The High-Order ADI Difference Method and Extrapolation Method for Solving the Two-Dimensional Nonlinear Parabolic Evolution Equations

In this paper, the numerical solution for two-dimensional nonlinear parabolic equations is studied using an alternating-direction implicit (ADI) Crank–Nicolson (CN) difference scheme. Firstly, we use the CN format in the time direction, and then use the CN format in the space direction before discre...

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Main Authors: Xin Shen, Xuehua Yang, Haixiang Zhang
Format: Article
Language:English
Published: MDPI AG 2024-11-01
Series:Mathematics
Subjects:
Online Access:https://www.mdpi.com/2227-7390/12/22/3469
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author Xin Shen
Xuehua Yang
Haixiang Zhang
author_facet Xin Shen
Xuehua Yang
Haixiang Zhang
author_sort Xin Shen
collection DOAJ
description In this paper, the numerical solution for two-dimensional nonlinear parabolic equations is studied using an alternating-direction implicit (ADI) Crank–Nicolson (CN) difference scheme. Firstly, we use the CN format in the time direction, and then use the CN format in the space direction before discretizing the second-order center difference quotient. In addition, we strictly prove that the proposed ADI difference scheme has unique solvability and is unconditionally stable and convergent. The extrapolation method is further applied to improve the numerical solution accuracy. Finally, two numerical examples are given to verify our theoretical results.
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issn 2227-7390
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spelling doaj-art-4abe32f00cd749adbb676a88169f56362025-08-20T02:04:54ZengMDPI AGMathematics2227-73902024-11-011222346910.3390/math12223469The High-Order ADI Difference Method and Extrapolation Method for Solving the Two-Dimensional Nonlinear Parabolic Evolution EquationsXin Shen0Xuehua Yang1Haixiang Zhang2School of Science, Hunan University of Technology, Zhuzhou 412007, ChinaSchool of Science, Hunan University of Technology, Zhuzhou 412007, ChinaSchool of Science, Hunan University of Technology, Zhuzhou 412007, ChinaIn this paper, the numerical solution for two-dimensional nonlinear parabolic equations is studied using an alternating-direction implicit (ADI) Crank–Nicolson (CN) difference scheme. Firstly, we use the CN format in the time direction, and then use the CN format in the space direction before discretizing the second-order center difference quotient. In addition, we strictly prove that the proposed ADI difference scheme has unique solvability and is unconditionally stable and convergent. The extrapolation method is further applied to improve the numerical solution accuracy. Finally, two numerical examples are given to verify our theoretical results.https://www.mdpi.com/2227-7390/12/22/3469nonlinear evolution equationfinite difference methodalternate direction implicitstabilityconvergence
spellingShingle Xin Shen
Xuehua Yang
Haixiang Zhang
The High-Order ADI Difference Method and Extrapolation Method for Solving the Two-Dimensional Nonlinear Parabolic Evolution Equations
Mathematics
nonlinear evolution equation
finite difference method
alternate direction implicit
stability
convergence
title The High-Order ADI Difference Method and Extrapolation Method for Solving the Two-Dimensional Nonlinear Parabolic Evolution Equations
title_full The High-Order ADI Difference Method and Extrapolation Method for Solving the Two-Dimensional Nonlinear Parabolic Evolution Equations
title_fullStr The High-Order ADI Difference Method and Extrapolation Method for Solving the Two-Dimensional Nonlinear Parabolic Evolution Equations
title_full_unstemmed The High-Order ADI Difference Method and Extrapolation Method for Solving the Two-Dimensional Nonlinear Parabolic Evolution Equations
title_short The High-Order ADI Difference Method and Extrapolation Method for Solving the Two-Dimensional Nonlinear Parabolic Evolution Equations
title_sort high order adi difference method and extrapolation method for solving the two dimensional nonlinear parabolic evolution equations
topic nonlinear evolution equation
finite difference method
alternate direction implicit
stability
convergence
url https://www.mdpi.com/2227-7390/12/22/3469
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