Editing Appendix/Ramblings/BordeauxSequences (section)

====Eriguchi &amp; Hachisu (1983)====

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Fig. 3 extracted without modification from p. 1134 of [https://ui.adsabs.harvard.edu/abs/1983PThPh..69.1131E/abstract Eriguchi &amp; Hachisu (1983)]<p></p>
"''Two Kinds of Axially Symmetric Equilibrium Sequences of Self-Gravitating and Rotating Incompressible Fluids:<br />Two-Ring Sequence and Core-Ring Sequence''"<p></p>
Progress of Theoretical Physics, <p></p>
vol. 69, pp. 1131-1136 &copy; Progress of Theoretical Physics
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[[File:EriguchiHachisu83 Fig3.png|center|800px|Figure 3 from Eriguchi &amp; Hachisu (1983)]]
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CAPTION: &nbsp;The angular momentum-angular velocity relations.  Solid curves represent uniformly rotating equilibrium sequences.
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<li>MS: &nbsp; Maclaurin spheroid sequence</li>
<li>JE: &nbsp; Jacobi ellipsoid sequence</li>
<li>OR: &nbsp; one-ring sequence</li>
</ul>
The number and letter ''R'' or ''C'' attached to a curve denote mass ratio and two-ring or core-ring sequence, respectively.  If differential rotation is allowed, the equilibrium sequences may continue to exist as shown by the dashed curves.
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