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==Preamble==
{| class="wikitable" width=100% style="margin-right: auto; margin-left: 0px; border-style: solid; border-width: 3px; border-color:black;"
|-
! style="height: 50px; background-color:black;"|[[File:HBook_title_Fluids2.png|780px|link=H_BookTiledMenu|Tiled Menu]]
|}
Much of the astrophysics community's present understanding of the structure, stability, and dynamical evolution of individual stars, short-period binary star systems, and the gaseous disks that are associated with numerous types of stellar systems (including galaxies) are derived from an examination of the behavior of a [[PGE#Principal_Governing_Equations|specific set of coupled, partial differential equations]].  These equations &#8212; also heavily used to model continuum flows in terrestrial environments &#8212; are thought to govern the underlying physics of the vast majority of macroscopic fluid configurations in astronomy.  Although relatively simple in form, they prove to be very rich in nature.


Consult the [https://www.mediawiki.org/wiki/Special:MyLanguage/Help:Contents User's Guide] for information on using the wiki software.
The literature on this subject is enormous, as serious discussions of the structure and dynamical properties of stars and galaxies date back well over a century. The primary purpose of ''this'' work is two-fold:
 
<ol>
==Pages Worth Visiting==
<li>To document in an electronically accessible format many of the key physical principles that underlie modern discussions of the structure, stability, and dynamics of self-gravitating (astrophysical) fluid systems.</li>
 
<li>To take advantage of the added dimensions offered by the hypertext medium &#8212; such as color, text/equation linkages, animation, and virtual reality environments &#8212; to effectively illustrate many of these physical principles.</li>
<ul>
  <li>[https://tohline.education Introductory Web Page]</li>
  <li>[[A2HostingEnvironment|Experimenting With the a2Hosting Environment]]</li>
  <li>[[3Dconfigurations/RiemannEllipsoids|Riemann (1860)]]</li>
  <li>[[Appendix/EquationTemplates|Appendix:  Equation Templates]]</li>
  <li>[[Appendix/SGFimages|Appendix:  SGF Images]]</li>
  <li>[[Appendix/Mathematics/EulerAngles|Appendix:  Mathematics/EulerAngles]]</li>
</ul>
 
== Getting started ==
* [https://www.mediawiki.org/wiki/Special:MyLanguage/Manual:Configuration_settings Configuration settings list]
* [https://www.mediawiki.org/wiki/Special:MyLanguage/Manual:FAQ MediaWiki FAQ]
* [https://lists.wikimedia.org/mailman/listinfo/mediawiki-announce MediaWiki release mailing list]
* [https://www.mediawiki.org/wiki/Special:MyLanguage/Localisation#Translation_resources Localise MediaWiki for your language]
* [https://www.mediawiki.org/wiki/Special:MyLanguage/Manual:Combating_spam Learn how to combat spam on your wiki]
 
==Various Trials &amp; Tests==
 
<ol type="I">
  <li>First (bad) [[User:Jet53man/Tests|MediaWiki tests]]</li>
  <li>Learning how to modify and enhance the [[A2HostingEnvironment|a2Hosting MediaWiki environment]].</li>
</ol>
</ol>
We have adopted ''[https://www.mediawiki.org/wiki/MediaWiki MediaWiki]'' as the hosting environment of choice most significantly because, after incorporating the proper set of extensions, it facilitates the insertion of complex, LaTeX-formulated mathematical expressions into the text.


If you are interested in learning about, or extending your understanding and appreciation of, the behavior of self-gravitating astrophysical fluids, we recommend that you proceed to the [[H_BookTiledMenu#Tiled_Menu|accompanying table of contents]], which we have assembled in a form that will be referred to as a ''Tiled Menu''; each tile is linked to one of approximately 100<sup>&dagger;</sup> separate chapter discussions. From each chapter you will be able to return to this ''Main_Page'' or to the overarching [[H_BookTiledMenu#Tiled_Menu|Tiled Menu]] by clicking the appropriately named link near the top of the indexed column that resides on the left of each MediaWiki page.


