Generally a dipole has a broader H pattern than its
E pattern (the E pattern being in the plane containing the dipole). Recall
from the discussion in section 19.4.1 that for good
cross-polarization properties it was essential to have matched
and
plane patterns. An elegant method for achieving this pattern
matching was given by P.S.Kildal [10], and involves placing a
beam forming ring (BFR) above the dipole19.5.
The conducting ring is placed above the dipole in a plane parallel to
the reflector and is supported by dielectric rods. The beam forming
ring compresses the H-plane pattern while it has no significant effect
on the E-plane.
The optimum dimensions of the dipole, BFR and reflector were arrived at by careful measurements done on a scaled-up version (i.e. at 610 MHz) and a follow-up measurements on a prototype 327 MHz model. The values arrived at were :
The measured phase center is at 26 mm above the reflector for both E and H- planes. Crossed dipoles are employed for dual polarization. The 327 MHz feed actually deviates slightly from the original Kildal's design - there are sleeves over the dipoles. These sleeves increase the bandwidth of the feed [5]. The VSWR plot for the 327 MHz feed is given in Figure 19.10.
For SWR , the bandwidth is 138 MHz.(286 to 424 MHz.)
The measured antenna pattern is given in Fig 19.11.
The edge taper,
is
dB. Fig 19.9 shows
the cross-polar pattern. It is seen that a cross-polar maximum of
dB (mean value) has been achieved.
The linear polarized outputs of the dipoles are mixed in a quadrature hybrid at one of the front-end chassis to produce two circular polarized (both left and right) signals, which go further into the amplifying, signal conditioning circuits of front-end Electronics.