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

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9-24<br />

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

Vertical polarization may be employed at elevation angles above 8°. At lower angles,<br />

errors due to Brewster angle effects may arise.<br />

9.7.2 Fading Depth Durations <strong>and</strong> Occurrence Intervals<br />

The procedures outlined by (9-28) through (9-32) may be employed to establish the<br />

bounds <strong>of</strong> the mean fading occurrence interval <strong>and</strong> the mean fading depth <strong>for</strong> circular<br />

polarization at L-B<strong>and</strong>. Figure 9-12 through Figure 9-14 depict the bounds <strong>for</strong> the mean<br />

fading occurrence interval as a function <strong>of</strong> elevation angle at fade exceedance<br />

percentages <strong>of</strong> 99%, 95%, <strong>and</strong> 90%, respectively. Figure 9-15 through Figure 9-17 give<br />

the bounds <strong>for</strong> the mean fade duration intervals as a function <strong>of</strong> elevation angle at the<br />

same percentages.<br />

9.7.3 Fading Depth Dependence on Frequency <strong>and</strong> Significant Wave Height<br />

Figure 9-18 <strong>and</strong> Figure 9-19 describe the dependence <strong>of</strong> fading at different frequencies as<br />

a function <strong>of</strong> significant wave height. Figure 9-18 shows contours <strong>of</strong> fading depth<br />

isopleths at frequencies ranging from 1 to 10 GHz <strong>and</strong> significant wave heights up to<br />

3 m. Figure 9-19 gives the fading depths versus significant wave height at 3 GHz,<br />

5 GHz, <strong>and</strong> 10 GHz derived from Figure 9-18.<br />

9.8 References<br />

Abbe, B., M. Agan, <strong>and</strong> T. Jedrey [1996], “ACTS mobile terminals,” International<br />

Journal <strong>of</strong> Satellite Communications, Vol. 14, No. 3, pp. 175-190, January.<br />

Beard, C. I. [1961], “Coherent <strong>and</strong> Incoherent Scattering <strong>of</strong> Microwaves from the<br />

Ocean,” IEEE Transactions on Antennas <strong>and</strong> <strong>Propagation</strong>, Vol. AP-9, Sept.<br />

Beckmann, P. <strong>and</strong> A. Spizzichino [1963], “The Scattering <strong>of</strong> Electromagnetic Waves<br />

from Rough Surfaces,” Elms<strong>for</strong>d, NY: Pergamon.<br />

Brown, G. S. [1980], “Backscattering from a Gaussian-distributed perfectly conducting<br />

rough surface,” IEEE Transactions on Antennas <strong>and</strong> <strong>Propagation</strong>, Vol. AP-26, pp.<br />

472-482, May (see correction in ibidem, Vol. AP-28, pp. 943-946, Nov. 1980).<br />

CCIR [1990], “<strong>Propagation</strong> Data <strong>for</strong> Maritime Mobile-Satellite Systems <strong>for</strong> Frequencies<br />

Above 100 MHz,” Reports <strong>of</strong> the CCIR, Annex to Volume V, <strong>Propagation</strong> in Non-<br />

Ionized Media, Report 884-2, pp. 515-535. (International Radio Consultative<br />

Committee, XVIIth Plenary Assembly, Dusseldorf, 1990; International<br />

Telecommunications Union, Geneva, 1990).<br />

Fang, D. J., F. T. Tseng <strong>and</strong> T. O. Calvit [1982a], “A Low Elevation Angle <strong>Propagation</strong><br />

Measurement <strong>of</strong> 1.5 GHz Satellite Signals in the Gulf <strong>of</strong> Mexico,” IEEE<br />

Transactions on Antennas <strong>and</strong> <strong>Propagation</strong>, Vol. AP-30, No. 1, Jan., pp. 10-15.<br />

Fang, D. J., F. T. Tseng, <strong>and</strong> T. O. Calvit [1982b], “A Measurement <strong>of</strong> the Marisat L-<br />

B<strong>and</strong> Signals at Low Elevation Angles Onboard Mobil Aero,” IEEE Transactions on<br />

Communications, Vol. COM-30, No. 2, Feb., pp. 359-365.

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