I'm just testing to see if I'm properly editing.
<table border="0" align="center" cellpadding="5" width="50%">
<math>
E = mc^2
</math>
 
<div align="center">
<math>H = \int\frac{dP}{\rho}</math> .
</div>
 
Try another way:  {{math|sin &pi; {{=}} 0}}
 
{{math|<VAR>&alpha;</VAR>}}
 
{{ Template:TeX|\alpha \, \! }}
 
{{ &alpha; }}
 
==Lagrangian Representation==
 
===in terms of velocity:===
Among the [[User:Tohline/PGE#Principal_Governing_Equations|principal governing equations]] we have included the
 
<div align="center">
<span id="ConservingMomentum:Lagrangian"><font color="#770000">'''Lagrangian Representation'''</font></span><br />
of the Euler Equation,
 
{{User:Tohline/Math/EQ_Euler01}}
 
[<b>[[User:Tohline/Appendix/References#BLRY07|<font color="red">BLRY07</font>]]</b>], p. 13, Eq. (1.55)
</div>
 
===in terms of momentum density:===
Multiplying this equation through by the mass density {{User:Tohline/Math/VAR_Density01}} produces the relation,
<div align="center">
<math>\rho\frac{d\vec{v}}{dt} = - \nabla P - \rho\nabla \Phi</math> ,
</div>
which may be rewritten as,
<div align="center">
<math>\frac{d(\rho\vec{v})}{dt}- \vec{v}\frac{d\rho}{dt} = - \nabla P - \rho\nabla \Phi</math> .
</div>
Combining this with the [[User:Tohline/PGE/ConservingMass#ConservingMass:Lagrangian|Standard Lagrangian Representation of the Continuity Equation]], we derive,
<div align="center">
<math>\frac{d(\rho\vec{v})}{dt}+ (\rho\vec{v})\nabla\cdot\vec{v} = - \nabla P - \rho\nabla \Phi</math> .
</div>
 
 
==Eulerian Representation==
 
===in terms of velocity:===
 
By replacing the so-called Lagrangian (or "material") time derivative <math>d\vec{v}/dt</math> in the Lagrangian representation of the Euler equation by its Eulerian counterpart (see, for example, the wikipedia discussion titled, "[https://en.wikipedia.org/wiki/Material_derivative Material_derivative]", to understand how the Lagrangian and Eulerian descriptions of fluid motion differ from one another conceptually as well as how to mathematically transform from one description to the other), we directly obtain the
 
<div align="center">
<span id="ConservingMomentum:Eulerian"><font color="#770000">'''Eulerian Representation'''</font></span><br />
of the Euler Equation,
 
{{User:Tohline/Math/EQ_Euler02}}
</div>
 
===in terms of momentum density:===
 
As was done above in the context of the Lagrangian representation of the Euler equation, we can multiply this expression through by {{User:Tohline/Math/VAR_Density01}} and combine it with the continuity equation to derive what is commonly referred to as the,
 
<div align="center">
<span id="ConservingMomentum:Conservative"><font color="#770000">'''Conservative Form'''</font></span><br />
of the Euler Equation,
 
{{User:Tohline/Math/EQ_Euler03}}
 
[<b>[[User:Tohline/Appendix/References#BLRY07|<font color="red">BLRY07</font>]]</b>], p. 8, Eq. (1.31)
</div>
 
The second term on the left-hand-side of this last expression represents the divergence of the "[https://en.wikipedia.org/wiki/Dyadics dyadic product]" or "[https://en.wikipedia.org/wiki/Outer_product outer product]" of the vector momentum density and the velocity vector, and is sometimes written as, <math>~\nabla\cdot [(\rho \vec{v}) \otimes \vec{v}]</math>.
 
