Rapid changes (<• s) have been observed in the depolarization of earth-space radio signals propagating through ice clouds. This paper presents the first observations of the rapid changes in the degree of alignment and in the orientation of the anisotropy axis of the ice particles producing the depolarization. The ice particles appear to be aligned by the intense electric field in thunderstorms and appear to realign rapidly with the new field directions existing after lightning discharges. INTRODUCTION It has become generally accepted that the anisotropy of aligned ice particles in clouds along earth-space propagation paths causes significant depolarization of centimeter wavelength radio waves. [Cox and Arnold, 1976; McEwan et al., 1977; Shutie et al., 1977a, b,' Cox et al., 1977; Cox et al., 1978; Haworth et al., 1977; Arnold and Cox, 1977; Rustako, 1977; Rustako, 1978]. Early investigators of this ice depolarization reported occasional rapid changes in the depolarization magnitude that was sometimes coincident with lightning strokes [McEwan et al., 1977; Shutie et al., 1977a; Haworth et al., 1977; Arnold and Cox, 1977; Rustako, 1977; and Rustako, 1978]. These rapid changes were attributed to rapid changes in the degree of alignment or the orientation of the alignment of small ice crystals that were observed with radar by Hendry and McCormick [1976]. This paper presents the first observations of rapid changes in the degree of alignment and in the orientation of the anisotropy axis for ice particles producing depolarization on an earth-space radio path. The observations were made using a 19-GHz Cornstar satellite beacon [Cox, 1974; Cox, 1978] and the Bell Laboratories Crawford Hill receiving site [Cox, 1974; Cox, 1978; Chu et al., 1978; Arnold et al. , 1978]. The unique feature of this experiment that makes these observations possible is the measurement of differential phase between two copolarized received signals that have orthogonal polarizations. An example is shown also of rapid changes observed simultaneously in the atmospheric electric field and in the depolarization of linearly polarized 19-and 28-GHz satellite signals and circular polarized 12-GHz satellite signals [Rusteko, 1978]. THE EXPERIMENT The experimental equipment is described in detail by Cox [ 1978], Chu et al. [ 1978], and Arnold et al. [ 1978]. Briefly, a 19-GHz carrier is switched at a 1-kHz rate between two orthogonal linearly polarized antennas on a geosynchronous Comstar satellite. These signals are received with a 7-m antenna and narrow band receiving system at the Crawford Hill, New Jersey, receiving site. Amplitudes and phases are measured and recorded digitally for the two received signal components that are copolarized with the transmitted signals and for the two signal components that are cross polarized to the transmitted signals. The propagation path is at an azimuth of 210.5 ø and an elevation of 38.5 ø from Crawford Hill. The clear air received signal polarizations are rotated 21 ø from horizontal and vertical. (The horizontal ...