系数显含时间变量的拟线性双曲型方程Galerkin方法误差估计

本文讨论系数显含时间变量的拟线性双曲型方程的Galerkin方法,导出的有限元方程是关于U_j~(n 1)的线性代数方程组.给出的H~1模误差估计适用于Dirichlet边界条件、混合边界条件以及第三边界条件,误差估计不依赖于任何辅助函数且其逼近阶是最优的.     

半线性伪双曲方程最低阶的H~1-Galerkin混合元方法

研究在半离散和全离散格式下,半线性伪双曲方程最低阶的协调H~1-Galerkin混合有限元逼近.具体地,用双线性元逼近原始变量u,用零阶Raviart-Thomas(R-T)元逼近流量p.首先通过泰勒展式和积分恒等式技巧得到了p的一个新的误差估计式.然后,导出了u在H~1模和p在H(div;Ω)模意义下的超逼近性质,改进了已有文献的结果.     

二阶双曲方程一个新的非协调混合元超收敛性分析

研究了一类二阶双曲型方程在新混合元格式下的非协调混合有限元方法.在抛弃传统有限元分析的必要工具-Ritz投影算子的前提下,直接利用单元的插值性质,运用高精度分析和对时间t的导数转移技巧,借助于插值后处理技术,分别导出了关于原始变量u的H~1-模和通量=-▽u在L~2-模下的O(h~2)阶超逼近性质和整体超收敛结果.进一步,给出了一些数值算例验证了理论分析的正确性.     

非线性四阶双曲方程低阶混合元方法的超收敛分析

对一类非线性四阶双曲方程利用双线性元Q_(11)及Q_(01)×Q_(10)元给出了一个低阶混合元格式.基于上述两个单元的高精度结果,采用插值和投影相结合的方法,利用对时间t的导数转移技巧,借助插值后处理技术,在半离散格式下导出了原始变量u和中间变量u=-△u在H~1模意义下及流量p=-▽u在(L~2)~2模意义下具有O(h~2)阶的超逼近和超收敛结果.与此同时,在全离散格式下,证明了u和v在H~1模意义下及p在(L~2)~2模意义下单独利用插值或投影所无法得到的具有O(h~2+(△t)~2)阶的超逼近和超收敛结果.     

抛物型积分微分方程新混合元格式的超逼近分析

基于双二次元及其梯度空间,建立了抛物型积分微分方程的一种新混合有限元逼近格式.在不需要Ritz-Volterra投影的前提下,直接利用双二次元插值的高精度结果及关于时间变量的导数转移技巧,在半离散格式下,得到了原始变量u和中间变量p=▽u+integral from n=0 to t▽u(s)ds分别关于H~1模和L~2模的O(h~4)阶超逼近结果,相比插值误差估计,提高了二阶精度.与此同时,对向后Euler格式,导出了u和p分别在H~1模与L~2模意义下的O(h~4+τ)阶超逼近;对Crank-Nicolson-Galerkin格式,在L~2模意义下证明了u和p分别具有O(h~4+τ~2)和O(h~3+τ~2)阶的超逼近性质.其中,h,τ分别表示空间剖分参数和时间步长,t代表时间变量.     

正对称组在角状区域内的合格边值问题

本文考虑角状区域内正对称组的稳定合格边值问题,在“恰当定号”的假设下,对于非特征边界,得到了非齐次边值问题当资料为H~1时的H~1强解存在性及相应的能量不等式(定理2);对于一侧为特征的边界,用逼近法证明了其L~2适定性(定理3)。以上结果用于讨论对称双曲组,得劈状区域中的H~1及L~2适定性(定理4、5)。     

一类具有吸收边界条件的二阶非线性双曲方程的混合元法分析

1　引　　言关于二阶双曲型方程的有限元解的收敛性问题 ,目前已经有不少结果 .Dupont[1 ] 给出了一类线性双曲方程 Galerkin解的 L2 误差估计 ,Baker[2 ] 对此作了改进 ,用的是一种所谓“非标准的能量方法”.这一方法为 Cowsar,Dupont,Wheeler[3] 所采用 ,分析了一类具有吸收边界条件的线性双曲方程的混合元格式的 L2收敛性 .对于非线性双曲型问题 ,袁益让 ,王宏[4,5] 等给出了标准有限元方法的 H1 与 L2 误差估计 .本文试图把 [3]的工作更进一步研究 ,我们考虑如下非线性双曲问题 :φ(x) utt= mi,j=1 xi(aij(x) p(x,u) u xj) + mi=1…     

一类三维拟线性双曲型方程交替方向有限元法

对一类一般的三维拟线性双曲型方程通过转化二阶时间导数得到关于一阶时间导数的耦合方程组,然后进行离散得到交替方向有限元格式,应用微分方程先验估计的理论和技巧得到了最优阶H~1-模和L~2-模误差估计,并给出了数值算例,数值结果和理论分析得到很好的吻合.     

