Godunov's method
E680772
Godunov's method is a numerical scheme for solving hyperbolic partial differential equations that uses exact or approximate Riemann solvers to compute fluxes at cell interfaces in finite-volume discretizations.
All labels observed (3)
| Label | Occurrences |
|---|---|
| Godounov | 1 |
| Godunov's method canonical | 1 |
| Godunov's scheme | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T7678176 — 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: Godunov's method Context triple: [Godunov-type schemes, basedOn, Godunov's method]
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A.
Gauss–Seidel method
The Gauss–Seidel method is an iterative numerical technique used to solve systems of linear equations, particularly in large, sparse problems arising in scientific and engineering computations.
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B.
Picard iteration
Picard iteration is a successive approximation method used to construct solutions to ordinary differential equations and establish their existence and uniqueness.
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C.
Jacobi method
The Jacobi method is an iterative numerical algorithm used to solve systems of linear equations by repeatedly updating each variable using values from the previous iteration.
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D.
Richardson iteration
Richardson iteration is an early iterative method for solving linear systems and other operator equations, based on repeated relaxation steps to progressively improve an approximate solution.
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E.
Successive Over-Relaxation
Successive Over-Relaxation is an iterative numerical method that accelerates the convergence of the Gauss–Seidel algorithm for solving large systems of linear equations by introducing a relaxation factor.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Godunov's method Target entity description: Godunov's method is a numerical scheme for solving hyperbolic partial differential equations that uses exact or approximate Riemann solvers to compute fluxes at cell interfaces in finite-volume discretizations.
-
A.
Gauss–Seidel method
The Gauss–Seidel method is an iterative numerical technique used to solve systems of linear equations, particularly in large, sparse problems arising in scientific and engineering computations.
-
B.
Picard iteration
Picard iteration is a successive approximation method used to construct solutions to ordinary differential equations and establish their existence and uniqueness.
-
C.
Jacobi method
The Jacobi method is an iterative numerical algorithm used to solve systems of linear equations by repeatedly updating each variable using values from the previous iteration.
-
D.
Richardson iteration
Richardson iteration is an early iterative method for solving linear systems and other operator equations, based on repeated relaxation steps to progressively improve an approximate solution.
-
E.
Successive Over-Relaxation
Successive Over-Relaxation is an iterative numerical method that accelerates the convergence of the Gauss–Seidel algorithm for solving large systems of linear equations by introducing a relaxation factor.
- F. None of above. chosen
Statements (47)
| Predicate | Object |
|---|---|
| instanceOf |
conservative scheme
ⓘ
finite volume method ⓘ method for hyperbolic partial differential equations ⓘ numerical method ⓘ shock-capturing scheme ⓘ |
| appliesTo |
Euler equations of gas dynamics
NERFINISHED
ⓘ
magnetohydrodynamics equations ⓘ shallow water equations ⓘ traffic flow models ⓘ |
| basedOn |
Riemann problem at cell interfaces
ⓘ
finite volume discretization ⓘ |
| canBeExtendedTo | higher-order Godunov-type schemes ⓘ |
| category |
computational fluid dynamics
ⓘ
computational physics ⓘ numerical analysis ⓘ |
| computes | numerical fluxes at cell interfaces ⓘ |
| designedFor |
contact discontinuities
ⓘ
discontinuous solutions ⓘ shock waves ⓘ |
| ensures |
conservation of energy
ⓘ
conservation of mass ⓘ conservation of momentum ⓘ |
| hasOrderOfAccuracy |
first order in space
ⓘ
first order in time ⓘ |
| hasProperty |
L1-contractive for scalar convex conservation laws
ⓘ
monotone for scalar convex conservation laws ⓘ |
| introducedBy | Sergei K. Godunov NERFINISHED ⓘ |
| introducedIn | 1959 ⓘ |
| isSpecialCaseOf | Godunov-type finite volume schemes NERFINISHED ⓘ |
| namedAfter | Sergei K. Godunov NERFINISHED ⓘ |
| preserves | conservation form of PDEs ⓘ |
| relatedTo |
ENO schemes
ⓘ
HLL Riemann solver NERFINISHED ⓘ HLLC Riemann solver NERFINISHED ⓘ MUSCL scheme NERFINISHED ⓘ Roe scheme NERFINISHED ⓘ TVD schemes ⓘ WENO schemes NERFINISHED ⓘ |
| requires | CFL stability condition ⓘ |
| solves | local Riemann problems at each cell interface ⓘ |
| timeDiscretization | explicit time stepping ⓘ |
| usedFor |
computational fluid dynamics
ⓘ
gas dynamics simulations ⓘ solving hyperbolic conservation laws ⓘ solving systems of hyperbolic PDEs ⓘ |
| uses |
approximate Riemann solvers
ⓘ
exact Riemann solvers ⓘ |
How these facts were elicited
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Subject: Godunov's method Description of subject: Godunov's method is a numerical scheme for solving hyperbolic partial differential equations that uses exact or approximate Riemann solvers to compute fluxes at cell interfaces in finite-volume discretizations.
Referenced by (3)
Full triples — surface form annotated when it differs from this entity's canonical label.