Digital Library of Mathematical Functions
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14 Legendre and Related FunctionsReal Arguments

§14.19 Toroidal (or Ring) Functions

Contents

§14.19(i) Introduction

When \nu=n-\frac{1}{2}, n=0,1,2,\dots, \mu\in\Real, and x\in(1,\infty) solutions of (14.2.2) are known as toroidal or ring functions. This form of the differential equation arises when Laplace’s equation is transformed into toroidal coordinates (\eta,\theta,\phi), which are related to Cartesian coordinates (x,y,z) by

where the constant c is a scaling factor. Most required properties of toroidal functions come directly from the results for \mathop{P^{{\mu}}_{{\nu}}\/}\nolimits\!\left(x\right) and \mathop{\boldsymbol{Q}^{{\mu}}_{{\nu}}\/}\nolimits\!\left(x\right). In particular, for \mu=0 and \nu=\pm\frac{1}{2} see §14.5(v).

§14.19(ii) Hypergeometric Representations

With \mathop{\mathbf{F}\/}\nolimits as in §14.3 and \xi>0,

14.19.2\mathop{P^{{\mu}}_{{\nu-\frac{1}{2}}}\/}\nolimits\!\left(\mathop{\cosh\/}%
\nolimits\xi\right)=\frac{\mathop{\Gamma\/}\nolimits\!\left(\frac{1}{2}-\mu%
\right)}{\pi^{{1/2}}\left(1-e^{{-2\xi}}\right)^{\mu}e^{{(\nu+(1/2))\xi}}}\*%
\mathop{\mathbf{F}\/}\nolimits\!\left(\tfrac{1}{2}-\mu,\tfrac{1}{2}+\nu-\mu;1-%
2\mu;1-e^{{-2\xi}}\right),\mu\neq\frac{1}{2},\frac{3}{2},\frac{5}{2},\ldots.