Relativity and gravitational theory Definition
Komar mass
Builds on Lorentzian manifoldKilling vector fieldHodge star operatorStress–energy tensor
Definition
Let be an oriented 4-dimensional Lorentzian manifold of signature with volume form . Let be a Killing vector field that is timelike near infinity and normalised by at infinity. Let be a closed spacelike 2-surface in . In units with , the Komar mass of is where is oriented as the boundary of a spacelike region that it encloses. In the notation of forms, up to the factor fixed by the convention for the Hodge star.
Remarks
Assume that bounds a spacelike hypersurface with future unit normal , and that the Einstein equations hold. Then Stokes' theorem gives where is the stress–energy tensor and its trace. Hence depends only on the matter enclosed, and it is the same for all surfaces that are homologous in a vacuum region. Example: for the Schwarzschild metric with , one has and . Integrating its dual over the sphere of radius , of area , gives , and with the orientation above . Non-example: if is not a Killing field, the integral generally depends on the surface , so it does not define a mass.
Reading path
To understand this page from the ground up, read these 15 pages in order. The foundations come first.
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- no evidence level
- Differential form concept
- Exterior algebra concept
- Inner product concept
- Levi-Civita connection concept
- Lie derivative concept
- Orientation of a real vector space concept
- Pseudo-Riemannian manifold concept
- Riemannian manifold concept
- Signature of a quadratic form concept
- Stress–energy tensor concept
- Tangent bundle concept
- Hodge star operator definition
- Killing vector field definition
- Lorentzian manifold definition
- Komar mass definition
Further reading
About this page
| Tag | Z6MZG1FMD5 |
|---|---|
| URI | m2://Z6MZG1FMD5 |
| Kind | definition |
| Writing | W0 stub |
| MSC | 83C40, 83C57 |
| Defines | Komar mass |
| Uses | Lorentzian manifold, Killing vector field, Hodge star operator, Stress–energy tensor |
| Changed | 3 November 2026 |
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