With the large number of operators and wide availability of inexpensive, single-band radios, the 10-m band could well become the hangout for local ragchewers that it was before the advent of 2-m FM, even at a low point in the solar cycle.
This simple antenna provides gain over a dipole or inverted V. It is a resonant loop with a particular shape. It provides 2.1dB gain over a dipole at low radiation angles when mounted well above ground. The antenna is simple to feed— no matching network is necessary. When fed with 50-Ù coax, the SWR is close to 1:1 at the design frequency, and is less than 2:1 from 28.0-28.8 MHz for an antenna resonant at 28.4 MHz.
The antenna is made from #12 AWG wire (see Fig ) and is fed at the center of the bottom wire. Coil the coax into a few turns near the feedpoint to provide a simple balun. A coil diameter of about a foot will work fine. You can support the antenna on a mast with spreaders made of bamboo, fiberglass,
wood, PVC or other nonconducting material. You can also use aluminum tubing both for support and conductors, but you’ll have to readjust the antenna dimensions for resonance. This rectangular loop has two advantages over a resonant square loop. First, a square loop has just 1.1 dB gain over a
dipole. This is a power increase of only 29%. Second, the input impedance of a square loop is about 125 W. You must use a matching network to feed a square loop with 50-Ù coax. The rectangular loop achieves gain by compressing its radiation pattern in the elevation plane. The azimuth plane pattern is slightly wider than that of a dipole (it’s about the same as that of an inverted V). A broad pattern is an advantage for a general- purpose, fixed antenna. The rectangular loop provides a
bidirectional gain over a broad azimuth region. Mount the loop as high as possible. To provide 1.7 dB gain at low angles over an inverted V, the top wire must be at least 30 ft high. The loop will work at lower heights, but its gain advantage disappears. For example, at 20 ft the loop provides the same gain at low angles as an inverted V.