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	<id>https://selfgravitatingfluids.education/JETohline/index.php?action=history&amp;feed=atom&amp;title=Template%3ALSU_CT99CommonTheme3</id>
	<title>Template:LSU CT99CommonTheme3 - Revision history</title>
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	<updated>2026-04-25T05:31:01Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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		<id>https://selfgravitatingfluids.education/JETohline/index.php?title=Template:LSU_CT99CommonTheme3&amp;diff=1399&amp;oldid=prev</id>
		<title>Joel2: Created page with &quot;Now, beginning with Version 2 of our expression for the &#039;&#039;Gravitational Potential of Axisymmetric Mass Distributions&#039;&#039;, let&#039;s also map the (unprimed) cylindrical coordinate pair, &lt;math&gt;~(\varpi, z)&lt;/math&gt;, to the same (but, unprimed) toroidal coordinate system, &lt;math&gt;~(\eta,\theta)&lt;/math&gt;, and place the toroidal coordinate system&#039;s &#039;&#039;anchor ring&#039;&#039; in the equatorial plane of the cylindrical-coordinate system such that, &lt;math&gt;~(\varpi_a,z_a) = (a,0)&lt;/math&gt;.  This gives, wh...&quot;</title>
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		<updated>2024-06-21T23:47:46Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;Now, beginning with Version 2 of our expression for the &amp;#039;&amp;#039;Gravitational Potential of Axisymmetric Mass Distributions&amp;#039;&amp;#039;, let&amp;#039;s also map the (unprimed) cylindrical coordinate pair, &amp;lt;math&amp;gt;~(\varpi, z)&amp;lt;/math&amp;gt;, to the same (but, unprimed) toroidal coordinate system, &amp;lt;math&amp;gt;~(\eta,\theta)&amp;lt;/math&amp;gt;, and place the toroidal coordinate system&amp;#039;s &amp;#039;&amp;#039;anchor ring&amp;#039;&amp;#039; in the equatorial plane of the cylindrical-coordinate system such that, &amp;lt;math&amp;gt;~(\varpi_a,z_a) = (a,0)&amp;lt;/math&amp;gt;.  This gives, wh...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;Now, beginning with Version 2 of our expression for the &amp;#039;&amp;#039;Gravitational Potential of Axisymmetric Mass Distributions&amp;#039;&amp;#039;, let&amp;#039;s also map the (unprimed) cylindrical coordinate pair, &amp;lt;math&amp;gt;~(\varpi, z)&amp;lt;/math&amp;gt;, to the same (but, unprimed) toroidal coordinate system, &amp;lt;math&amp;gt;~(\eta,\theta)&amp;lt;/math&amp;gt;, and place the toroidal coordinate system&amp;#039;s &amp;#039;&amp;#039;anchor ring&amp;#039;&amp;#039; in the equatorial plane of the cylindrical-coordinate system such that, &amp;lt;math&amp;gt;~(\varpi_a,z_a) = (a,0)&amp;lt;/math&amp;gt;.  This gives, what we will refer to as the,&lt;br /&gt;
&lt;br /&gt;
&amp;lt;table border=&amp;quot;0&amp;quot; cellpadding=&amp;quot;5&amp;quot; align=&amp;quot;center&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;tr&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;center&amp;quot; colspan=&amp;quot;3&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;font color=&amp;quot;#770000&amp;quot;&amp;gt;&amp;#039;&amp;#039;&amp;#039;Gravitational Potential of an Axisymmetric Mass Distribution (Version 3)&amp;#039;&amp;#039;&amp;#039;&amp;lt;/font&amp;gt;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;/tr&amp;gt;&lt;br /&gt;
&amp;lt;tr&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;right&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;~\Phi(\varpi,z)\biggr|_\mathrm{axisym}&amp;lt;/math&amp;gt;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;center&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;~=&amp;lt;/math&amp;gt;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;left&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;~&lt;br /&gt;
