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Last modified
7/28/2009 2:37:45 PM
Creation date
4/16/2008 11:05:50 AM
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Template:
Weather Modification
Contract/Permit #
14-06-D-6801
Title
Structure and Seedability of San Juan Storms
Date
11/1/1976
Weather Modification - Doc Type
Report
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<br />49 <br /> <br />dissipation rates in the longitudinal (c 1/3). <br />x <br />1/3 <br />(E ) components were calculated from the power spectrum of each flight <br />z <br /> <br />1/3 <br />lateral (c ). and vertical <br />y <br /> <br />segment. <br /> <br />The largest value of the turbulent intensities was either p u'u' or <br /> <br />p v'v' depending whether the flight path was parallel or orthogonal to the <br /> <br />wind direction. The smallest turbulent intensity \vas 'always p u 'v ' . <br /> <br />The pmver spectra of U, V and W were calculated for each flight segment <br /> <br />(u. V and Ware the longitudinal, lateral and vertical winds with respect to <br /> <br />the aircraft). In that portion of the spectrum where the -5/3 power law <br /> <br />best fits the data a line was drawn. The -5/3 line corresponds to a par- <br /> <br />ticular value of <br /> <br />1/3 <br />E. . <br />1 <br /> <br />It was noted that E 1/3 < E 1/3 and E 1/3, for all <br />z x y <br /> <br />four flights and at every level. Other researchers have noted that the <br /> <br />vertical diffusion is less than or equal to the horizontal diffusion unless <br /> <br />convection is pronounced. <br /> <br />For each of the power spectra of W, a -2 po,ver law was fitted to that por- <br /> <br />tion of the spectra where it was appropriate. From Equations 3.6 and 3.8, the <br /> <br />values of TA, TE and TL were calculated for each -2 power spectra. In some <br /> <br />cases the -5/3 power law fits the spectra best while in other cases the -2 <br /> <br />power law fits best. No general pattern was evident and in most cases either <br /> <br />power law fits the data equally well. <br /> <br />,2 <br />Substituting the values of TL and w from each flight segment into <br /> <br />Equation 3.10, it was straightfonvard to calculate the standard deviation <br /> <br />in the vertical as a function of time [o3(t)]. The values of o3(t) vs. t <br /> <br />were calculated for each of the flight segments obtained upwind of the moun- <br /> <br />tain. The general functional relationship for each of tIle altitudes for the <br /> <br />10 March case are plotted in Fig. 3.7. The vertical diffusion was greatest <br /> <br />near the ground and decreased by 1/2 to 1/3 above Lt. 6 km (15 kft). From the <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />I <br /> <br />\~ <br /> <br />I <br />I <br />
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