Difference between revisions of "User:Tohline/SSC/Perspective Reconciliation"
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(Begin reconciliation discussion) |
(→Linearizing the Key Relations: Begin laying out derivation table) |
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<table border="3" align="center" cellpadding="10"> | <table border="3" align="center" cellpadding="10"> | ||
<tr> | |||
<th align="center" colspan="2"><font color="darkgreen" size="+1">Continuity Equation</font></th> | |||
</tr> | |||
<tr> | <tr> | ||
<th align="center" width="50%">Lagrangian Perspective</th> | <th align="center" width="50%">Lagrangian Perspective</th> | ||
<th align="center" width="50%">Eulerian Perspective</th> | <th align="center" width="50%">Eulerian Perspective</th> | ||
</tr> | |||
<tr> | |||
<td align="center"> | |||
<div align="center"> | |||
<table border="0" cellpadding="5" align="center"> | |||
<tr> | |||
<td align="right"> | |||
<math>~\frac{d\rho}{dt}</math> | |||
</td> | |||
<td align="center"> | |||
<math>~=</math> | |||
</td> | |||
<td align="left"> | |||
<math>~- \rho \nabla\cdot\vec{v}</math> | |||
</td> | |||
</tr> | |||
</table> | |||
</div> | |||
</td> | |||
<td align="center"> | |||
<div align="center"> | |||
<table border="0" cellpadding="5" align="center"> | |||
<tr> | |||
<td align="right"> | |||
<math>~\frac{\partial\rho}{\partial t}</math> | |||
</td> | |||
<td align="center"> | |||
<math>~=</math> | |||
</td> | |||
<td align="left"> | |||
<math>~- \rho \nabla\cdot\vec{v} - \vec{v}\cdot \nabla\rho</math> | |||
</td> | |||
</tr> | </tr> | ||
</table> | </table> | ||
</div> | |||
</td> | |||
</tr> | |||
<tr> | |||
<th align="center" colspan="2">Spherically Symmetric Initial Configurations & Purely Radial Perturbations</th> | |||
</tr> | |||
<tr> | |||
<td align="center"> | |||
<div align="center"> | |||
<table border="0" cellpadding="5" align="center"> | |||
<tr> | |||
<td align="right"> | |||
<math>~\frac{d\rho}{dt}</math> | |||
</td> | |||
<td align="center"> | |||
<math>~=</math> | |||
</td> | |||
<td align="left"> | |||
<math>~- \frac{\rho}{r^2} \frac{\partial}{\partial r} \biggl( r^2 v_r \biggr)</math> | |||
</td> | |||
</tr> | |||
</table> | |||
</div> | |||
</td> | |||
<td align="center"> | |||
<div align="center"> | |||
<table border="0" cellpadding="5" align="center"> | |||
<tr> | |||
<td align="right"> | |||
<math>~\frac{\partial\rho}{\partial t}</math> | |||
</td> | |||
<td align="center"> | |||
<math>~=</math> | |||
</td> | |||
<td align="left"> | |||
<math>~- \frac{\rho}{r^2} \frac{\partial}{\partial r} \biggl( r^2 v_r \biggr) - v_r \frac{\partial \rho}{\partial r}</math> | |||
</td> | |||
</tr> | |||
</table> | |||
</div> | |||
</td> | |||
</tr> | |||
</table> | |||
=See Also= | =See Also= |
Revision as of 23:44, 11 December 2014
Reconciling Eulerian versus Lagrangian Perspectives
| Tiled Menu | Tables of Content | Banner Video | Tohline Home Page | |
Linearizing the Key Relations
Continuity Equation | |||||||
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Lagrangian Perspective | Eulerian Perspective | ||||||
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Spherically Symmetric Initial Configurations & Purely Radial Perturbations | |||||||
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