Logo
Unionpedia
Communication
Get it on Google Play
New! Download Unionpedia on your Android™ device!
Free
Faster access than browser!
 

Kerr metric

Index Kerr metric

The Kerr metric or Kerr geometry describes the geometry of empty spacetime around a rotating uncharged axially-symmetric black hole with a spherical event horizon. [1]

92 relations: Alfred Schild, Angular momentum, Asymptotically flat spacetime, Axial symmetry, Black hole, Boyer–Lindquist coordinates, Brandon Carter, Carter constant, Cartesian coordinate system, Cauchy horizon, Circular symmetry, Closed timelike curve, Colatitude, Constant of motion, Coordinate singularity, Coordinate system, Cosmic censorship hypothesis, Covariance and contravariance of vectors, Differential operator, Dust solution, Eddington–Finkelstein coordinates, Einstein field equations, Electric charge, Epicyclic gearing, Equations of motion, Equivalence principle, Ergosphere, Event horizon, Exact solutions in general relativity, First observation of gravitational waves, Four-gradient, Four-momentum, Frame-dragging, Gamma-ray burst, General relativity, Geodesic, Gravitational plane wave, Gravitational singularity, Gravity Probe B, Hamilton–Jacobi equation, Homotopy, Integrable system, Invariant mass, Karl Schwarzschild, Kerr–Newman metric, Killing horizon, Killing tensor, Killing vector field, Lense–Thirring precession, Mach's principle, ..., Mass, Mass–energy equivalence, Metric tensor, Momentum, Multipole expansion, Naked singularity, Neutron star, Noether's theorem, Oblate spheroidal coordinates, Paul Davies, Penrose process, Petrov classification, Photon sphere, Poincaré group, Point source, Proper time, Reissner–Nordström metric, Ring singularity, Roger Penrose, Rotating black hole, Rotational energy, Roy Kerr, Schwarzschild coordinates, Schwarzschild metric, Schwarzschild radius, Singularity (mathematics), Spacetime, Spacetime topology, Spherical coordinate system, Spin-flip, Static spacetime, Static spherically symmetric perfect fluid, Stationary spacetime, Taub–NUT space, Test particle, Thibault Damour, Time translation symmetry, Unit vector, Vacuum solution, Wahlquist fluid, Weyl tensor, World line. Expand index (42 more) »

Alfred Schild

Alfred Schild (September 7, 1921 – May 24, 1977) was a leading German-American physicist, well known for his contributions to the Golden age of general relativity (1960–1975).

New!!: Kerr metric and Alfred Schild · See more »

Angular momentum

In physics, angular momentum (rarely, moment of momentum or rotational momentum) is the rotational equivalent of linear momentum.

New!!: Kerr metric and Angular momentum · See more »

Asymptotically flat spacetime

An asymptotically flat spacetime is a Lorentzian manifold in which, roughly speaking, the curvature vanishes at large distances from some region, so that at large distances, the geometry becomes indistinguishable from that of Minkowski spacetime.

New!!: Kerr metric and Asymptotically flat spacetime · See more »

Axial symmetry

Axial symmetry is symmetry around an axis; an object is axially symmetric if its appearance is unchanged if rotated around an axis.

New!!: Kerr metric and Axial symmetry · See more »

Black hole

A black hole is a region of spacetime exhibiting such strong gravitational effects that nothing—not even particles and electromagnetic radiation such as light—can escape from inside it.

New!!: Kerr metric and Black hole · See more »

Boyer–Lindquist coordinates

In the mathematical description of general relativity, the Boyer–Lindquist coordinates are a generalization of the coordinates used for the metric of a Schwarzschild black hole that can be used to express the metric of a Kerr black hole.

New!!: Kerr metric and Boyer–Lindquist coordinates · See more »

Brandon Carter

Brandon Carter, FRS (born 1942) is an Australian theoretical physicist, best known for his work on the properties of black holes and for being the first to name and employ the anthropic principle in its contemporary form.