===in terms of the vorticity:===
Drawing on one of the standard [https://en.wikipedia.org/wiki/Vector_calculus_identities#Dot_product_rule dot product rule vector identities], the nonlinear term on the left-hand-side of the Eulerian representation of the Euler equation can be rewritten as,
<div align="center">
<math>
(\vec{v}\cdot\nabla)\vec{v} = \frac{1}{2}\nabla(\vec{v}\cdot\vec{v}) - \vec{v}\times(\nabla\times\vec{v})
= \frac{1}{2}\nabla(v^2) + \vec{\zeta}\times \vec{v} ,
</math>
</div>
where,
<div align="center">
<math>
\vec\zeta \equiv \nabla\times\vec{v}
</math>
</div>
is commonly referred to as the [https://en.wikipedia.org/wiki/Vorticity vorticity].  Making this substitution leads to an expression for the,
 
<div align="center">
Euler Equation<br />
<span id="ConservingMomentum:Vorticity"><font color="#770000">'''in terms of the Vorticity'''</font></span>,
 
{{User:Tohline/Math/EQ_Euler04}}
</div>
 
==Double Check Vector Identities==
 
In a subsection of an accompanying chapter titled, [[User:Tohline/AxisymmetricConfigurations/SolutionStrategies#Double_Check_Vector_Identities|''Double Check Vector Identities,'']] we explicitly demonstrate for four separate "simple rotation profiles" that these two separate terms involving a nonlinear velocity expression do indeed generate identical mathematical relations, namely.
<table border="0" cellpadding="5" align="center">
 
<tr>
<tr>
  <td align="right">
<td align="center" bgcolor="lightgrey">
<math>~(\vec{v} \cdot \nabla) \vec{v}</math>
<font color="white" size="+1">Proceed to [[H_BookTiledMenu|Tiled Menu]]</font>
  </td>
</td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\vec\zeta \times \vec{v} + \frac{1}{2}\nabla (v^2) \, ;</math>
  </td>
</tr>
</tr>
</table>
</table>
and we explicitly demonstrate that they are among the set of velocity profiles that can also be expressed in terms of the gradient of a "centrifugal potential," <math>~\nabla\Psi</math>.
===Relationship Between State Variables===


If the two normalized state variables, <math>~\chi</math> and <math>~z</math>, are known, then the third normalized state variable, <math>~p_\mathrm{total}</math>, can be obtained directly from the [[User:Tohline/SR/PressureCombinations#Total_Pressure|above key expression for the total pressure]], that is,
==Highlights==


<div align="center">
===Tiled Menu===
<math>p_\mathrm{total}(\chi, z) = 8(C_g \chi)^3  z + F(\chi) + \biggl(\frac{8\pi^4}{15}\biggr) z^4 \, ,</math>
[[H_BookTiledMenu#Tiled_Menu|Individual tiles]] are linked to<sup>&dagger;</sup> &hellip;
</div>
<ul>
where,
  <li>Introductory discussions of the ''Principal Governing Equations''.</li>
<div align="center">
  <li>Roughly 50 chapters that examine the structure, stability, and dynamical evolution of (1D) spherically symmetric configurations.</li>
<math>C_g \equiv \biggl(\frac{\mu_e m_p}{\bar\mu m_u}\biggr)^{1/3} \, .</math>
  <li>Approximately 30 chapters that focus on the properties and behavior of (2D) axisymmetric configurations.</li>
</div>
  <li>Approximately 15 chapters that review what is presently understood about the structure and dynamical evolution of fully 3D configurations.</li>
</ul>
<sup>&dagger;</sup><font size="-1">April 2022: &nbsp;Presently our ''Tiled Menu'' provides links to roughly 100 separate chapter discussions; these chapters, in turn, contain links to at least a hundred additional pages of supporting material. These numbers will steadily increase as we continue to examine the behavior of a wider variety of astrophysical fluid systems.</font>


