Kruskal–Szekeres coordinates
E11652
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.
All labels observed (6)
How this entity was disambiguated
This entity first appeared as the object of triple T65783 — 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: Kruskal–Szekeres coordinates Context triple: [Schwarzschild black hole, alternativeCoordinates, Kruskal–Szekeres coordinates]
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A.
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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B.
Schwarzschild black hole
A Schwarzschild black hole is the simplest theoretical black hole solution in general relativity, describing a static, spherically symmetric, non-rotating, uncharged mass with an event horizon defined by the Schwarzschild radius.
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C.
Oppenheimer–Snyder model
The Oppenheimer–Snyder model is a pioneering theoretical description of gravitational collapse in general relativity, providing one of the first rigorous treatments of how a massive star can form a black hole.
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D.
Schwarzschild radius
The Schwarzschild radius is the critical distance from the center of a non-rotating, spherically symmetric mass at which its escape velocity equals the speed of light, defining the boundary of a black hole.
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E.
The Mathematical Theory of Black Holes
The Mathematical Theory of Black Holes is a landmark monograph that presents a rigorous, comprehensive treatment of the physics and mathematics underlying black hole solutions in general relativity.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Kruskal–Szekeres coordinates Target entity description: 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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A.
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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B.
Schwarzschild black hole
A Schwarzschild black hole is the simplest theoretical black hole solution in general relativity, describing a static, spherically symmetric, non-rotating, uncharged mass with an event horizon defined by the Schwarzschild radius.
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C.
Oppenheimer–Snyder model
The Oppenheimer–Snyder model is a pioneering theoretical description of gravitational collapse in general relativity, providing one of the first rigorous treatments of how a massive star can form a black hole.
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D.
Schwarzschild radius
The Schwarzschild radius is the critical distance from the center of a non-rotating, spherically symmetric mass at which its escape velocity equals the speed of light, defining the boundary of a black hole.
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E.
The Mathematical Theory of Black Holes
The Mathematical Theory of Black Holes is a landmark monograph that presents a rigorous, comprehensive treatment of the physics and mathematics underlying black hole solutions in general relativity.
- F. None of above. chosen
Statements (49)
| Predicate | Object |
|---|---|
| instanceOf |
coordinate system
ⓘ
maximal analytic extension ⓘ spacetime coordinate chart ⓘ |
| appearsIn |
literature on black hole physics
ⓘ
textbooks on general relativity ⓘ |
| appliesTo |
Schwarzschild black hole
ⓘ
surface form:
Schwarzschild metric
spherically symmetric vacuum solution ⓘ |
| assumes |
non-rotating black hole
ⓘ
uncharged black hole ⓘ |
| basedOn | Schwarzschild coordinates ⓘ |
| coordinateType |
global coordinates
ⓘ
null-like coordinates ⓘ regular coordinates at the event horizon ⓘ |
| describes |
regions inside the Schwarzschild event horizon
ⓘ
regions outside the Schwarzschild event horizon ⓘ second asymptotically flat region of Schwarzschild spacetime ⓘ white hole region of Schwarzschild spacetime ⓘ |
| domain | regions I, II, III, and IV of Schwarzschild spacetime ⓘ |
| enables |
analysis of geodesic completeness of Schwarzschild spacetime
ⓘ
study of causal connections between different regions ⓘ visualization of black hole and white hole regions ⓘ |
| feature |
light cones appear at 45 degrees in Kruskal diagrams
ⓘ
metric is finite at the event horizon ⓘ timelike and spacelike character of coordinates changes across regions ⓘ |
| field | general relativity ⓘ |
| introducedBy |
George Szekeres
ⓘ
Martin David Kruskal ⓘ |
| massParameter | M ⓘ |
| mathematicalNature |
analytic coordinate transformation
ⓘ
conformal to part of Minkowski-like plane ⓘ |
| namedAfter |
George Szekeres
ⓘ
Martin David Kruskal ⓘ |
| preserves | curvature singularity at r = 0 ⓘ |
| relatedConcept |
Schwarzschild radius
ⓘ
causal structure ⓘ curvature singularity ⓘ event horizon ⓘ geodesic completeness ⓘ |
| relatedTo |
Eddington–Finkelstein coordinates
ⓘ
Penrose–Carter diagrams ⓘ maximal analytic extension of black hole spacetimes ⓘ |
| removes | coordinate singularity at r = 2M ⓘ |
| usedFor |
describing Schwarzschild spacetime
ⓘ
describing the full maximally extended Schwarzschild black hole ⓘ drawing Kruskal diagrams ⓘ extending Schwarzschild solution across the event horizon ⓘ removing coordinate singularity at the Schwarzschild radius ⓘ studying causal structure of Schwarzschild spacetime ⓘ |
| yearProposed | 1960 ⓘ |
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Subject: Kruskal–Szekeres coordinates Description of subject: 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.
Referenced by (12)
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