不可压双曲型液晶的Ericksen-Leslie方程的大Ericksen数的极限的形式分析

该文考虑了参数化的液晶的不可压双曲型的Ericksen-Leslie方程.形式上,让参数消失该文证明了这个极限方程存在一个局部的经典解.更进一步,该文形式上得出一个关于这个参数化的液晶的双曲型方程和极限方程的解的误差估计,这对应的是关于它们的经典解在L2空间中的一个形式上的能量估计.     

一类拟线性椭圆型方程广义解最大模的先验估计

对于拟线性椭圆型方程(1),能在很一般的结构条件下证明广义解的有界性,但却一直没有给出过解的最大模的先验估计.本文将第一次给出一类拟线性椭圆型方程广义解的最大模的先验估计.     

一类拟线性椭圆型方程广义解最大模的先验估计

对于拟线性椭圆型方程(1),能在很一般的结构条件下证明广义解的有界性,但却一直没有给出过解的最大模的先验估计.本文将第一次给出一类拟线性椭圆型方程广义解的最大模的先验估计.     

一类高阶微分方程亚纯解的增长性

研究了几种类型的高阶线性亚纯系数微分方程的亚纯解的增长性,对方程的亚纯解的增长率得到了精确估计.     

一类具耗散项双曲系统解的存在性问题

讨论具有非线性耗散项双曲系统的初值问题,对初值的模不加小性假设,而要求其一阶导数适当小情形下,证明其光滑解的整体存在性,并用经典解的特征线法获得解的模估计,同时应用极值原理得到解的偏导数的一致估计.     

微分方程解的迭代级

本文研究了几类高阶迭代级系数微分方程存在某个系数对方程的解的性质起支配作用时,方程解的增长性问题.利用Nevanlinna理论与Valiron理论的方法,得到方程解的迭代增长级的精确估计.推广了上述方程对解的性质起支配作用的系数为固定系数时的结果.     

具有Cauchy-Ventcel边界条件的有界域中亚临界半线性波方程的稳定与控制

分析RN 的有界域中半线性波方程解的指数衰减特性,有界域具有Cauchy-Ventcel型边界条件,并且球体外部作用着阻尼项.在对非线性作出适当又自然的假设后,倘若非线性在无穷大处为亚临界时,有限能量解的指数衰减性满足局部一致性.粗略地说,亚临界性意味着,在无穷大处非线性增长率次数不大于5.B.Dehman、G.Lebeau和E.Zuazua得到了R3 和RN 中的经典能量(用于估计局限于球体外部以能量形式表示的解的总能量)不等式和Strichartz估计的结果,使得研究RN 有界域(域内及其边界上是亚临界非线性,边界为Cauchy-Ventcel型连续)中半线性波方程的稳定性与可控性成为可能.     

奇数维可压缩液晶流方程解的逐点估计

首先, 本文利用标准的能量估计方法得到高维(3 维及以上) 的液晶流方程组小初值经典解的整体存在性. 然后, 本文运用Green 函数方法, 得到奇数维情形(3 维及以上) 该解的逐点估计. 该结果表明, 密度ρ和动量m同Navier-Stokes 方程组一样满足一般Huygens 原理, 而单位向量场d则没有这种现象, 其有着与热方程的解类似的时空估计.     

对角型拟线性双曲组的整体经典解

本文在特征值部分线性退化、部分弱线性退化时,考察一阶拟线性对角型严格双曲组的柯西问题,当初值满足适当的条件时得到了其整体经典解的存在性.     

中立型比例延迟微分系统线性θ-方法的渐近估计

本文研究了一类线性非自治中立型比例延迟微分系统线性θ-方法的渐近稳定性,并借助于泛函不等式得到了数值解的渐近估计.此渐近估计不仅比数值渐近稳定性描述得更加精确,而且还能给出非稳定情形数值解的上界估计式.数值算例验证了相关理论结果.     