If it is the two normalized state variables, <math>~\chi</math> and <math>~p_\mathrm{total}</math>, that are known, the third normalized state variable &#8212; namely, the normalized temperature, <math>~z</math> &#8212; also can be obtained analytically. But the governing expression is not as simple because it results from an inversion of the total pressure equation and, hence, the solution of a quartic equation.  As is [[User:Tohline/SR/Ptot_QuarticSolution#Determining_Temperature_from_Density_and_Pressure|detailed in the accompanying discussion]], the desired solution is,
===Classic Works===
<ol>
  <li>[[Apps/MaclaurinSpheroids/GoogleBooks#Excerpts_from_A_Treatise_of_Fluxions|Maclaurin's (1742)]] Original Text &amp; Analysis</li>
  <li>[[3Dconfigurations/RiemannEllipsoids#Riemann_(1826_-_1866)|Bernhard Riemann's (1861)]] collected works</li>
  <li>[[SSC/Structure/Lane1870#Lane.27s_1870_Work|J. H. Lane (1870)]]</li>
  <li>[[SSC/Perturbations#Classic_Papers_that_Derive_&_Use_this_Relation|Eddington's (1926)]] Derivation of the LAWE</li>
  <li>[[SSC/Structure/WhiteDwarfs#Chandrasekhar_mass|Chandrasekhar Limiting (White Dwarf) Mass (1935)]]</li>
  <li>[[SSC/Structure/LimitingMasses#Sch.C3.B6nberg-Chandrasekhar_Mass|Sch&ouml;nberg - Chandrasekhar Mass (1942)]]</li>
  <li>[[SSC/Structure/BonnorEbert#Pressure-Bounded_Isothermal_Sphere|Bonnor - Ebert Isothermal Spheres (1955 - 56)]]</li>
  <li>[[Appendix/References#EFE|S. Chandrasekhar's (1969)]] ''Ellipsoidal Figures of Equilibrium''</li>
  <li>[[Apps/PapaloizouPringleTori#Massless_Polytropic_Tori|Papaloizou - Pringle Tori (1984)]]</li>
</ol>


<div align="center">
===Under-Appreciated Works===
<math>
<!-- <table border="0" align="right" width="150px" cellpadding="12"><tr><td align="center">
z(\chi, p_\mathrm{total}) = \theta_\chi \phi^{-1/3}\biggl[ (\phi - 1)^{1/2} - 1 \biggr] ,
[[File:MovieWongN4b.gif|thumb|Contribution to potential by mode n = 3 (magnified by 100)]]
</math>
</td></tr></table>
</div>
-->
<ol>
  <li>[[ThreeDimensionalConfigurations/FerrersPotential|Ferrers (1877) Gravitational Potential for Inhomogeneous Ellipsoids]]</li>
  <li>[[SSC/Structure/Polytropes#Srivastava's_F-Type_Solution|Srivastava's (1968) analytic (F-type) solution]] to the Lane-Emden equation of index, <math>n=5</math> &#8212; hereinafter referred to as <math>\theta_{5F}(\xi)</math>.</li>
  <li>[[Apps/Wong1973Potential|Wong's (1973) Analytic Potential for a Uniform-Density Torus]]</li>
  <li>[[SSC/Stability/InstabilityOnsetOverview#Yabushita.27s_Insight_Regarding_Stability|Yabushita's (1974) Analytic Eigenvector for Marginally Unstable, Pressure-Truncated Isothermal Spheres]]</li>
  <li>[[Apps/HayashiNaritaMiyama82|Hayashi, Narita, &amp; Miyama's (1982) Analytic Description of Rotating Isothermal Configurations with Flat Rotation Curves]]</li>
  <li>[[SSC/Structure/BiPolytropes/Analytic15|Murphy's (1985) Analytic Prescription]] of the Equilibrium Structure of <math>(n_c, n_e) = (1, 5)</math> Bipolytropes</li>
  <li>[[SSC/Structure/BiPolytropes/Analytic51|Eggleton, Faulkner &amp; Cannon's (1998) Analytic Prescription]] of the Equilibrium Structure of <math>(n_c, n_e) = (5, 1)</math> Bipolytropes</li>
</ol>


