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m (User:Tohline/SphericallySymmetricStructures moved to User:Tohline/SphericallySymmetricConfigurations: "Structures" in the title causes problems when trying to break discussion into Structure-Stability-Dynamics categories.)
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=Spherically Symmetric Structures=
=Spherically Symmetric Configurations=


==Principal Governing Equations==
If we assume that our self-gravitating configurations are spherically symmetric, then the coupled set of multidimensional, partial differential equations that serve as our [http://www.vistrails.org/index.php/User:Tohline/PGE principal governing equations] can be simplified to a coupled set of one-dimensional, ordinary differential equations.  This is accomplished by expressing each of the multidimensional spatial operators &#8212; gradient (<math>\nabla</math>), divergence (<math>\nabla\cdot</math>), and Laplacian (<math>\nabla^2</math>) &#8212; in spherical coordinates (<math>r, \theta, \phi</math>) then setting to zero all derivatives that are taken with respect to the angular coordinates <math>\theta</math> and <math>\phi</math>.  After making this simplification, our governing equations become,
<div align="center">
<math>\nabla \rightarrow \frac{d}{dr}</math><br />
<math>\nabla\cdot \rightarrow \frac{1}{r}\frac{d}{dr}</math><br />
<math>\nabla \rightarrow \frac{d}{dr}</math>
</div>
==Summaries==


<div align="right">
<div align="right">

Revision as of 22:58, 31 January 2010

Whitworth's (1981) Isothermal Free-Energy Surface
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Spherically Symmetric Configurations

Principal Governing Equations

If we assume that our self-gravitating configurations are spherically symmetric, then the coupled set of multidimensional, partial differential equations that serve as our principal governing equations can be simplified to a coupled set of one-dimensional, ordinary differential equations. This is accomplished by expressing each of the multidimensional spatial operators — gradient (<math>\nabla</math>), divergence (<math>\nabla\cdot</math>), and Laplacian (<math>\nabla^2</math>) — in spherical coordinates (<math>r, \theta, \phi</math>) then setting to zero all derivatives that are taken with respect to the angular coordinates <math>\theta</math> and <math>\phi</math>. After making this simplification, our governing equations become,

<math>\nabla \rightarrow \frac{d}{dr}</math>
<math>\nabla\cdot \rightarrow \frac{1}{r}\frac{d}{dr}</math>
<math>\nabla \rightarrow \frac{d}{dr}</math>


Summaries

Structure
LSU Structure still.gif

SUMMARY: The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically.

Stability
LSU Stable.animated.gif

SUMMARY: The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically.

Dynamics
Minitorus.animated.gif

SUMMARY: The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically. The equilibrium structure of a self-gravitating, non-rotating, uniform-density sphere can be described analytically.

Appendices

Whitworth's (1981) Isothermal Free-Energy Surface

© 2014 - 2021 by Joel E. Tohline
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Recommended citation:   Tohline, Joel E. (2021), The Structure, Stability, & Dynamics of Self-Gravitating Fluids, a (MediaWiki-based) Vistrails.org publication, https://www.vistrails.org/index.php/User:Tohline/citation