Design of Transonic Cascades By Conformal Transformation of the Complex Characte
Design of Transonic Cascades By Conformal Transformation of the Complex Characte
Eldon a Mcintyre
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This, in turn, leads to a further refinement of the singular solution. Consider the system of characteristic equations (2. 17). We recall that we have, in essence, already solved (2. 17a, c), since equations (2 . 14) - (2 . 16) have the effect of specifying u and V as functions of C and n . It follows then, that we need only solve the remaining equations. Since we have already determined the form of the solution, we substitute (2. 19) into (2. 17b, d) to obtain x^ + A_y. = (X^ + \_Y^) In (?-C^)... X^+X Y-"- 2 2 2 2 ^ "^^-^ 3 3 + (x|+x_y|) In (C-?g) + -^r^ + X^ + X_Y^ = B on n= constant, and + X^ + X^Y^^ = on E, = constant. -32- We can satisfy the first equation by setting (2. 21a) X^ + X_yJ = (2. 21b) X^ + X_Y^ = and 11 2 2 7, r, X^+X_Y^ X +X Y^ (2. 21c) X^ + X Y^ = — + ■= ^ on n = constant. Similarly, we can satisfy the second by requiring (2. 21d) X-"- + X Y"'^ = (2. 21e) X^ + X^Y^ = and n + n 2 2 r + X Y^ n + n (2. 21f) x-^ + X^Y^ = 3 3 on C = constant. Finally, if X and Y are to be regular solutions of (2.
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