New!!: Kerr metric and Brandon Carter · See more »

Carter constant

The Carter constant is a conserved quantity for motion around black holes in the general relativistic formulation of gravity.

New!!: Kerr metric and Carter constant · See more »

Cartesian coordinate system

A Cartesian coordinate system is a coordinate system that specifies each point uniquely in a plane by a pair of numerical coordinates, which are the signed distances to the point from two fixed perpendicular directed lines, measured in the same unit of length.

New!!: Kerr metric and Cartesian coordinate system · See more »

Cauchy horizon

In physics, a Cauchy horizon is a light-like boundary of the domain of validity of a Cauchy problem (a particular boundary value problem of the theory of partial differential equations).

New!!: Kerr metric and Cauchy horizon · See more »

Circular symmetry

In geometry, circular symmetry is a type of continuous symmetry for a planar object that can be rotated by any arbitrary angle and map onto itself.

New!!: Kerr metric and Circular symmetry · See more »

Closed timelike curve

In mathematical physics, a closed timelike curve (CTC) is a world line in a Lorentzian manifold, of a material particle in spacetime that is "closed", returning to its starting point.

New!!: Kerr metric and Closed timelike curve · See more »

Colatitude

In spherical coordinates, colatitude is the complementary angle of the latitude, i.e. the difference between 90° and the latitude, where southern latitudes are denoted with a minus sign.

New!!: Kerr metric and Colatitude · See more »

Constant of motion

In mechanics, a constant of motion is a quantity that is conserved throughout the motion, imposing in effect a constraint on the motion.

New!!: Kerr metric and Constant of motion · See more »

Coordinate singularity

A coordinate singularity occurs when an apparent singularity or discontinuity occurs in one coordinate frame, which can be removed by choosing a different frame.

New!!: Kerr metric and Coordinate singularity · See more »

Coordinate system

In geometry, a coordinate system is a system which uses one or more numbers, or coordinates, to uniquely determine the position of the points or other geometric elements on a manifold such as Euclidean space.

New!!: Kerr metric and Coordinate system · See more »

Cosmic censorship hypothesis

The weak and the strong cosmic censorship hypotheses are two mathematical conjectures about the structure of singularities arising in general relativity.

New!!: Kerr metric and Cosmic censorship hypothesis · See more »

Covariance and contravariance of vectors

In multilinear algebra and tensor analysis, covariance and contravariance describe how the quantitative description of certain geometric or physical entities changes with a change of basis.

New!!: Kerr metric and Covariance and contravariance of vectors · See more »

Differential operator

In mathematics, a differential operator is an operator defined as a function of the differentiation operator.

New!!: Kerr metric and Differential operator · See more »

Dust solution

In general relativity, a dust solution is a fluid solution, a type of exact solution of the Einstein field equation, in which the gravitational field is produced entirely by the mass, momentum, and stress density of a perfect fluid that has positive mass density but vanishing pressure.

New!!: Kerr metric and Dust solution · See more »

Eddington–Finkelstein coordinates

In general relativity, Eddington–Finkelstein coordinates are a pair of coordinate systems for a Schwarzschild geometry (i.e. a spherically symmetric black hole) which are adapted to radial null geodesics.

New!!: Kerr metric and Eddington–Finkelstein coordinates · See more »

Einstein field equations

The Einstein field equations (EFE; also known as Einstein's equations) comprise the set of 10 equations in Albert Einstein's general theory of relativity that describe the fundamental interaction of gravitation as a result of spacetime being curved by mass and energy.

New!!: Kerr metric and Einstein field equations · See more »

Electric charge

Electric charge is the physical property of matter that causes it to experience a force when placed in an electromagnetic field.

New!!: Kerr metric and Electric charge · See more »

Epicyclic gearing

An epicyclic gear train (also known as planetary gear) consists of two gears mounted so that the center of one gear revolves around the center of the other.

