In
metric theories of gravitation, particularly
general relativity
General relativity, also known as the general theory of relativity and Einstein's theory of gravity, is the geometric theory of gravitation published by Albert Einstein in 1915 and is the current description of gravitation in modern physics. ...
, a static spherically symmetric perfect fluid solution (a term which is often abbreviated as ssspf) is a
spacetime
In physics, spacetime is a mathematical model that combines the three dimensions of space and one dimension of time into a single four-dimensional manifold. Spacetime diagrams can be used to visualize relativistic effects, such as why diffe ...
equipped with suitable
tensor field
In mathematics and physics, a tensor field assigns a tensor to each point of a mathematical space (typically a Euclidean space or manifold). Tensor fields are used in differential geometry, algebraic geometry, general relativity, in the analys ...
s which models a static round ball of a fluid with
isotropic pressure
Pressure (symbol: ''p'' or ''P'') is the force applied perpendicular to the surface of an object per unit area over which that force is distributed. Gauge pressure (also spelled ''gage'' pressure)The preferred spelling varies by country a ...
.
Such solutions are often used as idealized models of
star
A star is an astronomical object comprising a luminous spheroid of plasma held together by its gravity. The nearest star to Earth is the Sun. Many other stars are visible to the naked eye at night, but their immense distances from Earth make ...
s, especially compact objects such as
white dwarf
A white dwarf is a stellar core remnant composed mostly of electron-degenerate matter. A white dwarf is very dense: its mass is comparable to the Sun's, while its volume is comparable to the Earth's. A white dwarf's faint luminosity comes ...
s and especially
neutron star
A neutron star is the collapsed core of a massive supergiant star, which had a total mass of between 10 and 25 solar masses, possibly more if the star was especially metal-rich. Except for black holes and some hypothetical objects (e.g. w ...
s. In general relativity, a model of an ''isolated'' star (or other fluid ball) generally consists of a fluid-filled
interior region
Interior may refer to:
Arts and media
* ''Interior'' (Degas) (also known as ''The Rape''), painting by Edgar Degas
* ''Interior'' (play), 1895 play by Belgian playwright Maurice Maeterlinck
* ''The Interior'' (novel), by Lisa See
* Interior d ...
, which is technically a
perfect fluid
In physics, a perfect fluid is a fluid that can be completely characterized by its rest frame mass density \rho_m and ''isotropic'' pressure ''p''. Real fluids are "sticky" and contain (and conduct) heat. Perfect fluids are idealized models in whi ...
solution of the
Einstein field equation
In the general theory of relativity, the Einstein field equations (EFE; also known as Einstein's equations) relate the geometry of spacetime to the distribution of matter within it.
The equations were published by Einstein in 1915 in the form ...
, and an
exterior region
In mathematics, specifically in topology,
the interior of a subset of a topological space is the union of all subsets of that are open in .
A point that is in the interior of is an interior point of .
The interior of is the complement o ...
, which is an
asymptotically flat vacuum solution
In general relativity, a vacuum solution is a Lorentzian manifold whose Einstein tensor vanishes identically. According to the Einstein field equation, this means that the stress–energy tensor also vanishes identically, so that no matter or n ...
. These two pieces must be carefully ''matched'' across the ''world sheet'' of a spherical surface, the ''surface of zero pressure''. (There are various mathematical criteria called
matching conditions for checking that the required matching has been successfully achieved.) Similar statements hold for other metric theories of gravitation, such as the
Brans–Dicke theory.
In this article, we will focus on the construction of exact ssspf solutions in our current Gold Standard theory of gravitation, the theory of general relativity. To anticipate, the figure at right depicts (by means of an embedding diagram) the spatial geometry of a simple example of a stellar model in general relativity. The euclidean space in which this two-dimensional Riemannian manifold (standing in for a three-dimensional Riemannian manifold) is embedded has no physical significance, it is merely a visual aid to help convey a quick impression of the kind of geometrical features we will encounter.
Short history
We list here a few milestones in the history of exact ssspf solutions in general relativity:
*1916:
Schwarzschild fluid solution,
*1939: The relativistic equation of
hydrostatic equilibrium
In fluid mechanics, hydrostatic equilibrium (hydrostatic balance, hydrostasy) is the condition of a fluid or plastic solid at rest, which occurs when external forces, such as gravity, are balanced by a pressure-gradient force. In the planetar ...
, the
Oppenheimer-Volkov equation, is introduced,
*1939: Tolman gives seven ssspf solutions, two of which are suitable for stellar models,
*1949: Wyman ssspf and first generating function method,
*1958: Buchdahl ssspf, a relativistic generalization of a Newtonian
polytrope
In astrophysics, a polytrope refers to a solution of the Lane–Emden equation in which the pressure depends upon the density in the form
:P = K \rho^,
where is pressure, is density and is a constant of proportionality. The constant is ...
,
*1967: Kuchowicz ssspf,
*1969: Heintzmann ssspf,
*1978: Goldman ssspf,
*1982: Stewart ssspf,
*1998: major reviews by Finch & Skea and by Delgaty & Lake,
*2000: Fodor shows how to generate ssspf solutions using one generating function and differentiation and algebraic operations, but no integrations,
*2001: Nilsson & Ugla reduce the definition of ssspf solutions with either
linear
Linearity is the property of a mathematical relationship ('' function'') that can be graphically represented as a straight line. Linearity is closely related to '' proportionality''. Examples in physics include rectilinear motion, the linear ...
or
polytropic
A polytropic process is a thermodynamic process that obeys the relation:
p V^ = C
where ''p'' is the pressure, ''V'' is volume, ''n'' is the polytropic index, and ''C'' is a constant. The polytropic process equation describes expansion and co ...
equations of state to a system of regular ODEs suitable for stability analysis,
*2002: Rahman & Visser give a generating function method using one differentiation, one square root, and one definite integral, in
isotropic coordinates, with various physical requirements satisfied automatically, and show that every ssspf can be put in Rahman-Visser form,
*2003: Lake extends the long-neglected generating function method of Wyman, for either
Schwarzschild coordinates or isotropic coordinates,
*2004: Martin & Visser algorithm, another generating function method which uses Schwarzschild coordinates,
*2004: Martin gives three simple new solutions, one of which is suitable for stellar models,
*2005: BVW algorithm, apparently the simplest variant now known
References
* The original paper presenting the Oppenheimer-Volkov equation.
*
* See ''section 23.2'' and ''box 24.1'' for the Oppenheimer-Volkov equation.
* See ''chapter 10'' for the Buchdahl theorem and other topics.
* See ''chapter 6'' for a more detailed exposition of white dwarf and neutron star models than can be found in other gtr textbooks.
eprint version An excellent review stressing problems with the traditional approach which are neatly avoided by the Rahman-Visser algorithm.
*Fodor; Gyula
Generating spherically symmetric static perfect fluid solutions(2000). Fodor's algorithm.
eprint versioneprint versionThe Nilsson-Uggla dynamical systems.
eprint versionLake's algorithms.
eprint versionThe Rahman-Visser algorithm.
*{{cite journal , author1=Boonserm, Petarpa , author2=Visser, Matt , author3=Weinfurtner, Silke , name-list-style=amp , title=Generating perfect fluid spheres in general relativity , journal=Phys. Rev. D , year=2005 , volume=71 , issue= 12 , pages=124037 , doi=10.1103/PhysRevD.71.124037, arxiv = gr-qc/0503007 , bibcode = 2005PhRvD..71l4037B , s2cid=10332787 }
eprint version The BVW solution generating method.
Exact solutions in general relativity