磁场微极流方程组弱解的正则性准则

本文研究了三维空间中磁场微极流方程组弱解的正则性准则问题.利用能量估计的方法证明了如果速度场以及磁场满足一定的条件,则弱解在(0,T]是唯一的强解.     

非均匀温度影响下格栅夹芯结构微极梁等效方法

通过胞元能量等效的方法,将格栅夹芯结构等效为连续的微极弹性材料,得到了等效微极弹性材料的本构关系.利用几何关系与平衡条件建立了微极梁受热变形的控制方程组,给出了微极梁位移随温度载荷变化的表达式.通过对比等效微极梁模型、夹层梁模型和ANSYS有限元软件计算的非均匀温度影响下悬臂格栅夹层梁受热弯曲变形的数值结果,验证了微极弹性等效的有效性.结果表明,将不连续的格栅夹芯结构等效为连续介质构成的模型时,由于约束的增加、自由度的减少,需要更多的应力、应变参量来描述其非局部的特性.     

微极流体润滑在径向轴承中应用

本文从微极流体场方程出发,在润滑层的通常假设下,把它化简为两个独立的常微分方程组,并求得速度、微转动角速度的解析表达式.推导了微极流体润滑的雷诺方程,把它应用于有限长径向轴承的求解.通过数值计算得到了微极效应对各种动力参数、几何参数下轴承的压力分布、承载力、流量系数和摩擦系数的影响,并析了它的实际意义,使微极流体理论应用到工程问题又接近了一步.     

格栅夹层梁热弯曲的等效微极热弹性分析

将格栅夹层梁热弯曲等效为微极热弹性梁的受热变形,利用平面微极热弹性理论建立了微极梁受热变形的控制方程组,给出了温度载荷下微极梁的位移表达式.通过胞元能量等效的方法,得到了研究的格栅夹层梁等效微极热弹性梁材料参数.对比了等效微极梁模型和ANSYS有限元软件计算得到的温度载荷下悬臂格栅夹层梁受热弯曲变形的数值结果,两种方法得到的结果非常接近,证明了微极热弹性梁是一种简单有效的模拟格栅夹层梁热变形的等效模型.     

微极流体蠕动泵经由滑移边界管道输送的Stokes流动

计及管道边界条件滑移的影响,研究微极流体蠕动泵,经由圆柱形管道输运的Stokes流动.壁面运动的控制方程为正弦波方程.使用润滑理论,得到了轴向速度、微转动向量、流函数、压力梯度、摩擦力和机械效率的解析数值解.用图形表示出构成参数,如像耦合参数、微极参数和表征蠕流泵特性的滑移参数、摩擦力和俘获现象的影响.数值计算表明,当耦合参数较大时,需要蠕动泵的压力更大,而微极参数和滑移参数正相反.俘获团块的大小随耦合参数和微极参数的减小而缩小,而随滑移参数的增大而缩小.     

可压缩流方程组的大范围解和渐近展开

近年来,对数学物理方程中含有大参数的奇异情况进行了一系列的研究。 [1]—[4]引入了“平衡能量”的概念和带权模的技巧研究了可压缩流方程组及磁流体力学方程组Cauchy问题的奇异极限,得到了局部可微解的存在和唯一性定理。 [5]—[8]利用各种不同的方法克服了边界区域能量估计的困难,研究了大参数可压缩流初边值问题的奇异极限,得到了相应的结果。     

磁微极流体方程组在临界Sobolev空间强解的存在性

在临界Sobolev空间H~(1/2)(R~3)中,本文研究了三维不可压磁微极流体方程组的适定性.设(u_0,ω_0,b_0)是H~(1/2)(R~3)中的小初值,则三维不可压磁微极流体方程组存在唯一整体强解(u,ω,b)∈C([0,+∞);H~(1/2)(R~3))∩L~2((0,+∞);H~(3/2)(R~3))∩L~4((0,+∞);H~1(R~3));设大初值(u_0,ω_0,b_0)∈H~(1/2)(R~3),则存在一个正的时间T=T(u_0,ω_0,b_0)使得三维不可压磁微极流体方程组在[0,T]内存在唯一局部强解(u,ω,b)∈C([0,T];H~(1/2)(R~3))∩L~2((0,T];H~(3/2)(R~3))∩L~4((0,T];H~1(R~3)),这些改进了Yuan J的结果(Existence theorem and blow-up criterion of the strong solutions to the magnetomicropolar fluid equations,Math.Methods Appl.Sci.,31(2008),1113-1130).     

回归模型参数的距离估计方法

本从二次可积函数类出发,设计了函数或向量函数的距离,导出了可 微函数方程或方程组的d解,利用d解给出可微函数方程或方程组的回归模型参数的距离估计式。     

运动气流的二维激波动力学方程组

本文把原来适用于波前为静止气体的激波动力学方法,推广到波前为运动气流的情况中。导出了以激波马赫数和波面方向角表示的波前为均匀流的二维激波动力学方程组和波前为非均匀流的二维激波动力学方程组。文中还简单介绍了运动气流的激波动力学方程组在“双波干扰”中的应用。     

一类交叉耦合非线性反应扩散方程组的爆破分析

主要研究了具有混合型的多重非线性项的抛物方程组的初边值问题.方程组中的非线性项是幂函数和指数混合型的.这些非线性项组合出了源-流交叉耦合,通过比较原理得到了方程组的上下解,并得到了解有限时刻爆破的临界指标.     

