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Fluid sources for Bianchi I and III space‐times

dc.contributor.authorBayin, Selçuk Ş.en_US
dc.contributor.authorKrisch, Jean P.en_US
dc.date.accessioned2010-05-06T22:29:29Z
dc.date.available2010-05-06T22:29:29Z
dc.date.issued1986-01en_US
dc.identifier.citationBayin, 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.urihttps://hdl.handle.net/2027.42/70647
dc.description.abstractFour 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.extent3102 bytes
dc.format.extent254052 bytes
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dc.format.mimetypeapplication/octet-stream
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleFluid sources for Bianchi I and III space‐timesen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Physics, University of Michigan, Ann Arbor, Michigan 48109en_US
dc.contributor.affiliationotherDepartment of Physics, Canisius College, Buffalo, New York 14208en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/70647/2/JMAPAQ-27-1-262-1.pdf
dc.identifier.doi10.1063/1.527371en_US
dc.identifier.sourceJournal of Mathematical Physicsen_US
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dc.identifier.citedreferenceThis 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.citedreferenceHere Ai,Ci,Ai,Ci, and B are constants of integration.en_US
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dc.identifier.citedreferenceS. Ş. Bayin and J. P. Krisch, unpublished.en_US
dc.identifier.citedreferenceThese are calculated in the comoving, noncoordinated orthonormal system.en_US
dc.owningcollnamePhysics, Department of


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