistent
with the values presented in Table 2 (preferably less than
the recommended wire tension).
4) Draw a line from the tension value chosen (plotted on
the tension axis) through the point where the work axis
crosses the original line constructed in step 2, and continue
this new line to the sag axis.
5) Read the sag in feet on the sag axis.
Example:
Weight = 11 pounds/1000 feet
Span = 210 feet
Tension = 50 pounds
Answer: Sag = 4.7 feet
WIRE TENSION
If the tension on a wire can be adjusted to a known
value, the expected sag of the wire ( Fig 1 ) may be determined
before installation using Table 2 and the nomograph of
Fig 2 . Even though there may be no convenient method to
determine the tension in pounds, calculation of the expected
sag for practicable working tensions is often desirable. If
the calculated sag is greater than allowable it may be reduced
by any one or a combination of the following:
1) Providing additional supports, thereby decreasing the span
2) Increasing the tension in the wire if less than
recommended
3) Decreasing the size of the wire
These calculations do not take into account the weight of a
feed line supported by the antenna wire.
Instructions for Using the Nomograph
1) From Table 2 , find the weight (pounds/1000 feet) for
the particular wire size and material to be used.
2) Draw a line from the value obtained above, plotted on
the weight axis, to the desired span (feet) on the span axis,
Fig 2 . Note in Fig 1 that the span is one half the distance
between the supports.
Fig 1—The span and sag of a long-wire antenna.
Table 1
Copper-Wire Table
Turns
Turns
Wire
per
Feet
Ohms
Cont.-duty
Wire
per
Feet
Ohms
Cont.-duty
Size
Dia
Linear
per
per
current 2
Size
Dia
Linear
per
per
current 2
AWG
in
Dia
Inch
Pound
1000 ft
Single Wire
AWG
in
Dia
Inch
Pound
1000 ft
Single Wire
(B&S)
Mils 1
in mm
Enamel
Bare
25
°
C
in Open Air
(B&S)
Mils 1
in mm
Enamel
Bare
25
°
C
in Open Air
1
289.3
7.348
—
3.947
0.1264
—
22
25.3
0.644
37.0
514.2
16.46
—
2
257.6
6.544
—
4.977
0.1593
—
23
22.6
0.573
41.3
648.4
20.76
—
3
229.4
5.827
—
6.276
0.2009
—
24
20.1
0.511
46.3
817.7
26.17
—
4
204.3
5.189
—
7.914
0.2533
—
25
17.9
0.455
51.7
1031
33.00
—
5
181.9
4.621
—
9.980
0.3195
—
26
15.9
0.405
58.0
1300
41.62
—
6
162.0
4.115
—
12.58
0.4028
—
27
14.2
0.361
64.9
1639
52.48
—
7
144.3
3.665
—
15.87
0.5080
—
28
12.6
0.321
72.7
2067
66.17
—
8
128.5
3.264
7.6
20.01
0.6405
73
29
11.3
0.286
81.6
2607
83.44
—
9
114.4
2.906
8.6
25.23
0.8077
—
30
10.0
0.255
90.5
3287
105.2
—
10
101.9
2.588
9.6
31.82
1.018
55
31
8.9
0.227
101
4145
132.7
—
11
90.7
2.305
10.7
40.12
1.284
—
32
8.0
0.202
113
5227
167.3
—
12
80.8
2.053
12.0
50.59
1.619
41
33
7.1
0.180
127
6591
211.0
—
13
72.0
1.828
13.5
63.80
2.042
—
34
6.3
0.160
143
8310
266.0
—
14
64.1
1.628
15.0
80.44
2.575
32
35
5.6
0.143
158
10480
335
—
15
57.1
1.450
16.8
101.4
3.247
—
36
5.0
0.127
175
13210
423
—
16
50.8
1.291
18.9
127.9
4.094
22
37
4.5
0.113
198
16660
533
—
17
45.3
1.150
21.2
161.3
5.163
—
38
4.0
0.101
224
21010
673
—
18
40.3
1.024
23.6
203.4
6.510
16
39
3.5
0.090
248
26500
848
—
19
35.9
0.912
26.4
256.5
8.210
—
40
3.1
0.080
282
33410
1070
—
20
32.0
0.812
29.4
323.4
10.35
11
1 A mil is 0.001 inch.
2 Max wire temp of 212 ° F and max ambient temp of 135 ° F.
21
28.5
0.723
33.1
407.8
13.05
—
20-2
Chapter 20
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Table 2
Stressed Antenna Wire
American Recommended Tension 1 (pounds) Weight (pounds per 1000 feet)
Wire Gauge Copper-clad Hard-drawn Copper-clad Hard-drawn
steel 2 copper steel 2 copper
4 495 214 115.8 126.0
6 310 130 72.9 79.5
8 195 84 45.5 50.0
10 120 52 28.8 31.4
12 75 32 18.1 19.8
14 50 20 11.4 12.4
16 31 13 7.1 7.8
18 19 8 4.5 4.9
20 12 5 2.8 3.1
1 Approximately one-tenth the breaking load. Might be increased 50% if end supports are firm and there is no danger of ice loading.
