Fluid sources for Bianchi I and III space‐times
dc.contributor.author | Bayin, Selçuk Ş. | en_US |
dc.contributor.author | Krisch, Jean P. | en_US |
dc.date.accessioned | 2010-05-06T22:29:29Z | |
dc.date.available | 2010-05-06T22:29:29Z | |
dc.date.issued | 1986-01 | en_US |
dc.identifier.citation | Bayin, Selçuk Ş.; Krisch, J. P. (1986). "Fluid sources for Bianchi I and III space‐times." Journal of Mathematical Physics 27(1): 262-264. <http://hdl.handle.net/2027.42/70647> | en_US |
dc.identifier.uri | https://hdl.handle.net/2027.42/70647 | |
dc.description.abstract | Four analytic solutions to the Einstein field equations are presented. The solutions are parametrized to have either Bianchi I or Bianchi III symmetry. The associated fluid parameters are given and some of them are discussed in detail. | en_US |
dc.format.extent | 3102 bytes | |
dc.format.extent | 254052 bytes | |
dc.format.mimetype | text/plain | |
dc.format.mimetype | application/octet-stream | |
dc.publisher | The American Institute of Physics | en_US |
dc.rights | © The American Institute of Physics | en_US |
dc.title | Fluid sources for Bianchi I and III space‐times | en_US |
dc.type | Article | en_US |
dc.subject.hlbsecondlevel | Physics | en_US |
dc.subject.hlbtoplevel | Science | en_US |
dc.description.peerreviewed | Peer Reviewed | en_US |
dc.contributor.affiliationum | Department of Physics, University of Michigan, Ann Arbor, Michigan 48109 | en_US |
dc.contributor.affiliationother | Department of Physics, Canisius College, Buffalo, New York 14208 | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/70647/2/JMAPAQ-27-1-262-1.pdf | |
dc.identifier.doi | 10.1063/1.527371 | en_US |
dc.identifier.source | Journal of Mathematical Physics | en_US |
dc.identifier.citedreference | L. Bianchi, Mem. Soc. Ital. Sci. Nat. Mus. Civ. Stor. Nat. Milano 11, 267 (1978). | en_US |
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dc.identifier.citedreference | This equation for Bianchi I space‐time can also be written in the following convenient form: 1γ1γ2ddt(γ1γ̇2)−12ddt(γ̇1γ1lnγ1γ23)+ddt(γ̇1γ1)[−1+12lnγ1γ23]=0. This is analogous to the Tolman equation given for the relativistic fluid sphere field equation. | en_US |
dc.identifier.citedreference | Here Ai,Ci,Ai,Ci, and B are constants of integration. | en_US |
dc.identifier.citedreference | E. Kasner, Am. J. Math. 43, 217 (1921). | en_US |
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dc.identifier.citedreference | W. Gröbner and N. Hofreiter, Integraltafel (Springer, Berlin, 1949), Vol. 1. | en_US |
dc.identifier.citedreference | S. Ş. Bayin and J. P. Krisch, unpublished. | en_US |
dc.identifier.citedreference | These are calculated in the comoving, noncoordinated orthonormal system. | en_US |
dc.owningcollname | Physics, Department of |
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