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Last modified
7/28/2009 2:35:15 PM
Creation date
3/11/2008 11:30:14 AM
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Weather Modification
Title
Cloud Physics Investigations - University of Wyoming - 1977-1981
Date
11/1/1982
State
WY
Weather Modification - Doc Type
Report
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<br />. <br /> <br />spectra result at later times while the initial spectra were unimodal. <br /> <br />The processes responsible for this modification of the droplet <br /> <br /> <br />spectra actually produce an increase in the concel1tration of small <br /> <br /> <br />droplets in some cases, but the concentration of large droplets was <br /> <br /> <br />not observed to increase during the entrainment process. <br /> <br />The observations suggest that the development of broad spectra is <br /> <br /> <br />not accomplished in the initial stages of an inhomogeneous mixing <br /> <br /> <br />process. While the mixing appears to be highly inhomogeneous, it does <br /> <br />not lead to substantial broadening. Rather, the passage of time appears <br /> <br /> <br />to be required for broadening,. and the broadening occurs primarily via <br /> <br /> <br />the increase in the number of small droplets. Perhaps the fluctuating <br /> <br />supersaturation fields characteristic of a highly mixed and turbulent <br /> <br /> <br />cloud region can lead to sufficient fluctuations in the <br /> <br /> <br />time-integrated supersaturation encountered by various droplets to <br /> <br />lead to such a broadening. If cloud droplets in a highly mixed and <br /> <br /> <br />turbulent cloud follow varying trajectories in the course of arriving <br /> <br /> <br />at a given location, such varying saturation ratios may lead to some <br /> <br />broadening of the spectrum with time. <br /> <br /> <br />2.6: Liquid water content. Fig. 2.11 shows the frequency wi th which <br /> <br /> <br />the (JW) liquid water content exceeded various thresholds. Measurements <br /> <br /> <br />were made each second, and thus were separated by about 100 mi all <br /> <br /> <br />values exceeding 0.1 g/m3 were used to calculate relative frequencies. <br /> <br /> <br />The truncation at values above 2.5 g/m3 is artificial, as explained <br /> <br />in Cooper et al. (1982a) i this results from the zero offset and <br /> <br /> <br />airspeed corrections which we apply, and the inherent 3 g/m3 limit of <br /> <br /> <br />our instrument. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />18 <br /> <br />. <br />
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