Appendix/Ramblings/Interrelating51and00Bipolytropes/Organization: Difference between revisions
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==Structure of (n<sub>c</sub>, n<sub>e</sub>) = (0, 0) Bipolytropes== | ==Structure of (n<sub>c</sub>, n<sub>e</sub>) = (0, 0) Bipolytropes== | ||
Here we draw heavily from an [[SSC/Structure/BiPolytropes/Analytic00|accompanying discussion]] to construct a [[SSC/Structure/BiPolytropes#BiPolytropes|bipolytrope]] in which both the core and the envelope have uniform densities, that is, the structure of both the core and the envelope will be modeled using an <math>n = 0</math> polytropic index. | Here we draw heavily from an [[SSC/Structure/BiPolytropes/Analytic00|accompanying discussion]] to construct a [[SSC/Structure/BiPolytropes#BiPolytropes|bipolytrope]] in which both the core and the envelope have uniform densities, that is, the structure of both the core and the envelope will be modeled using an <math>n = 0</math> polytropic index. | ||
Assuming that the central density, <math>\rho_0</math>, and central pressure, <math>P_0</math>, are specified, the natural dimensionless radius is given by the expression, | |||
<table border="0" cellpadding="5" align="center"> | |||
<tr> | |||
<td align="right"> | |||
<math>\chi</math> | |||
</td> | |||
<td align="center"> | |||
<math>\equiv</math> | |||
</td> | |||
<td align="left"> | |||
<math> | |||
r \biggl[ \frac{G\rho_0^2}{P_0} \biggr]^{1 / 2} | |||
\, .</math> | |||
</td> | |||
</tr> | |||
</table> | |||
===Throughout the core (0 ≤ χ ≤ χ<sub>i</sub>)=== | |||
In equilibrium, the radial profile of the density, pressure, and integrated mass are, respectively, | |||
<table border="0" cellpadding="5" align="center"> | |||
<tr> | |||
<td align="right"> | |||
<math>\rho</math> | |||
</td> | |||
<td align="center"> | |||
<math>=</math> | |||
</td> | |||
<td align="left"> | |||
<math>\rho_0</math> | |||
</td> | |||
</tr> | |||
<tr> | |||
<td align="right"> | |||
<math>P</math> | |||
</td> | |||
<td align="center"> | |||
<math>=</math> | |||
</td> | |||
<td align="left"> | |||
<math>P_0 \biggl( 1 - \frac{2\pi}{3}\chi^2 \biggr)</math> | |||
</td> | |||
</tr> | |||
<tr> | |||
<td align="right"> | |||
<math>M_r</math> | |||
</td> | |||
<td align="center"> | |||
<math>=</math> | |||
</td> | |||
<td align="left"> | |||
<math>\frac{4\pi}{3} \biggl[ \frac{P_0^3}{G^3 \rho_0^4} \biggr]^{1/2} \chi^3 \, .</math> | |||
</td> | |||
</tr> | |||
</table> | |||
===Interface Conditions=== | |||
In terms of the (as yet unspecified) total radius, <math>R</math>, we use <math>q</math> to specify the fractional radial location of the core/envelope interface, that is, | |||
<table border="0" cellpadding="5" align="center"> | |||
<tr> | |||
<td align="right"> | |||
<math>q</math> | |||
</td> | |||
<td align="center"> | |||
<math>\equiv</math> | |||
</td> | |||
<td align="left"> | |||
<math> | |||
\frac{r_i}{R} | |||
</math> | |||
</td> | |||
</tr> | |||
<tr> | |||
<td align="right"> | |||
<math>\Rightarrow ~~~ \chi_i</math> | |||
</td> | |||
<td align="center"> | |||
<math>\equiv</math> | |||
</td> | |||
<td align="left"> | |||
<math> | |||
q ~ \biggl[ \frac{G\rho_0^2 R^2}{P_0} \biggr]^{1 / 2} \, . | |||
</math> | |||
</td> | |||
</tr> | |||
</table> | |||
And whether viewed from the perspective of the core or the envelope, the pressure at the interface is given by the expression, | |||
<table border="0" cellpadding="5" align="center"> | |||
