Much interest is shown about ground systems on various Part 15 boards -- what they are, and why they are important. The following comments are a bit technical, but then this is a technical subject. Hopefully the comments will have some useful bits for most readers.
Monopole radiators such as used by licensed and unlicensed transmit systems in the AM broadcast band need a good "r-f ground" in order to radiate as efficiently as possible.
The transmitter provides a source for the r-f current, and the r-f ground provides the completion of the path caused by radiation from the monopole, back into the ground side of the transmitter circuits.
A monopole antenna system can be thought of as a closed circuit where energy circulates back and forth at an r-f rate between the radiator and the r-f ground connection. The path between a monopole and an r-f ground is produced by the capacitance of the monopole to the r-f ground, across which path displacement currents flow.
Those displacement currents become conducted currents at, and just below the surface of the earth out to about 1/2-wavelength from a monopole, regardless of the monopole height in wavelengths. Once those currents enter the earth they need to be conducted back to the ground terminal of the transmitter in order to complete the path needed for r-f current to flow in the antenna system.
Soil is a rather poor (lossy) conductor of radio waves, so a system of buried radial wires often is used to provide a low-resistance path back to the transmit system in the area of the earth where those currents are highest -- within 1/2-wavelength radius of the monopole.
Carefully done physical experiments back in the 1930s determined that an r-f ground consisting of about 120 buried radials spaced 3 degrees apart around the tower base, and each radial about 0.4 wavelengths long (in free space) would produce an antenna system that radiated about 95% of the power applied to it for monopole heights of about 45 degrees or more.
Such an r-f ground is the norm for licensed AM broadcast stations, but beyond the practical range of most "Part 15" stations.
Also - it should be noted that an r-f ground consisting of one or more "ground rods" buried vertically at or near the base of a monopole, or a few buried radial wires of any length do not constitute a good r-f ground. The r-f resistance of such paths is very high to the r-f earth currents surrounding the monopole, because they are forced to travel long paths through the lossy earth from up to 1/2-wavelength away to reach those conductors.
For reference, the r-f resistance of a "broadcast type" buried radial system is 2 ohms or less, while the r-f resistance of a few buried ground rods or wires may be 50 ohms or more. This added loss makes a big difference in the percentage of available r-f energy that will be radiated by a 3-meter monopole in the AM broadcast band.
Note that the r-f grounds discussed here do not exist along the length in space of any wire or other conductor such as a tower, billboard, water tower etc that is connected to them. All of those conductors will radiate into free space as a result of the r-f current flowing along them. And by definition, an r-f ground does not and cannot radiate.
RF
Monopole radiators such as used by licensed and unlicensed transmit systems in the AM broadcast band need a good "r-f ground" in order to radiate as efficiently as possible.
The transmitter provides a source for the r-f current, and the r-f ground provides the completion of the path caused by radiation from the monopole, back into the ground side of the transmitter circuits.
A monopole antenna system can be thought of as a closed circuit where energy circulates back and forth at an r-f rate between the radiator and the r-f ground connection. The path between a monopole and an r-f ground is produced by the capacitance of the monopole to the r-f ground, across which path displacement currents flow.
Those displacement currents become conducted currents at, and just below the surface of the earth out to about 1/2-wavelength from a monopole, regardless of the monopole height in wavelengths. Once those currents enter the earth they need to be conducted back to the ground terminal of the transmitter in order to complete the path needed for r-f current to flow in the antenna system.
Soil is a rather poor (lossy) conductor of radio waves, so a system of buried radial wires often is used to provide a low-resistance path back to the transmit system in the area of the earth where those currents are highest -- within 1/2-wavelength radius of the monopole.
Carefully done physical experiments back in the 1930s determined that an r-f ground consisting of about 120 buried radials spaced 3 degrees apart around the tower base, and each radial about 0.4 wavelengths long (in free space) would produce an antenna system that radiated about 95% of the power applied to it for monopole heights of about 45 degrees or more.
Such an r-f ground is the norm for licensed AM broadcast stations, but beyond the practical range of most "Part 15" stations.
Also - it should be noted that an r-f ground consisting of one or more "ground rods" buried vertically at or near the base of a monopole, or a few buried radial wires of any length do not constitute a good r-f ground. The r-f resistance of such paths is very high to the r-f earth currents surrounding the monopole, because they are forced to travel long paths through the lossy earth from up to 1/2-wavelength away to reach those conductors.
For reference, the r-f resistance of a "broadcast type" buried radial system is 2 ohms or less, while the r-f resistance of a few buried ground rods or wires may be 50 ohms or more. This added loss makes a big difference in the percentage of available r-f energy that will be radiated by a 3-meter monopole in the AM broadcast band.
Note that the r-f grounds discussed here do not exist along the length in space of any wire or other conductor such as a tower, billboard, water tower etc that is connected to them. All of those conductors will radiate into free space as a result of the r-f current flowing along them. And by definition, an r-f ground does not and cannot radiate.
RF