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#Com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference Classes and Interfaces - 18 results found.
NameDescriptionTypePackageFramework
AlternatingDirectionImplicitMethodAlternating direction implicit (ADI) method is an implicit method for obtaining numerical approximations to the solution of a HeatEquation2D.Classcom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim2SuanShu
ConvectionDiffusionEquation1DClasscom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim1.convectiondiffusionequationSuanShu
CrankNicolsonConvectionDiffusionEquation1DThis class uses the Crank-Nicolson scheme to obtain a numerical solution of a one-dimensional convection-diffusion PDE.Classcom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim1.convectiondiffusionequationSuanShu
CrankNicolsonConvectionDiffusionEquation1D .CoefficientsGets the coefficients of a discretized 1D convection-diffusion equation for each time step.Classcom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim1.convectiondiffusionequationSuanShu
CrankNicolsonHeatEquation1DThe Crank-Nicolson method is an algorithm for obtaining a numerical solution to parabolic PDE problems.Classcom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim1.heatequationSuanShu
CrankNicolsonHeatEquation1D .CoefficientsGets the coefficients of a discretized 1D heat equation for each timeSee Also:"section 9.Classcom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim1.heatequationSuanShu
ExplicitCentralDifference1DThis explicit central difference method is a numerical technique for solving the one-dimensional wave equation by the following explicitClasscom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.hyperbolic.dim1SuanShu
ExplicitCentralDifference2DThis explicit central difference method is a numerical technique for solving the two-dimensional wave equation by the following explicitClasscom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.hyperbolic.dim2SuanShu
HeatEquation1DA one-dimensional heat equation (or diffusion equation) is a parabolic PDE that takes the frac{partial u}{partial t} = eta frac{partial^2 u}{partial x^2},Classcom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim1.heatequationSuanShu
HeatEquation2DA two-dimensional heat equation (or diffusion equation) is a parabolic PDE that takes the frac{partial u}{partial t}Classcom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim2SuanShu
IterativeCentralDifferenceAn iterative central difference algorithm to obtain a numerical approximation to Poisson's equations with Dirichlet boundary conditions.Classcom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.elliptic.dim2SuanShu
PDESolutionGrid2DA solution to a bivariate PDE, which is applicable to methods which produce the solution as a two-dimensional grid.Interfacecom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifferenceSuanShu
PDESolutionTimeSpaceGrid1DA solution to an one-dimensional PDE, which is applicable to methods which produce the solutionInterfacecom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifferenceSuanShu
PDESolutionTimeSpaceGrid2DA solution to a two-dimensional PDE, which is applicable to methods which produce the solution as a three-dimensional grid of time and space.Interfacecom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifferenceSuanShu
PDETimeSpaceGrid1DThis grid numerically solves a 1D PDE, e.Classcom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifferenceSuanShu
PoissonEquation2DPoisson's equation is an elliptic PDE that takes the following general form.Classcom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.elliptic.dim2SuanShu
WaveEquation1DA one-dimensional wave equation is a hyperbolic PDE that takes the following form.Classcom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.hyperbolic.dim1SuanShu
WaveEquation2DA two-dimensional wave equation is a hyperbolic PDE that takes the following form.Classcom.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.hyperbolic.dim2SuanShu