Difference between revisions of "User:Tohline/SSC/Structure/Polytropes/VirialSummary"
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<math>~\frac{1}{x^3} \biggl[ \biggl( \frac{3b}{n} \biggr)\biggl(\frac{n+3}{n}\biggr) x^{(n-3)/n} + 6c x^4 - 2a \biggr] | <math>~\frac{1}{x^3} \biggl[\biggl(\frac{n+3}{n}\biggr) \biggl( \frac{3b}{n} \biggr) x^{(n-3)/n} + 6c x^4 - 2a \biggr] \, .</math> | ||
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Virial equilibrium is obtained when <math>~d\mathfrak{G}^*/dx = 0</math>, that is, when | |||
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<math>~0</math> | |||
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<math>~=</math> | |||
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<math>~a - \biggl( \frac{3b}{n} \biggr) x^{(n-3)/n} + 3c x^4</math> | |||
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<math>~\Rightarrow ~~~ \biggl( \frac{3b}{n} \biggr) x_\mathrm{eq}^{(n-3)/n} </math> | |||
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<math>~=</math> | |||
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<math>~ a + 3c x_\mathrm{eq}^4 \, .</math> | |||
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And along an equilibrium ''sequence'', the ''specific'' equilibrium state — henceforth labeled as having the ''critical'' radius, <math>~x_\mathrm{crit}</math> — that marks a transition from dynamically stable to dynamically unstable configurations is identified by setting <math>~d^2\mathfrak{G}^*/dx^2 = 0</math>, that is, it is the configuration for which, | |||
<table border="0" cellpadding="5" align="center"> | |||
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<math>~0</math> | |||
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<td align="center"> | |||
<math>~=</math> | |||
</td> | |||
<td align="left"> | |||
<math>~\biggl[\biggl(\frac{n+3}{n}\biggr) \biggl( \frac{3b}{n} \biggr) x^{(n-3)/n} + 6c x^4 - 2a \biggr]_{x = x_\mathrm{eq}}</math> | |||
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<math>~\Rightarrow ~~~ | |||
x_\mathrm{crit}^4 | |||
</math> | |||
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<math>~=</math> | |||
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<math>~ | |||
\frac{a}{3^2c}\biggl(\frac{n - 3}{n+1}\biggr) \, . | |||
</math> | |||
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Revision as of 21:02, 7 February 2019
Virial Equilibrium of Pressure-Truncated Polytropes
Here we will draw heavily from an accompanying Free Energy Synopsis.
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In the context of spherically symmetric, pressure-truncated polytropic configurations, the relevant free-energy expression is,
<math>~\mathfrak{G}</math> |
<math>~=</math> |
<math>~W_\mathrm{grav} + U_\mathrm{int} + P_e V \, .</math> |
When rewritten in a suitably dimensionless form — see two useful alternatives, below — this expression becomes,
<math>~\mathfrak{G}^*</math> |
<math>~=</math> |
<math>~- a x^{-1} + bx^{-3/n} + c x^3 \, ,</math> |
where <math>~x</math> is the configuration's dimensionless radius and <math>~a</math>, <math>~b</math>, and <math>~c</math> are constants. We therefore have,
<math>~\frac{d\mathfrak{G}^*}{dx}</math> |
<math>~=</math> |
<math>~\frac{1}{x^2} \biggl[ a - \biggl( \frac{3b}{n} \biggr) x^{(n-3)/n} + 3c x^4 \biggr] \, ,</math> |
and,
<math>~\frac{d^2\mathfrak{G}^*}{dx^2}</math> |
<math>~=</math> |
<math>~\frac{1}{x^3} \biggl[\biggl(\frac{n+3}{n}\biggr) \biggl( \frac{3b}{n} \biggr) x^{(n-3)/n} + 6c x^4 - 2a \biggr] \, .</math> |
Virial equilibrium is obtained when <math>~d\mathfrak{G}^*/dx = 0</math>, that is, when
<math>~0</math> |
<math>~=</math> |
<math>~a - \biggl( \frac{3b}{n} \biggr) x^{(n-3)/n} + 3c x^4</math> |
<math>~\Rightarrow ~~~ \biggl( \frac{3b}{n} \biggr) x_\mathrm{eq}^{(n-3)/n} </math> |
<math>~=</math> |
<math>~ a + 3c x_\mathrm{eq}^4 \, .</math> |
And along an equilibrium sequence, the specific equilibrium state — henceforth labeled as having the critical radius, <math>~x_\mathrm{crit}</math> — that marks a transition from dynamically stable to dynamically unstable configurations is identified by setting <math>~d^2\mathfrak{G}^*/dx^2 = 0</math>, that is, it is the configuration for which,
<math>~0</math> |
<math>~=</math> |
<math>~\biggl[\biggl(\frac{n+3}{n}\biggr) \biggl( \frac{3b}{n} \biggr) x^{(n-3)/n} + 6c x^4 - 2a \biggr]_{x = x_\mathrm{eq}}</math> |
<math>~\Rightarrow ~~~ x_\mathrm{crit}^4 </math> |
<math>~=</math> |
<math>~ \frac{a}{3^2c}\biggl(\frac{n - 3}{n+1}\biggr) \, . </math> |
See Also
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