New!!: Kerr metric and Epicyclic gearing · See more »

Equations of motion

In physics, equations of motion are equations that describe the behavior of a physical system in terms of its motion as a function of time.

New!!: Kerr metric and Equations of motion · See more »

Equivalence principle

In the theory of general relativity, the equivalence principle is any of several related concepts dealing with the equivalence of gravitational and inertial mass, and to Albert Einstein's observation that the gravitational "force" as experienced locally while standing on a massive body (such as the Earth) is the same as the pseudo-force experienced by an observer in a non-inertial (accelerated) frame of reference.

New!!: Kerr metric and Equivalence principle · See more »

Ergosphere

page.

New!!: Kerr metric and Ergosphere · See more »

Event horizon

In general relativity, an event horizon is a region in spacetime beyond which events cannot affect an outside observer.

New!!: Kerr metric and Event horizon · See more »

Exact solutions in general relativity

In general relativity, an exact solution is a Lorentzian manifold equipped with tensor fields modeling states of ordinary matter, such as a fluid, or classical nongravitational fields such as the electromagnetic field.

New!!: Kerr metric and Exact solutions in general relativity · See more »

First observation of gravitational waves

The first observation of gravitational waves was made on 14 September 2015 and was announced by the LIGO and Virgo collaborations on 11 February 2016.

New!!: Kerr metric and First observation of gravitational waves · See more »

Four-gradient

In differential geometry, the four-gradient (or 4-gradient) \mathbf is the four-vector analogue of the gradient \vec from Gibbs–Heaviside vector calculus.

New!!: Kerr metric and Four-gradient · See more »

Four-momentum

In special relativity, four-momentum is the generalization of the classical three-dimensional momentum to four-dimensional spacetime.

New!!: Kerr metric and Four-momentum · See more »

Frame-dragging

Frame-dragging is an effect on spacetime, predicted by Einstein's general theory of relativity, that is due to non-static stationary distributions of mass–energy.

New!!: Kerr metric and Frame-dragging · See more »

Gamma-ray burst

In gamma-ray astronomy, gamma-ray bursts (GRBs) are extremely energetic explosions that have been observed in distant galaxies.

New!!: Kerr metric and Gamma-ray burst · See more »

General relativity

General relativity (GR, also known as the general theory of relativity or GTR) is the geometric theory of gravitation published by Albert Einstein in 1915 and the current description of gravitation in modern physics.

New!!: Kerr metric and General relativity · See more »

Geodesic

In differential geometry, a geodesic is a generalization of the notion of a "straight line" to "curved spaces".

New!!: Kerr metric and Geodesic · See more »

Gravitational plane wave

In general relativity, a gravitational plane wave is a special class of a vacuum pp-wave spacetime, and may be defined in terms of Brinkmann coordinates by ds^2.

New!!: Kerr metric and Gravitational plane wave · See more »

Gravitational singularity

A gravitational singularity or spacetime singularity is a location in spacetime where the gravitational field of a celestial body becomes infinite in a way that does not depend on the coordinate system.

New!!: Kerr metric and Gravitational singularity · See more »

Gravity Probe B

Gravity Probe B (GP-B) was a satellite-based mission which launched on 20 April 2004 on a Delta II rocket.

New!!: Kerr metric and Gravity Probe B · See more »

Hamilton–Jacobi equation

In mathematics, the Hamilton–Jacobi equation (HJE) is a necessary condition describing extremal geometry in generalizations of problems from the calculus of variations, and is a special case of the Hamilton–Jacobi–Bellman equation.

New!!: Kerr metric and Hamilton–Jacobi equation · See more »

Homotopy

In topology, two continuous functions from one topological space to another are called homotopic (from Greek ὁμός homós "same, similar" and τόπος tópos "place") if one can be "continuously deformed" into the other, such a deformation being called a homotopy between the two functions.

New!!: Kerr metric and Homotopy · See more »

Integrable system

In the context of differential equations to integrate an equation means to solve it from initial conditions.

