Benjamin方程的Baecklund变换、非线性叠加公式及无穷守恒律

利用屠格式求出了Benjamin方程的Baecklund变换、精确孤波解、非线性叠加公式及其无穷守恒律,这种算法具有普适性。     

求解非定常对流扩散方程的流函数松弛方法

提出了一种求解线性和非线性对流扩散方程的流函数松弛方法.方法的主要思想是利用流函数松弛近似将原始的方程转化成等价的松弛方程组,新的松弛方程组是带源项的双曲系统.通过稳定性分析可以知道新系统的耗散系数可由松弛系数调整.数值实现亦证明这个方法可以快速有效地描述对流扩散方程的解.     

双Sine-Gordon方程的对称和守恒律

通过使用经典李对称方法建立双Sine-Gordon方程的李点对称和LieBcklund对称,并证明此方程是非线性自伴随的.根据双Sine-Gordon方程的对称和它的伴随方程构造它的守恒律.     

二维非线性对流-扩散方程的特征-差分解法

1.引言 近年来,求解对流-扩散方程的修正特征线法日渐被人们重视,已有不少人讨论了这一方法,如[1]-[5]。其中[1]和[2]是该领域的奠基性工作。[6]讨论了对流-扩散方程的特征-差分方法,改善并推广了[1]中某些重要结果。本文将讨论二维非线性对流-扩     

扰动Boussinesq方程的近似守恒律

构造了具有扰动项的Boussinesq方程的近似守恒向量和近似守恒律.在方程允许拉格朗日函数的情况下,利用欧拉方程的部分拉格朗日函数方法,研究了含有一阶线性组合扰动项的Boussineq方程的近似守恒律.给出了该方程的近似守恒向量及近似守恒律的分类结果.     

二维非线性对流扩散方程的非振荡特征差分方法

１．引言 近十几年来,双曲守恒律问题的高分辨率格式已取得很大发展,具有局部自适应选取节点的非振荡插值算法（如 ＵＮＯ［１］, ＥＮＯ［２］等）在这些格式的构造中起着重要的作用．特征差分法是求解对流扩散问题的一种较为有效方法,但在求解具有陡峭前线问题时,也会产生非物理振荡阻（见４）．本文将把特征差分法与非振荡插值算法相结合构造对流扩散问题的高分辨率差分格式． ［１］中的 ＵＮＯ及［２］中的 ＥＮＯ插值都是一维的,有关讨论二维 ＵＮＯ及ＥＮＯ插值的文章还不多见,本文将构造二维基于六节点的二次非振荡插值以及…     

广义Heisenberg方程的无穷守恒律

本文给出了Heisenberg方程的无穷守恒律,并具体给出了其前三个守恒律,特别得到了铁磁链方程无穷多个微分形式与积分形式的守恒律。     

非线性对流扩散问题的差分-流线扩散法

1．引言流线扩散法（简称SD方法）是由Huzhes和Brooks在1980年前后提出的一种数值求解对流占优扩散问题的新型有限元算法．随后，Johnson和N8vert将SD方法推广到发展型对流扩散问题（［1］，［2］，［3］）．熟知，对于对流扩散问题，标准有限元法虽具有高阶精度，但常产生数值振荡；古典人工粘性Galerkin法更具有较好的稳定性，但仅具有一阶精度．而（SD方法兼具良好的数值稳定性和高阶精度，因此得到了越来越多的重视，对于发展型对流扩散问题，传统的SD方法均采用时空有限元．这样做，虽然可使时间和空间方向上的精度很好的协调起…     

非线性对流扩散方程的逆风型差分格式

§1 对流扩散方程可以用来描述水中和大气中污染物质的分布、流体流动和流体中的传热等,以上均有对流扩散的特征。数值求解对流扩散方程很重要,近年来工作不少,如[1,2]。我们考虑二维非线性对流扩散方程的初边值问题     

三阶Airy方程满足两个守恒律的非线性差分格式

近年来,学者们对发展型偏微分方程设计了一种能保持多个守恒律的数值方法,这类方法无论在解的精度还是长时间的数值模拟方面都表现出非常好的性质.将这类思想应用到三阶Airy方程,即三阶散射方程,对其设计了满足两个守恒律的非线性差分格式.该格式不仅计算数值解,同时计算数值能量,并且保证数值解和数值能量同时守恒.从数值结果可以看出,该格式在长时间的数值模拟中具有更好的保结构性质.     

Conservation laws for nonlinear telegraph equations

A complete conservation law classification is given for nonlinear telegraph (NLT) systems with respect to multipliers that are functions of independent and dependent variables. It turns out that a very large class of NLT systems admits four nontrivial local conservation laws. The results of this work are summarized in tables which display all multipliers, fluxes and densities for the corresponding conservation laws. A physical example is considered for possible applications.     

非线性守恒律高阶谱粘性法的收敛性

讨论守恒型方程周期边界问题的高阶谱粘性方法逼近解的收敛性.在逼近解一致有界的假设下,通过建立其高阶导数的上界估计,证明了高阶谱粘性方法逼近解具有同二阶谱粘性方法逼近解相类似的高频衰减性质.以此为基础,用补偿列紧法证明了高阶谱粘性方法逼近解收敛于守恒型方程的物理解.     

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].     

A basis of hierarchy of generalized symmetries and their conservation laws for the (3+1)-dimensional diffusion equation

We determine, by hierarchy, dependencies between higher order linear symmetries which occur when generating them using recursion operators. Thus, we deduce a formula which gives the number of independent generalized symmetries (basis) of several orders. We construct a basis for conservation laws (with respect to the group admitted by the system of differential equations) and hence generate infinitely many conservation laws in each equivalence class.     

Application of regularization technique to variational adjoint method: A case for nonlinear convection-diffusion problem

A discrete assimilation system for a one-dimensional variable coefficient convection-diffusion equation is constructed. The variational adjoint method combined with the regularization technique is employed to retrieve the initial condition and diffusion coefficient with the aid of a set of simulated observations. Several numerical experiments are performed: (a) retrieving both the initial condition and diffusion coefficient jointly (Experiment JR), (b) retrieving either of them separately (Experiment SR), (c) retrieving only the diffusion coefficient with the iteration count increased to 800 (Experiment NoR-SR), and (d) retrieving only the diffusion coefficient with the consideration of a regularization term based on the Experiment NoR-SR (Experiment AdR-SR). The results indicate that within the limit of 100 iterations, the retrieval quality of the Experiment SR is better than those from the Experiment JR. Compared with the initial condition, the diffusion coefficient is a little difficult to retrieve, whereas we still achieve the desired result by increasing the iterations or integrating the regularization term into the cost functional for the improvement with respect to the diffusion coefficient. Further comparisons between the Experiment NoR-SR and AdR-SR show that the regularization term can really help not only improve the precision of retrieval to a large extent, but also speed up the convergence of solution, even if some perturbations are imposed on those observations.     

Finite element algorithm based on high-order time approximation for time fractional convection-diffusion equation

In this paper, finite element method with high-order approximation for time fractional derivative is considered and discussed to find the numerical solution of time fractional convection-diffusion equation. Some lemmas are introduced and proved, further the stability and error estimates are discussed and analyzed, respectively. The convergence result $O(h^{r+1}+\tau^{3-\alpha})$ can be derived, which illustrates that time convergence rate is higher than the order $(2-\alpha)$ derived by $L1$-approximation. Finally, to validate our theoretical results, some computing data are provided.