Fokker Planck方程的非古典广义势对称及精确解

分析了Fokker-Planck方程的非古典势对称,通过广义势系统而不是一般势系统求得了这些非古典势对称.文中得到了这些方程的新的对称,同时也得到了伴随系统的新的对称,并用其求出了一些精确解.这些解对进一步研究Fokker-Planck方程所描述的物理现象具有广泛的应用价值.     

几个非线性偏微分方程的非古典对称及相似解

研究了一些非线性偏微分方程的非古典势对称和非古典对称,得到了某些方程的新的势对称和新的对称,同时也得到了其伴随系统的新的对称,并求出了一些相似解．这些解对进一步研究这些非线性偏微分方程所描述的物理现象具有广泛的应用价值．     

Benney方程的势对称和不变解

利用微分形式的吴方法计算了Benney方程的势对称及其不变解．由于Benney方程中包含不稳定项和耗散项,使得直接求其不变解较为困难,利用吴一微分特征列算法可大大降低其中确定方程组的计算难度．本文全面讨论了Benney方程不同系数情况下的对称,并且得到了新的势对称,同时利用这些对称求得了相应的不变解,这些解对进一步研究Benney方程所描述的物理现象具有广泛的应用价值．文章表明,对于守恒形式的偏微分方程,可通过其辅助系统求得的势对称来构造其不变解．     

广义预测控制中Diophantine方程的显式解

利用被控对象的离散差分方程与其状态空间能观标准型之间的关系,推导出广义预测控制中Diophantine方程的显式解,从而避免了其递推求解,使广义预测控制的应用更加方便。     

广义预测控制中Diophantine矩阵多项式方程的显式解

直接利用被控对象的离散差分方程推导出多变量广义预测控制中Diophantine矩阵多项式方程的显式解,从而避免了其递推求解或迭代求解,使广义预测控制的应用更加方便．     

Fokker-Planck方程的守恒量

利用系统运动方程的线性化方程及其伴随方程的相互关系,以及散度表达式在全Euler算子作用下为零这一特性,通过引进守恒量乘子来求得运动系统的守恒量．该方法不需要运动系统的Lagrange函数．以Fokker-Planck方程为例,利用该方法可以很容易给出它的无穷多守恒量．     

多变量H-控制问题的显式解

5 退化情形的显式解 问题(2)有解的充要条件是Pick矩阵P≥0,其中detP=0时发生了退化,这时P的逆不存在,公式(13)无法使用,需要另作处理,在H_∞最优控制问题求解时,必定出现退化情形,所以退化情形的显式解值得专门研究。P为Hermite矩阵,可以做Cholesky分解     

关于一般耦合矩阵方程的迭代对称解

本文构造了一个有效的迭代方法(CGL)去求解一般耦合矩阵方程的对称解.若一般耦合矩阵方程关于对称解相容,则对于任意给定的初始对称矩阵组,利用所构造的迭代算法,都能在有限步迭代出所求问题的一组对称解,若选用一些特殊的初值,则可获得矩阵方程的极小范数对称解.最后的数值例子表明了所给算法的有效性.     

一类非线性系统Fokker-Planck方程的解法

通过对一类典型非线性反馈系统的分析,提出一处对一阶和二阶反馈非线性系统的稳态Fokker-Planck方程的解析解法.根据这一方法,再利用最优降阶技术,提出高阶系统的近似解,并将其与RDF方法得出的近似解在精度上加以比较,得出有益的结论.     

矩阵方程AXB=C的D反对称最佳逼近解的算法

本文利用广义共轭梯度法设计求矩阵方程AXB=C的D反对称最佳逼近解的算法,证明了算法的有限步收敛性,数值实例说明算法是有效的。     

An explicit finite-difference scheme for the solution of the kadomtsev-petviashvili equation

A finite-difference method is used to transform the initial/boundary-value problem associated with the nonlinear Kadomtsev-Petviashvili equation, into an explicit scheme.

The numerical method is developed by replacing the time and space derivatives by central-difference approximants. The resulting finite-difference method is analysed for local truncation error, stability and convergence. The results of a number of numerical experiments are given.     

A higher-order alternating group explicit scheme for the diffusion equation

In this paper, a higher-order alternating group explicit scheme for the diffusion equation is developed. The scheme has fourth-order truncation error approximately. The numerical simulations show that the new scheme can provide more accurate solutions. A discussion on the numerical stability of the scheme is also included.     

Alternating group explicit method with exponential-type for the diffusion–convection equation

Based on the semi-explicit asymmetric exponential schemes constructed by the author, a new alternating group explicit (AGE) method with exponential-type for the numerical solution of the convection–diffusion equation is derived in the paper. The method has the obvious property of parallelism and is unconditionally stable. The results of numerical examples are given to show the effectiveness of the present methods that are in preference to the Evans and Abdullah' method in [Evans, D.J. and Abdullah, A.R., 1985, A new explicit method for the diffusion–convection equation. Computers & Mathematics with Application, 11, 145–154].     

A new unconditionally stable explicit scheme for the convection–diffusion equation with Robin boundary conditions

An alternating direction explicit (ADE) scheme to solve the unsteady convection–diffusion equation with Robin boundary conditions is presented and discussed in this paper. It was derived based on the local series expansion method and proved unconditionally stable by von Neumann stability analysis. Thereafter, the ADE scheme is compared with the conventional schemes, and a comparison between the amplification factor of all schemes and the exact one shows that the proposed scheme can simulate well both convection- and diffusion-dominated problems. Finally, the proposed method was validated by a numerical experiment which indicates that, for large cell Reynolds numbers, the proposed scheme, which has unconditional stability, is more accurate than implicit schemes and most explicit schemes. It is also shown that the proposed scheme is simple to implement, economical to use, effective for dealing with Robin boundary conditions and easy to apply to multidimensional problems.     

对流扩散方程并行求解方法研究综述

对流扩散方程是一类典型的偏微分方程,其并行求解方法对其他微积分方程的并行求解具有借鉴意义。对对流扩散方程的并行求解方法进行综述,分为显式直接并行、隐式迭代并行、交替分组显式并行和Monte Carlo并行四种并行求解方法,对其中涉及的计算原理进行描述,给出示例,并指出进一步研究方向。