New!!: Kerr metric and Integrable system · See more »

Invariant mass

The invariant mass, rest mass, intrinsic mass, proper mass, or in the case of bound systems simply mass, is the portion of the total mass of an object or system of objects that is independent of the overall motion of the system.

New!!: Kerr metric and Invariant mass · See more »

Karl Schwarzschild

Karl Schwarzschild (October 9, 1873 – May 11, 1916) was a German physicist and astronomer.

New!!: Kerr metric and Karl Schwarzschild · See more »

Kerr–Newman metric

The Kerr–Newman metric is a solution of the Einstein–Maxwell equations in general relativity that describes the spacetime geometry in the region surrounding a charged, rotating mass.

New!!: Kerr metric and Kerr–Newman metric · See more »

Killing horizon

A Killing horizon is a null hypersurface defined by the vanishing of the norm of a Killing vector field (both are named after Wilhelm Killing).

New!!: Kerr metric and Killing horizon · See more »

Killing tensor

A Killing tensor, named after Wilhelm Killing, is a symmetric tensor, known in the theory of general relativity, K that satisfies where the parentheses on the indices refer to the symmetric part.

New!!: Kerr metric and Killing tensor · See more »

Killing vector field

In mathematics, a Killing vector field (often just Killing field), named after Wilhelm Killing, is a vector field on a Riemannian manifold (or pseudo-Riemannian manifold) that preserves the metric.

New!!: Kerr metric and Killing vector field · See more »

Lense–Thirring precession

In general relativity, Lense–Thirring precession or the Lense–Thirring effect (named after Josef Lense and Hans Thirring) is a relativistic correction to the precession of a gyroscope near a large rotating mass such as the Earth.

New!!: Kerr metric and Lense–Thirring precession · See more »

Mach's principle

In theoretical physics, particularly in discussions of gravitation theories, Mach's principle (or Mach's conjecture) is the name given by Einstein to an imprecise hypothesis often credited to the physicist and philosopher Ernst Mach.

New!!: Kerr metric and Mach's principle · See more »

Mass

Mass is both a property of a physical body and a measure of its resistance to acceleration (a change in its state of motion) when a net force is applied.

New!!: Kerr metric and Mass · See more »

Mass–energy equivalence

In physics, mass–energy equivalence states that anything having mass has an equivalent amount of energy and vice versa, with these fundamental quantities directly relating to one another by Albert Einstein's famous formula: E.

New!!: Kerr metric and Mass–energy equivalence · See more »

Metric tensor

In the mathematical field of differential geometry, a metric tensor is a type of function which takes as input a pair of tangent vectors and at a point of a surface (or higher dimensional differentiable manifold) and produces a real number scalar in a way that generalizes many of the familiar properties of the dot product of vectors in Euclidean space.

New!!: Kerr metric and Metric tensor · See more »

Momentum

In Newtonian mechanics, linear momentum, translational momentum, or simply momentum (pl. momenta) is the product of the mass and velocity of an object.

New!!: Kerr metric and Momentum · See more »

Multipole expansion

A multipole expansion is a mathematical series representing a function that depends on angles—usually the two angles on a sphere.

New!!: Kerr metric and Multipole expansion · See more »

Naked singularity

In general relativity, a naked singularity is a gravitational singularity without an event horizon.

New!!: Kerr metric and Naked singularity · See more »

Neutron star

A neutron star is the collapsed core of a large star which before collapse had a total of between 10 and 29 solar masses.

New!!: Kerr metric and Neutron star · See more »

Noether's theorem

Noether's (first) theorem states that every differentiable symmetry of the action of a physical system has a corresponding conservation law.

New!!: Kerr metric and Noether's theorem · See more »

Oblate spheroidal coordinates

Oblate spheroidal coordinates are a three-dimensional orthogonal coordinate system that results from rotating the two-dimensional elliptic coordinate system about the non-focal axis of the ellipse, i.e., the symmetry axis that separates the foci.

