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1: Sidebar 5.SB1: Gamma & Digamma Phase Plots
In the upper half of the image, the poles of Γ ( z ) are clearly visible at negative integer values of z : the phase changes by 2 π around each pole, showing a full revolution of the color wheel. …
2: 12.17 Physical Applications
In a similar manner coordinates of the paraboloid of revolution transform the Helmholtz equation into equations related to the differential equations considered in this chapter. … …
3: 14.31 Other Applications
The conical functions 𝖯 1 2 + i τ m ( x ) appear in boundary-value problems for the Laplace equation in toroidal coordinates (§14.19(i)) for regions bounded by cones, by two intersecting spheres, or by one or two confocal hyperboloids of revolution (Kölbig (1981)). …
4: 30.14 Wave Equation in Oblate Spheroidal Coordinates
The coordinate surfaces ξ = const . are oblate ellipsoids of revolution with focal circle z = 0 , x 2 + y 2 = c 2 . The coordinate surfaces η = const . are halves of one-sheeted hyperboloids of revolution with the same focal circle. …
5: 30.13 Wave Equation in Prolate Spheroidal Coordinates
The coordinate surfaces ξ = const . are prolate ellipsoids of revolution with foci at x = y = 0 , z = ± c . The coordinate surfaces η = const . are sheets of two-sheeted hyperboloids of revolution with the same foci. …
6: 1.6 Vectors and Vector-Valued Functions
For a surface of revolution, y = f ( x ) , x [ a , b ] , about the x -axis, …
7: Bibliography M
  • J. Meixner (1944) Die Laméschen Wellenfunktionen des Drehellipsoids. Forschungsbericht No. 1952 ZWB (German).