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Recirculatory flow in a cylindrical cavity
Sequence 36
-- 29 Therefore, in order for ) < 'll/ell , we must have,).. -E:. I and, since in our case ~ = 1, the solution is…
Sequence 37
30 APPENDIX II The integral e := j;k erf(/if :) [ <=xp l-'/~"i ~-J)~ _ e:.xp(-'/4-X)('f'f-J)…
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31 we have 19 This expression when integrated and simplified yields E = 2/~()( ... f)' frexp (- (r--Yj/f(X+<fJ…
Sequence 39
32 APPENDIX III The condition /1 AB 1/ tC 1/ A II /I B 1/ for the kernels given in equation 1-1 may be shown in the…
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33 or where H(r,jf ) is defined as the inner integral, and Z H 6 /tIRX'RJ (See Reference 20, p. 156) Thus (b 60 /…
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Now since we have :J l (e-) 0 27;;., { exp {-Ct. -~)X ,(~) -aP (-( to -t ctJ; x,j ] 4d z-) ~ l~ { cxPl- (Jo-?;)/1xJ - e!(P( -…
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35 REFERENCES 1. Prandtl, L., "Uber Flussigkei tsbewegung bei sehr kleiner Reibung," Proe. III International Math…
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36 17. Howarth, L., "On the Solution of the Laminar Boundary Layer Equations," Proc. Roy. Soc., London, A, 164, p.…
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1.0 .75 K .50 .25 FIXED FREE STREAMLINE STREAMLINE _{ERNST (th.l I ROSHKO (exp.) WOOD (th.) 0 SQUIRE (th.) • MILLS…
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ttl - Lf"l p:: :>. -.~ :>. 5.0-- 4.0 .. _ 3.0L. 2.0 , 1.0 + x/c a x/c '"It x/c v x/c…
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• C'j - 111 p::: >. /I ~ >. 4.0 + x/a 0 x/a lX x/a f7 x/a = 3.0 2.0 . 1.0 0.1 0.25 0.5 1.0…
Sequence 47
- til - II) p:: >. II ~ >. i 8. O~ 6. O~_ 4.0 2.0 I \ + x/c 0.1 0 x/c 0.25 ~ x/c 0.5 V x/c 1.0…
Sequence 48
- 10.<r I I I I I I I I 8.0- I I I I I I I I I i 6.0_ 4.0- 0.0 of- x/a = 0.1 a x/a = 0.25 J:t x/a…
Recirculatory flow in peripheral-jet supports
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PROJECT TUBER/DNT
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TR PT 6805 RECIRCULATORY FLOW IN PERIPHERAL-JET SUPPORTS by Chen-C. Sun This research was supported by the National…
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ACKNOWLEDGMENT The author wishes to express his appreciation and gratitude to Dr. Thomas J. Black for his guidance and con~…
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LIST OF SYMBOLS b H J k pa pc po R * r t = = = = = = = = = constant R - Po. if v:1. Pc. - Pc1. p .. -…
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INTRODUCTION One type of ground effect machine is designed so that the pressure of the air cushion is contained by a…
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- 2 - A major object of the present study is therefore to derive a more de- tailed analysis of the mixing process in a highly…
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- 3 - where VQ , V(" , f and t are tangential velocity component, radial velocity component, fluid density and the eddy…
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- 4 - We obtain (14) (15) so that 'dVe* 1/ e3h -4 J'(7) "0 r* = (16) d:J. V~f. -R 3 4,.b - 6 f'll…
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- 5 - 2. Preliminary Approximation Solution of Jet Mixing Process As discussed later in Section 4 a major objective of the…
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- 6 - In the case of the wall jet, the maximum velocity (which occurs at y = Y1) decreases steadily with distance along the…
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I Multiplying (25) by f (~) we get - 7 - Again integrate (26) from 7 to ~ yields Evaluating equation (27) at 7 ~ 0 results…
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- 8 - boundary conditions ~(o) = 0 ) if 1/( 00) .:;::. 0 (36) Equation (35) with boundary conditions (36) has been solved…
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