New!!: Kerr metric and Oblate spheroidal coordinates · See more »

Paul Davies

Paul Charles William Davies, AM (born 22 April 1946) is an English physicist, writer and broadcaster, a professor at Arizona State University as well as the Director of BEYOND: Center for Fundamental Concepts in Science.

New!!: Kerr metric and Paul Davies · See more »

Penrose process

The Penrose process (also called Penrose mechanism) is a process theorised by Roger Penrose wherein energy can be extracted from a rotating black hole.

New!!: Kerr metric and Penrose process · See more »

Petrov classification

In differential geometry and theoretical physics, the Petrov classification (also known as Petrov–Pirani–Penrose classification) describes the possible algebraic symmetries of the Weyl tensor at each event in a Lorentzian manifold.

New!!: Kerr metric and Petrov classification · See more »

Photon sphere

A photon sphere is a spherical region of space where gravity is strong enough that photons are forced to travel in orbits.

New!!: Kerr metric and Photon sphere · See more »

Poincaré group

The Poincaré group, named after Henri Poincaré (1906), was first defined by Minkowski (1908) as the group of Minkowski spacetime isometries.

New!!: Kerr metric and Poincaré group · See more »

Point source

A point source is a single identifiable localised source of something.

New!!: Kerr metric and Point source · See more »

Proper time

In relativity, proper time along a timelike world line is defined as the time as measured by a clock following that line.

New!!: Kerr metric and Proper time · See more »

Reissner–Nordström metric

In physics and astronomy, the Reissner–Nordström metric is a static solution to the Einstein-Maxwell field equations, which corresponds to the gravitational field of a charged, non-rotating, spherically symmetric body of mass M. The metric was discovered by Hans Reissner, Hermann Weyl, Gunnar Nordström and G. B. Jeffery.

New!!: Kerr metric and Reissner–Nordström metric · See more »

Ring singularity

A ring singularity or ringularity is the gravitational singularity of a rotating black hole, or a Kerr black hole, that is shaped like a ring.

New!!: Kerr metric and Ring singularity · See more »

Roger Penrose

Sir Roger Penrose (born 8 August 1931) is an English mathematical physicist, mathematician and philosopher of science.

New!!: Kerr metric and Roger Penrose · See more »

Rotating black hole

A rotating black hole is a black hole that possesses angular momentum.

New!!: Kerr metric and Rotating black hole · See more »

Rotational energy

Rotational energy or angular kinetic energy is kinetic energy due to the rotation of an object and is part of its total kinetic energy.

New!!: Kerr metric and Rotational energy · See more »

Roy Kerr

Roy Patrick Kerr (born 16 May 1934) is a New Zealand mathematician who discovered the Kerr geometry, an exact solution to the Einstein field equation of general relativity.

New!!: Kerr metric and Roy Kerr · See more »

Schwarzschild coordinates

In the theory of Lorentzian manifolds, spherically symmetric spacetimes admit a family of nested round spheres.

New!!: Kerr metric and Schwarzschild coordinates · See more »

Schwarzschild metric

In Einstein's theory of general relativity, the Schwarzschild metric (also known as the Schwarzschild vacuum or Schwarzschild solution) is the solution to the Einstein field equations that describes the gravitational field outside a spherical mass, on the assumption that the electric charge of the mass, angular momentum of the mass, and universal cosmological constant are all zero.

New!!: Kerr metric and Schwarzschild metric · See more »

Schwarzschild radius

The Schwarzschild radius (sometimes historically referred to as the gravitational radius) is a physical parameter that shows up in the Schwarzschild solution to Einstein's field equations, corresponding to the radius defining the event horizon of a Schwarzschild black hole.

New!!: Kerr metric and Schwarzschild radius · See more »

Singularity (mathematics)

In mathematics, a singularity is in general a point at which a given mathematical object is not defined, or a point of an exceptional set where it fails to be well-behaved in some particular way, such as differentiability.

