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Propagation Effects Handbook for Satellite Systems - DESCANSO ...

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path length of the turbulence Lt is computed from ht = 6 km, re =<br />

6371 km and 8 = 10 degrees using the equation<br />

* 1/2<br />

Lt = lh~ + Zreht + (resine) ] - resine = 34 km<br />

The other constants are:<br />

LO = 180 km<br />

621 = 1.18 X 10-3<br />

622 = 8.35 X 10-4<br />

Ii =<br />

0.17<br />

IC = 0.83<br />

and the signal variance relative to the average power is<br />

“ 4<br />

S2X10 109109”79 X1:83+014<br />

+ 0.14396 - 0.14297<br />

. .<br />

= 10 loglo (2.03 X 10 -3<br />

) = -27 cIB<br />

(6.5-10)<br />

Note that this agrees well with the results in Figure 6.5-2.<br />

Reference to Tatarski (1961) would have allowed evaluation in terms<br />

of Can rather than the <strong>for</strong>mulation by Theobold and Hedge (1978)<br />

utilized here. .<br />

Reference to Figure 6.5-4b indicates that 50% of the time the Ss<br />

would be between -24 and -3o dB, while 90% of the time S2 WOUld be<br />

between -20 and -34 dB.<br />

The power spectrum density of the fluctuations decreases at 26.5<br />

dB/decade (see Figure ’6.5-6). If one considers some lower -<br />

frequency cutoff <strong>for</strong> the amplitude fluctuations (say 0.1 Hz) the<br />

6-102

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