<tr> | |||
<td align="right"> | |||
<math>P_i</math> | |||
</td> | |||
<td align="center"> | |||
<math>=</math> | |||
</td> | |||
<td align="left"> | |||
<math>P_0 \biggl( 1 - \frac{2\pi}{3}\chi_i^2 \biggr)</math> | |||
</td> | |||
</tr> | |||
</table> | |||
===Envelope Solution (χ ≥ χ<sub>i</sub>)=== | |||
After specifying the envelope-to-core density ratio, <math>\rho_e/\rho_0</math>, the envelope's equilibrium radial profile of the density, pressure, and integrated mass are, respectively, | |||
<table border="0" cellpadding="3" align="center"> | |||
<tr> | |||
<td align="right"> | |||
<math>~\rho</math> | |||
</td> | |||
<td align="center"> | |||
<math>~=</math> | |||
</td> | |||
<td align="left"> | |||
<math>~\rho_e</math> | |||
</td> | |||
</tr> | |||
<tr> | |||
<td align="right"> | |||
<math>~\frac{P}{P_0}</math> | |||
</td> | |||
<td align="center"> | |||
<math>~=</math> | |||
</td> | |||
<td align="left"> | |||
<math>1 - \frac{2\pi}{3}\chi_i^2 + | |||
\frac{2\pi}{3} \biggl(\frac{\rho_e}{\rho_0}\biggr) \chi_i^2 | |||
\biggl[ 2 \biggl(1 - \frac{\rho_e}{\rho_0} \biggr) \biggl( \frac{\chi_i}{\chi} - | |||
1\biggr) - \frac{\rho_e}{\rho_0} \biggl(\frac{\chi^2}{\chi_i^2} - 1 \biggr) \biggr]</math> | |||
</td> | |||
</tr> | |||
<tr> | |||
<td align="right"> | |||
<math>M_r</math> | |||
</td> | |||
<td align="center"> | |||
<math>=</math> | |||
</td> | |||
<td align="left"> | |||
<math>\frac{4\pi}{3} \biggl[ \frac{P_0^3}{G^3 \rho_0^4} \biggr]^{1/2} \chi_i^3\biggl[1 +\frac{\rho_e}{\rho_0} | |||
\biggl( \frac{\chi^3}{\chi_i^3} - 1\biggr) \biggr]</math> | |||
</td> | |||
</tr> | |||
</table> | |||
=Related Discussions= | =Related Discussions= | ||
* [[SSC/Structure/BiPolytropes/Analytic51#BiPolytrope_with_nc_.3D_5_and_ne_.3D_1|Analytic solution]] with <math> | * [[SSC/Structure/BiPolytropes/Analytic51#BiPolytrope_with_nc_.3D_5_and_ne_.3D_1|Analytic solution]] with <math>(n_c, n_e) = (5,1)</math>. | ||
{{ SGFfooter }} | {{ SGFfooter }} | ||
Latest revision as of 17:12, 16 October 2022
Interrelating (5, 1) and (0, 0) Bipolytropes
Structure of (nc, ne) = (0, 0) Bipolytropes
Here we draw heavily from an accompanying discussion to construct a bipolytrope in which both the core and the envelope have uniform densities, that is, the structure of both the core and the envelope will be modeled using an polytropic index.
Assuming that the central density, , and central pressure, , are specified, the natural dimensionless radius is given by the expression,
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Throughout the core (0 ≤ χ ≤ χi)
In equilibrium, the radial profile of the density, pressure, and integrated mass are, respectively,
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Interface Conditions
In terms of the (as yet unspecified) total radius, , we use to specify the fractional radial location of the core/envelope interface, that is,
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And whether viewed from the perspective of the core or the envelope, the pressure at the interface is given by the expression,
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Envelope Solution (χ ≥ χi)
After specifying the envelope-to-core density ratio, , the envelope's equilibrium radial profile of the density, pressure, and integrated mass are, respectively,
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Related Discussions
- Analytic solution with .
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