scholarly journals Types of Stellar Instabilities

1980 ◽  
Vol 5 ◽  
pp. 433-436
Author(s):  
P. Ledoux

Aside from violent phenomena, regular forms of motions originate often in instabilities and the linear theory with terms ∞ exp (st) yields already significant information. The system, here a spherical star, will be the seat of an instability if R (s) > 0. In general, s will be complex as both conservative (adiabatic) and non-conservative (non-adiabatic) factors are present. However if the latter (small) are neglected, the eigen-values s2 often denoted -σ2 are real. If at least one σ2 < 0, then the star is dynamically unstable.Radial perturbations. If an appropriate average value Γ1 > 4/3, then all σ2 are positive. If Γ < 4/3 (formation phase: ionization; late evolution: nuclear equilibrium; degeneracy in white dwarfs and neutron stars or radiation in very large masses plus general relativistic effects) the fundamental eigenvalue of only becomes negative.

1971 ◽  
Vol 46 ◽  
pp. 334-340
Author(s):  
Jeffrey M. Cohen

Except in cosmology, astrophysicists are used to thinking of general relativistic effects as small (e.g., light bending, perihelion advance, red shift) and have generally left such problems to general relativists. However, the discovery of pulsars (Hewish et al., 1968) may have changed this. Not only is general relativity necessary to treat rotating neutron stars, but relativity was also partly responsible for the elimination of pulsating white dwarfs as pulsar models.


2011 ◽  
Vol 20 (supp01) ◽  
pp. 141-148
Author(s):  
JORGE A. RUEDA ◽  
REMO RUFFINI

We summarize recent progress in the formulation of a theory for white dwarfs and neutron stars based on the general relativistic Thomas-Fermi equations of equilibrium.


2013 ◽  
Vol 22 (11) ◽  
pp. 1360007 ◽  
Author(s):  
JORGE A. RUEDA ◽  
REMO RUFFINI

We summarize recent progress in the formulation of a theory for white dwarfs and neutron stars taking into account the strong, weak, electromagnetic and gravitational interactions based on the general relativistic Thomas–Fermi equations of equilibrium and the Einstein–Maxwell equations.


1969 ◽  
Vol 5 (1) ◽  
pp. 113-125 ◽  
Author(s):  
Jeffrey M. Cohen ◽  
Arnold Lapidus ◽  
A. G. W. Cameron

2011 ◽  
Vol 20 (10) ◽  
pp. 1789-1796 ◽  
Author(s):  
JORGE A. RUEDA ◽  
M. ROTONDO ◽  
R. RUFFINI ◽  
S.-S. XUE

We address the description of neutron-proton-electron degenerate matter in beta equilibrium subjected to compression both in the case of confined nucleons into a nucleus as well as in the case of deconfined nucleons. We follow a step-by-step generalization of the classical Thomas–Fermi model to special and general relativistic regimes, which leads to a unified treatment of beta equilibrated neutron-proton-electron degenerate matter applicable from the case of nuclei all the way up to the case of white-dwarfs and neutron stars. New gravito-electrodynamical effects, missed in the traditional approach for the description of neutron star configurations, are found as a consequence of the new set of general relativistic equilibrium equations.


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