Editing H BookTiledMenu (section)

====Sheroidal &amp; Spheroidal-Like====


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! style="height: 150px; width: 150px; background-color:#ffff99; border-right:2px solid black; " |<b>Incompressible<br />Sequences</b>
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! style="height: 150px; width: 150px; border-right:2px dashed black;" |[[Appendix/Ramblings/MacSphCriticalPoints|Critical Points<br />Along<br />Maclaurin Spheroid<br />Sequence]]
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! style="height: 150px; width: 150px;" |[[Apps/EriguchiHachisu/Models|Eriguchi, Hachisu<br />&amp; Colleagues]]
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! style="height: 150px; width: 150px; background-color:#ffff99; border-right:2px solid black; " |<b>Linear<br />Analysis<br /> of<br />Bar-Mode<br />Instability</b>
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! style="height: 150px; width: 150px; border-right:2px dashed black;" |[[Apps/RotatingPolytropes/BarmodeIncompressible|Bifurcation<br />from<br />Maclaurin<br />Sequence]]
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! style="height: 150px; width: 150px;" |[[Apps/RotatingPolytropes/BarmodeEigenvector|Traditional<br />Analyses]]
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<font color="green">The equilibrium models are calculated using the polytrope version (Bodenheimer &amp; Ostriker 1973) of the Ostriker and Mark (1968) self-consistent field (SCF) code &hellip; the equilibrium models rotate on cylinders and are completely specified by <math>~n</math>, the total angular momentum, and the specific angular momentum distribution <math>~j(m_\varpi)</math>.  Here <math>~m_\varpi</math> is the mass contained within a cylinder of radius <math>~\varpi</math> centered on the rotation axis.  The angular momentum distribution is prescribed in several ways:  (1) imposing strict uniform rotation;  (2) using the same <math>~j(m_\varpi)</math> as that of a uniformly rotating spherical polybrope of index <math>~n^'</math> (see Bodenheimer and Ostriker 1973); and (3) using <math>~j(m_\varpi) \propto m_\varpi</math>, which we refer to as <math>~n^' = L</math>, <math>~L</math> for "linear."</font>
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