非线附曲型方程数值积分的有限元逼近

众所周知,解偏微分方程的有限元方法最终归结为求解线性代数方程组,其系数的计算心须求助于数值积分。本文讨论非线性二阶双曲型方程带数值积分的有限元方法,导出了最佳L_2,L_∞误差估计。具有第一类齐次边界条件双曲型方程混合问题的弱形式是求u(x,t)∈H~1(Ω),0≤t≤T,使得     

非线性四阶双曲方程扩展的非协调混合元方法的超收敛分析及外推

对一类非线性四阶双曲方程,利用EQ_1~(rot)元及零阶Raviart-Thomas元建立一个新的扩展的非协调混合元逼近格式.首先证明了逼近解的存在唯一性.其次,基于EQ_1~(rot)元特殊性质,再利用零阶Raviart-Thomas元的高精度分析结果和插值后处理技术,在半离散格式下导出了原始变量u和中间变量v=-?u在H~1模及中间变量q=?u,σ=-?(?u)在(L~2)~2模意义下具有O(h~2)阶的超逼近性质和超收敛结果.最后,利用EQ_1~(rot)元的渐近展开式,构造一个新的合适的外推格式,得到相关变量O(h~3)阶的外推解.     

平面双调和问题的第一类边界积分方程的高精度求积方法与外推

借助位势理论,平面双调和方程的Dirichlet问题被转化为第一类边界积分方程组,本文使用新型的反常积分的求积公式构造出解造解此类边界积分方程的机械求积方法,证明了该方法具有O（h^3)阶精度和误差的h^3幂渐近展开,故借助Richardson外推还能提高精度阶。     

阻尼Sine-Gordon方程的H1-Galerkin混合元方法数值解

利用H1-Galerkin混合有限元方法讨论阻尼Sine-Gordon方程,得到一维情况下半离散和全离散格式的最优阶误差估计,并且推广应用到二维和三维情况,而且不用验证LBB相容性条件.     

To the theory of asymptotically stable second-order accurate two-stage scheme for an inhomogeneous parabolic initial-boundary value problem

An asymptotically stable two-stage difference scheme applied previously to a homogeneous parabolic equation with a homogeneous Dirichlet boundary condition and an inhomogeneous initial condition is extended to the case of an inhomogeneous parabolic equation with an inhomogeneous Dirichlet boundary condition. It is shown that, in the class of schemes with two stages (at every time step), this difference scheme is uniquely determined by ensuring that high-frequency spatial perturbations are fast damped with time and the scheme is second-order accurate and has a minimal error. Comparisons reveal that the two-stage scheme provides certain advantages over some widely used difference schemes. In the case of an inhomogeneous equation and a homogeneous boundary condition, it is shown that the extended scheme is second-order accurate in time (for individual harmonics). The possibility of achieving second-order accuracy in the case of an inhomogeneous Dirichlet condition is explored, specifically, by varying the boundary values at time grid nodes by O(τ ²), where τ is the time step. A somewhat worse error estimate is obtained for the one-dimensional heat equation with arbitrary sufficiently smooth boundary data, namely, $O\left( {\tau ^2 \ln \frac{T} {\tau }} \right) $ , where T is the length of the time interval.     

