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An elliptic
partial differential equation given by
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(1)
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where is a scalar function and is the scalar
Laplacian, or
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(2)
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where is a vector
function and is the vector
Laplacian (Moon and Spencer 1988, pp. 136-143).
When , the Helmholtz differential equation
reduces to Laplace's equation.
When (i.e., for imaginary ), the equation
becomes the space part of the diffusion equation.
The Helmholtz differential equation can be solved by separation of variables in only 11 coordinate systems, 10 of
which (with the exception of confocal
paraboloidal coordinates) are particular cases of the confocal ellipsoidal system: Cartesian, confocal
ellipsoidal, confocal
paraboloidal, conical,
cylindrical, elliptic cylindrical, oblate spheroidal, paraboloidal, parabolic cylindrical, prolate spheroidal, and spherical coordinates (Eisenhart 1934ab). Laplace's equation (the Helmholtz differential equation with
) is separable in the two additional
bispherical coordinates
and toroidal coordinates.
If Helmholtz's equation is separable in a three-dimensional coordinate system, then Morse and Feshbach (1953, pp. 509-510) show that
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(3)
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where . The Laplacian is therefore of
the form
![del ^2=1/(h_1h_2h_3){g_1(u_2,u_3)partial/(partialu_1)[f_1(u_1)partial/(partialu_1)]+g_2(u_1,u_3)partial/(partialu_2)[f_2(u_2)partial/(partialu_2)]+g_3(u_1,u_2)partial/(partialu_3)[f_3(u_3)partial/(partialu_3)]},](/images/equations/HelmholtzDifferentialEquation/NumberedEquation4.gif) |
(4)
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which simplifies to
![del ^2=1/(h_1^2f_1)partial/(partialu_1)[f_1(u_1)partial/(partialu_1)]+1/(h_2^2f_2)partial/(partialu_2)[f_2(u_2)partial/(partialu_2)]+1/(h_3^2f_3)partial/(partialu_3)[f_3(u_3)partial/(partialu_3)].](/images/equations/HelmholtzDifferentialEquation/NumberedEquation5.gif) |
(5)
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Such a coordinate system obeys the Robertson condition, which means that the Stäckel
determinant is of the form
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(6)
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Eisenhart, L. P. "Separable Systems in Euclidean 3-Space." Physical
Review 45, 427-428, 1934a.
Eisenhart, L. P. "Separable Systems of Stäckel." Ann. Math. 35,
284-305, 1934b.
Eisenhart, L. P. "Potentials for Which Schroedinger Equations Are Separable."
Phys. Rev. 74, 87-89, 1948.
Kriezis, E. E.; Tsiboukis, T. D.; Panas, S. M.; and Tegopoulos, J. A. "Eddy Currents:theory and Applications,." Proc. IEEE 80,
1559-1589, 1992.
Moon, P. and Spencer, D. E. "Eleven Coordinate Systems" and "The Vector Helmholtz Equation." §1 and 5 in Field Theory Handbook, Including Coordinate Systems, Differential
Equations, and Their Solutions, 2nd ed. New York: Springer-Verlag, pp. 1-48
and 136-143, 1988.
Morse, P. M. and Feshbach, H. Methods of Theoretical Physics, Part I. New York: McGraw-Hill,
pp. 125-126, 271, and 509-510, 1953.
Zwillinger, D. (Ed.). CRC Standard Mathematical Tables and Formulae. Boca Raton,
FL: CRC Press, p. 417, 1995.
Zwillinger, D. Handbook of Differential Equations, 3rd ed. Boston, MA:
Academic Press, p. 129, 1997.
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