单词 | Helmholtz Differential Equation | ||||||||||||||||||||||||||||||||||||||||||||||||||||||
释义 | Helmholtz Differential EquationA Partial Differential Equation which can be written in a Scalar version
The Helmholtz differential equation can be solved by Separation of Variables in only 11 coordinate systems, 10 ofwhich (with the exception of Confocal Paraboloidal Coordinates) are particular cases of the ConfocalEllipsoidal system: Cartesian, ConfocalEllipsoidal, Confocal Paraboloidal,Conical, Cylindrical, EllipticCylindrical, Oblate Spheroidal,Paraboloidal, Parabolic Cylindrical,Prolate Spheroidal, and Spherical Coordinates (Eisenhart 1934). Laplace's Equation (the Helmholtz differential equation with ) is separable in the two additionalBispherical Coordinates and Toroidal Coordinates. If Helmholtz's equation is separable in a 3-D coordinate system, then Morse and Feshbach (1953, pp. 509-510) show that
Eisenhart, L. P. ``Separable Systems in Euclidean 3-Space.'' Physical Review 45, 427-428, 1934. Eisenhart, L. P. ``Separable Systems of Stäckel.'' Ann. Math. 35, 284-305, 1934. Eisenhart, L. P. ``Potentials for Which Schroedinger Equations Are Separable.'' Phys. Rev. 74, 87-89, 1948. Morse, P. M. and Feshbach, H. Methods of Theoretical Physics, Part I. New York: McGraw-Hill, pp. 125-126 and 509-510, 1953. |
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