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C h a p t e r 2 : r a d i o - W a v e P r o p a g a t i o n 59<br />

Ionospheric Sky-Wave Propagation<br />

Sky-wave propagation occurs because signals in the ionosphere are refracted sufficiently<br />

to be bent back toward the earth’s surface. To observers on the ground, the signal appears<br />

to have been reflected from a radio “mirror” at the virtual height somewhere<br />

above the junction of the stratosphere with the lower boundary of the ionosphere. The<br />

skip distance is the shortest distance along the surface of the earth from the transmitter<br />

site (A in Fig. 2.32) to the nearest of all points on the earth (point C in Fig. 2.32) for which<br />

the ionosphere is capable of refracting the transmitted signal back to earth. At shorter<br />

distances, the higher-angle radiation from the transmitted signal either remains in the<br />

ionospheric layer or continues on out into outer space. The ground-wave zone is the distance<br />

from the transmitter site (A in Fig. 2.32) to the locus of points where the ground<br />

wave fades to an unusably low level (point B in Fig. 2.32). The skip zone is the distance<br />

from the outer edge of the ground-wave zone to the skip distance, or the distance from<br />

B to C in Fig. 2.32. Note carefully that only one of these distances, the ground-wave zone,<br />

is strongly dependent upon transmitter power level (or, more precisely, effective radiated<br />

power). The other distances are a function primarily of transmitter frequency and<br />

the state of the ionosphere at any given time.<br />

At some frequencies and power levels the sky wave and the ground wave may interfere<br />

with each other. When this happens, the sky wave arrives at the receiver with a<br />

signal whose amplitude and phase relative to the ground-wave signal depend on the<br />

specifics of its path up to the ionosphere and back down. Since the ionosphere is in<br />

constant motion (think slow undulations, like a snake), the sky wave will arrive with<br />

randomly varying amplitude and phase relative to the ground wave. Thus, the sky<br />

wave can selectively strengthen or cancel the ground wave, giving rise to a class of fading<br />

mechanisms discussed further under “Ionospheric Fading”.<br />

Angle of Incidence and Radiation Angle<br />

One of the factors determining skip distance is the angle at which the radio wave enters<br />

the ionosphere. If the transmit antenna is relatively omnidirectional, it “sprays” the<br />

Ionosphere<br />

Sky wave not<br />

effective<br />

Sky wave<br />

Ground wave<br />

A<br />

Ground-wave zone<br />

B<br />

Skip distance<br />

Skip zone<br />

C<br />

Figure 2.32 Ground-wave zone and skip zone.

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