Approximation of the incompressible non‐Newtonian fluid equations by the artificial compressibility method

This paper studies the approximation of the non‐Newtonian fluid equations by the artificial compressibility method. We first introduce a family of perturbed compressible non‐Newtonian fluid equations (depending on a positive parameter ε) that approximates the incompressible equations as ε → 0⁺. Then, we prove the unique existence and convergence of solutions for the compressible equations to the solutions of the incompressible equations. Copyright © 2012 John Wiley & Sons, Ltd.     

On the regularity of weak solutions to the magnetohydrodynamic equations

In this paper, we study the regularity of weak solution to the incompressible magnetohydrodynamic equations. We obtain some sufficient conditions for regularity of weak solutions to the magnetohydrodynamic equations, which is similar to that of incompressible Navier-Stokes equations. Moreover, our results demonstrate that the velocity field of the fluid plays a more dominant role than the magnetic field does on the regularity of solution to the magneto-hydrodynamic equations.     

Navier-Stokes方程五模类Lorenz方程组的动力学行为及数值仿真

本文对平面正方形区域上不可压缩的Navier-Stokes方程,进行傅立叶展开后,截断得到五模类Lorenz方程组.给出了该方程组定常解及其稳定性的讨论,证明了该方程组吸引子的存在性,并对其全局稳定性进行了分析和讨论,数值模拟了雷诺数在一定范围内变化时,类Lorenz方程组的动力学行为.     

非定常的热传导──对流问题的混合有限元法

1．引言设oCRZ是足够光滑的有界区域，考虑非定常的、无量纲化的，而且带有热传导的粘性不可压缩流体力学运动问题：问题（I）．求。＝（。1，。2），p，T满足；其中。是流体的速度向量，P为压力，T是温度，。＞0是运动粘性系数，入＞0是GroshoffM，j＝（0，1）是M维向量。x二hi，x。）·当温度T是常数时，问题（I）变为Navier－StokesIW题，而当！是常数时，问题（I）变为定常问题．到目前为止，对问题（I）的研究尚不多，只给出了一些计算方法（见11－4］等），对于有限元解的误差分析就更少．1994年，沈树民在问中首先对定常的问…     

One method for constructing exact solutions of equations of two-dimensional hydrodynamics of an incompressible fluid

We propose a simple algebraic method for constructing exact solutions of equations of two-dimensional hydrodynamics of an incompressible fluid. The problem reduces to consecutively solving three linear partial differential equations for a nonviscous fluid and to solving three linear partial differential equations and one first-order ordinary differential equation for a viscous fluid. __________ Translated from Teoreticheskaya i Matematicheskaya Fizika, Vol. 147,No. 1, pp. 64–72, April, 2006.     

Nonlinear Stationary Surface Waves Above an Underwater Ridge

Given an ideal incompressible heavy irrotational fluid, we consider the exact statement of the problem on gravitational-capillary surface waves of small amplitude travelling along an underwater ridge. We show that, under some requirements on the shape of the bottom and the surface tension, the equations of an ideal incompressible fluid have smooth solutions periodic in the variable directed along the underwater ridge and decreasing exponentially with a small positive exponent in the perpendicular direction.     

Well-posedness of the free-surface incompressible Euler equations with or without surface tension

We provide a new method for treating free boundary problems in perfect fluids, and prove local-in-time well-posedness in Sobolev spaces for the free-surface incompressible 3D Euler equations with or without surface tension for arbitrary initial data, and without any irrotationality assumption on the fluid. This is a free boundary problem for the motion of an incompressible perfect liquid in vacuum, wherein the motion of the fluid interacts with the motion of the free-surface at highest-order.

     

Equivalence transformations of the Clebsch equations

We consider the Clebsch equations describing the motion of an ideal incompressible fluid in the absence of mass forces. These equations contain an arbitrary element, namely a function of three variables. We find the equivalence transformations of the variables which act on the arbitrary element and preserve the structure of the equations. The equivalence transformation is pointed out that takes the arbitrary element to zero. Some examples are given.     

Strong solutions to the equations of electrically conductive magnetic fluids

We study the equations of flow of an electrically conductive magnetic fluid, when the fluid is subjected to the action of an external applied magnetic field. The system is formed by the incompressible Navier–Stokes equations, the magnetization relaxation equation of Bloch type and the magnetic induction equation. The system takes into account the Kelvin and Lorentz force densities. We prove the local-in-time existence of the unique strong solution to the system equipped with initial and boundary conditions. We also establish a blow-up criterion for the local strong solution.     

On the thermodynamics of fluids defined by implicit constitutive relations

In this paper, we develop a thermodynamically consistent theory for describing the response of nonlinear viscous fluids whose constitutive equations are of the form f (T, D) = 0. We show that such constitutive equations which include classical constitutive equations wherein the stress is expressed explicitly in terms of the kinematical quantities, provide a rich class of physically meaningful fluid response functions which allows us to describe a wider range of material behavior, including that of a general class of incompressible fluids, incompressible fluids with pressure dependent viscosity, and Bingham (or pseudoplastic) materials.