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<br />should thus be most valuable in those cloudy regions where the hydrome- <br /> <br /> <br />teors are in the middle stages of growth. <br /> <br /> <br />Although hydrometeor trajectories will be derived primarily from <br /> <br /> <br />the Doppler radar data they can be estimated to an extent and in a sup- <br /> <br /> <br />porting way from the time-height diagrams of Iidar linear depolariza- <br /> <br /> <br />tion ratio. Successively higher ratios along a path leading from a <br /> <br /> <br />higher level to a lower level of a cloud would be suggestive of a tra- <br /> <br /> <br />jectory of growing, falling precipitation particles. Because the lidar <br /> <br />data are collected primarily overhead this kind of analysis will require <br /> <br /> <br />separating time-dependent and advective effects. Radar data upwind of <br /> <br />the Iidar should be of help in this. <br /> <br /> <br />The surface microphysics observations will be used to confirm some <br /> <br /> <br />of the radar and Iidar ~stimates of particle trajectories. Confirmation <br /> <br />should be in terms of surface terminal point of the trajectory, <br /> <br /> <br />(equivalent) radar reflectivity factor of the particles, and circular or <br /> <br /> <br />linear depolarization ratio of the particles. <br /> <br />32 <br /> <br />.- <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />i- <br /> <br />~--.. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br />