伪双曲型积分-微分方程的H~1-Galerkin混合元法误差估计

<正>1引言考虑如下一类具有Lipschitz连续边界(?)Ω的凸有界区域Ω上的伪双曲型积分微分方程其中Ω(?)R~d,(d=1,2,3)J=(0,T],对于固定的T,0T∞,函数0a_0≤a(x,t)≤     

Analysis of a meshless method for the time fractional diffusion-wave equation

In this paper a numerical technique is proposed for solving the time fractional diffusion-wave equation. We obtain a time discrete scheme based on finite difference formula. Then, we prove that the time discrete scheme is unconditionally stable and convergent using the energy method and the convergence order of the time discrete scheme is \(\mathcal {O}(\tau ^{3-\alpha })\). Firstly, we change the main problem based on Dirichlet boundary condition to a new problem based on Robin boundary condition and then, we consider a semi-discrete scheme with Robin boundary condition and show when \(\beta \rightarrow +\infty \) solution of the main semi-discrete problem with Dirichlet boundary condition is convergent to the solution of the new semi-discrete problem with Robin boundary condition. We consider the new semi-discrete problem with Robin boundary condition and use the meshless Galerkin method to approximate the spatial derivatives. Finally, we obtain an error bound for the new problem. We prove that convergence order of the numerical scheme based on Galekin meshless is \(\mathcal {O}(h)\). In the considered method the appeared integrals are approximated using Gauss Legendre quadrature formula. The main aim of the current paper is to obtain an error estimate for the meshless Galerkin method based on the radial basis functions. Numerical examples confirm the efficiency and accuracy of the proposed scheme.     

An Element-Free Galerkin Method for Time-Fractional Diffusion-Wave Equations北大核心CSCD

利用无单元Galerkin法,对Caputo意义下的时间分数阶扩散波方程进行了数值求解和相应误差理论分析。首先用L1逼近公式离散该方程中的时间变量,将时间分数阶扩散波方程转化成与时间无关的整数阶微分方程;然后采用罚函数方法处理Dirichlet边界条件,并利用无单元Galerkin法离散整数阶微分方程;最后推导该方程无单元Galerkin法的误差估计公式。数值算例证明了该方法的精度和效果。     

NATURAL BOUNDARY ELEMENT METHOD FOR THREE DIMENSIONAL EXTERIOR HARMONIC PROBLEM WITH AN INNER PROLATE SPHEROID BOUNDARY

In this paper, we study natural boundary reduction for Laplace equation with Dirichletor Neumann boundary condition in a three-dimensional unbounded domain, which is theoutside domain of a prolate spheroid. We express the Poisson integral formula and naturalintegral operator in a series form explicitly. Thus the original problem is reduced to aboundary integral equation on a prolate spheroid. The variational formula for the reducedproblem and its well-posedness are discussed. Boundary element approximation for thevariational problem and its error estimates, which have relation to the mesh size andthe terms after the series is truncated, are also presented. Two numerical examples arepresented to demonstrate the effectiveness and error estimates of this method.     

边界元方法的抽象误差估计及其应用

§1.引言 边界元方法是近二十年来发展的一种求解偏微分方程的数值方法,其基本思想是:先利用Green公式或位势将区域上的偏微分方程转化成边界上的积分方程,此时偏微分方程的解由边界积分方程的解表出;然后数值求解边界积分方程,进而求得偏微分方程的近     

Fourth‐order compact scheme for the one‐dimensional sine‐Gordon equation

Finite difference scheme to the generalized one‐dimensional sine‐Gordon equation is considered in this paper. After approximating the second order derivative in the space variable by the compact finite difference, we transform the sine‐Gordon equation into an initial‐value problem of a second‐order ordinary differential equation. Then Padé approximant is used to approximate the time derivatives. The resulting fully discrete nonlinear finite‐difference equation is solved by a predictor‐corrector scheme. Both Dirichlet and Neumann boundary conditions are considered in our proposed algorithm. Stability analysis and error estimate are given for homogeneous Dirichlet boundary value problems using energy method. Numerical results are given to verify the condition for stability and convergence and to examine the accuracy and efficiency of the proposed algorithm. © 2008 Wiley Periodicals, Inc. Numer Methods Partial Differential Eq, 2009     

Local exact controllability of Schr\"{o}dinger equation with Sturm- Liouville boundary value problems

In this paper, we investigate the controllability of 1D bilinear Schr\"{o}dinger equation with Sturm-Liouville boundary value condition. The system represents a quantumn particle controlled by an electric field. K. Beauchard and C. Laurent have proved local controllability of 1D bilinear Schr\"{o}dinger equation with Dirichlet boundary value condition in some suitable Sobolev space based on the classical inverse mapping theorem. Using a similar method, we extend this result to Sturm-Liouville boundary value proplems.