1964
DOI: 10.1086/147949
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The Structure and Stability of Rotating Gas Masses.

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Cited by 212 publications
(183 citation statements)
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“…This is consistent with previous studies that have indicated that the Jacobi sequence cannot exist for n > 0:808 (James 1964;Hachisu & Eriguchi 1982;Lai et al 1993). Furthermore, as was pointed out by Hachisu & Eriguchi (1982) in their analysis of uniformly rotating polytropes, the mass-shedding limit never extends much beyond the bifurcation point (where the Jacobi/ Dedekind sequence branches off the Maclaurin spheroid sequence) even for very small n: for 0:1 n 0:5, this mass-shedding limit corresponds to 0:14 T /jW j 0:16.…”
Section: Resultssupporting
confidence: 94%
“…This is consistent with previous studies that have indicated that the Jacobi sequence cannot exist for n > 0:808 (James 1964;Hachisu & Eriguchi 1982;Lai et al 1993). Furthermore, as was pointed out by Hachisu & Eriguchi (1982) in their analysis of uniformly rotating polytropes, the mass-shedding limit never extends much beyond the bifurcation point (where the Jacobi/ Dedekind sequence branches off the Maclaurin spheroid sequence) even for very small n: for 0:1 n 0:5, this mass-shedding limit corresponds to 0:14 T /jW j 0:16.…”
Section: Resultssupporting
confidence: 94%
“…Finding the ratio of Rp/Re corresponding to the critical configuration is a subtle numerical issue. James (1964 , Table 4) and Hurley & Roberts (1964 , Table 1) give the values 0.558 and 0.493, respectively. Cook et al (1992 , Table 7), who consider general-relativistic configurations report a Newtonian-limit polytropic solution with n = 1 and Rp/Re = 0.552.…”
Section: Numerical Solutionsmentioning
confidence: 99%
“…On the other hand, for uniformly rotating polytropes, the m ¼ 2 secular instability cannot occur for polytropes with the polytropic index N > 0:808, because equilibrium sequences terminate due to mass shedding from the equatorial surface before the instability sets in (James 1964).…”
Section: Introductionmentioning
confidence: 99%