2 Copperweld, TM 40% copper.
Wire Splicing
Wire antennas should preferably be made with unbroken
lengths of wire. In instances where this is not feasible, wire
sections should be spliced as shown in Fig 3 . The enamel
insulation should be removed for a distance of about 6 inches
from the end of each section by scraping with a knife or
rubbing with sandpaper until the copper underneath is bright.
The turns of wire should be brought up tight around the
standing part of the wire by twisting with broad-nose pliers.
The crevices formed by the wire should be completely
filled with rosin-core solder. An ordinary soldering iron or
gun may not provide sufficient heat to melt solder outdoors;
a propane torch is desirable. The joint should be heated
sufficiently so the solder flows freely into the joint when the
source of heat is removed momentarily. After the joint has
cooled completely, it should be wiped clean with a cloth, and
then sprayed generously with acrylic to prevent corrosion.
ANTENNA INSULATION
To prevent loss of RF power, the antenna should be
well insulated from ground, unless of course it is a shunt-
fed system. This is particularly important at the outer end or
ends of wire antennas, since these points are always at a
comparatively high RF potential. If an antenna is to be
installed indoors (in an attic, for instance) the antenna may
be suspended directly from the wood rafters without
additional insulation, if the wood is permanently dry. Much
greater care should be given to the selection of proper
insulators when the antenna is located outside where it is
exposed to wet weather.
Fig 2—Nomograph for determining wire sag. (John
Elengo, Jr, K1AFR)
Insulator Leakage
Antenna insulators should be made of material that will
not absorb moisture. The best insulators for antenna use are
made of glass or glazed porcelain. Depending on the type of
material, plastic insulators may be suitable. The length of an
insulator relative to its surface area is indicative of its
comparative insulating ability. A long thin insulator will have
less leakage than a short thick insulator. Some antenna
insulators are deeply ribbed to increase the surface leakage
path without increasing the physical length of the insulator.
Shorter insulators can be used at low-potential points, such
as at the center of a dipole. If such an antenna is to be fed
Antenna Materials and Accessories
20-3
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with open-wire line and used on several bands, however,
the center insulator should be the same as those used at the
ends, because high RF potential may exist across the center
insulator on some bands.
stress ratings of antenna insulators are typical:
5 / 8 in. square by 4 in. long—400 lb
1 in. diameter by 7 or 12 in. long—800 lb
1 1 / 2 in. diameter by 8, 12 or 20 in. long, with special
metal end caps—5000 lb
These are rated breaking tensions. The actual working
tensions should be limited to not more than 25% of the
breaking rating.
The antenna wire should be attached to the insulators
as shown in Fig 4 . Care should be taken to avoid sharp
angular bends in the wire when it is looped through the
insulator eye. The loop should be generous enough in size
that it will not bind the end of the insulator tightly. If the
length of the antenna is critical, the length should be
measured to the outward end of the loop, where it passes
through the eye of the insulator. The soldering should be
done as described earlier for the wire splice.
Insulator Stress
As with the antenna wire, the insulator must have
sufficient physical strength to support the stress of the
antenna without danger of breakage. Long elastic bands or
lengths of nylon fishing line provide long leakage paths and
make satisfactory insulators within their limits to resist
mechanical strain. They are often used in antennas of the
“invisible” type mentioned earlier.
For low-power work with short antennas not subject
to appreciable stress, almost any small glass or glazed-
porcelain insulator will do. Homemade insulators of Lucite
rod or sheet will also be satisfactory. More care is required
in the selection of insulators for longer spans and higher
transmitter power.
