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Integral Elliptic Representations

The integral elliptic representations of the ellipsoidal coordinate system are given by the following three equations (, ):
$\displaystyle \beta =$ $\displaystyle c \int_{b}^{\xi_1} \frac{{\rm d}
\xi_1}{(c^2-\xi_1^2)(\xi_1^2-c^2)} =$ $\displaystyle F\left[
\sqrt{1-\frac{b^2}{c^2}},{\rm sin}^{-1}
\left( \sqrt{ \frac{1-\frac{b^2}{\xi_1^2}}{1-\frac{b^2}{c^2}} }
\right) \right],$  
$\displaystyle \gamma =$ $\displaystyle c \int_{0}^{\xi_1} \frac{{\rm d}
\xi_1}{(b^2-\xi_1^2)(c^2-\xi_1^2)} =$ $\displaystyle F\left[ \frac{b}{c}, {\rm sin}^{-1}\left(\frac{\xi_2}{b} \right)
\right],$ (A-1)
$\displaystyle \alpha =$ $\displaystyle c \int_{c}^{\xi_2} \frac{{\rm d}
\xi_2}{(\xi_2^2-b^2)(\xi_2^2-c^2)} =$ $\displaystyle F\left[ \frac{b}{c},\frac{\pi}{2} \right] - F\left[ \frac{b}{c},{\rm
sin}^{-1}\left(\frac{c}{\xi_3}\right) \right] ,$  

where $ F\left[ \cdot \right]$ are elliptic integrals of the first kind defined by

$\displaystyle u = F\left[\phi,k\right] = \int_{0}^{\phi} \frac{{\rm d}\theta}{\sqrt{1 - k^2 {\rm sin}^2 \theta}},$ (A-2)

where the elliptic modulus $ k$ satisfies $ 0 < k^2 <1$ and $ \phi$ is the Jacobi amplitude. Solutions to equation A-2 are calculated using the method of arithmetic-geometric mean and descending Landen Transformation described in ().

The integral transforms are invertible and can be represented in terms of Jacobi elliptic functions $ {\rm dc}(u,k), {\rm nd}(u,k)$ and $ {\rm
sn}(u,k)$ (, ):

$\displaystyle \xi_1$ $\displaystyle =$ $\displaystyle b\,{\rm nd} \left[ \beta,\sqrt{1-\frac{b^2}{c^2}} \right],$  
$\displaystyle \xi_2$ $\displaystyle =$ $\displaystyle b\,{\rm sn} \left[\gamma, \frac{b}{c} \right],$ (A-3)
$\displaystyle \xi_3$ $\displaystyle =$ $\displaystyle c\,{\rm dc} \left[ \alpha,\frac{b}{c} \right],$  

where $ k$ is again elliptic modulus and $ u$ is defined by equation A-2. The Jacobi elliptic functions are calculated using the method of the arithmetic-geometric mean described in ().
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Next: About this document ... Up: Shragge and Shan: Ellipsoidal Previous: APPENDIX A

2009-04-13