Newton方程周期解存在唯一性的新证明

本文首先将Newton方程周期边值问题转化为初值问题，然后在较弱的条件下利用微分连续法构造性地证明了该方程周期解的存在唯一性．证明方法同时也提供了一种计算该周期解的大范围收敛方法．     

中立型时滞差分方程的振性与正解存在性

本文研究了一类中立型时滞差分方程的振动性和正解存在性，获得了该方程所有解振动的“Sharp”条件及存在正解的一个充分条件．     

奇异Hammerstein型积分方程解的存在性

本文讨论奇异Hammerstein型积分方程u λAFu=h1其中称该方程是奇异的，是指算子F的定义域不一定包含算子A的值域．利用Orlicz空间的一个嵌入性质，给出了奇异Hammerstein积分方程解的一个存在条件．     

一类强退化的抛物型方程的双曲特性

MBertsch和R．DalPasso在［1］中研究了方程（其中ψ为严格增函数且为有限数）具有严格增初值的Cauchy问题．讨论了该问题的解与一阶守恒律方程的解的相似性．在[1]中，条件是一个基本假设．本文主要讨论以上方程在退化（即的情况下），相应于特殊初值的Cauchy问题的解仍具有以上双曲现象．     

带调和势的超临界非线性Schrdinger方程的最佳门槛

考虑带调和势的超临界非线性Schroedinger方程，解决了该方程整体解和爆破解存在所依赖的初始条件的最佳分界门槛．通过构造两类强制变分问题和建立局部不变半流，运用势井方法和凹方法，获得了该方程在两个不同的空间中的整体解和爆破解的最佳门槛条件．     

一类拟线性Schrdinger方程

在二维空间中讨论一类拟线性Schrdinger方程,该方程在物理学上描述了吸引玻色-爱因斯坦凝聚.通过建立这个方程的性质,运用能量方法,证明了该方程所对应的初值问题的解在一定条件下爆破.同时利用变分方法,也得到了整体解存在的一个充分条件,该条件与一个经典的椭圆方程的基态有关.     

一类拟线性Schr(o)dinger方程

在二维空间中讨论一类拟线性Schr(o)dinger方程,该方程在物理学上描述了吸引玻色-爱因斯坦凝聚.通过建立这个方程的性质,运用能量方法,证明了该方程所对应的初值问题的解在一定条件下爆破.同时利用变分方法,也得到了整体解存在的一个充分条件,该条件与一个经典的椭圆方程的基态有关.     

Pasternak地基上简支板振动问题的准格林函数方法

提出一种新的数值方法——准格林函数方法．以Pasternak地基上简支多边形薄板的振动问题为例,详细阐明了准格林函数方法的思想．即利用问题的基本解和边界方程构造一个准格林函数,这个函数满足了问题的齐次边界条件,采用格林公式将Pasternak地基上薄板自由振动问题的振型控制微分方程化为两个耦合的第二类Fredholm积分方程．边界方程有多种选择,在选定一种边界方程的基础上,可以通过建立一个新的边界方程来表示问题的边界,以克服积分核的奇异性,最后由积分方程的离散化方程组有非平凡解的条件,求得固有频率．数值方法表明,该方法具有较高的精度．     

关于双特征Beltrami方程

该文研究空间Ｂｅｌｔｒａｍｉ方程的推广形式，即双特征Ｂｅｌｔｒａｍｉ方程．利用外微分形式与矩阵的外代数等工具，将双特征Ｂｅｌｔｒａｍｉ方程转化为一个非齐次的狆 调和方程，转化过程中只用到加于特征矩阵的一致椭圆型条件．然后验证了算子犃满足的条件：Ｌｉｐｓｃｈｉｔｚ型条件、单调不等式、齐次性条件以及算子犅满足的控制增长条件．并利用得到的狆 调和方程，给出了双特征Ｂｅｌｔｒａｍｉ方程广义解分量函数的弱单调性结果．     

非线性波动方程的交替显-隐差分方法

1．引言众所周知，非线性波动方程在自然科学领域有广泛的物理背景，诸如物理、化学反应方程，机械动力学方程，地球物理与大气海洋方程等．差分方法求解非线性波动方程已有研究，如［1］和IZ］就给出了非线性波动方程组的显式和隐式差分格式以及收敛性分析．虽然古典的显式差分格式易于并行计算，但是它的稳定性条件差（条件稳定）；古典的隐式差分格式稳定性条件好（绝对稳定）；但对非线性问题，一般需要线性化，然后求解一个线性代数方程组，并行计算能力差．本文正是在这样一种前题下，给出了一维问题的一种交替分段显一隐差分格式，…     

压电热弹性体的变分原理及正则方程和齐次方程

结合对偶变量理论,为压电热弹性体混合层合板问题推导了齐次的控制方程和Hamilton等参元列式．首先根据广义的Hamilton变分原理推导了压电热弹性体非齐次的Hamilton正则方程．然后进一步考虑了热平衡方程与导热方程中变量的对偶关系,通过增加正则方程的维数,成功地将非齐次的正则方程转化为能独立求解压电热弹性体耦合问题的齐次控制方程．为了推导四节点Hamilton等参元列式的方便,可将温度梯度关系类比成本构关系并构建新的变分原理．齐次方程大大简化了人们在分析压电热弹性体耦合问题时,通常要求解非齐次方程和关于平衡方程和导热方程的二阶微分方程的繁琐方法,同时也减少了数值计算工作量．     

Exact solutions of a two-dimensional nonlinear Schrödinger equation

In the present study, we converted the resulting nonlinear equation for the evolution of weakly nonlinear hydrodynamic disturbances on a static cosmological background with self-focusing in a two-dimensional nonlinear Schrödinger (NLS) equation. Applying the function transformation method, the NLS equation was transformed to an ordinary differential equation, which depended only on one function ξ and can be solved. The general solution of the latter equation in ζ leads to a general solution of NLS equation. A new set of exact solutions for the two-dimensional NLS equation is obtained.     