where,
===Our (Tohline's) Recent Contributions===
<ol>
  <li>The maximum of [[SSC/Structure/Polytropes#Srivastava's_F-Type_Solution|Srivastava's <math>\theta_{5F}(\xi)</math> function]] occurs precisely when the function argument, <math>\xi = \xi_\mathrm{crit} \equiv e^{2\tan^{-1}(1+2^{1/3})}.</math></li>
  <li>Analytic Determination of the [[SSC/Stability/InstabilityOnsetOverview#Polytropic|Eigenvector Associated with Marginally Unstable, Pressure-Truncated Polytropic Spheres]]</li>
  <li>
The task of evaluating the gravitational potential (both inside and outside) of a uniform-density, axisymmetric configuration having any surface shape [[2DStructure/ToroidalCoordinates#Using_Toroidal_Coordinates_to_Determine_the_Gravitational_Potential|has been reduced to a problem of carrying out a single, line integration]].
  </li>
  <li>
[[Appendix/Ramblings/NonlinarOscillation|Exact demonstration of the validity of the B-KB74 conjecture]] &#8212; see {{ B-KB74 }} &#8212; in the context of spherically symmetric, pressure-truncated, <math>n = 5</math> polytropes.
  </li>
  <li>[[3Dconfigurations/DescriptionOfRiemannTypeI#Lagrangian_Fluid_Trajectories|Analytic Prescription of the Trajectories of Lagrangian Fluid Elements in Riemann Type I Ellipsoids]]</li>
  <li>Virtual Reality: &nbsp;[[ThreeDimensionalConfigurations/MeetsCOLLADAandOculusRiftS|Riemann meets COLLADA &amp; Oculus Rift S]]; see, for example, our [[Appendix/Ramblings/COLLADA/RiemannSType|Table of Accessible COLLADA Models]]</li>
</ol>


<div align="center">
=What's Next? (Ideas for Future Doctoral Dissertations)=
<table border="0" cellpadding="5" align="center">
<ul>
<li>Formation of Binary Stars:  The classic fission hypothesis proposes that binary stars form from dynamic (or </li>
</ul>


<tr>
=Personal Reflections=
  <td align="right">
<ul>
<math>~\theta_\chi</math>
<li>[http://www.phys.lsu.edu/~tohline/TinsleyNotes1978.pdf Notes] from [https://en.wikipedia.org/wiki/Beatrice_Tinsley#Death Beatrice Tinsley] showing that she, too, had given some thought to the implications of a 1/r force-law for gravity in 1978.</li>
  </td>
<li>[[DarkMatter/VeraRubin|My early interactions]] with [https://en.wikipedia.org/wiki/Vera_Rubin Vera Rubin].</li>
  <td align="center">
<li>[[Appendix/Ramblings/MyDoctoralStudents|Doctoral students whom I have advised]].</li>
<math>~\equiv</math>
<li>[[Appendix/CGH/WhatIsReal|What is Real?]]</li>
  </td>
</ul>
  <td align="left" bgcolor="yellow">
<math>~\biggl( \frac{3\cdot 5}{2^2 \pi^4} \biggr)^{1/3} C_g\chi \, ,</math>
  </td>
</tr>
 
<tr>
  <td align="right">
<math>~\phi</math>
  </td>
  <td align="center">
<math>~\equiv</math>
  </td>
  <td align="left" bgcolor="lightblue">
<math>~ 2^{3/2} \biggl[ 1 + (1 + \lambda^3)^{1/2} \biggr]^{1/2}
\biggl\{ \biggl[ 1 + (1 + \lambda^3)^{1/2} \biggr]^{2/3} - \lambda \biggr\}^{-3/2}\, ,</math>
  </td>
</tr>


<tr>
=See Also=
  <td align="right">
<math>~\lambda</math>
  </td>
  <td align="center">
<math>~\equiv</math>
  </td>
  <td align="left" bgcolor="pink">
<math>~
\biggl(\frac{\pi^4}{2\cdot 3^4\cdot 5} \biggr)^{1/3} \biggl[\frac{p_\mathrm{total}-F(\chi)}{(C_g \chi)^{4}}\biggr] \, .
</math>
  </td>
</tr>
</table>
</div>


