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Seismic solar model: both of the radiative core and the convective envelope

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dc.contributor.author Shibahashi, H
dc.contributor.author Hiremath, K. M
dc.contributor.author Takata, M
dc.date.accessioned 2008-09-01T09:20:16Z
dc.date.available 2008-09-01T09:20:16Z
dc.date.issued 1999
dc.identifier.citation Advances in Space Research, Vol. 24, No. 2, pp. 177 - 180 en
dc.identifier.issn 0273-1177
dc.identifier.uri http://hdl.handle.net/2248/3283
dc.description.abstract We determine the solar internal structure by solving the basic stellar structure equations with the imposition of the sound speed, which is inferred from helioseismology. As for the radiative core, all the four structure equations are solved with the boundary conditions set at the center and at the top of the radiative core. As for the convective envelope, we only have to solve the basic equations for mass conservation and hydrostatic equilibrium with the imposition of the sound-speed profile determined from helioseismology, as an intial value problem from the base of the convection zone. The helium abundance is obtained as a part of the solutions. The extent of the convection zone is also determined so that the temperature gradient matches the adiabatic gradient at the bottom of the zone, and the deduced depth is 0.718Rsolar. en
dc.language.iso en en
dc.publisher Elsevier en
dc.relation.uri http://dx.doi.org/10.1016/S0273-1177(99)00498-6 en
dc.subject State:zone en
dc.subject Seismic solar model en
dc.subject Radiative core en
dc.title Seismic solar model: both of the radiative core and the convective envelope en
dc.type Article en


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