- 2G a^2 \biggl[ \frac{(\cosh\eta - \cos\theta)}{\sinh\eta} \biggr]^{1 / 2} \iint\limits_\mathrm{config}  &lt;br /&gt;
 \biggl[\frac{ \sinh\eta^&amp;#039;}{(\cosh\eta^&amp;#039; - \cos\theta^&amp;#039;)^5} \biggr]^{1 / 2} \mu K(\mu) \rho(\eta^&amp;#039;, \theta^&amp;#039;) d\eta^&amp;#039; d\theta^&amp;#039; \, ,&amp;lt;/math&amp;gt;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;/tr&amp;gt;&lt;br /&gt;
&amp;lt;tr&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;center&amp;quot; colspan=&amp;quot;3&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;\mathrm{where:}~~~\mu^2 = \frac{ 2 \sinh\eta^&amp;#039;\cdot \sinh\eta}{ \sinh\eta^&amp;#039;\cdot \sinh\eta + \cosh\eta^&amp;#039;\cdot\cosh\eta -\cos(\theta^&amp;#039; - \theta) }  \, .&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;/tr&amp;gt;&lt;br /&gt;
&amp;lt;/table&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;!--&lt;br /&gt;
&amp;lt;table border=&amp;quot;0&amp;quot; cellpadding=&amp;quot;5&amp;quot; align=&amp;quot;center&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;tr&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;right&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;~\mu^2&amp;lt;/math&amp;gt;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;center&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;~=&amp;lt;/math&amp;gt;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;left&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;~\mu^2 =&lt;br /&gt;
\frac{ 4 \sinh\eta^&amp;#039;}{(\cosh\eta^&amp;#039; - \cos\theta^&amp;#039;)}&lt;br /&gt;
\biggl[  \frac{\sinh\eta}{(\cosh\eta - \cos\theta)} \biggr]&lt;br /&gt;
\biggl\{ \biggl[ \frac{\sinh\eta}{(\cosh\eta - \cos\theta)}+ \frac{\sinh\eta^&amp;#039;}{(\cosh\eta^&amp;#039; - \cos\theta^&amp;#039;)} \biggr]^2 + &lt;br /&gt;
\biggl[\frac{ \sin\theta}{(\cosh\eta - \cos\theta)} - \frac{ \sin\theta^&amp;#039;}{(\cosh\eta^&amp;#039; - \cos\theta^&amp;#039;)} \biggr]^2 \biggr\}^{-1} &lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;/tr&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;tr&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;right&amp;quot;&amp;gt;&lt;br /&gt;
&amp;amp;nbsp;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;center&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;~=&amp;lt;/math&amp;gt;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;left&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;~&lt;br /&gt;
\frac{ 2 \sinh\eta^&amp;#039;\cdot \sinh\eta}{ \sinh\eta^&amp;#039;\cdot \sinh\eta + \cosh\eta^&amp;#039;\cdot\cosh\eta -\cos(\theta^&amp;#039; - \theta) } \, .&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;/tr&amp;gt;&lt;br /&gt;
&amp;lt;/table&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;table border=&amp;quot;0&amp;quot; cellpadding=&amp;quot;5&amp;quot; align=&amp;quot;center&amp;quot;&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;tr&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;right&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;~\mu^2&amp;lt;/math&amp;gt;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;center&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;~=&amp;lt;/math&amp;gt;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
  &amp;lt;td align=&amp;quot;left&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;~&lt;br /&gt;
\frac{ 2 \sinh\eta^&amp;#039;\cdot \sinh\eta}{ \sinh\eta^&amp;#039;\cdot \sinh\eta + \cosh\eta^&amp;#039;\cdot\cosh\eta -\cos(\theta^&amp;#039; - \theta) } \, .&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
  &amp;lt;/td&amp;gt;&lt;br /&gt;
&amp;lt;/tr&amp;gt;&lt;br /&gt;
&amp;lt;/table&amp;gt;&lt;br /&gt;
--&amp;gt;&lt;/div&gt;</summary>
		<author><name>Joel2</name></author>
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