一类半线性变系数抛物型方程的紧差分格式

对一类半线性变系数抛物型方程初边值问题建立了紧差分格式,用能量分析方法证明了差分格式解的存在唯一性、关于初值的无条件稳定性和在L_∞范数下阶数为O(τ~2+h~4)的收敛性,最后给出的数值算例验证了理论结果.     

一类反应扩散方程组的保持正性的差分格式

本文研究一类具有正解的反应扩散方程组的有限差分解法.构造了一个保持正性的差分格式.利用离散的最大值原理证明了差分格式解的非负性,有界性及差分格式的无条件稳定性.这些估计的证明不依赖于微分方程的解而仅仅与初边值条件有关.当微分方程的解适当光滑时,证明了差分格式的一致收敛性.最后给出了数值计算结果,并与以往方法进行了比较.计算结果说明了本文给出的方法的有效性.     

一类半线性抛物型方程的紧差分格式

本文构造了一类半线性抛物方程初边值问题的紧差分格式．利用离散能量估计证明了差分格式解的存在唯一性、收敛性和无条件稳定性，并给出了在离散L^∞模意义下收敛阶数为O（h^4＋τ^2）．数值例子验证了理论分析结果。     

解三维抛物型方程的一个高精度显式差分格式

提出了求解三维抛物型方程的一个高精度显式差分格式.首先,推导了一个特殊节点处一阶偏导数(■u)/(■/t)的一个差分近似表达式,利用待定系数法构造了一个显式差分格式,通过选取适当的参数使格式的截断误差在空间层上达到了四阶精度和在时间层上达到了三阶精度.然后,利用Fourier分析法证明了当r1/6时,差分格式是稳定的.最后,通过数值试验比较了差分格式的解与精确解的区别,结果说明了差分格式的有效性.     

分布控制中一类半线性抛物方程的差分格式

本文讨论了在分布控制中出现的一类半线性抛物方程的有限差分方法.构造了一个线性化隐式差分格式.证明了差分格式解的存在唯一性、收敛性和无条件稳定性.并给出了L2和L∞范数意义下的收敛阶数为O(h2 τ2).数值例子验证了理论分析结果.     

一维对流扩散方程CRANK—NICOLSON特征差分格式

本文针对一维线性和非线性对流扩散方程提出一种Crank-Nicolson类型的特征差分格式,给出了该格式形成的线性代数方程组可解的一个充条件,证明了该格式按离散L^2模是收敛的,且其收敛阶为O（△t^ h^2).     

一类非线性延迟抛物偏微分方程的紧致差分格式

对于一类带有Dirichlet边界条件的延迟非线性抛物型偏微分方程的初边值问题建立了一个紧差分格式,用能量分析法证明该差分格式在L_∞范数下是无条件收敛的,且收敛阶为O(τ~2+h~4).最后,通过数值算例验证了理论结果.     

解三维抛物型方程的一个新的高精度显格式

本文构造了一个解三维抛物型方程的高精度三层显式差分格式,其稳定性条件为r=Δt/Δx2=Δt/Δy2=Δt/Δz2≤1/4,截断误差为O(Δt2+Δx4).     

Locally One-Dimensional Difference Scheme for the Third Boundary Value Problem for a Parabolic Equation of the General Form with a Nonlocal Source

We consider a locally one-dimensional scheme for an equation of parabolic type of the general form in a p-dimensional parallelepiped, obtain an a priori estimate for its solution, and prove that the solutions of this scheme converge to a solution of the equation at the rate O(|h|² + τ), where |h|² = h ₁ ² + · · · + h _p ² and p_α, α = 1,..., p, and τ are the steps in the space and time variables. We do not assume that the operator in the leading part of the equation is sign definite.     

