Name | Description | Type | Package | Framework |
AlternatingDirectionImplicitMethod | Alternating direction implicit (ADI) method is an implicit method for obtaining numerical approximations to the solution of a HeatEquation2D. | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim2 | SuanShu |
ConvectionDiffusionEquation1D | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim1.convectiondiffusionequation | SuanShu | |
CrankNicolsonConvectionDiffusionEquation1D | This class uses the Crank-Nicolson scheme to obtain a numerical solution of a one-dimensional convection-diffusion PDE. | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim1.convectiondiffusionequation | SuanShu |
CrankNicolsonConvectionDiffusionEquation1D .Coefficients | Gets the coefficients of a discretized 1D convection-diffusion equation for each time step. | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim1.convectiondiffusionequation | SuanShu |
CrankNicolsonHeatEquation1D | The Crank-Nicolson method is an algorithm for obtaining a numerical solution to parabolic PDE problems. | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim1.heatequation | SuanShu |
CrankNicolsonHeatEquation1D .Coefficients | Gets the coefficients of a discretized 1D heat equation for each timeSee Also:"section 9. | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim1.heatequation | SuanShu |
ExplicitCentralDifference1D | This explicit central difference method is a numerical technique for solving the one-dimensional wave equation by the following explicit | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.hyperbolic.dim1 | SuanShu |
ExplicitCentralDifference2D | This explicit central difference method is a numerical technique for solving the two-dimensional wave equation by the following explicit | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.hyperbolic.dim2 | SuanShu |
HeatEquation1D | A 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}, | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim1.heatequation | SuanShu |
HeatEquation2D | A two-dimensional heat equation (or diffusion equation) is a parabolic PDE that takes the frac{partial u}{partial t} | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.parabolic.dim2 | SuanShu |
IterativeCentralDifference | An iterative central difference algorithm to obtain a numerical approximation to Poisson's equations with Dirichlet boundary conditions. | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.elliptic.dim2 | SuanShu |
PDESolutionGrid2D | A solution to a bivariate PDE, which is applicable to methods which produce the solution as a two-dimensional grid. | Interface | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference | SuanShu |
PDESolutionTimeSpaceGrid1D | A solution to an one-dimensional PDE, which is applicable to methods which produce the solution | Interface | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference | SuanShu |
PDESolutionTimeSpaceGrid2D | A solution to a two-dimensional PDE, which is applicable to methods which produce the solution as a three-dimensional grid of time and space. | Interface | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference | SuanShu |
PDETimeSpaceGrid1D | This grid numerically solves a 1D PDE, e. | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference | SuanShu |
PoissonEquation2D | Poisson's equation is an elliptic PDE that takes the following general form. | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.elliptic.dim2 | SuanShu |
WaveEquation1D | A one-dimensional wave equation is a hyperbolic PDE that takes the following form. | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.hyperbolic.dim1 | SuanShu |
WaveEquation2D | A two-dimensional wave equation is a hyperbolic PDE that takes the following form. | Class | com.numericalmethod.suanshu.analysis.differentialequation.pde.finitedifference.hyperbolic.dim2 | SuanShu |