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Abstract
Based on the satellite retrieval methodology, the spectral characteristics and cloud microphysical properties were analyzed that included brightness temperatures of Channels 4 and 5, and their brightness temperature di erence (BTD), the particle effective radius of seeded cloud track caused by an operational cloud seeding and the microphysical effects of cloud seeding were revealed by the comparisons of their differences inside and outside the seeded track. The cloud track was actually a cloud channel reaching 1.5-km deep and 14-km wide lasting for more than 80 min. The effective radius of ambient clouds was 10-15 μm, while that within the cloud track ranged from 15 to 26 μm. The ambient clouds were composed of supercooled droplets, and the composition of the cloud within the seeding track was ice. With respect to the rather stable reflectance of two ambient sides around the track, the visible spectral reflectance in the cloud track varied at least 10%, and reached a maximum
of 35%, the reflectance of 3.7 μm in the seeded track relatively decreased at least 10%. As cloud seeding advanced ,the width and depth were gradually increased. Simultaneously the cloud top temperature within the track became progressively warmer with respect to the ambient clouds,and the maximum temperature differences reached 4.2 and 3.9℃ at the first seeding position for Channels
4 and 5. In addition, the BTD in the track also increased steadily to a maximum of 1.4℃, compared with 0.2-0.4℃ of the ambient clouds. The evidence that the seeded cloud became thinner comes from the visible image showing a channel, the warming of the cloud tops, and the increase of BTD in the seeded track.The seeded cloud became thinner mainly because the cloud top descended and it lost water to precipitation throughout its depth. For this cloud seeding case, the glaciation became apparent at cloud tops about 22 min after seeding. The formation of a cloud track in the supercooled stratiform clouds was mainly because that the seeded cloud volume glaciated into ice hydrometeors that precipitated and so lowered cloud top height. A thin line of new water clouds formed in the middle of the seeded track between 38 and 63 min after seeding, probably as a result of rising motion induced by the released latent heat of freezing. These clouds disappeared in the earlier segments of the seeded track, which suggested that the maturation of the seeding track was associated with its narrowing and eventual dissipation due to expansion of the tops of the ambient clouds from the sides inward.
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Citation
DAI Jin, YU Xin, Daniel ROSENFELD, XU Xiaohong. 2007: Microphysical Effects of Cloud Seeding in Supercooled Stratiform Clouds Observed from NOAA Satellite. Journal of Meteorological Research, 21(2): 224-233.
DAI Jin, YU Xin, Daniel ROSENFELD, XU Xiaohong. 2007: Microphysical Effects of Cloud Seeding in Supercooled Stratiform Clouds Observed from NOAA Satellite. Journal of Meteorological Research, 21(2): 224-233.
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DAI Jin, YU Xin, Daniel ROSENFELD, XU Xiaohong. 2007: Microphysical Effects of Cloud Seeding in Supercooled Stratiform Clouds Observed from NOAA Satellite. Journal of Meteorological Research, 21(2): 224-233.
DAI Jin, YU Xin, Daniel ROSENFELD, XU Xiaohong. 2007: Microphysical Effects of Cloud Seeding in Supercooled Stratiform Clouds Observed from NOAA Satellite. Journal of Meteorological Research, 21(2): 224-233.
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