Reissner–Nordström metric

E14555

The Reissner–Nordström metric is an exact solution in general relativity describing the spacetime geometry outside a static, spherically symmetric, electrically charged black hole.


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.

Einstein field equations admitsSolution Reissner–Nordström metric
Penrose–Carter diagrams appliesTo Reissner–Nordström metric
subject surface form: "Penrose–Carter diagram"
this entity surface form: "Reissner–Nordström spacetime"
Israel–Carter–Robinson uniqueness theorems concerns Reissner–Nordström metric
this entity surface form: "Reissner–Nordström black hole"
Schwarzschild radius contrastsWith Reissner–Nordström metric
this entity surface form: "Reissner–Nordström radius for charged black holes"
The Mathematical Theory of Black Holes covers Reissner–Nordström metric
Reissner–Nordström Penrose diagram describes Reissner–Nordström metric
this entity surface form: "Reissner–Nordström spacetime"
Kerr–Newman black hole generalizes Reissner–Nordström metric
this entity surface form: "Reissner–Nordström black hole"
general relativity includes Reissner–Nordström metric
The Mathematical Theory of Black Holes mainSubject Reissner–Nordström metric
this entity surface form: "Reissner–Nordström black hole"
Hans Reissner notableConcept Reissner–Nordström metric
this entity surface form: "Reissner–Nordström black hole"
Hans Reissner notableWork Reissner–Nordström metric
Hans Reissner notableWork Reissner–Nordström metric
this entity surface form: "Reissner–Nordström solution"
Einstein–Maxwell equations usedFor Reissner–Nordström metric
this entity surface form: "Reissner–Nordström solution"

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