The Evanston Colloquium Lectures On Mathematics Delivered From Aug 28 to Sept

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As to the conformal representation (Fig. 6), it can be shown that the upper half of the ^r-plane, with the points a, b, c on Fig. 6.
the real axis and \, /z, v assumed as real, is transformed for each branch of the ^-function into a triangular area abc bounded by 36 LECTURE V.
three circular arcs ; let us call such an area a circular triangle (Kreisbogendreieck). The angles at the vertices of this triangle are XTT, pir, VTT.
This, then, is the geometrical representation we have to take as our b
...asis. In order to derive from it conclusions as to the nature of the transcendental functions defined by the differential equation, it will evidently be necessary to inquire what are the forms of such circular triangles in the most general case. For it is to be noticed that there is no restric- tion laid upon the values of the constants X, p, v, so that the angles of our triangle are not necessarily acute, nor even convex ; in other words, in the general case the vertices will be branch-points. The triangle itself is here to be regarded as something like an extensible and flexible membrane spread out between the circles forming the boundary.

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