利用对称方法求解非线性偏微分方程组边值问题的数值解

本文研究微分方程对称方法在非线性偏微分方程组边值问题中的应用.首先,利用吴-微分特征列集算法确定给定非线性偏微分方程组边值问题的多参数对称;其次,利用对称将非线性偏微分方程组边值问题约化为常微分方程组初值问题;最后,利用龙格-库塔法求解常微分方程组初值问题的数值解.     

偏微分方程(组)完全对称分类微分特征列集算法

给出了一个确定含参数偏微分方程(组)的完全对称分类微分特征列集算法,该算法能够直接、系统地确定偏微分方程(组)的完全对称分类.用给出的算法获得了含任意函数类参数的线性和非线性波动方程完全势对称分类.这也是微分形式特征列集算法(微分形式吴方法)在微分方程领域中的新应用.     

一类偏微分方程(组)非古典对称存在性的判定方法

基于微分特征集理论和算法,提出在一定条件下判定偏微分方程(组)非古典对称存在性的机械化方法.该方法对Clarkson P A提出的关于偏微分方程(组)的非古典对称的公开问题给出了部分回答,为完全解决该问题提供了一个思路.通过若干个发展方程的非古典对称的确定说明了该方法的有效性.     

一类自伴随Lubrication方程的对称,守恒律,拉格朗日函数和精确解

本文借助李对称分析研究了一类自伴随的Lubrication方程,此类方程可用来描述液体薄膜动力学行为.基于非奇异的局域守恒律乘子和李对称方法,我们系统地推导出了此类方程的局域守恒律,非局域相关系统,李对称和一些有趣的精确解.此模型的非局域相关系统在本文中被首次研究,可用于寻找原方程更丰富的解空间.此外,基于局域守恒律和变分原则,我们推导出原方程的四类拉格朗日函数.     

二维欧拉流体动力学方程的完全守恒差分格式

一、引言 众所周知,描述流体动力学三个守恒律的偏微分方程组是质量方程、散度型或非散度型的动量方程和散度型的总能量方程。后者也可以写成非散度型的比内能方程或熵的方程。流体动力学偏微分方程组可以用各种形式来表达,它们是等价的,即从一种形式能够转换成另一种形式,反之亦然。但是,在一般情形下,逼近一种形式偏微分方程组的差分方程不一定能够推导出逼近其它等价的偏微分方程的差分方程。因而,在这种情况下,或者导致破坏总能量守恒律,或者不保持内能和动能的各自平衡。为了消除这个缺点,[2]     

双曲型守恒律方程的熵稳定格式的一些讨论

本文讨论双曲型守恒律方程的熵稳定格式.对于给定的熵对,格式所满足的熵条件中的数值熵通量是不唯一的.Tadmor的充分条件可以唯一地确定标量方程的熵守恒通量,但不能唯一确定方程组的熵守恒通量,却可以给出方程组的空间一阶精度的熵守恒格式.也讨论了在熵守恒通量上添加数值粘性得到的显式熵稳定格式需要满足的条件及常见的时间离散对熵守恒和熵稳定的影响.     

基于坏单元指示子的p自适应RKDG算法

Runge-Kutta间断Galerkin(RKDG)方法是求解双曲守恒律方程的主流方法之一.很多双曲守恒律问题的规模特别巨大,数值计算求解时需要耗费大量的时间和计算机存储空间.为此我们设计了一个基于坏单元指示子的p自适应RKDG算法,它不仅能够保持原RKDG方法在光滑区域的高阶逼近,而且能够有效降低存储空间.同时,这也为后续进一步开展hp自适应RKDG算法的研究奠定了基础.     

线性传输方程带二次多项式重构的熵格式（英文）

最近几年来,茅德康等发展了一类有限体积格式计算偏微分方程[1,3-4,6-9].该类格式得到比较好的计算结果.在文[8]中王和茅提出一个满足两个守恒律和三个守恒律的熵格式计算线性发展方程,但是该格式是基于线性多项式重构.本文发展了一个基于二次多项式重构满足两个守恒律的熵格式.数值试验表明本文的格式在长时间计算方面优于文[8].     

修正Broer-Kaup-Kupershmidt(mBKK)方程组的李对称分析,非线性自伴随及守恒律

利用李群分析法研究修正Broer-Kaup-Kupershmidt(mBKK)方程组,求得方程组的李对称.根据Ibragimov定理证明mBKK方程组具有非线性自伴随性,并由此构造方程组对称对应的无穷多守恒律.     

流变计算的高性能有限元收敛性分析

文中研究非Newton(牛顿)流体流变问题的混合型双曲抛物一阶偏微分方程的收敛性,采用耦合的偏微分方程组(Cauchy流体方程、P-T/T应力方程),模拟自由表面元或由过度拉伸元素产生的流域.使用半离散有限元方法进行求解,对于含有时间变量的耦合方程,在空间上用有限元法,利用三线性泛函来解决偏微分方程组的非线性;在时间上用Euler(欧拉)格式,得出方程组的收敛精度可达到O(h2+Δt).通过高性能计算的预估计和后估计得到方程的数值结果,并显示网格变形的大小.     

A method for computing symmetries and conservation laws of integra-differential equations

A method for computing symmetries and conservation laws of integro-differential equations is proposed. It resides in reducing an integro-differential equation to a system of boundary differential equations and in computing symmetries and conservation laws of this system. A geometry of boundary differential equations is constructed like the differential case. Results of the computation for the Smoluchowski's coagulation equation are given.     

