By Holt Ashley

This wonderful, leading edge reference bargains a wealth of invaluable details and an outstanding heritage within the basics of aerodynamics. Fluid mechanics, consistent density inviscid circulation, singular perturbation difficulties, viscosity, thin-wing and narrow physique theories, drag minimalization, and different necessities are addressed in a full of life, literate demeanour and followed by means of diagrams.

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Additional info for Aerodynamics of Wings and Bodies

Example text

The combined conditions of irrotationality and continuity assure the existence of a velocity potential +(r, t ) and a stream function *(r, t ) , such that Q = V+ = V X Here r = xi (kq). (2-101) + yj. (2-102) If (2-101) is written out in component form, we obtain, (2-103) The latter equalities will be recognized as the Cauchy-Riemann relations. For constant-density fluid, V - Q = '7% (2-104) is the volume divergence, whereas for a rotational flow, V X Q = -kV% (2-1 05) is the vorticity vector. Therefore, in the case under consideration, v2+ = 0 = v2*.

2-14. Trailing-edge angle T of the sort produced by the transformation equation (2-1 39). We have no trouble in showing that the Joukowsky and von Mises transformations are cases of n = 2. For instance, the Joukowsky can be manipulated into (2-1 38) Von K B r m h and Trefftz (1918) suggested replacing (2-138) as follows: (2-139) As in Fig. ) is now ( 2 ~ T ) , so a finite interior angle has been introduced and can be selected at will. I n a similar fashion a factor 54 CONSTANT-DENSITY INVISCID FLOW [CHAP.

Ds. (2-92) These two results will not necessarily be equal, since we cannot prove the identity of the two line integrals when the region between them is not entirely occupied by fluid. As a matter of fact, the circulation around the closed path is exactly (2-93) It is an obvious result of Stokes’ theorem that r is the same for any path completely surrounding just the body illustrated. Hence the difference in the values of @ taken between paths on one side or the other always turns out to be exactly r, wherever the two points A and B are chosen.