It also would be desirable to have an analytic expression for the function, <math>~\chi(z, p_\mathrm{total})</math>, in order to be able to immediately determine the normalized density from any specified values of the normalized temperature and normalized pressure.  However, it does not appear that the [[User:Tohline/SR/PressureCombinations#Total_Pressure|above key expression for the total pressure]] can be inverted to provide such a closed-form expression.
<ul>
 
  <li>[[OldVistrailsCoverPage|Old (VisTrails) Cover Page]]</li>
 
</ul>
<span id="Step2"><font color="red"><b>STEP #2</b></font></span>


As viewed from the ''tipped'' coordinated frame, the curve that is identified by this intersection should be an
<table border="0" cellpadding="5" align="center">
<tr>
<td align="center" colspan="3"><font color="maroon">'''Off-Center Ellipse'''</font></td>
</tr>
<tr>
  <td align="right">
<math>~1</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\biggl[\frac{x'}{x_\mathrm{max}} \biggr]^2 + \biggl[\frac{y' - y_c}{y_\mathrm{max}} \biggr]^2 </math>
  </td>
</tr>
<tr>
  <td align="right">
&nbsp;
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\biggl[\frac{x'}{x_\mathrm{max}} \biggr]^2 + \biggl[\frac{(y')^2  - 2y' y_c + y_c^2}{y^2_\mathrm{max}} \biggr] \, ,</math>
  </td>
</tr>
</table>


<span id="Result3">that lies in the</span> x'-y' plane &#8212; that is, <math>~z' = 0</math>.  Let's see if the intersection expression can be molded into this form.
{{ SGFfooter }}
<table border="0" cellpadding="5" align="center">
 
<tr>
  <td align="right">
<math>~1 - \frac{z_0^2}{c^2} - \frac{(x')^2}{a^2} </math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~(y')^2  \biggl[\frac{c^2 + b^2\tan^2\theta}{b^2c^2} \biggr]\cos^2\theta  + 2y' \biggl[ \frac{z_0 \sin\theta}{c^2} \biggr]  </math>
  </td>
</tr>
 
<tr>
  <td align="right">
&nbsp;
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\biggl[\frac{c^2 + b^2\tan^2\theta}{b^2c^2} \biggr]\cos^2\theta \biggl\{ (y')^2 - 2y' \biggl[ \frac{-z_0 \sin\theta}{c^2 \cos^2\theta} \biggr]\biggl[\frac{b^2c^2}{c^2 + b^2\tan^2\theta} \biggr]  \biggr\}</math>
  </td>
</tr>
 
<tr>
  <td align="right">
&nbsp;
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\kappa^2 \biggl[ (y')^2 - 2y' \underbrace{\biggl( \frac{-z_0 \sin\theta}{c^2 \kappa^2} \biggr)}_{y_c}  \biggr] \, ,</math>
  </td>
</tr>
</table>
 
<table border="1" align="center" cellpadding="10" width="60%" bordercolor="orange">
<tr><td align="center" bgcolor="lightblue">'''RESULT 3'''<br />(same as [[User:Tohline/ThreeDimensionalConfigurations/ChallengesPt2#Result1|Result 1]], but different from [[#Result2|Result 2, below]])
</td></tr>
<tr><td align="left">
<table border="0" cellpadding="5" align="center">
 
<tr>
  <td align="right">
<math>~\frac{y_c}{z_0}</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~
-\frac{\sin\theta}{c^2\kappa^2}
</math>
  </td>
</tr>
</table>
 
</td></tr>
</table>
 
where,
<table border="0" cellpadding="5" align="center">
 
<tr>
  <td align="right">
<math>~\kappa^2</math>
  </td>
  <td align="center">
<math>~\equiv</math>
  </td>
  <td align="left">
<math>~
\frac{c^2 \cos^2\theta + b^2 \sin^2\theta}{b^2c^2} \, .
</math>
  </td>
</tr>
</table>
Dividing through by <math>~\kappa^2</math>, then adding <math>~y_c^2</math> to both sides gives,
 