New exact solutions of a generalised Boussinesq equation with damping term and a system of variant Boussinesq equations via double reduction theory.

The conservation laws of a generalised Boussinesq (GB) equation with damping term are derived via the partial Noether approach. The derived conserved vectors are adjusted to satisfy the divergence condition. We use the definition of the association of symmetries of partial differential equations with conservation laws and the relationship between symmetries and conservation laws to find a double reduction of the equation. As a result, several new exact solutions are obtained. A similar analysis is performed for a system of variant Boussinesq (VB) equations.     

Symmetries,Conservation Laws,and Noether's Theorem for Differential‐Difference Equations

This paper mainly contributes to the extension of Noether's theorem to differential‐difference equations. For this purpose, we first investigate the prolongation formula for continuous symmetries, which makes a characteristic representation possible. The relations of symmetries, conservation laws, and the Fréchet derivative are also investigated. For nonvariational equations, because Noether's theorem is now available, the self‐adjointness method is adapted to the computation of conservation laws for differential‐difference equations. Several differential‐difference equations are investigated as illustrative examples, including the Toda lattice and semidiscretizations of the Korteweg–de Vries (KdV) equation. In particular, the Volterra equation is taken as a running example.     

Nonlinear self-adjointness through differential substitutions

It is known (Ibragimov, 2011; Galiakberova and Ibragimov, 2013) [14,18] that the property of nonlinear self-adjointness allows to associate conservation laws of the equations under study, with their symmetries. In this paper we show that, even when the equation is nonlinearly self-adjoint with a non differential substitution, finding the explicit form of the differential substitution can provide new conservation laws associated to its symmetries. By using the general theorem on conservation laws (Ibragimov, 2007) [11] and the property of nonlinear self-adjointness we find some new conservation laws for the modified Harry-Dym equation. By using a differential substitution we construct a conservation law for the Harry-Dym equation, which has not been derived before using Ibragimov method.     

Conservation Laws For the (1+2)-Dimensional Wave Equation in Biological Environment

The derivation of conservation laws for the wave equation on sphere, cone and flat space is considered. The partial Noether approach is applied for wave equation on curved surfaces in terms of the coefficients of the first fundamental form (FFF) and the partial Noether operator's determining equations are derived. These determining equations are then used to construct the partial Noether operators and conserved vectors for the wave equation on different surfaces. The conserved vectors for the wave equation on the sphere, cone and flat space are simplified using the Lie point symmetry generators of the equation and conserved vectors with the help of the symmetry conservation laws relation.     

Relations between symmetries and conservation laws for difference systems

This paper presents a relation between divergence variational symmetries for difference variational problems on lattices and conservation laws for the associated Euler–Lagrange system provided by Noether's theorem. This inspires us to define conservation laws related to symmetries for arbitrary difference equations with or without Lagrangian formulations. These conservation laws are constrained by partial differential equations obtained from the symmetries generators. It is shown that the orders of these partial differential equations have been reduced relative to those used in a general approach. Illustrative examples are presented.     

Soil water redistribution and extraction flow models: Conservation laws

We determine all the nontrivial conservation laws for soil water redistribution and extraction flow equations which are modelled by a class of (2+1) nonlinear evolution partial differential equations with three arbitrary elements. It is shown that for arbitrary elements in the model equation there exist trivial conservation laws. We point out that nontrivial conservation laws exist for certain classes of equations which admit point symmetries.     

Conservation laws for the Black–Scholes equation

In the search for solutions to the important partial differential equation due to Black, Scholes and Merton potential symmetries are very useful as new solutions of the equation can be obtained as a result. These potential symmetries require that the equation be written in conserved form, ie. we need to determine conservation laws for the equation. We calculate the conservation laws utilizing the point symmetries of the equation following the method of Kara and Mahomed [A.H. Kara, F.M. Mahomed, The relationship between symmetries and conservation laws, Int. J. Theor. Phys. 39 (2000) 23–40].     

Lie symmetries and conservation laws of the Fokker-Planck equation with power diffusion

We concentrate on Lie symmetries and conservation laws of the Fokker-Planck equation with power diffusion describing the growth of cell populations. First, we perform a complete symmetry classification of the equation, and then we find some interesting similarity solutions by means of the symmetries and the variable coefficient heat equation. Local dynamical behaviors are analyzed via the solutions for the growing cell populations. Second, we show that the conservation law multipliers of the equation take the form Λ=Λ(t,x,u), which satisfy a linear partial differential equation, and then give the general formula of conservation laws. Finally, symmetry properties of the conservation law are investigated and used to construct conservation laws of the reduced equations.     

Approximate Noether-type symmetries and conservation laws via partial Lagrangians for PDEs with a small parameter

We show how one can construct approximate conservation laws of approximate Euler-type equations via approximate Noether-type symmetry operators associated with partial Lagrangians. The ideas of the procedure for a system of unperturbed partial differential equations are extended to a system of perturbed or approximate partial differential equations. These approximate Noether-type symmetry operators do not form a Lie algebra in general. The theory is applied to the perturbed linear and nonlinear (1+1) wave equations and the Maxwellian tails equation. We have also obtained new approximate conservation laws for these equations.