Planar and axisymmetric flows of a multicomponent compressible gas in a laminar boundary layer with nonzero tangential component of the velocity on a permeable surface are considered.The asymptotic solutions of the boundary-layer equations obtained earlier [1][2][3][4] for large values of the blowing and suction parameters are generalized to the case when the velocity vector of the blown or extracted gas makes an acute angle with th e surface of the body, this angle depending on the longitudinal coordinate. The region of applicability of the asymptotic formulas is estimated on the basis of the results of numerical solution of the boundary-layer equations.The results are given of some calculations of the boundary layer on a partly moving surface. ~any investigations have been made into the flow of liquids or gases in the boundary layer on amoving surface [5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20].The solution of similarity boundary-layer equations was considered in [5L10] and of nonsimilarity equations in [11][12][13][14][15].In [16][17] the transition of a laminar boundary layer from a fixed section of the surface to a moving section was studied.The solution of the boundary~layer equations in the neighborhood of the velocity discontinuity point on the surface was constructed by an asymptotic method of outer and inner expansions.The problem of inclined blowing was considered in [20] in the framework of the equations of an inviscid boundary layer with a longitudinal pressure gradient that is determined in the process of solution.We also mention the experimental papers [18,19].
i. Asymptotic Solution of the Boundary-Layer Equations in the Case of Strong Inclined Blowin~We generalize the asymptotic solution of the laminar boundary-layer equations at large values of the blowing parameter ~ (see [I, 2]) to the case when the velocity vector of the blown gas makes an acute angle with the surface of the body. The notation is given in [1,2].At large values of the parameter $, the flow in the wall layer in the absence of chemical reactions is described by the system of equations (2.7) of [1] or (1.6) of [2], whose solution with the boundary conditions (1.1) has the form u~(x't) --nw(t~ pw(t) [P(t) J } +a.2(t), (i=l,... N),
T(x,t) [ P(x) l~*(t' p(x,t)_[ P(x) 1~-'(') C,(x,t)=C,~(t)
Tw(t) =[ P(t----)-J ' "9-~ I. P(t) JMoscow.