<table border="0" cellpadding="5" align="center">
 
<tr>
  <td align="right">
<math>~(y')^2 - 2y' y_c  + y_c^2</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\underbrace{\biggl[ \frac{1}{\kappa^2} - \frac{z_0^2}{c^2 \kappa^2} + y_c^2 \biggr]}_{y^2_\mathrm{max}} - \frac{(x')^2}{a^2\kappa^2} \, .</math>
  </td>
</tr>
</table>
Finally, we have,
 
<table border="0" cellpadding="5" align="center">
 
<tr>
  <td align="right">
<math>\frac{1}{y^2_\mathrm{max}} \biggl[ (y')^2 - 2y' y_c  + y_c^2 \biggr]</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left" bgcolor="yellow">
<math>~1 - (x')^2 \underbrace{\biggl[ \frac{1}{a^2\kappa^2 y_\mathrm{max}^2} \biggr]}_{ 1/x^2_\mathrm{max} } \, .</math>
  </td>
</tr>
</table>
So &hellip; the intersection expression can be molded into the form of an off-center ellipse if we make the following associations:
 
<table border="1" cellpadding="8" align="center" width="60%"><tr><td align="left">
<table border="0" cellpadding="5" align="center">
 
<tr>
  <td align="right">
<math>~\frac{y_c}{z_0}</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~- \frac{\sin\theta}{c^2 \kappa^2} \, ,</math>
  </td>
</tr>
 
<tr>
  <td align="right">
<math>~y_\mathrm{max}^2</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~\frac{1}{\kappa^2}\biggl[ 1 - \frac{z_0^2}{c^2 } - \frac{z_0 \sin\theta}{c^2} \biggr] \, ,</math>
  </td>
</tr>
 
<tr>
  <td align="right">
<math>~x_\mathrm{max}^2</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~a^2 \biggl[ 1 - \frac{z_0^2}{c^2 } - \frac{z_0 \sin\theta}{c^2} \biggr] \, .</math>
  </td>
</tr>
</table>
Note as well that,
<table border="0" cellpadding="5" align="center">
 
<tr>
  <td align="right">
<math>~\biggl( \frac{x_\mathrm{max}}{y_\mathrm{max}}\biggr)^2</math>
  </td>
  <td align="center">
<math>~=</math>
  </td>
  <td align="left">
<math>~a^2\kappa^2 = \frac{a^2}{b^2 c^2} \biggl[ c^2 \cos^2\theta + b^2 \sin^2\theta \biggr] \, .</math>
  </td>
</tr>
</table>
 
</td></tr></table>

Latest revision as of 18:40, 1 May 2024

Preamble

Tiled Menu

Much of the astrophysics community's present understanding of the structure, stability, and dynamical evolution of individual stars, short-period binary star systems, and the gaseous disks that are associated with numerous types of stellar systems (including galaxies) are derived from an examination of the behavior of a specific set of coupled, partial differential equations. These equations — also heavily used to model continuum flows in terrestrial environments — are thought to govern the underlying physics of the vast majority of macroscopic fluid configurations in astronomy. Although relatively simple in form, they prove to be very rich in nature.

The literature on this subject is enormous, as serious discussions of the structure and dynamical properties of stars and galaxies date back well over a century. The primary purpose of this work is two-fold:

  1. To document in an electronically accessible format many of the key physical principles that underlie modern discussions of the structure, stability, and dynamics of self-gravitating (astrophysical) fluid systems.
  2. To take advantage of the added dimensions offered by the hypertext medium — such as color, text/equation linkages, animation, and virtual reality environments — to effectively illustrate many of these physical principles.

We have adopted MediaWiki as the hosting environment of choice most significantly because, after incorporating the proper set of extensions, it facilitates the insertion of complex, LaTeX-formulated mathematical expressions into the text.

