Reissner–Nordström metric
E14555
Lorentzian metric
black hole metric
electrovacuum solution
exact solution of Einstein field equations
spherically symmetric spacetime
static spacetime
The Reissner–Nordström metric is an exact solution in general relativity describing the spacetime geometry outside a static, spherically symmetric, electrically charged black hole.
Aliases (4)
Statements (47)
| Predicate | Object |
|---|---|
| instanceOf |
Lorentzian metric
→
black hole metric → electrovacuum solution → exact solution of Einstein field equations → spherically symmetric spacetime → static spacetime → |
| associatedElectromagneticPotential | A_\mu dx^\mu = -\frac{Q}{r} dt → |
| BekensteinHawkingEntropy | S = \frac{A_+}{4} with A_+ = 4\pi r_+^2 → |
| belongsToTheory | general relativity → |
| canBeExtendedBy |
Eddington–Finkelstein coordinates
→
Kruskal-like coordinates → |
| dependsOnParameter |
electric charge parameter Q
→
mass parameter M → |
| describes |
electrically charged black hole
→
spacetime geometry outside a static spherically symmetric electrically charged mass → |
| energyMomentumSource | electromagnetic field of a point charge → |
| generalizes | Schwarzschild solution to include electric charge → |
| hasCauchyHorizon | at r = r_- for |Q| < M → |
| hasCausalStructure | with multiple asymptotic regions in maximal analytic extension → |
| hasCoordinateSingularity | at r = r_+ in Schwarzschild-like coordinates → |
| hasCoordinateSystem |
Schwarzschild coordinates
→
surface form: "Schwarzschild-like coordinates"
|
| hasCurvatureSingularity | at r = 0 → |
| hasEventHorizon | at r = r_+ for |Q| \le M → |
| hasInnerHorizonRadius | r_- = M - \sqrt{M^2 - Q^2} → |
| hasIsometryGroup | R × SO(3) → |
| hasKillingVectorField |
\partial_t
→
generators of SO(3) rotations → |
| hasNakedSingularityWhen | |Q| > M → |
| hasOuterHorizonRadius | r_+ = M + \sqrt{M^2 - Q^2} → |
| hasSymmetry |
spherical symmetry
→
time-translation symmetry → |
| HawkingTemperature | T_H = \frac{\kappa_+}{2\pi} → |
| HawkingTemperatureExtremal | T_H = 0 for |Q| = M → |
| isAsymptotically | flat → |
| isExtremalWhen | |Q| = M → |
| isSolutionType | static spherically symmetric electrovacuum solution → |
| isUsedIn |
analyses of cosmic censorship conjecture
→
studies of charged black hole thermodynamics → studies of inner horizon instability → |
| lineElement | ds^2 = -\left(1 - \frac{2M}{r} + \frac{Q^2}{r^2}\right) dt^2 + \left(1 - \frac{2M}{r} + \frac{Q^2}{r^2}\right)^{-1} dr^2 + r^2 d\Omega^2 → |
| namedAfter |
Gunnar Nordström
→
Hans Reissner → |
| obeys | Birkhoff-like theorem for charged spherically symmetric solutions → |
| reducesTo | Schwarzschild metric when Q = 0 → |
| satisfies | vacuum Einstein equations with electromagnetic stress-energy tensor → |
| solves | Einstein–Maxwell equations → |
| surfaceGravityAtOuterHorizon | \kappa_+ = \frac{\sqrt{M^2 - Q^2}}{r_+^2} → |
Referenced by (13)
Full triples — surface form annotated when it differs from this entity's canonical label.
subject surface form: "Penrose–Carter diagram"
this entity surface form: "Reissner–Nordström spacetime"
this entity surface form: "Reissner–Nordström black hole"
this entity surface form: "Reissner–Nordström radius for charged black holes"
this entity surface form: "Reissner–Nordström spacetime"
this entity surface form: "Reissner–Nordström black hole"
this entity surface form: "Reissner–Nordström black hole"
this entity surface form: "Reissner–Nordström black hole"
this entity surface form: "Reissner–Nordström solution"
this entity surface form: "Reissner–Nordström solution"