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====Introduce Coordinate-Parameter η==== Following the lead of [http://adsabs.harvard.edu/abs/1985MNRAS.216..553B Blaes (1985)], and without loss of generality, we can everywhere replace the dimensionless function representing the unperturbed equilibrium enthalpy distribution, <math>~\Theta_H</math> — that varies from unity at the cross-sectional center of the torus to zero at the torus surface — with the parameter, <div align="center"> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~\eta^2</math> </td> <td align="center"> <math>~\equiv</math> </td> <td align="left"> <math>~1 - \Theta_H \, ,</math> </td> </tr> </table> </div> that varies from zero at the (cross-sectional) center to unity at the surface. Making this substitution, our governing PDE becomes, <div align="center"> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~0</math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ (1-\eta^2) x^2\cdot \frac{\partial^2(\delta W)}{\partial x^2} +(1-\eta^2) \cdot \frac{\partial^2(\delta W)}{\partial\theta^2} + \biggl\{(1-\eta^2) x \biggl[\frac{1-2x \cos\theta}{ 1-x\cos\theta}\biggr] + nx^2 \cdot \frac{\partial(1-\eta^2) }{\partial x} \biggr\} \cdot \frac{\partial (\delta W)}{\partial x} </math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> </td> <td align="left"> <math>~ + \biggl[\frac{(1-\eta^2) x\sin\theta}{ (1-x\cos\theta) } + n\cdot \frac{\partial (1-\eta^2) }{\partial\theta} \biggr] \cdot \frac{\partial (\delta W)}{\partial\theta} + \biggl[ \frac{2n x^2}{\beta^2}\biggl( \frac{{\bar\sigma}}{\Omega_0} \biggr)^2 - \frac{m^2 x^2(1-\eta^2) }{(1-x\cos\theta)^2} \biggr]\delta W </math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ x^2 (1-\eta^2)\cdot \frac{\partial^2(\delta W)}{\partial x^2} + (1-\eta^2) \cdot \frac{\partial^2(\delta W)}{\partial\theta^2} + \biggl\{x (1-\eta^2) \biggl[\frac{1-2x \cos\theta}{ 1-x\cos\theta}\biggr] -2 nx^2 \eta \cdot \frac{\partial \eta }{\partial x} \biggr\} \cdot \frac{\partial (\delta W)}{\partial x} </math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> </td> <td align="left"> <math>~ + \biggl[\frac{(1-\eta^2) x\sin\theta}{ (1-x\cos\theta) } -2n\eta \cdot \frac{\partial \eta }{\partial\theta} \biggr] \cdot \frac{\partial (\delta W)}{\partial\theta} + \biggl[ \frac{2n x^2}{\beta^2}\biggl( \frac{{\bar\sigma}}{\Omega_0} \biggr)^2 - \frac{m^2 x^2(1-\eta^2) }{(1-x\cos\theta)^2} \biggr]\delta W \, . </math> </td> </tr> </table> </div>
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