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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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–Friedrichs–Lewy condition
surface form: Courant number
namedAfter Hans Lewy
Kurt Friedrichs NERFINISHED
Richard Courant
relatedConcept Lax equivalence theorem
von Neumann stability analysis
surface form: 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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