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By Robert G. Fleagle (auth.), Yih-Ho Pao, Arnold Goldburg (eds.)

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Additional info for Clear Air Turbulence and Its Detection: Proceedings of a Symposium on Clear Air Turbulence and Its Detection, Organized and Sponsored by the Flight Sciences Laboratories, Boeing Scientific Research Laboratories, Office of the Vice President — Research and

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8 in this case) than with the more rapid "breaking" shown in Case 4. This confirms the evident conclusion that with a sudden breaking of waves energy will be transferred more readily into smaller eddies than with a slowly breaking process. 009• 3 1160 1168 1176 Figure 21. - lcr~l---2~--~4~6-ta~~--~~~~~~ Same as Fig. 19, except for finer resolution in data points. For explanation, see text. From the foregoing it is quite evident that the processes of steepening wave fronts and of ultimate "breaking" of these waves produce spectra of eddy kinetic energy which are surprisingly similar to those observed with CAT.

10). 4). 12). = w2 s Ri 0 w2 so {1 + ~v q (1 --;-)approximately. 11) This means that although the static stability is increased by a strearnwise stretching (acceleration) the secondary vorticity is increased so as to decrease the Richardson number. This result is in contrast to the effect of acceleration when there is only a transverse vorticity component, for this component is unaltered in horizontal 2D motion. 12) However, this seems likely to be spectacular only where the flow is brought almost to rest.

39, this point was only one data point behind the location of the minimum points of the wave. From thereon through wave No. 25 sec) behind the minimum point. Results of the computations are shown in Fig. 20. 28 ELMAR R. REITER I0°r--------------, 40~ =~~~ -4 :t:~~ 12 4 10 0 -4 -8 -12 CASE 4 Figure 20. Same as Fig. 17, except for finer resolution in data points. For explanation, see text. The finer resolution of 20 data points per wave permits the calculation of eddy kinetic energy at larger wave numbers than was possible in the previous cases under consideration.

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