Using generating functions to convert an implicit \((3,3)\) finite difference method to an explicit form on diffusion equation with different boundary conditions (Q281472)
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scientific article; zbMATH DE number 6579003
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Using generating functions to convert an implicit \((3,3)\) finite difference method to an explicit form on diffusion equation with different boundary conditions |
scientific article; zbMATH DE number 6579003 |
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Using generating functions to convert an implicit \((3,3)\) finite difference method to an explicit form on diffusion equation with different boundary conditions (English)
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11 May 2016
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The authors solve the time-dependent diffusion equation \(u_t=\alpha u_{xx}\) using the well-known finite difference approximations. They propose to convert the well-known \(\theta\) scheme into a new function involving infinite summation and use this new function to obtain the numerical solution. The most direct method has been known to be the solution of a tridiagonal linear system for the case when \(\theta\) is nonzero. Stability of the \(\theta\) scheme is well known as well as the fact that \(\theta = 0.5\) provides the Crank-Nicolson method with truncation errors of second order. Stability of this method is well known for \(\theta \geq 0.5\) and the authors re-derive many of the results that have been available in the literature for more than 5 decades. The authors state nothing about the implementation of their method. Converting a standard problem into an infinite series and extracting solutions from that series is not a novelty.
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finite difference method
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stability analysis
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time-dependent diffusion equation
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tridiagonal linear system
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Crank-Nicolson method
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0.8580639
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0.83657235
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0.83413744
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