When , , , and 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 , which are related to Cartesian coordinates by
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where the constant is a scaling factor. Most required properties of toroidal functions come directly from the results for and . In particular, for and see §14.5(v).
With as in §14.3 and ,
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With ,
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With ,
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With ,
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