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=Elliptic Cylinder Coordinates=
=Elliptic Cylinder Coordinates=
Building on our [[User:Tohline/Appendix/Ramblings/DirectionCosines|general introduction to ''Direction Cosines'']] in the context of orthogonal curvilinear coordinate systems, here we detail the properties of [https://en.wikipedia.org/wiki/Elliptic_cylindrical_coordinates Elliptic Cylinder Coordinates].  First, we will present this coordinate system in the manner described by [<b>[[User:Tohline/Appendix/References#MF53|<font color="red">MF53</font>]]</b>]; second, we will provide an alternate presentation, obtained from Wikipedia; then, third, we will investigate whether or not a related coordinate system based on ''concentric'' (rather than ''confocal'') elliptic surfaces can be satisfactorily described.


{{LSU_HBook_header}}
{{LSU_HBook_header}}
Building on our [[User:Tohline/Appendix/Ramblings/DirectionCosines|general introduction to ''Direction Cosines'']] in the context of orthogonal curvilinear coordinate systems, here we detail the properties of [https://en.wikipedia.org/wiki/Elliptic_cylindrical_coordinates Elliptic Cylinder Coordinates].  First, we will present this coordinate system in the manner described by [<b>[[User:Tohline/Appendix/References#MF53|<font color="red">MF53</font>]]</b>]; second, we will provide an alternate presentation, obtained from Wikipedia; then, third, we will investigate whether or not a related coordinate system based on ''concentric'' (rather than ''confocal'') elliptic surfaces can be satisfactorily described.


==MF53==
==MF53==
[https://ui.adsabs.harvard.edu/abs/2020MNRAS.494.5825H/abstract J. -M. Hur&eacute;, B. Basillais, V. Karas, A. Trova, &amp; O. Semer&aacute;k (2020), MNRAS, 494, 5825-5838] have published a paper titled, ''The Exterior Gravitational Potential of Toroids.''  Here we examine how their work relates to the published work by [http://adsabs.harvard.edu/abs/1973AnPhy..77..279W C.-Y. Wong (1973, Annals of Physics, 77, 279)], which we have separately [[User:Tohline/Apps/Wong1973Potential#Wong.27s_.281973.29_Analytic_Potential|discussed in detail]].


From [[User:Tohline/Appendix/References#MF53|MF53]]'s ''Table of Separable Coordinates in Three Dimensions'' (see their Chapter 5, beginning on p. 655), we find the following description of '''Elliptic Cylinder Coordinates''' (p. 657).
<table border="0" cellpadding="5" align="center">
<tr>
  <td align="right">
<math>~x</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\xi_1 \xi_2 \, ;</math>
  </td>
</tr>
<tr>
  <td align="right">
<math>~y</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\biggl[ (\xi_1^2 - d^2)(1 - \xi_2^2)  \biggr]^{1 / 2} \, ;</math>
  </td>
</tr>
<tr>
  <td align="right">
<math>~z</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\xi_3 \, .</math>
  </td>
</tr>
</table>
Appreciating that,
<table border="0" cellpadding="5" align="center">
<tr>
  <td align="right">
<math>~\frac{\partial y}{\partial \xi_1}</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~
+\biggl[ (\xi_1^2 - d^2)(1 - \xi_2^2)  \biggr]^{- 1 / 2}\xi_1(1-\xi_2^2) \, ,
</math> &nbsp; &nbsp; &nbsp; and that,
  </td>
</tr>
<tr>
  <td align="right">
<math>~\frac{\partial y}{\partial \xi_2}</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~
- \biggl[ (\xi_1^2 - d^2)(1 - \xi_2^2)  \biggr]^{- 1 / 2}\xi_2(\xi_1^2 - d^2) \, ,
</math>
  </td>
</tr>
</table>
we find that the respective [[User:Tohline/Appendix/Ramblings/DirectionCosines#Scale_Factors|scale factors]] are given by the expressions,
<table border="0" cellpadding="5" align="center">
<tr>
  <td align="right">
<math>~ h_1^2</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\biggl(\frac{\partial x}{\partial\xi_1} \biggr)^2 + \biggl(\frac{\partial y}{\partial\xi_1} \biggr)^2 + \biggl(\frac{\partial z}{\partial\xi_1} \biggr)^2 </math>
  </td>
</tr>
<tr>
  <td align="right">
&nbsp;
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\xi_2^2 +\biggl[ (\xi_1^2 - d^2)(1 - \xi_2^2)  \biggr]^{- 1 / 2}\xi_1(1-\xi_2^2) </math>
  </td>
</tr>
<tr>
  <td align="right">
&nbsp;
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\biggl\{ \xi_2^2(\xi_1^2 - d^2)^{1 / 2} +(1 - \xi_2^2)^{- 1 / 2}\xi_1(1-\xi_2^2)\biggr\} (\xi_1^2 - d^2)^{-1 / 2}</math>
  </td>
</tr>
</table>


=See Also=
=See Also=

Revision as of 16:24, 15 October 2020

Elliptic Cylinder Coordinates

Whitworth's (1981) Isothermal Free-Energy Surface
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Building on our general introduction to Direction Cosines in the context of orthogonal curvilinear coordinate systems, here we detail the properties of Elliptic Cylinder Coordinates. First, we will present this coordinate system in the manner described by [MF53]; second, we will provide an alternate presentation, obtained from Wikipedia; then, third, we will investigate whether or not a related coordinate system based on concentric (rather than confocal) elliptic surfaces can be satisfactorily described.

MF53

From MF53's Table of Separable Coordinates in Three Dimensions (see their Chapter 5, beginning on p. 655), we find the following description of Elliptic Cylinder Coordinates (p. 657).

<math>~x</math>

<math>~=</math>

<math>~\xi_1 \xi_2 \, ;</math>

<math>~y</math>

<math>~=</math>

<math>~\biggl[ (\xi_1^2 - d^2)(1 - \xi_2^2) \biggr]^{1 / 2} \, ;</math>

<math>~z</math>

<math>~=</math>

<math>~\xi_3 \, .</math>

Appreciating that,

<math>~\frac{\partial y}{\partial \xi_1}</math>

<math>~=</math>

<math>~ +\biggl[ (\xi_1^2 - d^2)(1 - \xi_2^2) \biggr]^{- 1 / 2}\xi_1(1-\xi_2^2) \, , </math>       and that,

<math>~\frac{\partial y}{\partial \xi_2}</math>

<math>~=</math>

<math>~ - \biggl[ (\xi_1^2 - d^2)(1 - \xi_2^2) \biggr]^{- 1 / 2}\xi_2(\xi_1^2 - d^2) \, , </math>

we find that the respective scale factors are given by the expressions,

<math>~ h_1^2</math>

<math>~=</math>

<math>~\biggl(\frac{\partial x}{\partial\xi_1} \biggr)^2 + \biggl(\frac{\partial y}{\partial\xi_1} \biggr)^2 + \biggl(\frac{\partial z}{\partial\xi_1} \biggr)^2 </math>

 

<math>~=</math>

<math>~\xi_2^2 +\biggl[ (\xi_1^2 - d^2)(1 - \xi_2^2) \biggr]^{- 1 / 2}\xi_1(1-\xi_2^2) </math>

 

<math>~=</math>

<math>~\biggl\{ \xi_2^2(\xi_1^2 - d^2)^{1 / 2} +(1 - \xi_2^2)^{- 1 / 2}\xi_1(1-\xi_2^2)\biggr\} (\xi_1^2 - d^2)^{-1 / 2}</math>

See Also


Whitworth's (1981) Isothermal Free-Energy Surface

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