Microwave depolarization of an earth-space path

The nonspherical shapes of both rain and ice particles contribute to microwave depolarization on an earth-space path. A two-tier Gaussian model for rain, which assumes Gaussian distributions both for instantaneous canting angle and time-varying mean canting angle, together with gross features of ice particles, provides a theoretical framework to organize the experimental data and to yield functional dependence of cross polarization on freqency, polarization, and elevation angle. In spite of the lack of physical data on ice clouds, we have obtained agreement between measured depolarization data and theoretical results that are essentially independent of details of ice clouds. In particular, we have found a linear relation between cross-polarization amplitude and frequency throughout the centimeter wavelengths for a given earth-space path. The dependence of depolarization on orientation of an arbitrary linear polarization can be described by a simple, nearly sinusoidal expression that is relatively insensitive to the mean canting angle except within about ten degrees of the local “vertical” or horizonta1l direction. We show measured depolarization data for paths of various elevation angles to be consistent with each other using an empirical effective path length and the approximate cos2 θel factor for the differential attenuation and differential phase shift. Procedures of estimating cross polarizations for satellite communication systems and typical numerical results are summarized.

[1]  T. S. Chu,et al.  Rain-induced cross-polarization at centimeter and millimeter wavelengths , 1974 .

[2]  Tomohiro Oguchi,et al.  Scattering properties of Pruppacher‐and‐Pitter form raindrops and cross polarization due to rain: Calculations at 11, 13, 19.3, and 34.8 GHz , 1977 .

[3]  W. L. Nowland,et al.  Theoretical relationship between rain depolarisation and attenuation , 1977 .

[4]  D. C. Cox,et al.  Dependence of depolarization on incident polarization for 19-GHz satellite signals , 1978, The Bell System Technical Journal.

[5]  D. C. Cox,et al.  Characteristics of rain and ice depolarization for a 19- and 28-GHz propagation path from a Comstar satellite , 1980 .

[6]  Sing Lin,et al.  Empirical Rain Attenuation Model for Earth-Satellite Paths , 1979, IEEE Trans. Commun..

[7]  A. J. Rustako An earth-space propagation measurement at crawford hill using the 12-GHz CTS satellite beacon , 1978, The Bell System Technical Journal.

[8]  G. Brussaard,et al.  A meteorological model for rain-induced cross polarization , 1976 .

[9]  M. Saunders,et al.  Cross polarization at 18 and 30 GHz due to rain , 1971 .

[10]  D. C. Cox,et al.  Depolarization of 19 and 28 GHz earth‐space signals by ice particles , 1978 .

[11]  T. Chu,et al.  B.S.T.J. Brief: Perturbation calculations of rain-induced differential attenuation and differential phase shift at microwave frequencies , 1973 .

[12]  David C. Hogg,et al.  The role of rain in satellite communications , 1975, Proceedings of the IEEE.

[13]  S. H. Lin Dependence of rain-rate distribution on rain-gauge integration time , 1976, The Bell System Technical Journal.

[14]  H. Booker,et al.  Techniques for Handling Elliptically Polarized Waves with Special Reference to Antennas: Introduction , 1951, Proceedings of the IRE.