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8
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85038284536
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152, 673 (1967).
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(1967)
, vol.152
, pp. 673
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14
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85038288875
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The function (Formula presented) vanishes linearly at the surface of any equilibrium stellar model. This makes (Formula presented) the most slowly vanishing thermodynamic function at the stellar suface having a finite gradient there. Imposing the boundary condition (Formula presented) at the surface of the star ensures that the Lagrangian changes in other more rapidly vanishing potentials (such as the pressure) will also vanish there
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The function (Formula presented) vanishes linearly at the surface of any equilibrium stellar model. This makes (Formula presented) the most slowly vanishing thermodynamic function at the stellar suface having a finite gradient there. Imposing the boundary condition (Formula presented) at the surface of the star ensures that the Lagrangian changes in other more rapidly vanishing potentials (such as the pressure) will also vanish there.
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17
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85038335845
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N. Stergioulas, Ph.D. thesis, University of Wisconsin at Milwaukee, 1996
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N. Stergioulas, Ph.D. thesis, University of Wisconsin at Milwaukee, 1996.
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18
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85038292980
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Unfortunately the (Formula presented) dependence of the exact expression for (Formula presented) is a very slowly converging series in (Formula presented). Adding the first order (Formula presented) correction to the imaginary part of Eq. (28) can be accomplished by multiplying that term by (Formula presented). This correction reduces the accuracy of the frequencies of the modes in the most relativistic models. Presumably a more accurate boundary condition than Eq. (28) could be constructed by adding the appropriate higher-order terms in (Formula presented)
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Unfortunately the (Formula presented) dependence of the exact expression for (Formula presented) is a very slowly converging series in (Formula presented). Adding the first order (Formula presented) correction to the imaginary part of Eq. (28) can be accomplished by multiplying that term by (Formula presented). This correction reduces the accuracy of the frequencies of the modes in the most relativistic models. Presumably a more accurate boundary condition than Eq. (28) could be constructed by adding the appropriate higher-order terms in (Formula presented).
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