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Propagation Effects Handbook for Satellite Systems - DESCANSO ...

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6.5.2 Amplitude Fluctuations<br />

6.5.2.1 Overview. The phenomena of amplitude and angle-of-arrival<br />

fluctuations combine to <strong>for</strong>m received signal amplitude fluctuations.<br />

For many cases of propagation one or more of these effects may often<br />

be neglected. For example, a receiving system which employs an<br />

antenna with a wide beamwidth will not experience angle-of-arrivalinduced<br />

amplitude fluctuations <strong>for</strong> most elevation angles. However,<br />

such simplification is not always possible. The theory of wave<br />

propagation and scattering in random media allows a combination of<br />

the turbulence induced effects to be per<strong>for</strong>med in the context of<br />

weak fluctuations along a line-of-sight path. The work of Ishimaru<br />

(1978), which defines coherent and incoherent field components as a<br />

plane wave propagates through a random medium, provides a method of<br />

combining amplitude and angle-of-arrival effects into a model of<br />

received signal amplitude fluctuation. A model utilizing the<br />

concept of incident plane wave decomposition (see Figure 6.6-1) has<br />

been proposed by Theobold and Hedge (1978).<br />

6.5.2.2 Variance of Received Signal Amplitude. The assumption of<br />

weak turbulence is invoked <strong>for</strong> a plane wave incident on a region of<br />

turbulence, propagating a distance Lt (km) and impinging on a<br />

circular aperture of diameter da (meters). The antenna is assumed to<br />

have a Gaussian pattern function with half-power beamwidth B<br />

(degrees). If vd is the received signal voltage, assuming a<br />

square-law first mixer? an expression <strong>for</strong> signal variance relative<br />

to average power is<br />

S2 = 10 IO!J,*<br />

where<br />

(dd<br />

~2>.~>2<br />

U 2<br />

~*>2<br />

11=’<br />

= lolog,o<br />

- exp [-Lt/Lo]<br />

Ic =(1 - Ii) /(1+0;)<br />

1<br />

(IC012 + “62<br />

= electric field amplitude variance<br />

6-76<br />

‘-‘i (27$2+ J<br />

5.55~2 + B<br />

‘c+ ‘i (27$2+ ~)<br />

(6.5-1)

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