If you are interested in learning about, or extending your understanding and appreciation of, the behavior of self-gravitating astrophysical fluids, we recommend that you proceed to the accompanying table of contents, which we have assembled in a form that will be referred to as a Tiled Menu; each tile is linked to one of approximately 100 separate chapter discussions. From each chapter you will be able to return to this Main_Page or to the overarching Tiled Menu by clicking the appropriately named link near the top of the indexed column that resides on the left of each MediaWiki page.

Proceed to Tiled Menu

Highlights

Tiled Menu

Individual tiles are linked to

  • Introductory discussions of the Principal Governing Equations.
  • Roughly 50 chapters that examine the structure, stability, and dynamical evolution of (1D) spherically symmetric configurations.
  • Approximately 30 chapters that focus on the properties and behavior of (2D) axisymmetric configurations.
  • Approximately 15 chapters that review what is presently understood about the structure and dynamical evolution of fully 3D configurations.

April 2022:  Presently our Tiled Menu provides links to roughly 100 separate chapter discussions; these chapters, in turn, contain links to at least a hundred additional pages of supporting material. These numbers will steadily increase as we continue to examine the behavior of a wider variety of astrophysical fluid systems.

Classic Works

  1. Maclaurin's (1742) Original Text & Analysis
  2. Bernhard Riemann's (1861) collected works
  3. J. H. Lane (1870)
  4. Eddington's (1926) Derivation of the LAWE
  5. Chandrasekhar Limiting (White Dwarf) Mass (1935)
  6. Schönberg - Chandrasekhar Mass (1942)
  7. Bonnor - Ebert Isothermal Spheres (1955 - 56)
  8. S. Chandrasekhar's (1969) Ellipsoidal Figures of Equilibrium
  9. Papaloizou - Pringle Tori (1984)

Under-Appreciated Works

  1. Ferrers (1877) Gravitational Potential for Inhomogeneous Ellipsoids
  2. Srivastava's (1968) analytic (F-type) solution to the Lane-Emden equation of index, n=5 — hereinafter referred to as θ5F(ξ).
  3. Wong's (1973) Analytic Potential for a Uniform-Density Torus
  4. Yabushita's (1974) Analytic Eigenvector for Marginally Unstable, Pressure-Truncated Isothermal Spheres
  5. Hayashi, Narita, & Miyama's (1982) Analytic Description of Rotating Isothermal Configurations with Flat Rotation Curves
  6. Murphy's (1985) Analytic Prescription of the Equilibrium Structure of (nc,ne)=(1,5) Bipolytropes
  7. Eggleton, Faulkner & Cannon's (1998) Analytic Prescription of the Equilibrium Structure of (nc,ne)=(5,1) Bipolytropes

Our (Tohline's) Recent Contributions

  1. The maximum of Srivastava's θ5F(ξ) function occurs precisely when the function argument, ξ=ξcrite2tan1(1+21/3).
  2. Analytic Determination of the Eigenvector Associated with Marginally Unstable, Pressure-Truncated Polytropic Spheres
  3. The task of evaluating the gravitational potential (both inside and outside) of a uniform-density, axisymmetric configuration having any surface shape has been reduced to a problem of carrying out a single, line integration.
  4. Exact demonstration of the validity of the B-KB74 conjecture — see 📚 Bisnovatyi-Kogan & Blinnikov (1974) — in the context of spherically symmetric, pressure-truncated, n=5 polytropes.
  5. Analytic Prescription of the Trajectories of Lagrangian Fluid Elements in Riemann Type I Ellipsoids
  6. Virtual Reality:  Riemann meets COLLADA & Oculus Rift S; see, for example, our Table of Accessible COLLADA Models

What's Next? (Ideas for Future Doctoral Dissertations)

  • Formation of Binary Stars: The classic fission hypothesis proposes that binary stars form from dynamic (or

Personal Reflections

See Also


Tiled Menu

Appendices: | VisTrailsEquations | VisTrailsVariables | References | Ramblings | VisTrailsImages | myphys.lsu | ADS |