Amateur Radio Report Card
1 - Free and Open Source Software
1 - Free and Open Source Software
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TYPE<br />
uN" CONNECTOR<br />
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~ 11 8 SOFT COPPER WI RE<br />
----- , · "'''~-----<br />
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------ 6 - 5 / 8"~------_I<br />
Fig. 4 . Balun dimension s.<br />
long and 14 inches high should be attached<br />
to the dipole side of the mast.<br />
The mesh can be held in place with wire<br />
and then spot soldered to the mast with a<br />
heavy iron or propane torch.<br />
The dipoles should then be soldered in<br />
place.<br />
It will be noted from Fig. 3 that the J<<br />
wave phasings stubs are actually longer than<br />
the length required and that shorting bars are<br />
used to set the final adjustment. In all probability,<br />
this array will perform properly if<br />
the shorts are set to the measurements given,<br />
however, if the time can be spared, a simple<br />
diode test stand step up with a signal source<br />
of some sort will allow the array to be<br />
tweaked just to be sure.<br />
If the test stand method is used, it should<br />
be found that, when the shorts are tweaked<br />
for maximum gain, the horizontal beam width<br />
of th e antenna is at a minimum which should<br />
be about 16 degrees.<br />
As with many antennas, the beam direction<br />
can be changed by altering the phasing<br />
balance among the dipoles. Be sure to set<br />
all the shorts the same distance. It is possible<br />
to achieve the proper beam width and then<br />
squirt the beam out sideways, if the shorts<br />
are not pretty close to the same length.<br />
To illustrate the necessity of proper phasing,<br />
Fig. 5 shows the E plane pattern of the<br />
first trial collinear which was built "by the<br />
book." The screen reflector was not used in<br />
this test. The unidirectionalness of the pattern<br />
was apparently due to the reflecting action<br />
of the length of tubing used to support the<br />
dipole string.<br />
In contrast, Fig. 6 shows the pattern obtained<br />
in the E plane with the second trial<br />
collinear, which was also without screen re<br />
Bector. In this case, the phasing stubs were<br />
made longer and the movable shorting stubs<br />
added and adjusted for maximum gain.<br />
It can be seen that the second antenna has<br />
a much cleaner pattern, lower sidelobes and<br />
narrower beamwidth.<br />
Though not shown, the H plane beamwidth<br />
of this antenna is much too broad to satisfy<br />
the feed requirements of the parabolic sheet.<br />
Fig. 7 shows E plane plot the final array.<br />
This was built like the second trial except<br />
that the reflector screen was added and the<br />
stubs retuned as required.<br />
The sidelobes are further reduced and the<br />
back lobe is almost completely suppressed.<br />
The H plane beamwidth is reduced to about<br />
100 degrees which is a quite satisfactory<br />
value for the feeding sheet. In fact, the array<br />
is, in itself, a fairly decent antenna, which,<br />
if used without the parabolic reflector, will<br />
have about 10 db gain.<br />
The collinear is mounted at the focus of<br />
the sheet by using four additional lengths of<br />
TV mast. Two 5 foot lengths and two 8<br />
foot 4 inch lengths are used to form the<br />
collinear support which is held together and<br />
to the sheet by antenna U clamps.<br />
Reference to the photographs will provide<br />
the details of this construction. The U clamp<br />
which ties the mast behind the sheet to the<br />
center tubing in the framework is particularly<br />
important if the collinear support is to remain<br />
rigid.<br />
The collinear is then clamped at the focus<br />
of the sheet.<br />
T wo lengths of nylon rope were tied between<br />
the edges of the framework and th e<br />
ends of the collinear to insure against the<br />
collinear twisting on its mount. If this were<br />
to happen the pattern would be upset and,<br />
if carried to an extreme, the effectiveness of<br />
the antenna would be destroyed altogether.<br />
To this point, nothing has been said about<br />
the matching scheme used. It will be noted<br />
that the middle dipole in the array is split<br />
at the center and a shorted stub has been<br />
inserted.<br />
The center impedence of the array is rather<br />
low and requires a balanced feed. The simplest<br />
matching arrangement seemed to be the "beer<br />
can balun," in this case, a soft drink can<br />
balun" and shorted stub match.<br />
The balun is used to transform the 50<br />
ohm unbalanced transmission line to a 50<br />
ohms balanced shorted line. The 50 ohms balanced<br />
line is tapped onto the shorted stub.<br />
The tap point and the short are positioned<br />
for minimum VSWR.<br />
The details of the balun are shown in<br />
Fig. 4. These details vary slightly from the<br />
balun shown in the photographs, however,<br />
they are essentially the same. It is also well<br />
to note that the short 50 ohm balanced line<br />
is not actually 50 ohms but somewhat higher,<br />
56 73 MAGAZINE