Finite Difference Method with Nonuniform Meshes for Quasilinear Parabolic Systems

1.lnthestudyoftheprobleminphysics,mechanics,chemicalreactions,biologyandotherpracticalsciences,thelinearandnonlinearparabolicequationsandsystemsareappearedveryfrequently.Manynumericalinvestigationsinscientificandengineeringproblemsespeciallyinthelargescalecomputationalproblemsoftencontainthenumer-icalsolutionsofparabolicequationsandsystems.ThemethodwithunequalmeshstePSisnotavoidableinthesecomputations.Manyunexpectedandselfcontradictoryphe-nomenonraisingfromtheuseofunequalmeshstepscallourgreata…     

抛物型方程的一个高精度隐格式

利用待定参数法,对一维抛物型方程构造出了一个截断误差为Ｏ（△ｘ＾４＋△ｘ＾４）的隐式差分格式,格式的稳定性条件为ｒ＝ａ△ｔ／△ｘ＾２≤１／√２,可用追赶法求解。     

解二维抛物型方程的高精度差分格式

本文构造了一个解二维抛物型方程的高精度三层显式差分格式,其稳定性条件为r=△t/△x2=△t/△y2≤1/4,截断误差为O(△t2+△x4).     

解四阶抛物型方程高精度紧致差分格式

针对四阶抛物型方程周期初值问题,提出了一个两层隐式差分格式和一个三层隐式差分格式.它们的局部截断误差分别为O((Δt)2+(Δx)4)和O((Δt)2+(Δt)(Δx)2+(Δx)4),其中Δt,Δx分别为时间步长和空间步长.误差分析和数值实验均表明,本文构造的差分格式比经典的Crank-Nicolson格式和Saul’ev构造的差分格式精度更高.从精度及稳定性方面考虑,本文构造的格式也比文[5]的显式格式要好.     

解三维热传导方程的一种高精度的显格式

对解三维热传导方程利用待定参数方法构造出一种精度O(Δt2+Δx4+Δy4+Δz4)的高精度易于计算的显式差分格式,并给出了其稳定性,通过数值例子可见其精度较其它方法提高2～3位有效数字。     

解一维热传导方程的高精度的隐式差分格式

本文对求解一维热传导方程利用待定参数法构造出截断误差为O(Δt~3+Δx~4)的高精度的隐式差分格式,并讨论了其绝对稳定性.     

A Finite Difference Scheme on a Priori Adapted Meshes for a Singularly Perturbed Parabolic Convection-Diffusion Equation

A boundary value problem is considered for a singularly perturbed parabolic convection-diffusion equation;we construct a finite difference scheme on a priori (se-quentially) adapted meshes and study its convergence.The scheme on a priori adapted meshes is constructed using a majorant function for the singular component of the discrete solution,which allows us to find a priori a subdomain where the computed solution requires a further improvement.This subdomain is defined by the perturbation parameterε,the step-size of a uniform mesh in x,and also by the required accuracy of the discrete solution and the prescribed number of refinement iterations K for im- proving the solution.To solve the discrete problems aimed at the improvement of the solution,we use uniform meshes on the subdomains.The error of the numerical so- lution depends weakly on the parameterε.The scheme converges almostε-uniformly, precisely,under the condition N~(-1)=o(ε~v),where N denotes the number of nodes in the spatial mesh,and the value v=v(K) can be chosen arbitrarily small for suitable K.     

Convergence of Iterative Difference Method with Nonuniform Meshes for Quasilinear Parabolic Systems

In this paper, we study the general difference schemes with nonuniform meshes for the following problem: u_t = A(x,t,u,u_x)u_{xx}, + f(x,t,u,u_x), 0 < x < l, 0 < t ≤ T \qquad (1) u(0,t) = u(l ,t) = 0, 0 < t ≤ T \qquad\qquad (2) u(x,0) = φ(x), 0 ≤ x ≤ l \qquad\qquad (3) where u, φ, and f are m-dimensional vector valued functions, u_t = \frac{∂u}{∂t}, u_x = \frac{∂u}{∂x}, u_{xx} = \frac{∂²u}{∂_x²}. In the practical computation, we usually use the method of iteration to calculate the approximate solutions for the nonlinear difference schemes. Here the estimates of the iterative sequence constructed from the iterative difference schemes for the problem (1)-(3) is proved. Moreover, when the coefficient matrix A = A(x, t, u) is independent of u_x, t he convergence of the approximate difference solution for the iterative difference schemes to the unique solution of the problem (1)-(3) is proved without imposing the assumption of heuristic character concerning the existence of the unique smooth solution for the original problem (1)-(3).