用格子Boltzmann方法模拟非线性热传导方程

对具有非线性源项和非线性扩散项的热传导方程建立格子Boltzmann求解模型.在演化方程中增加了两个关于源项分布函数的微分算子,对演化方程实施Chapman-Enskog展开.通过对演化方程的进一步改进,恢复出具有高阶截断误差的宏观方程.对不同参数选取下的非线性热传导方程进行了数值模拟,数值解与精确解吻合得很好.该模型也可以用于同类型的其他偏微分方程的数值计算中.     

Fokker-planck equation for brownian motion of rotating spherical particles : PMM vol. 40, n 6, 1976, pp. 1127–1131

The Langevin equation to derive the Fokker-Planck equation is used for the Brownian motion of particles in translational motion. The Fokker-Planck equation for the Brownian motion of particles which have, in addition to the translational velocity also an angular velocity, has not, so far, been derived. This can apparently be explained by the fact that in the case of the rotational motion, the Langevin equation for the translational motion velocity vector must be supplemented by a corresponding equation for an angular velocity vector. The latter equation must contain, in addition to the systematic moment of reaction linearly dependent on the angular velocity of rotation itself, a random moment rapidly varying with time. Moreover, to ensure the compatibility of two differential vector equations within the system, additional relations which must be introduced, must connect not only the coefficients of the systematic reactions, but also the. random vectors varying rapidly with time.In [1],the Boltzmann's equation for a mixture of two gases was used to derive a Fokker-Planck equation for a translational motion of Brownian particles. The same method can be applied to the Brownian motion of spherical particles which have, in addition to the translational velocities, angular velocities of self-rotations. In this case there is no need to introduce additional relations connecting the random rapidly varying vectors.In the present paper we derive the Fokker-Planck equations for a new model of rotating spherical molecules which was used in [2].     

广义Boussinesq方程的多辛方法

广义Boussinesq方程作为一类重要的非线性方程有着许多有趣的性质,基于Hamilton空间体系的多辛理论研究了广义Boussinesq方程的数值解法,构造了一种等价于多辛Box格式的新隐式多辛格式,该格式满足多辛守恒律、局部能量守恒律和局部动量守恒律．对广义Boussinesq方程孤子解的数值模拟结果表明,该多辛离散格式具有较好的长时间数值稳定性．     

Evolution of Bounding Functions for the Solution of the KPP–Fisher Equation in Bounded Domains

The KPP–Fisher equation was proposed by R. A. Fisher as a model to describe the propagation of advantageous genes. Subsequently, it was studied rigorously by Kolmogorov, Petrovskii, and Piskunov. In this paper, we study the dynamics of the KPP–Fisher equation in bounded domains by giving bounds on its solution. The bounding functions satisfy nonlinear equations which are linearizable to the heat equation. In addition to describing the dynamics of the KPP–Fisher equation, we also recover some previous results concerning its asymptotic behavior. We perform numerical simulations to compare the solution of the Fisher equation and the bounding functions.     

Modeling of water surface profile in subterranean channel by differential quadrature method (DQM)

This study, investigates the hydraulic of flow in a subterranean channel headspring. The continuity and momentum equations of flow in porous media considering real conditions were used and the basic equation of flow in a subterranean channel was resulted. This equation is very similar to the spatially varied flow with increasing discharge. An equation, defining the hydraulic parameters of a subterranean channel section was adopted. Then differential quadrature method (DQM), was applied to the equation of flow in subterranean channel, consequently the water surface profile was resulted. To illustrate the rightness of model, the hydraulic parameters of flow in the Gavgard branch of the Joopar Goharriz Qanat were measured and the water surface profile was determined. This water surface profile was compared to the water surface profile computed by the model, which are in good agreement.     

非线性粘弹性梁的动力学行为

建立了描述受周期荷载作用的均匀粘弹性梁动力学行为的非线性偏微分-积分方程,梁的材料满足Leaderman非线性本构关系,对于两端简支的情形用Galerkin方法进行了2阶截断后,简化为常微分-积分方程,进一步简化为便于进行数值实验的常微分方程,最后用数值方法比较了1阶和2阶截断系统的动力学行为。     

Upper bounds on the entropy of radiation systems

The upper bounds on the entropy of a radiation system confined to a spherical box are calculated in six cases by using the equation of state of radiation in flat spacetime and the equation of state of radiation near black-hole horizon, which was derived by Li and Liu (hereafter the Li-Liu equation). It turns out that the Li-Liu equation does have unique advantage in dealing with the entropy bound of critical self-gravitating radiation systems, while the usual equation of state will result in entropy divergence. In the case of non-self-gravitating radiation systems and non-critical self-gravitating radiation systems, there is no difference in the entropy bounds derived by these two equations of state.     

Explicit Peakon solutions to a family of wave-breaking equations

The singular traveling wave solutions of a general 4-parameter family equation which unifies the Camass-Holm equation, the Degasperis-Procesi equation and the Novikov equation are investigated in this paper. At first, we obtain the explicit peakon solutions for one of its specific case that $a=(p+2)c$, $b=(p+1)c$ and $c=1$, which is referred to a generalized Camassa-Holm-Novikov (CHN) equation, by reducing it to a second-order ordinary differential equation (ODE) and solving its associated first-order integrable ODE. By observing the characteristics of peakon solutions to the CHN equation, we construct the peakon solutions for the general 4-parameter breaking wave equation. It reveals that singularities of the peakon solutions come up only when the solutions attain singular points of the equation, which might be a universal principal for all singular traveling wave solutions for wave breaking equations.