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Department of Mathematics Numerical Solutions to Partial Differential Equations Ch 12. Applied mathematics. Korea University.
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Department of Mathematics Elliptic Partial Differential Equations Ch12.1 Index Parabolic Partial Differential Equations Ch 12.2 Hyperbolic Partial Differential Equations Ch 12.3 An Introduction to the Finite-Element Mothod Ch 12.4
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Department of Mathematics Elliptic Partial Differential Equations : poisson equation Parabolic Partial Differential Equations : Heat, diffusion equation Hyperbolic Partial Differential Equations : wave equation
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Department of Mathematics Ch 12.1 Elliptic Partial Differential Eqeations Poisson equation
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Department of Mathematics Using Taylor series in the variable about
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Department of Mathematics Poisson equation at the points Boundary condition
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Department of Mathematics Finite – Difference method with truncation error of order Boundary condition
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Department of Mathematics
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Ch 12.2 Parabolic Partial Differential Eqeations Parabolic partial differential equation : boundary condition : initial condition
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Department of Mathematics Using Taylor series in
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Department of Mathematics boundary condition initial condition : local truncation error
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Department of Mathematics let : initial condition : Forward Difference method
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Department of Mathematics is made in representing the initial data If At n-th time step the error in is. The method is stable The Forward Difference method is therefore stable only if
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Department of Mathematics : eigenvalues of A or The Forward Difference method is conditionally stable with rate of convergence
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Department of Mathematics To obtain a method that is unconditionally stable : Backward-Difference method where
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Department of Mathematics The matrix representation
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Department of Mathematics : eigenvalues of A At n-th time step the error in is. The Backward-Difference method is unconditionally stable method. The local truncation error for method is of order. Richardson’s method
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Department of Mathematics Crank-Nicolson method : Forward-Difference method at j-th step in : local truncation error : Backward-Difference method at (j+1)th step in : local truncation error Assume that average – difference method
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Department of Mathematics The matrix representation where
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Department of Mathematics Ch 12.3 Hyperbolic Partial Differential Eqeations Hyperbolic partial differential equation
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Department of Mathematics Using centered-difference quotient
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Department of Mathematics
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Ch 12.4 An Introduction to Finite- Element Method boundary condition
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Department of Mathematics Polynomials of linear type in and
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Department of Mathematics
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linear system
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Department of Mathematics
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