非定常修正下平面Poiseuille流动的线性稳定性性质

本文在文[1]的基础上,用多重尺度法进一步研究了在非定常修正剖面作用下平面Poiseuille流动的线性稳定性性质,发现文[1]所给出的修正剖面在扰动发展的初期,在一定条件下会促进扰动的发展,从而增大流动失稳的可能性.     

修正多重尺度法在求解圆簿板具有很大挠度问题时的应用*

本文利用修正的多重尺度法[1～2]重新研究固支圆薄板在均匀压力作用下,挠度很大时解的渐近性态.结果表明与钱伟长教授用首创的合成展开法求解该问题[3]的结果相一致,但较后者更简捷.本文结果还表明文[4]中所指出文[1～2]方法的局限性是非本质的,并改正文[3]中一些计算错误.     

经过修正的平面Couette流的非线性稳定性研究

本文讨论了经过修正的平面Couette流在二维扰动下的非线性稳定性性质,并同经过修正的平面Poiseuille流的非线性稳定性性质进行了比较.计算结果表明,对于有限振幅的扰动,平面Couette流比平面Poiseulle流更不稳定.     

边界层型问题的插值摄动解法

本文在文[1]的基础上用插值摄动法研究了最高阶导数乘以小参数的二阶常微分方程的定解问题。算例表明,本文方法计算过程简单,其精度甚至比多重尺度法的一级近似结果的精度还稍高一些。     

经过修正的层次流流动的流动稳定性问题(Ⅱ)——经过修正的平行剪切流的线性稳定性研究

本文根据文[1]给出的经过修正的层流流动的流动稳定性理论及平行剪切流中平均速度的一类修正剖面,研究了平行剪切流的线性稳定性性质,对于平面Couette流动和圆管Poiseuill流动,首次得到了二维扰动和轴对称扰动也能造成失稳的结果,并给出了这两种流动在某种定义下的中性曲线.     

自治系统的不稳定定理及其应用

本文建立了一个关于自治系统(2.1)的未被扰动运动为不稳定的定理,它是Красовский在文[2]中建立的不稳定定理的推广。运用这个定理,本文讨论了两个三阶非线性系统未被扰动运动为不稳定的条件,对文[3]中给出的零解不稳定条件进行了改进。     

角域上边界有限元的多重校正法

有关有限元法的校正技术,文[1]林群、杨一都作了较为系统的综述。文[2]林群、周爱辉提出了几个算子相乘的观点,并对二维一次有限元作了三重校正。文[3]朱起定等对两点边值问题和带光滑核边界积分方程的有限元解给出了多重校正公式。从理论上讲,这些问题可以任意次校正。然而,对多角形域上边界积分方程,由于角点的存在,解函数在角点有奇性,文[3]的方法失效。本文采用局部加密网格方法,对角域上边界有限元给出了多重校正公式。本文采用的符号同文[4]。     

在集中力和集中力偶作用下不同弹性材料圆形界面的裂纹问题

运用推广的Schwarz延拓原理结合对复应力函数的奇性主部分析,求解一类有集中荷载的平面弹性问题,十分有效。文[1]用此方法研究了同种材料的弹性问题。本文把它推广于在集中力和集中力偶作用下不同弹性材料的圆形界面上有多条裂纹的情形,求出了几种典型情况复应力函数的封闭解,算出了应力强度因子,并由此导出一系列特殊解答,其中两个在文[1]、[6]中找到一致结果。     

LAPLACE-STIELTJES变换所定义的函数在收敛半平面的零(R)级

文[5]以文[4]等为基础研究了 Dirichlet 级数在右半平面内的(R)级。文[6]进一步定义了零(R)级.文[7]又研究了准确零(R)级.本文在文[2]的基础上,引进 Laplace—Stieltjes 变换所定义的函数在收敛半平面零(R)级的概念,并得到了一些相应结果。考虑 Laplace—Stieltjes 变换所定义的函数     

对一个几何不等式的探究

文 [1 ]～ [3]先后用复数方法和三角方法证明了如下一个漂亮的几何不等式 :设 a,b,c分别表示△ ABC的三边 BC,CA,AB的长 ,则对△ ABC所在平面上的任意两点 P,Q,恒有a PA.QA+ b PB.QB+ c PC.QC≥ abc ( 1 )文 [2 ]作者特别指出 :不等式 ( 1 )难度较大 ,至今尚未找到其纯几何证法 .而且文 [1 ]～ [3]均未论及 ( 1 )式取等号的条件 .本文首先给出不等式 ( 1 )的两个纯几何证法 ,顺便引出 ( 1 )式取等号的条件 ,然后再由 ( 1 )式导出三角形中的几个新颖的不等式 .为方便叙述 ( 1 )式取等号的条件 ,我们需用到等角共轭点的概念 [4] :…     

