Kerr–Schild coordinates
E77413
Kerr–Schild coordinates are a coordinate system used to express the Kerr spacetime metric in a form that highlights its structure as a perturbation of flat Minkowski space along a principal null direction.
All labels observed (3)
| Label | Occurrences |
|---|---|
| Kerr–Schild coordinates canonical | 2 |
| Kerr–Schild ansatz | 1 |
| Kerr–Schild form of the metric | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T616521 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: Kerr–Schild coordinates Context triple: [Kerr metric, hasCoordinateSystem, Kerr–Schild coordinates]
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A.
Boyer–Lindquist coordinates
Boyer–Lindquist coordinates are a spheroidal coordinate system commonly used in general relativity to express the Kerr solution describing the spacetime around a rotating black hole.
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B.
Kruskal–Szekeres coordinates
Kruskal–Szekeres coordinates are a maximal extension coordinate system used in general relativity to smoothly describe the entire spacetime of a Schwarzschild black hole, including regions across the event horizon.
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C.
Eddington–Finkelstein coordinates
Eddington–Finkelstein coordinates are a coordinate system in general relativity that smoothly covers a black hole’s event horizon, avoiding the coordinate singularity present in standard Schwarzschild coordinates.
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D.
Painlevé–Gullstrand coordinates
Painlevé–Gullstrand coordinates are a coordinate system for the Schwarzschild black hole that is regular at the event horizon and represents spacetime as seen by freely falling observers.
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E.
Kerr metric
The Kerr metric is the exact general relativity solution describing the spacetime geometry around a rotating, uncharged black hole.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Kerr–Schild coordinates Target entity description: Kerr–Schild coordinates are a coordinate system used to express the Kerr spacetime metric in a form that highlights its structure as a perturbation of flat Minkowski space along a principal null direction.
-
A.
Boyer–Lindquist coordinates
Boyer–Lindquist coordinates are a spheroidal coordinate system commonly used in general relativity to express the Kerr solution describing the spacetime around a rotating black hole.
-
B.
Kruskal–Szekeres coordinates
Kruskal–Szekeres coordinates are a maximal extension coordinate system used in general relativity to smoothly describe the entire spacetime of a Schwarzschild black hole, including regions across the event horizon.
-
C.
Eddington–Finkelstein coordinates
Eddington–Finkelstein coordinates are a coordinate system in general relativity that smoothly covers a black hole’s event horizon, avoiding the coordinate singularity present in standard Schwarzschild coordinates.
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D.
Painlevé–Gullstrand coordinates
Painlevé–Gullstrand coordinates are a coordinate system for the Schwarzschild black hole that is regular at the event horizon and represents spacetime as seen by freely falling observers.
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E.
Kerr metric
The Kerr metric is the exact general relativity solution describing the spacetime geometry around a rotating, uncharged black hole.
- F. None of above. chosen
Statements (48)
| Predicate | Object |
|---|---|
| instanceOf |
coordinate system
ⓘ
general relativity concept ⓘ |
| advantage |
avoids coordinate singularity at the event horizon
ⓘ
linearizes some aspects of Einstein equations on a flat background ⓘ simplifies expression of curvature tensors ⓘ |
| appliesTo |
Kerr–Newman black hole
ⓘ
surface form:
Kerr–Newman spacetime
stationary axisymmetric spacetimes ⓘ |
| basedOn |
Minkowski space-time
ⓘ
surface form:
Minkowski spacetime
|
| containsTerm |
Minkowski metric η_{μν}
ⓘ
null vector field l_{μ} ⓘ scalar function H ⓘ |
| coordinateComponents |
azimuthal angle φ
ⓘ
polar angle θ ⓘ radial coordinate r ⓘ time coordinate t ⓘ |
| emphasizes |
perturbation of flat Minkowski space
ⓘ
principal null direction ⓘ |
| field |
black hole physics
ⓘ
gravitational physics ⓘ mathematical physics ⓘ |
| generalizationOf |
Kerr–Schild coordinates
self-linksurface differs
ⓘ
surface form:
Kerr–Schild ansatz
|
| hasProperty |
adapted to a principal null congruence
ⓘ
can be written in ingoing form ⓘ can be written in outgoing form ⓘ metric determinant equal to Minkowski determinant ⓘ metric written as flat metric plus null term ⓘ penetrating coordinates across the horizon ⓘ regular on the outer event horizon of Kerr black holes ⓘ simplifies Einstein field equations for Kerr spacetime ⓘ |
| metricForm | g_{μν} = η_{μν} + 2H l_{μ} l_{ν} ⓘ |
| namedAfter |
Alfred Schild
ⓘ
Roy Kerr ⓘ |
| nullVectorProperty |
l_{μ} is null with respect to g_{μν}
ⓘ
l_{μ} is null with respect to η_{μν} ⓘ |
| relatedTo |
Boyer–Lindquist coordinates
ⓘ
Eddington–Finkelstein coordinates ⓘ Kerr metric ⓘ Kerr–Schild coordinates self-linksurface differs ⓘ
surface form:
Kerr–Schild form of the metric
null tetrad formalism ⓘ |
| usedFor |
analytical calculations of geodesics in Kerr spacetime
ⓘ
constructing exact solutions via Kerr–Schild metrics ⓘ expressing the Kerr metric ⓘ highlighting Kerr spacetime structure ⓘ numerical relativity simulations of Kerr black holes ⓘ studying causal structure near Kerr horizons ⓘ studying rotating black holes ⓘ |
| usedIn |
Kerr metric
ⓘ
surface form:
Kerr spacetime
general relativity ⓘ |
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Subject: Kerr–Schild coordinates Description of subject: Kerr–Schild coordinates are a coordinate system used to express the Kerr spacetime metric in a form that highlights its structure as a perturbation of flat Minkowski space along a principal null direction.
Referenced by (4)
Full triples — surface form annotated when it differs from this entity's canonical label.