For a given material, the breaking tension of an insulator
will be proportional to its cross-sectional area. It should be
remembered, however, that the wire hole at the end of the
insulator decreases the effective cross-sectional area. For this
reason, insulators designed to carry heavy strains are fitted
with heavy metal end caps, the eyes being formed in the metal
cap, rather than in the insulating material itself. The following
Strain Insulators
Strain insulators have their holes at right angles, since
they are designed to be connected as shown in Fig 5 . It can
be seen that this arrangement places the insulating material
under compression, rather than tension. An insulator
connected this way can withstand much greater stress.
Furthermore, the wire will not collapse if the insulator breaks,
since the two wire loops are interlocked. Because the wire
is wrapped around the insulator, however, the leakage path
is reduced drastically, and the capacitance between the wire
loops provides an additional leakage path. For this reason,
the use of the strain insulator is usually confined to such
applications as breaking up resonances in guy wires, where
high levels of stress prevail, and where the RF insulation is
of less importance. Such insulators might be suitable for
use at low-potential points on an antenna, such as at the
center of a dipole. These insulators may also be fastened in
the conventional manner if the wire will not be under
sufficient tension to break out the eyes.
Insulators for Ribbon-Line Antennas
Fig 6A shows the sketch of an insulator designed to be
used at the ends of a folded dipole or a multiple dipole made
of ribbon line. It should be made approximately as shown,
out of Lucite or bakelite material about 1 / 4 inch thick. The
advantage of this arrangement is that the strain of the antenna
Fig 3—Correct method of splicing antenna wire. Solder
should be flowed into the wraps after the connection is
completed. After cooling, the joint should be sprayed
with acrylic to prevent oxidation and corrosion.
Fig 4—When fastening antenna wire to an insulator, do
not make the wire loop too snug. After the connection
is complete, flow solder into the turns. Then when the
joint has cooled completely, spray it with acrylic.
Fig 5—Conventional manner of fastening wire to a strain
insulator. This method decreases the leakage path and
increases capacitance, as discussed in the text.
20-4
Chapter 20
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is shared by the conductors and the plastic webbing of the
ribbon, which adds considerable strength. After soldering,
the screw should be sprayed with acrylic.
Fig 6B shows a similar arrangement for suspending
one dipole from another in a stagger-tuned dipole system. If
better insulation is desired, these insulators can be wired to
a conventional insulator.
clothesline pulley has a 4-inch diameter plastic wheel with
a 1 / 4 -inch shaft running in bronze bearings. The sheath is
made of cast or forged corrosion-proof alloy. Some look-
alike low-cost pulleys of this type have an aluminum shaft
with no bearings. For antenna work, these cheap pulleys are
of little long-term value.
Marine pulleys have good weather-resisting qualities,
since they are usually made of bronze, but they are
comparatively expensive and are not designed to carry heavy
loads. For extremely long spans, the wood-sheathed pulleys
used in “block and tackle” devices and for sail hoisting
should work well.
PULLEYS AND HALYARDS
Pulleys and halyards commonly used to raise and lower
a wire antenna must also be capable of taking the same strain
as the antenna wire and insulators. Unfortunately, little
specific information on the stress ratings of most pulleys is
available. Several types of pulleys are readily available at
almost any hardware store. Among these are small
galvanized pulleys designed for awnings and several styles
and sizes of clothesline pulleys. Heavier and stronger pulleys
are those used in marine work. The factors that determine
how much stress a pulley will handle include the diameter
of the shaft, how securely the shaft is fitted into the sheath
and the size and material of the frame.
Another important factor to be considered in the
selection of a pulley is its ability to resist corrosion.
Galvanized awning pulleys are probably the most susceptible
to corrosion. While the frame or sheath usually stands up
well, these pulleys usually fail at the shaft. The shaft rusts
out, allowing the grooved wheel to break away under tension.
Most good-quality clothesline pulleys are made of
alloys which do not corrode readily. Since they are designed
to carry at least 50 feet of line loaded with wet clothing in
stiff winds, they should be adequate for normal spans of
100 to 150 feet between stable supports. One type of
Fig 7—This is one type of knot that will hold with
smooth rope, such as nylon. Shown at A, the knot for
splicing two ends. B shows the use of a similar knot in
forming a loop, as might be needed for attaching an
insulator to a halyard. Knot A is first formed loosely
10 or 12 in. from the end of the rope; then the end is
passed through the eye of the insulator and knot A.
Knot B is then formed and both knots pulled tight.
(Richard Carruthers, K7HDB)
Fig 6—At A, an insulator for the ends of folded dipoles, or multiple dipoles made of 300-ohm ribbon. At B, a method
of suspending one ribbon dipole from another in a multiband dipole system.
Antenna Materials and Accessories
20-5
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