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.
Aliases (5)
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 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
→
|
Referenced by (11)
| Subject (surface form when different) | Predicate |
|---|---|
|
Eddington–Finkelstein coordinates
→
Painlevé–Gullstrand coordinates → Schwarzschild coordinates → |
relatedTo |
|
Einstein–Rosen bridge
("Region I of Kruskal–Szekeres diagram")
→
Einstein–Rosen bridge ("Region III of Kruskal–Szekeres diagram") → |
hasRegion |
|
George Szekeres
("Szekeres–Kruskal coordinates in general relativity")
→
Martin David Kruskal → |
notableWork |
|
Schwarzschild black hole
→
|
alternativeCoordinates |
|
Schwarzschild black hole
("maximally extended Kruskal–Szekeres spacetime")
→
|
hasCausalStructure |
|
Martin David Kruskal
("Kruskal–Szekeres extension of the Schwarzschild solution")
→
|
knownFor |
|
Einstein–Rosen bridge
→
|
visualizedUsing |