Schwarzschild–Milne equations
E46433
The Schwarzschild–Milne equations are fundamental integro-differential equations in radiative transfer theory that describe the propagation and scattering of radiation through a plane-parallel, absorbing and emitting medium.
All labels observed (4)
| Label | Occurrences |
|---|---|
| Eddington approximation | 1 |
| Milne problem in radiative transfer | 1 |
| Schwarzschild equation in radiative transfer | 1 |
| Schwarzschild–Milne equations canonical | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T365366 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: Schwarzschild–Milne equations Context triple: [Radiative Transfer, relatedConcept, Schwarzschild–Milne equations]
-
A.
Bardeen black hole model
The Bardeen black hole model is a theoretical proposal of a regular (non-singular) black hole solution in general relativity that avoids the central singularity by coupling gravity to nonlinear electrodynamics.
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B.
Oppenheimer–Snyder model
The Oppenheimer–Snyder model is a pioneering theoretical description of gravitational collapse in general relativity, providing one of the first rigorous treatments of how a massive star can form a black hole.
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C.
The Mathematical Theory of Black Holes
The Mathematical Theory of Black Holes is a landmark monograph that presents a rigorous, comprehensive treatment of the physics and mathematics underlying black hole solutions in general relativity.
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D.
Kruskal–Szekeres coordinates
Kruskal–Szekeres coordinates are a maximal extension coordinate system used in general relativity to smoothly describe the entire spacetime of a Schwarzschild black hole, including regions across the event horizon.
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E.
Kerr metric
The Kerr metric is the exact general relativity solution describing the spacetime geometry around a rotating, uncharged black hole.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Schwarzschild–Milne equations Target entity description: The Schwarzschild–Milne equations are fundamental integro-differential equations in radiative transfer theory that describe the propagation and scattering of radiation through a plane-parallel, absorbing and emitting medium.
-
A.
Bardeen black hole model
The Bardeen black hole model is a theoretical proposal of a regular (non-singular) black hole solution in general relativity that avoids the central singularity by coupling gravity to nonlinear electrodynamics.
-
B.
Oppenheimer–Snyder model
The Oppenheimer–Snyder model is a pioneering theoretical description of gravitational collapse in general relativity, providing one of the first rigorous treatments of how a massive star can form a black hole.
-
C.
The Mathematical Theory of Black Holes
The Mathematical Theory of Black Holes is a landmark monograph that presents a rigorous, comprehensive treatment of the physics and mathematics underlying black hole solutions in general relativity.
-
D.
Kruskal–Szekeres coordinates
Kruskal–Szekeres coordinates are a maximal extension coordinate system used in general relativity to smoothly describe the entire spacetime of a Schwarzschild black hole, including regions across the event horizon.
-
E.
Kerr metric
The Kerr metric is the exact general relativity solution describing the spacetime geometry around a rotating, uncharged black hole.
- F. None of above. chosen
Statements (46)
| Predicate | Object |
|---|---|
| instanceOf |
integro-differential equations
ⓘ
radiative transfer equations ⓘ |
| appliesTo |
absorbing media
ⓘ
emitting media ⓘ plane-parallel media ⓘ scattering media ⓘ |
| assumes |
one-dimensional variation with optical depth
ⓘ
radiative transfer in local thermodynamic equilibrium in some formulations ⓘ |
| assumesGeometry | plane-parallel slab ⓘ |
| context |
theory of stellar atmospheres
ⓘ
transfer of monochromatic radiation ⓘ |
| dependsOn |
absorption coefficient
ⓘ
emission coefficient ⓘ scattering coefficient ⓘ |
| describes |
propagation of radiation in a medium
ⓘ
scattering of radiation in a medium ⓘ |
| field | radiative transfer theory ⓘ |
| hasForm | coupled integro-differential equations for intensity and source function ⓘ |
| includes |
boundary conditions at slab surfaces
ⓘ
integral over angles ⓘ integral over optical depth ⓘ scattering kernel ⓘ |
| mathematicalDomain |
applied mathematics
ⓘ
mathematical physics ⓘ |
| namedAfter |
Edward Arthur Milne
ⓘ
Karl Schwarzschild ⓘ |
| relatedTo |
Schwarzschild–Milne equations
self-linksurface differs
ⓘ
surface form:
Milne problem in radiative transfer
Schwarzschild–Milne equations self-linksurface differs ⓘ
surface form:
Schwarzschild equation in radiative transfer
radiative transfer equation ⓘ |
| relatesQuantity |
optical depth
ⓘ
radiative flux ⓘ scattering albedo ⓘ source function ⓘ specific intensity of radiation ⓘ |
| solutionMethods |
Feautrier method
ⓘ
discrete ordinates methods ⓘ numerical integration ⓘ variational methods ⓘ |
| usedFor |
computing emergent intensity from a slab
ⓘ
computing reflection and transmission of radiation ⓘ determining source function in scattering atmospheres ⓘ modeling multiple scattering ⓘ |
| usedIn |
astrophysics
ⓘ
atmospheric radiative transfer ⓘ optical physics ⓘ stellar atmosphere modeling ⓘ |
How these facts were elicited
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Subject: Schwarzschild–Milne equations Description of subject: The Schwarzschild–Milne equations are fundamental integro-differential equations in radiative transfer theory that describe the propagation and scattering of radiation through a plane-parallel, absorbing and emitting medium.
Referenced by (4)
Full triples — surface form annotated when it differs from this entity's canonical label.