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==Three-Dimensional Configurations== {| class="Chap14A" width=100% style="margin-right: auto; margin-left: 0px; border-style: solid; border-width: 3px; border-color:navy;" |- ! style="height: 50px; width: 800px; background-color:lightgrey;"|<font color="navy" size="+2">(Initially) Three-Dimensional Configurations</font> |} <p> </p> ===Equilibrium Structures=== {| class="Chap14B" width=100% style="margin-right: auto; margin-left: 0px; border-style: solid; border-width: 3px; border-color:darkgrey;" |- ! style="height: 30px; width: 800px; background-color:lightgrey;"|<font color="white" size="+1">3D STRUCTURE</font> |} <!-- <table border="0" cellpadding="3" align="center" width="60%"> <tr><td align="left"> <font color="darkgreen">"One interesting aspect of our models … is the pulsation characteristic of the final central triaxial figure … our interest in the pulsations stems from a general concern about the equilibrium structure of self-gravitating, triaxial objects. In the past, attempts to construct hydrostatic models of any equilibrium, triaxial structure having both a high <math>~T/|W|</math> value and a compressible equation of state have met with very limited success … they have been thwarted by a lack of understanding of how to represent complex internal motions in a physically realistic way… We suggest … that a ''natural'' attribute of [such] configurations may be pulsation and that, as a result, a search for simple circulation hydrostatic analogs of such systems may prove to a fruitless endeavor.</font> </td></tr> <tr><td align="right"> — Drawn from §IVa of [https://ui.adsabs.harvard.edu/abs/1988ApJ...334..449W/abstract Williams & Tohline (1988)], ApJ, 334, 449 </td></tr></table> --> <table border="0" cellpadding="3" align="center" width="60%"> <tr><td align="left"> Special numerical techniques must be developed <font color="darkgreen">"to build three-dimensional compressible equilibrium models with complicated flows."</font> To date … <font color="darkgreen">"techniques have only been developed to build compressible equilibrium models of nonaxisymmetric configurations for a few systems with simplified rotational profiles, e.g., rigidly rotating systems ([https://ui.adsabs.harvard.edu/abs/1984PASJ...36..239H/abstract Hachisu & Eriguchi 1984]; [https://ui.adsabs.harvard.edu/abs/1986ApJS...62..461H/abstract Hachisu 1986)], irrotational systems ([https://ui.adsabs.harvard.edu/abs/1998ApJS..118..563U/abstract Uryū & Eriguchi 1998]), and configurations that are stationary in the inertial frame ([https://ui.adsabs.harvard.edu/abs/1996MNRAS.282..653U/abstract Uryū & Eriguchi 1996])."</font> </td></tr> <tr><td align="right"> — Drawn from §1 of {{ Ou2006full }} </td></tr></table> ====Ellipsoidal & Ellipsoidal-Like==== {| class="Chap15F" style="float:right; margin-left: 150px; border-style: solid; border-width: 3px; border-color:black;" |- ! style="height: 150px; width: 150px; background-color:#9390DB;"|[[VE/RiemannEllipsoids|Steady-State<br />2<sup>nd</sup>-Order<br />Tensor Virial<br />Equations]] |} {| class="Chap15G" style="margin-right: auto; margin-left: 75px; border-style: solid; border-width: 3px; border-color: black" |- ! style="height: 150px; width: 150px; background-color:#ffff99; border-right: 2px solid black; " |<b>Uniform-Density<br />Incompressible<br />Ellipsoids</b> | ! style="height: 