Spheroidal Wave Functions
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About this ebook
Topics include separation of the scalar wave equation in spheroidal coordinates, angle and radial functions, integral representations and relations, and expansions in spherical Bessel function products. Additional subjects include recurrence relations of Whittaker type, asymptotic expansions for large values of c, and vector wave functions. The text concludes with an appendix, references, and tables of numerical values.
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Spheroidal Wave Functions - Carson Flammer
Spheroidal Wave Functions
Spheroidal Wave Functions
Carson Flammer
Dover Publications, Inc.
Mineola, New York
DOVER PHOENIX EDITIONS
Bibliographical Note
This Dover edition, first published in 2005, is an unabridged republication of a Stanford Research Institute monograph, originally published by Stanford University Press, Stanford, California, 1957. Page 141 of this edition was intentionally left blank to allow the next table to spread across two pages.
International Standard Book Number: 0-486-44639-5
eISBN-13: 978-0-486-15851-8
Manufactured in the United States of America
Dover Publications, Inc., 31 East 2nd Street, Mineola, N.Y. 11501
preface
The purpose of this monograph is to facilitate the use and calculation of spheroidal wave functions by the presentation of a detailed and unified account of the properties of these functions as they are known to date, along with some useful tables.
From the beginning, the development of the spheroidal functions has been incited, for the most part, by investigations of physical problems. The present work is no exception. While treating the electromagnetic problems of the prolate spheroidal monopole antenna, on the one hand, and the scattering of electromagnetic waves by a perfectly conducting circular disk, on the other, the author was lead in turn to the prolate and oblate spheroidal wave functions. In each case, further development of the functions in certain directions seemed desirable for a better treatment of the physical problem. The great interest expressed by many people in a resulting report on the prolate functions has inspired the preparation of this more comprehensive treatment of both the prolate and oblate functions.
The notation (with a slight change in designation) and normalization of the functions originally proposed by J. A. Stratton and L. J. Chu have been adopted in this book. In much of the development, the analyses of the properties of the prolate and of the oblate functions proceed along parallel lines. The formulas for the one type are then obtained from the other by a simple transformation. But in some of the development there is considerable asymmetry. This is especially true in the case of asymptotic solutions, where satisfactory solutions have been obtained for the oblate, but not for the prolate functions. The included tables of numerical values of the various quantities are also very unsymmetrical and, regrettably, scanty. In regard to tables of spheroidal wave functions, it is a pleasure to note that a really significant contribution has been made in the book with the same title as the present one by J. A. Stratton, P. M. Morse, L. J. Chu, J. D. C. Little, and F. J. Corbat1ó, which has come to hand after the completion of the present text. The book by Stratton, et al, has five hundred and fifty pages of tables of eigenvalues and expansion coefficients!
In consonance with its express purpose, the present monograph is addressed to the applied mathematician, the mathematical physicist, and the mathematical engineer, and not to the pure mathematician. The existence of solutions and the completeness of sets of functions are presumed, not demonstrated, in the text that follows. To the pure mathematician the recent book, Mathieusche Funktionen und Sphäroidfunktionen, by J. Meixner and F. W. Schäfke, is heartily recommended.
I am greatly indebted to Miss Mary Humphrey for her assistance in the preparation of the tables. I should also like to thank Professor R. D. Spence for making available his computations of the prolate spheroidal functions. To Dr George W. Evans, II, I express my gratitude for his careful reading and criticism of the manuscript. Finally, it is a pleasure for me to express my appreciation to Stanford Research Institute for instituting the series of monographs of which this is the first.
The manuscript was prepared with the support of the United States Air Force, and I wish to acknowledge my obligation to this support.*
Carson Flammer
Menlo Park, California
February 1956
* The ideas expressed in this book represent the personal views of the author and are not necessarily those of the United States Air Force.
contents
preface
chapter 1 introduction
1.1 Historical Survey
1.2 Survey of Applications
Spheroidal antennas. Acoustic diffraction by circular disks and apertures. Acoustic radiation from a vibrating circular disk. Acoustic scattering by spheroids. Steady flow of a viscous fluid past a spheroid. Spheroidal potential well. Spheroidal cavity systems. Electromagnetic diffraction by circular disks and apertures. Electromagnetic scattering by spheroids
chapter 2 separation of the scalar wave equation in spheroidal coordinates
2.1 Spheroidal Coordinates
2.2 The Spheroidal Differential Equations
2.3 General Properties
table I Notations for Prolate Spheroidal Wave Functions
table II Notations for Oblate Spheroidal Wave Functions
chapter 3 the angle functions
3.1 The Functions Smn
Expansions in associated Legendre functions of the first kind. Power-series developments of the eigenvalues. Power-series developments of the expansion coefficients. Bouwkamp’s method of approximation. Normalization. The case of negative values of m
3.2 Expansions in Powers of 1 — η²
3.3 The Special Case of m = 1, c =
3.4 Other Expansions
3.5 The Functions
table III λon and λin in Powers of c²
chapter 4 the radial functions
4.1 Expansions in Spherical Bessel Functions
4.2 Relations Between the Radial and Angle Functions
4.3 The Special Case of m — 1, c =
4.4 Power-series Expansions
The prolate radial functions. The oblate radial functions
4.5 Other Expansions
4.6 Special Values
Special values of the prolate functions. Special values of the oblate functions table IV The Coefficients
chapter 5 integral representations and relations
5.1 A Theorem
5.2 Expansions of the Green’s Functions
5.3 Various Integral Relations
5.4 Generalization of F. Neumann’s Integral
chapter 6 expansions in spherical bessel function products
6.1 The Prolate Functions
6.2 The Oblate Functions
chapter 7 recurrence relations of whittaker type
7.1 Recurrence Relations for the Radial Functions
Relations between functions of order m. Relations between functions of order m and order m ± 1
chapter 8 asymptotic expansions for large values of c
8.1 The Prolate Functions
8.2 The Oblate Functions
The angle functions. The radial functions
chapter 9 vector wave functions
9.1 Definition of the Functions
9.2 Expansions in Vector Wave Functions
Expansions of plane polarized waves. Expansions of the radiation from Hertzian dipoles
table V Expressions of the Spheroidal Vector Wave Functions
appendix
references
tables of numerical values
Introduction
Comparison with the Tables of Stratton et al
Power-Series Expansion Coefficients for λmn
Power-Series Expansion Coefficients for
Power-Series Expansion Coefficients for
Prolate Spheroidal Functions:
Eigenvalues λmn
Expansion coefficients and
Expansion coefficients
Expansion coefficients
Joining factors
Angle functions Smn(c, η)
Normalization constants Nmn
Radial functions of the first kind
Derivative of the radial functions of the first kind
Radial functions of the second kind
Derivative of the radial functions of the second kind
Oblate Spheroidal Functions:
Eigenvalues λmn
Expansion coefficients
Angle functions Smn(–ic, η)
Radial functions of the first and second kinds
1
introduction
1.1 Historical Survey
The differential equations resulting from the separation of the scalar Helmholtz differential equation
in general ellipsoidal coordinates, were first obtained in the case of k² = 0, i.e., for the Laplace equation, by G. Lamé [l]¹ in 1837. This was three years after Lamé had for the first time effected the transformation of to general orthogonal coordinates [2]. Consequently the designation of ‘Lamé’s equation’ came into use, and the integrals of the separated differential equations became known as ‘Lamé’s functions.’ Later, as the wave equation with k² > 0 came under consideration, the designations ‘Lamé’s potential functions,’ or ellipsoidal harmonics, and ‘Lamé’s