Use of Adomian decomposition method in the study of parallel plate flow of a third grade fluid

In this paper, Adomian’s decomposition method is used to solve non-linear differential equations which arise in fluid dynamics. We study basic flow problems of a third grade non-Newtonian fluid between two parallel plates separated by a finite distance. The technique of Adomian decomposition is successfully applied to study the problem of a non-Newtonian plane Couette flow, fully developed plane Poiseuille flow and plane Couette–Poiseuille flow. The results obtained show the reliability and efficiency of this analytical method. Numerical solutions are also obtained by solving non-linear ordinary differential equations using Chebyshev spectral method. We present a comparative study between the analytical solutions and numerical solutions. The analytical results are found to be in good agreement with numerical solutions which reveals the effectiveness and convenience of the Adomian decomposition method.     

Stability analysis of the plane Couette flow for a model kinetic equation

The stability of the plane Couette flow is studied using the simplified Boltzmann equation (the BGK equation) in which the high modes in the space of velocities and coordinates are truncated. The solution to the Navier-Stokes equation with small additional terms depending on the Knudsen number is used as the stationary solution. We assume that the perturbations depend only on the coordinate that is orthogonal to the flow. The density perturbations are assumed to be nonzero. In this approximation, the problem is found to be unstable in the case of small Knudsen numbers.     

Stability of oscillatory two-phase Couette flow

The authors investigate the stability of two-phase Couette flowof different liquids bounded between plane parallel plates.One of the plates has a time-dependent velocity in its own plane,which is composed of a constant steady part and a time-harmoniccomponent. In the absence of time-harmonic modulations, theflow can be unstable to an interfacial instability if the viscositiesare different, and the more viscous fluid occupies the thinnerof the two layers. Using Floquet theory, it is shown analyticallyin the limit of long waves that time-periodic modulations inthe basic flow can have a significant influence on flow stability.In particular, flows which are otherwise unstable for extensiveranges of viscosity ratios can be stabilized completely by theinclusion of background modulations, a finding that can haveuseful consequences in many practical applications.     

Observations on the Role of Vorticity in the Stability Theory of Wall Bounded Flows

The linearized equations for the evolution of disturbances to four wall bounded flows are treated. The flows are plane Couette flow and plane Poiseuille flow, Hagen-Poiseuille pipe flow, and the asymptotic suction profile. By looking at the vorticity it is proved simply that plane Couette flow and Hagen-Poiseuille flow are linearly stable. Further study is made of the structure of the disturbance equation by the introduction of a special vorticity adjoint.     

On generalised MHD couette flow with heat transfer

In the case of short-circuited generalised MHD Couette flow the rate of heat transfer, in general, increases with the increase in the value of both the Hartmann number and the pressure gradient. Especially, at the lower stationary plate it is affected by the magnetic field, which is not observed in the case of plane MHD Couette flow.     

球Couette流的数值模拟

该文利用谱方法对同心旋转球间轴对称Couette流进行数值模拟.给出Navier Stokes方程的流函数涡度形式,利用Stokes流把边界条件齐次化, 选取Stokes算子的特征函数做为逼近子空间的基函数,对同心旋转球间轴对称Couette流进行谱逼近     

A Distribution- Theoretic Approach to a Stability Problem of Orr

In a classic paper [1] of 1907, W. M'Farr Orr discovered, among other things, the “infinitesimal” instability of inviscid plane Couette flow. Surprisingly, although Orr's paper remains a standard reference in the field, later investigators [2, 3] have been able to call inviscid plane Couette flow stable without finding it necessary to controvert Orr's result. What has happened is that, at least in problems governed by linear (or linearized) equations with time-independent coefficients, the term “instability” has come to be identified with the presence of solutions exhibiting exponential time-growth. Orr found instability indeed: a class of solutions certain members of which grow in time by more than each preassigned factor. Unlike the exponential instabilities, however, Orr's solutions die away like 1/t after achieving their greatest growth. This ephemerality probably accounts for the discounting of Orr's result. Orr did not look into the general initial value problem. This is done in the sequel, with the result that the situation becomes clear. Under general disturbances, Couette flow turns out to be neither stable nor quasi-asymptotically stable*. The rate of growth depends on the smoothness of the initial data: classical solutions grow no faster than t, but sufficiently rough distribution-valued initial data leads to growth matching any power of t. Before presenting detailed results, we briefly review Orr's fundamental work on the problem.     

The resolvent technique for investigating the stability of plane Couette flow: Bounds for the pressure terms

We derive bounds for the pressure terms of the operator used to prove nonlinear stability of plane Couette flow through the resolvent technique.