On the Properties of the Solution of a Strongly Degenerate Parabolic Equation

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不用克希霍夫—拉夫假设的弹性圆板理论再探

本文在不用克希霍夫一拉夫假设的弹性板一般理论的基础上,建立了不用克希霍夫一拉夫假设的弹性圆板的一级近似理论,对圆板在四周固定和均布载荷的条件下,得到了具体的轴对称分析解,并和经典的圆薄板解进行了比较,证明本文新解更加接近实验结果,本文也具体地讨论了理论结果中厚度增大时的影响。     

传统离散型报童决策模型的一个问题及其改进方案

实践表明 ,对状态变量的递增量较大的报童问题 ,应用传统的离散型报童模型所确定的最优决策量与实际最优方案之间可能存在较大偏差 .分析了这一偏差出现的原因 ,提出了状态变量递增量较大的情况下的离散变量报童模型和求解方法 ,并证明这一模型比原模型得出的求解结果更为精确 .最后 ,通过算例验证了新模型对原模型的改进 .     

A numerical study of the semi‐classical limit for three‐coupled long wave–short wave interaction equations

We study numerically the semi‐classical limit for three‐coupled long wave–short wave interaction equations. The Fourier–Galerkin semi‐discretization is proved to be spectrally convergent in an appropriate energy space. We propose a split‐step Fourier method in the semi‐classical regime with the discussion of the meshing strategy, which is necessary to obtain correct numerical solution. Plane wave solution with weak and strong initial phases, solitary wave solution and Gaussian solution are considered to investigate the semi‐classical limit.     

一个具有非线性边界条件的抛物系统整体存在性和爆破

In this paper the nonnegative classical solutions of a parabolic system with nonlinear boundary conditions are discussed. The existence and uniqueness of a nonnegative classical solution are proved. And some sufficient conditions to ensure the global existence and nonexistence of nonnegative classical solution to this problem are given.     

Classical solution of a problem with an integral condition for the one-dimensional wave equation

We find a closed-form classical solution of the homogeneous wave equation with Cauchy conditions, a boundary condition on the lateral boundary, and a nonlocal integral condition involving the values of the solution at interior points of the domain. A classical solution is understood as a function that is defined everywhere in the closure of the domain and has all classical derivatives occurring in the equation and conditions of the problem. The derivatives are defined via the limit values of finite-difference ratios of the function and corresponding increments of the arguments.     

Solution of prey–predator problem by numeric–analytic technique

In this paper, an analytical expression for the solution of the prey–predator problem by an adaptation of the classical Adomian decomposition method (ADM). The ADM is treated as an algorithm for approximating the solution of the problem in a sequence of time intervals, i.e. the classical ADM is converted into a hybrid numeric–analytic method called the multistage ADM (MADM). Numerical comparisons with the classical ADM, and the classical fourth-order Rungge–Kutta (RK4) methods are presented.     

Strain gradient plasticity solution for an internally pressurized thick-walled cylinder of an elastic linear-hardening material

An elastic-plastic solution is presented for an internally pressurized thick-walled plane strain cylinder of an elastic linear-hardening plastic material. The solution is derived in a closed form using a strain gradient plasticity theory. The inner radius of the cylinder enters the solution not only in non-dimensional forms but also with its own dimensional identity, which differs from that in classical plasticity based solutions and makes it possible to capture the size effect at the micron scale. The classical plasticity solution of the same problem is recovered as a special case of the current solution. To further illustrate the newly derived solution, formulas and numerical results for the plastic limit pressure are provided. These results reveal that the load-carrying capacity of the cylinder increases with decreasing inner radius at the micron scale. It is also seen that the macroscopic behavior of the pressurized cylinder can be well described by using classical plasticity based solutions.     

Symmetrisers and generalised solutions for strictly hyperbolic systems with singular coefficients

This paper is devoted to strictly hyperbolic systems and equations with non‐smooth coefficients. Below a certain level of smoothness, distributional solutions may fail to exist. We construct generalised solutions in the Colombeau algebra of generalised functions. Extending earlier results on symmetric hyperbolic systems, we introduce generalised strict hyperbolicity, construct symmetrisers, prove an appropriate Gårding inequality and establish existence, uniqueness and regularity of generalised solutions. Under additional regularity assumptions on the coefficients, when a classical solution of the Cauchy problem (or of a transmission problem in the piecewise regular case) exists, the generalised solution is shown to be associated with the classical solution (or the piecewise classical solution satisfying the appropriate transmission conditions).     

Quasi-stationary Stefan problem as limit case of Mullins-Sekerka problem

The existence of a local classical solution to the Mullins-Sekerka problem and the convergence to the two-phase quasi-stationary Stefan problem are proved when surface tension approaches zero. This convergence gives a proof of the existence of a local classical solution of quasi-stationary Stefan problem. The methods work in all dimensions.