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11: 14.31 Other Applications
§14.31(i) Toroidal Functions
§14.31(ii) Conical Functions
The conical functions 𝖯 1 2 + i τ m ( x ) appear in boundary-value problems for the Laplace equation in toroidal coordinates14.19(i)) for regions bounded by cones, by two intersecting spheres, or by one or two confocal hyperboloids of revolution (Kölbig (1981)). … Many additional physical applications of Legendre polynomials and associated Legendre functions include solution of the Helmholtz equation, as well as the Laplace equation, in spherical coordinates (Temme (1996b)), quantum mechanics (Edmonds (1974)), and high-frequency scattering by a sphere (Nussenzveig (1965)). …
12: 28.27 Addition Theorems
Addition theorems provide important connections between Mathieu functions with different parameters and in different coordinate systems. …
13: 30.14 Wave Equation in Oblate Spheroidal Coordinates
§30.14 Wave Equation in Oblate Spheroidal Coordinates
§30.14(i) Oblate Spheroidal Coordinates
Oblate spheroidal coordinates ξ , η , ϕ are related to Cartesian coordinates x , y , z by …
§30.14(ii) Metric Coefficients
§30.14(iii) Laplacian
14: 23.21 Physical Applications
§23.21(iii) Ellipsoidal Coordinates
Ellipsoidal coordinates ( ξ , η , ζ ) may be defined as the three roots ρ of the equation …where x , y , z are the corresponding Cartesian coordinates and e 1 , e 2 , e 3 are constants. The Laplacian operator 2 1.5(ii)) is given by
23.21.2 ( η ζ ) ( ζ ξ ) ( ξ η ) 2 = ( ζ η ) f ( ξ ) f ( ξ ) ξ + ( ξ ζ ) f ( η ) f ( η ) η + ( η ξ ) f ( ζ ) f ( ζ ) ζ ,
15: 30.13 Wave Equation in Prolate Spheroidal Coordinates
§30.13 Wave Equation in Prolate Spheroidal Coordinates
§30.13(i) Prolate Spheroidal Coordinates
§30.13(ii) Metric Coefficients
§30.13(iii) Laplacian
16: 10.73 Physical Applications
In cylindrical coordinates r , ϕ , z , (§1.5(ii) we have … See Krivoshlykov (1994, Chapter 2, §2.2.10; Chapter 5, §5.2.2), Kapany and Burke (1972, Chapters 4–6; Chapter 7, §A.1), and Slater (1942, Chapter 4, §§20, 25). … On separation of variables into cylindrical coordinates, the Bessel functions J n ( x ) , and modified Bessel functions I n ( x ) and K n ( x ) , all appear. … The functions 𝗃 n ( x ) , 𝗒 n ( x ) , 𝗁 n ( 1 ) ( x ) , and 𝗁 n ( 2 ) ( x ) arise in the solution (again by separation of variables) of the Helmholtz equation in spherical coordinates ρ , θ , ϕ 1.5(ii)): …
17: 14.30 Spherical and Spheroidal Harmonics
As an example, Laplace’s equation 2 W = 0 in spherical coordinates1.5(ii)): … Here, in spherical coordinates, L 2 is the squared angular momentum operator: …
18: 8 Incomplete Gamma and Related
Functions
19: 28 Mathieu Functions and Hill’s Equation
20: 8.26 Tables
  • Khamis (1965) tabulates P ( a , x ) for a = 0.05 ( .05 ) 10 ( .1 ) 20 ( .25 ) 70 , 0.0001 x 250 to 10D.

  • Abramowitz and Stegun (1964, pp. 245–248) tabulates E n ( x ) for n = 2 , 3 , 4 , 10 , 20 , x = 0 ( .01 ) 2 to 7D; also ( x + n ) e x E n ( x ) for n = 2 , 3 , 4 , 10 , 20 , x 1 = 0 ( .01 ) 0.1 ( .05 ) 0.5 to 6S.

  • Pagurova (1961) tabulates E n ( x ) for n = 0 ( 1 ) 20 , x = 0 ( .01 ) 2 ( .1 ) 10 to 4-9S; e x E n ( x ) for n = 2 ( 1 ) 10 , x = 10 ( .1 ) 20 to 7D; e x E p ( x ) for p = 0 ( .1 ) 1 , x = 0.01 ( .01 ) 7 ( .05 ) 12 ( .1 ) 20 to 7S or 7D.

  • Zhang and Jin (1996, Table 19.1) tabulates E n ( x ) for n = 1 , 2 , 3 , 5 , 10 , 15 , 20 , x = 0 ( .1 ) 1 , 1.5 , 2 , 3 , 5 , 10 , 20 , 30 , 50 , 100 to 7D or 8S.