SIAM Journal on Numerical Analysis · 1978 · 126 citations · 3 references
Natural SciencesPhysicsComputational Heat TransferComputational PhysicsHeat TransferConvergence AnalysisHeat Transfer AnalysisNumerical AlgorithmsNumerical AnalysisNumerical ConvergenceNumerical Methods For Differential EquationsDiscretizationHeat EquationNumerical Solutions Of Partial Differential EquationsOrder AccuracyPadé ApproximationParabolic Partial Differential EquationsSpatial DiscretizationTime Discretization
Splitting methods for parabolic partial differential equations based on $(1,1)$ Padé approximations (Crank–Nicolson replacements) are well known to produce poor numerical results when a time discretization is imposed with time steps which are "too large" relative to the spatial discretization. In particular such numerical solutions exhibit an oscillatory behaviour which increases in amplitude with a reduction in the spatial discretization, keeping the time step constant. In contrast, $(1,0)$ Padé approximations (backward-difference, or fully implicit replacements) do not suffer from these drawbacks but are of lower order accuracy. In the present paper, a combination of fully implicit methods is used to attain second order accuracy and to retain the favorable property of the fully implicit scheme. The method is tested on a heat equation in two space dimensions which possesses a discontinuity between the initial and boundary conditions.
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Difference Methods for Initial-Value Problems
E. I., Robert D. Richtmyer, K. W. Morton · Mathematics of Computation · 1968 · 3.4K citations