150px; width: 150px; background-color:#ffeeee;" |[[3Dconfigurations/RiemannEllipsoids|<b>Bernhard<br />Riemann<br />(1861)</b>]] |} <p> </p> {| class="Chap15C" style="margin-right: auto; margin-left: 230px; border-style: solid; border-width: 3px; border-color: black" |- ! style="height: 150px; width: 150px; background-color:white; border-right: 2px dashed black; " |[[ThreeDimensionalConfigurations/HomogeneousEllipsoids|<b>The<br />Gravitational<br />Potential</b>]]<br />(A<sub>i</sub> coefficients) | ! style="height: 150px; width: 150px; background-color:#ffeeee; border-right: 2px dashed black; " |[[ThreeDimensionalConfigurations/JacobiEllipsoids#Jacobi_Ellipsoids|<b>Jacobi<br />Ellipsoids</b>]] | ! style="height: 150px; width: 150px; background-color:#ffeeee; border-right: 2px dashed black;" |[[ThreeDimensionalConfigurations/RiemannStype#Riemann_S-type_Ellipsoids|<b>Riemann<br />S-Type<br />Ellipsoids</b>]] | ! style="height: 150px; width: 150px; background-color:#ffeeee; border-right: 2px dashed black;" |[[3Dconfigurations/DescriptionOfRiemannTypeI|<b>Type I<br />Riemann<br />Ellipsoids</b>]] | ! style="height: 150px; width: 150px; background-color:white;" |[[ThreeDimensionalConfigurations/MeetsCOLLADAandOculusRiftS|<b>Riemann<br />meets<br />COLLADA<br />&<br /> Oculus Rift S</b>]] |} <p> </p> {| class="Chap15D" style="margin-right: auto; margin-left: 550px; border-style: solid; border-width: 3px; border-color: black;" |- ! style="height: 150px; width: 150px; background-color:white; border-right: 2px dashed black; " |[https://www.aimspress.com/article/10.3934/math.2019.2.215/fulltext.html <b>A Gauge Theory<br />of<br />Riemann Ellipsoids</b>] | ! style="height: 150px; width: 150px; background-color:white; " |[https://ui.adsabs.harvard.edu/abs/2020PhRvL.124e2501S/abstract <b>Nuclear<br />Wobbling Motion</b>] |} <p> </p> {| class="Chap16A" style="margin-right: auto; margin-left: 75px; border-style: solid; border-width: 3px; border-color: black" |- ! style="height: 150px; width: 150px; background-color:#ffff99; border-right: 2px solid black; " |<b>Compressible<br />Analogs of<br />Riemann Ellipsoids</b> | ! style="height: 150px; width: 150px; background-color:#ffeeee; border-right: 2px dashed black;" |[[ThreeDimensionalConfigurations/FerrersPotential|<b>Ferrers<br />Potential<br />(1877)</b>]] | ! style="height: 150px; width: 150px; background-color:white; border-right: 2px dashed black;" |[https://ui.adsabs.harvard.edu/abs/2006ApJ...639..549O/abstract <b>Constructing<br />Ellipsoidal<br /> & Ellipsoidal-Like<br />Configurations</b>] | ! style="height: 150px; width: 150px; background-color:white;" |[[ThreeDimensionalConfigurations/CAREs|<b>Thoughts<br />&<br />Challenges</b>]] |} <p> </p> * [https://ui.adsabs.harvard.edu/abs/1985Ap.....23..654K/abstract B. P. Kondrat'ev (1985)], Astrophysics, 23, 654: ''Irrotational and zero angular momentum ellipsoids in the Dirichlet problem'' * {{ LRS93bfull }}: ''Ellipsoidal Figures of Equilibrium: Compressible models'' ====Binary Systems==== * [https://ui.adsabs.harvard.edu/abs/1933MNRAS..93..539C/abstract S. Chandrasekhar (1933)], MNRAS, 93, 539: ''The equilibrium of distorted polytropes. IV. the rotational and the tidal distortions as functions of the density distribution'' * {{ Chandrasekhar63_XIXfull }}: ''The Equilibrium and the Stability of the Roche Ellipsoids'' <table border="0" align="center" width="100%" cellpadding="1"><tr> <td align="center" width="5%"> </td><td align="left"> <font color="green">Roche's problem is concerned with the equilibrium and the stability of rotating homogeneous masses which are, further, distorted by the constant tidal action of an attendant rigid spherical mass.