general proof of the entropy principle for self-gravitating fluid in static spacetimes
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General proof of the entropy principle for self-gravitating fluid in static spacetimes. 高思杰 (Gao Sijie) 北京师范大学 (Beijing Normal University). Outline. Introduction Entropy principle in spherical case --radiation Entropy principle in spherical case –perfect fluid - PowerPoint PPT PresentationTRANSCRIPT
General proof of the entropy principle for self-gravitating fluid in static
spacetimes高思杰 (Gao Sijie)
北京师范大学(Beijing Normal University)
23/4/19 2014 Institute of Physics, Academia Sinica 1
Outline
1. Introduction2. Entropy principle in spherical case --radiation 3. Entropy principle in spherical case –perfect
fluid4. Entropy principle in static spacetime5. Related works6. Conclusions.
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1. Introduction
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Mathematical analogy beween thermodynamics and black holes:
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What is the relationship between ordinary thermodynamics and gravity?
We shall study thermodynamics of self-gravitating fluid in curved spacetime.
fluid
,S M N,S: total entropy of fluidM: total mass of fluid N: total particle number
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There are two ways to determine the distribution of the fluid:
1. General relativity: Einstein’s equation gives Tolman-Oppenheimer-Volkoff (TOV ) equation:
2. Thermodynamics: at thermal equilibrium.
Are they consistent?
Consider a self-gravitating perfect fluid with spherical symmetry in thermal equilibrium:
2. Entropy principle in spherical case---radiation Sorkin, Wald, Zhang, Gen.Rel.Grav. 13, 1127 (1981)
In 1981, Sorkin, Wald, and Zhang (SWZ) derived the TOV equation of a self-gravitating radiation from the maximum entropy principle.
Proof: The stress-energy tensor is given by
The radiation satisfies:
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Assume the metric of the spherically symmetric radiation takes the form
The constraint Einstein equation yields
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Since , the extrema of is equivalent to the Euler-Lagrange equation:
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Using to replace , , we arrive at the TOV
equation
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3. Entropy principle in spherical case---general perfect fluid
(Sijie Gao, arXiv:1109.2804, Phys. Rev. D 84, 104023 )
• To generalize SWZ’s treatment to a general fluid, we first need to find an expression for the entropy density .
• The first law of the ordinary thermodynamics: Rewrite in terms of densities:
Expand: The first law in a unit volume:
s
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4.Proof of the entropy principle for perfect fluid in static spacetimes
arXiv: 1311.6899
• In this work, we present two theorems relating the total entropy of fluid to Einstein’s equation in any static spacetimes.
• A static spacetime admits a timelike Killing vector field which is hypersurface orthogonal.
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a
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The total entropy
Its variation:
Total number of particle:
The constraint
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Integration by parts:
Integration by parts again and dropping the boundary terms:
5. Related works• Proof for stationary case----in process• Stability analysis (1) Z.Roupas [Class. Quantum Grav. 30, 115018 (2013)] calculated the
second variation of entropy, showing that the stability of thermal equilibrium is equivalent to stability of Einstein’s equations.
(2) Wald et. al. [Class. Quantum Grav. 31 (2014) 035023 ] proved the equivalence of dynamic equibrium and thermodynamic equibrium for stationary asymtotically flat spacetimes with axisymmetry.
• Beyond general relativity: Li-Ming Cao, Jianfei Xu, Zhe Zeng [Phys. Rev. D 87, 064005 (2013)] proved
the maximum entropy principle in the framework of Lovelock gravity.
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6. Conclusions
• We have rigorously proven the equivalence of the extrema of entropy and Einstein's equation under a few natural and necessary conditions. The significant improvement from previous works is that no spherical symmetry or any other symmetry is needed on the spacelike hypersurface. Our work suggests a clear connection between Einstein's equation and thermodynamics of perfect fluid in static spacetimes.
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