New!!: Kerr metric and Singularity (mathematics) · See more »

Spacetime

In physics, spacetime is any mathematical model that fuses the three dimensions of space and the one dimension of time into a single four-dimensional continuum.

New!!: Kerr metric and Spacetime · See more »

Spacetime topology

Spacetime topology is the topological structure of spacetime, a topic studied primarily in general relativity.

New!!: Kerr metric and Spacetime topology · See more »

Spherical coordinate system

In mathematics, a spherical coordinate system is a coordinate system for three-dimensional space where the position of a point is specified by three numbers: the radial distance of that point from a fixed origin, its polar angle measured from a fixed zenith direction, and the azimuth angle of its orthogonal projection on a reference plane that passes through the origin and is orthogonal to the zenith, measured from a fixed reference direction on that plane.

New!!: Kerr metric and Spherical coordinate system · See more »

Spin-flip

A black hole spin-flip occurs when the spin axis of a rotating black hole undergoes a sudden change in orientation due to absorption of a second (smaller) black hole.

New!!: Kerr metric and Spin-flip · See more »

Static spacetime

In general relativity, a spacetime is said to be static if it does not change over time and is also irrotational.

New!!: Kerr metric and Static spacetime · See more »

Static spherically symmetric perfect fluid

In metric theories of gravitation, particularly general relativity, a static spherically symmetric perfect fluid solution (a term which is often abbreviated as ssspf) is a spacetime equipped with suitable tensor fields which models a static round ball of a fluid with isotropic pressure.

New!!: Kerr metric and Static spherically symmetric perfect fluid · See more »

Stationary spacetime

In general relativity, specifically in the Einstein field equations, a spacetime is said to be stationary if it admits a Killing vector that is asymptotically timelike.

New!!: Kerr metric and Stationary spacetime · See more »

Taub–NUT space

The Taub–NUT metric is an exact solution to Einstein's equations.

New!!: Kerr metric and Taub–NUT space · See more »

Test particle

In physical theories, a test particle is an idealized model of an object whose physical properties (usually mass, charge, or size) are assumed to be negligible except for the property being studied, which is considered to be insufficient to alter the behavior of the rest of the system.

New!!: Kerr metric and Test particle · See more »

Thibault Damour

Thibault Damour (born 7 February 1951) is a French physicist.

New!!: Kerr metric and Thibault Damour · See more »

Time translation symmetry

Time translation symmetry or temporal translation symmetry (TTS) is a mathematical transformation in physics that moves the times of events through a common interval.

New!!: Kerr metric and Time translation symmetry · See more »

Unit vector

In mathematics, a unit vector in a normed vector space is a vector (often a spatial vector) of length 1.

New!!: Kerr metric and Unit vector · See more »

Vacuum solution

A vacuum solution is a solution of a field equation in which the sources of the field are taken to be identically zero.

New!!: Kerr metric and Vacuum solution · See more »

Wahlquist fluid

In general relativity, the Wahlquist fluid is an exact rotating perfect fluid solution to Einstein's equation with equation of state corresponding to constant gravitational mass density.

New!!: Kerr metric and Wahlquist fluid · See more »

Weyl tensor

In differential geometry, the Weyl curvature tensor, named after Hermann Weyl, is a measure of the curvature of spacetime or, more generally, a pseudo-Riemannian manifold.

New!!: Kerr metric and Weyl tensor · See more »

World line

The world line (or worldline) of an object is the path that object traces in -dimensional spacetime.

New!!: Kerr metric and World line · See more »

Redirects here:

Boyer-Lindquist coordinate, Kerr Black Hole, Kerr Metric, Kerr Solution, Kerr black hole, Kerr black holes, Kerr ring, Kerr solution, Kerr spacetime, Kerr vacuum.

References

[1] https://en.wikipedia.org/wiki/Kerr_metric

OutgoingIncoming
Hey! We are on Facebook now! »