If paralleled dipoles for different bands on a single feed line are called a
"fan dipole" it's a misnomer that can cause a lot of confusion. Sometimes
folks pick up short-hand term by accident, like assuming that a dipole is
always fed at the center to be a "dipole" when, in fact, a dipole is a
half-wave radiator and, being exactly 1/2 wave long it has an electrostatic
pole at each end, hence it is a "dipole". It's "dipole-ness" has nothing to
do with where or how it's fed RF. 

A "fan dipole" is a single-band affair. It's is a way of broadening the
bandwidth of a single-band dipole by simulating a "fat" wire using multiple
wires. Typically the wires join at an apex at the center and spread or "fan"
out at the far end with cross-wires connecting the ends. That forms larger
effective radiator diameter that reduces the "Q" of the antenna; hence the
bandwidth is increased. 

It's  not a commonly-used antenna because a simple wire dipole usually has
adequate bandwidth on 40 meters and up, and in practice even a large "fan"
doesn't broaden the bandwidth all that much; not enough to cover the 3.5 - 4
MHz range with a low SWR, for example. 

However, like any "fat radiator" dipole, the resonant length is shortened a
bit, which can be a help in limited space. 

Cebik has a good write-up on fan dipoles and their close cousin, the bow tie
antenna, at www.cebik.com as part of his discussion of small beams. 

Ron AC7AC

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