By W. L. Shields (auth.), John H. Olsen, Arnold Goldburg, Milton Rogers (eds.)
The mix of accelerating airport congestion and the advert vent of huge transports has triggered elevated curiosity in airplane wake turbulence. A quantitative realizing of the interplay among an airplane and the vortex wake of a previous plane is important for making plans destiny excessive density air site visitors styles and keep watch over platforms. the character of the interplay is dependent upon either the features of the next plane and the features of the wake. the various inquiries to be responded are: What deter mines the complete features of the vortex wake? What homes of the subsequent airplane are very important? what's the position of pilot reaction? How are the wake features relating to the genera ting plane parameters? How does the wake crumble and the place? lots of those questions have been addressed at this primary airplane Wake Turbulence Symposium backed by means of the Air strength workplace of Sci entific learn and The Boeing corporation. staff engaged in aero dynamic learn, airport operations, and software improvement got here from numerous count number ries to provide their effects and alternate info. the recent effects from the assembly supply a present photo of the country of the information on vortex wakes and their interactions with different airplane. Phenomena formerly considered as mere curiosities have emerged as very important instruments for realizing or controlling vortex wakes. the recent forms of instability taking place in the wake may well at some point be used for selling early dis integration of the damaging dual vortex structure.
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Extra info for Aircraft Wake Turbulence and Its Detection: Proceedings of a Symposium on Aircraft Wake Turbulence held in Seattle, Washington, September 1–3, 1970. Sponsored jointly by the Flight Sciences Laboratory, Boeing Scientific Research Laboratories and the Air F
2. Smith, T. , and P. B. , Final Report to Dugway Proving Ground, Dugway, Utah, Cont. DA-42-007-CML-545, 1963. 3. Andrews, W. " Paper presented at Symp. on Aircraft Wake Turbu1ence, Seatt1e, September 1-3, 1970. 4. MacCready, P. " Paper presented at Symp. on Aircraft Wake Turbu1ence, Seatt1e, September 1-3, 1970. 5. Turner, J. " J. , I (1960), 419-432. 6. Lamb, Sir Horace, Hydrodynamics. York, 1945, pp 221-222. 7. " Bull. Amer. Meteor. , 50 (1969), 719. 8. Lamb, op. , pp 161-162. 9. Prandt1, op.
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He Ring and the Vorticity Distribution Equation (36) is an ordinary differential equation in r for *(l)(t,~) with t appearing as a parameter, therefore, for each preII scribed vorticity distribution at each instant *(1) can be deter11 mined by eq. (36) and the boundary conditions at r = O. For example, if the initial vorticity distribution is that of a rotating disk (model B in Fig. 4) of radius 6 , the C(o) and v(o) distribution at the instant t=t is 0 o - (0) C and - (0) C - (0) 20 =0 v - (0) v 60 (42a) = I' I (2TTr) for r > 6 0 (42b) = Or = I' I (2TT6 0a ) and 60 = 60 IE.