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<br />4.2 <br /> <br />4.3 <br /> <br />5. I <br /> <br />a.2 <br /> <br />a.3 <br /> <br />a.4 <br /> <br />a.5 <br /> <br />5.6 <br /> <br />The comparison between the LTD model and the observed <br /> <br />plume sizes is valid for diffusion time longer than the <br /> <br />critical time (tc). The critical time is determined by <br /> <br />intersection of the size of the most energetic eddies <br /> <br />(A) with the LTD model. <br /> <br />A schematic diagram of the ratio, relative diffusion/ <br />2 2 <br />LTD model, as a function of diffusion time. y, Y , <br />2 <br />and a, represent the mean square particle displace- <br /> <br />ments as calculated according to relative diffusion, <br /> <br />Batchelor's E approach, and LTD model, respectively. <br /> <br />Comparison of the spatial spectra of vertical velocity <br /> <br />and temperature, measured from an aircraft and calcul- <br /> <br />sted from tower measurements using the Taylor frozen <br /> <br />turbulence hypothesis (after Monin and Yaglom, 1971b) <br /> <br />Eulerian-space power spectra of longitudinal wind com- <br /> <br />ponent on 23 June 1979. Numbers are average true air- <br /> <br />speed (m/s) at which data were collected. <br /> <br />The same as Fig. a.2, except of vertical wind component. <br /> <br />Eulerian-space power spectra of longitudinal (u') wind <br /> <br />component plotted as kE(k) versus k, on 23 June 1979. <br /> <br />Numbers are averaged true airspeed (m/s) at which data <br /> <br />were co llec ted. <br /> <br />The same as Fig. 5.4, except of lateral (v') wind <br /> <br />component <br /> <br />The same as Fig. 5.4, except of vertical (w') wind <br /> <br />component . <br /> <br />. <br /> <br />viii <br /> <br />.', <br /> <br />68 <br /> <br />. <br /> <br />.' <br /> <br />71 <br /> <br />. <br /> <br />80 <br /> <br />. <br /> <br />84 <br /> <br />.. <br /> <br />8a <br /> <br />-I <br /> <br />87 <br /> <br />. <br /> <br />88 <br /> <br />89 <br /> <br />. <br /> <br />.' <br />