</font> </td></tr></table> ===Stability Analysis=== {| class="Chap17A" width=100% style="margin-right: auto; margin-left: 0px; border-style: solid; border-width: 3px; border-color:darkgrey;" |- ! style="height: 30px; width: 800px; background-color:lightgrey;"|<font color="white" size="+1">3D STABILITY</font> |} ====Ellipsoidal & Ellipsoidal-Like==== {| class="Chap11C" style="margin-right: auto; margin-left: 75px; border-style: solid; border-width: 3px; border-color: black;" <!-- |+ style="text-align:left; height:40px;" | <font size="+2">'''CONTEXT'''</font> --> |- ! style="height: 150px; width: 150px; background-color:white; " |[[ThreeDimensionalConfigurations/Stability/RiemannEllipsoids|<b>Lebovitz & Lifschitz (1996)</b>]] |} <p> </p> ====Binary Systems==== * {{ Chandrasekhar63_XIXfull }}: ''The Equilibrium and the Stability of the Roche Ellipsoids'' * [https://ui.adsabs.harvard.edu/abs/2019ApJ...877....9H/abstract G. P. Horedt (2019)], ApJ, 877, 9: ''On the Instability of Polytropic Maclaurin and Roche Ellipsoids'' ===Nonlinear Evolution=== {| class="Chap18A" width=100% style="margin-right: auto; margin-left: 0px; border-style: solid; border-width: 3px; border-color:darkgrey;" |- ! style="height: 30px; width: 800px; background-color:lightgrey;"|<font color="white" size="+1">3D DYNAMICS</font> |} <p> </p> {| class="Chap18B" style="float:right; margin-left: 150px; border-style: solid; border-width: 3px; border-color:black;" |- ! style="height: 150px; width: 320px; background-color:#D0FFFF;"|[[File:JacobiMaclaurin2.gif|320px|link=ThreeDimensionalConfigurations/EFE_Energies#Animation|Animation related to Fig. 3 from Christodoulou1995]] | ! style="height: 150px; width: 150px; background-color:#9390DB; border-left:2px solid black;"|[[ThreeDimensionalConfigurations/EFE_Energies#Properties_of_Homogeneous_Ellipsoids_.282.29|Free-Energy<br />Evolution<br />from the Maclaurin<br />to the Jacobi<br />Sequence]] |} {| class="Chap18C" style="margin-right: auto; margin-left: 75px; border-style: solid; border-width: 3px; border-color: black;" |- ! style="height: 150px; width: 150px; background-color:#ffff99; border-right: 2px solid black; " |[[ThreeDimensionalConfigurations/BinaryFission#Fission_Hypothesis_of_Binary_Star_Formation|<b>Fission<br />Hypothesis</b>]] | ! style="height: 150px; width: 150px; background-color:white;" |[http://www.phys.lsu.edu/~tohline/fission.movies.html <b>"Fission"<br />Simulations<br />at LSU</b>] |} <p> </p> ====Secular==== * [https://ui.adsabs.harvard.edu/abs/1971ApJ...170..143F/abstract M. Fujimoto (1971)], ApJ, 170, 143: ''Nonlinear Motions of Rotating Gaseous Ellipsoids'' * [https://ui.adsabs.harvard.edu/abs/1973ApJ...181..513P/abstract W. H. Press & S. A. Teukolsky (1973)], ApJ, 181, 513: ''On the Evolution of the Secularly Unstable, Viscous Maclaurin Spheroids'' * [https://ui.adsabs.harvard.edu/abs/1977ApJ...213..193D/abstract S. L. Detweiler & L. Lindblom (1977)], ApJ, 213, 193: ''On the evolution of the homogeneous ellipsoidal figures.'' ====Dynamical====
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