Boyer–Lindquist coordinates

E77120

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.


Statements (50)
Predicate Object
instanceOf coordinate system
curvilinear coordinate system
spheroidal coordinate system
coordinateSingularityAt event horizon of Kerr black hole
Δ = 0
definesFunction Δ = r^2 - 2Mr + a^2 + Q^2
Σ = r^2 + a^2 cos^2θ
domainOfDefinition 0 ≤ θ ≤ π
0 ≤ φ < 2π
r > 0
generalizes Schwarzschild coordinates
hasCoordinate r
t
θ
φ
hasParameter charge Q
mass M
spin parameter a
hasProperty adapted to axial symmetry
asymptotically spherical at large r
reduce to Schwarzschild coordinates when a=0
time coordinate t is asymptotically Minkowskian
θ is polar angle from rotation axis
φ is azimuthal angle around rotation axis
hasSignature (-,+,+,+)
hasSymmetry axisymmetry
stationarity
introducedBy Richard W. Lindquist
Robert H. Boyer NERFINISHED
introducedInContext Kerr solution
metricComponent g_rr = Σ/Δ
g_tt = -(1 - 2Mr/Σ)
g_tφ = -2Mar sin^2θ / Σ
g_θθ = Σ
g_φφ = (r^2 + a^2 + 2Ma^2 r sin^2θ / Σ) sin^2θ
relatedTo Boyer–Lindquist r coordinate
Boyer–Lindquist time coordinate
Eddington–Finkelstein coordinates
Kerr–Schild coordinates
usedFor Kerr metric
Kerr–Newman metric
accretion disk modeling around rotating black holes
frame dragging analysis
geodesic calculations in Kerr spacetime
gravitational lensing in Kerr spacetime
quasinormal mode calculations of rotating black holes
rotating black hole spacetime
stationary axisymmetric spacetimes
usedIn general relativity
yearIntroduced 1967

Referenced by (5)
Subject (surface form when different) Predicate
Boyer–Lindquist coordinates ("Boyer–Lindquist r coordinate")
Boyer–Lindquist coordinates ("Boyer–Lindquist time coordinate")
Kerr–Schild coordinates
relatedTo
Kerr metric
Kerr–Newman black hole
hasCoordinateSystem

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