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Titlebook: Bergman’s Linear Integral Operator Method in the Theory of Compressible Fluid Flow; M. Z. Krzywoblocki Book 1960 Springer-Verlag Wien 1960

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31#
發(fā)表于 2025-3-26 21:45:11 | 只看該作者
List of Tables,Some tables will be given below. No attempt will be made to include long tables of various functions and coefficients which may be found in special papers by Bergman, as listed in Part VIII.
32#
發(fā)表于 2025-3-27 03:04:59 | 只看該作者
33#
發(fā)表于 2025-3-27 08:38:08 | 只看該作者
Errata in Previous Papers,A few errors and misprints were found here and there in previous papers. They will be corrected below, the numbers in brackets referring to the list of references at the end of the book.
34#
發(fā)表于 2025-3-27 12:17:06 | 只看該作者
35#
發(fā)表于 2025-3-27 15:35:21 | 只看該作者
36#
發(fā)表于 2025-3-27 20:04:02 | 只看該作者
37#
發(fā)表于 2025-3-27 23:51:56 | 只看該作者
General Remarks,). But for a mathematically advanced reader, it is obvious that the method presents some further possibilities which may be realized in the future. In the present section we shall briefly present a few of them.
38#
發(fā)表于 2025-3-28 05:19:12 | 只看該作者
39#
發(fā)表于 2025-3-28 08:38:26 | 只看該作者
Transonic Flow, regions. The complexity of the problem is the origin of several methods of solutions. Below, we shall try to outline and discuss a few of them. In the second half of this part a more general discussion of the problem of transonic flow will be presented without deriving the proofs which a reader who
40#
發(fā)表于 2025-3-28 11:11:11 | 只看該作者
Axially Symmetric Flow,ow past bodies of revolution. Let ., ., χ denote the cylindrical coordinates with the .-axis coincident with the axis of symmetry of the flow. The velocity vector then no longer depends on the rotation angle χ, but rather entirely on . and ., and always lies in a meridian plane (plane through the .-
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