CFL condition

E413440

The CFL condition is a stability criterion in numerical analysis that restricts the time step size in relation to the spatial grid size and wave speeds when solving partial differential equations.

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CFL condition canonical 1

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Statements (46)

Predicate Object
instanceOf concept in numerical analysis ⓘ
numerical stability criterion ⓘ
alsoKnownAs Courant–Friedrichs–Lewy condition ⓘ
appliesPrimarilyTo explicit schemes rather than implicit schemes ⓘ
appliesTo hyperbolic partial differential equations ⓘ
partial differential equations ⓘ
time-dependent PDEs ⓘ
category stability condition in numerical methods ⓘ
consequenceOfViolation blow-up of numerical solution ⓘ
numerical instability ⓘ
spurious oscillations ⓘ
coreIdea numerical domain of dependence must include the physical domain of dependence ⓘ
defines upper bound on Courant number for stability ⓘ
dependsOn dimensionality of the problem ⓘ
numerical scheme ⓘ
spatial discretization ⓘ
time integration method ⓘ
ensures stability of explicit time integration schemes ⓘ
field computational fluid dynamics ⓘ
computational physics ⓘ
numerical analysis ⓘ
hasAbbreviation CFL ⓘ
hasParameter grid spacing ⓘ
maximum allowable time step ⓘ
maximum signal speed in the system ⓘ
historicalPublication Courant–Friedrichs–Lewy 1928 paper on PDEs and finite differences ⓘ
involvesQuantity Courant number ⓘ
namedAfter Hans Lewy ⓘ
Kurt Friedrichs ⓘ
Richard Courant ⓘ
relatedConcept Lax equivalence theorem ⓘ
Von Neumann stability analysis ⓘ
time step restriction ⓘ
relates time step size to characteristic wave speed ⓘ
time step size to spatial grid size ⓘ
restricts time step size ⓘ
typicalForm c · Δt / Δx ≤ C_max ⓘ
usedFor choosing appropriate time step in CFD codes ⓘ
designing stable numerical simulations of wave propagation ⓘ
ensuring convergence of explicit discretizations under refinement ⓘ
usedIn explicit time-stepping schemes ⓘ
finite difference methods ⓘ
finite element methods for time-dependent problems ⓘ
finite volume methods ⓘ
numerical solution of advection equations ⓘ
numerical solution of wave equations ⓘ

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