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Handbook of Propagation Effects for Vehicular and ... - Courses

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9-20<br />

Mean Fade Duration, T D (sec)<br />

1.3<br />

1.2<br />

1.1<br />

1.0<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0.0<br />

Lower Bound f -10<br />

<strong>Propagation</strong> <strong>Effects</strong> <strong>for</strong> <strong>Vehicular</strong> <strong>and</strong> Personal Mobile Satellite Systems<br />

Upper Bound f -10<br />

P = 90%<br />

5 6 7 8 9 10 11 12 13 14 15<br />

Elevation Angle (deg)<br />

Figure 9-17: Bounds <strong>of</strong> mean fade duration TD (P)<br />

<strong>for</strong> multipath fade exceedance<br />

percentage P = 90% at L-B<strong>and</strong>.<br />

9.5 Multipath from Rough Seas <strong>and</strong> Frequency Dependence on Multipath<br />

Fading<br />

9.5.1 Rough Sea Model<br />

Karasawa et al. [1990] executed an analysis in which multipath fading from very rough<br />

seas (with significant wave heights H greater than 3 m) is examined. They developed a<br />

model that takes account <strong>of</strong> the effect <strong>of</strong> smaller-scale waves superimposed onto the<br />

dominant wave. They make use <strong>of</strong> the fact that the spectrum <strong>of</strong> ocean waves caused by<br />

wind may be approximated by the Pierson-Moskowitz spectrum [1964] <strong>and</strong> that ocean<br />

waves have the characteristics <strong>of</strong> gravity waves. The RMS slope <strong>of</strong> the sea surface is<br />

calculated <strong>and</strong> applied to a theoretical model <strong>for</strong> estimating fade depths. A series <strong>of</strong><br />

curves is presented <strong>of</strong> the 99 th percentile <strong>of</strong> fading depth versus significant wave height H<br />

<strong>for</strong> the following combinations <strong>of</strong> antenna gain <strong>and</strong> elevation angle (15 dBi, 5°), (21 dBi,<br />

5°), <strong>and</strong> (15 dBi, 10°). The analytically derived multipath fading <strong>for</strong> “wind-wave” <strong>and</strong><br />

“swell” conditions are compared with results derived from the experiments <strong>of</strong> Karasawa<br />

et al. [1986]; Matsudo et al., [1987], <strong>and</strong> Ohmori et al. [1985]. They show that the fading<br />

depth tends to reach a peak <strong>for</strong> H between 1 <strong>and</strong> 2 m. The multipath fading peaks are<br />

approximately 8 dB, 5 dB, <strong>and</strong> 4 dB <strong>for</strong> the above combinations <strong>of</strong> antenna gain <strong>and</strong><br />

elevation angle, respectively, consistent with their wind-wave model. For larger H, the<br />

multipath fading decreases slightly <strong>for</strong> wind-waves conditions <strong>and</strong> remains relatively

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