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1.
1.IntroductionConsiderthefollowinghomogeneous2-DincompressibleNavier-Stokesequations:whereV=(VI(t,x),VZ(t,x))isthevelocityofthefluid,Pisthescalarpressure,V'V=V101 V202,andtheconstantu>0isthekineticviscosityofthefluid(whenu=0,thissystemiscalledEulerequations,andwedenoteitby(1.1)).Byactingtheoperationofcurlon(1.1),wecanobtaintheevolutionequationforvorticityw=(a1VZ--02VI).Itisthevorticity-streamformof(1.1)(whenu=0,wedenoteitby(1.2)).For(1.1),in[4],R.DipernaandA.Majdaprovedtheglobalexiste…  相似文献   

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Consider the Cauchy problem for the n-dimensional incompressible NavierStokes equations:??tu-α△u+(u·?)u+?p = f(x, t), with the initial condition u(x, 0) = u0(x) and with the incompressible conditions ? · u = 0, ? · f = 0 and ? · u0= 0. The spatial dimension n ≥ 2.Suppose that the initial function u0∈ L1(Rn) ∩ L2(Rn) and the external force f ∈ L1(Rn× R+) ∩ L1(R+, L2(Rn)). It is well known that there holds the decay estimate with sharp rate:(1 + t)1+n/2∫Rn|u(x, t)|2 dx ≤ C, for all time t 0, where the dimension n ≥ 2, C 0 is a positive constant, independent of u and(x, t).The main purpose of this paper is to provide two independent proofs of the decay estimate with sharp rate, both are complete, systematic, simplified proofs, under a weaker condition on the external force. The ideas and methods introduced in this paper may have strong influence on the decay estimates with sharp rates of the global weak solutions or the global smooth solutions of similar equations, such as the n-dimensional magnetohydrodynamics equations, where the dimension n ≥ 2.  相似文献   

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用区域分解法求不可压N-S方程的差分解   总被引:1,自引:0,他引:1  
黄兰洁 《计算数学》1992,14(4):433-445
§1.引言 对不可压小粘性流的数值解,[1]和[2]用奇异摄动观点提出了一个区域分解法.从常微分方程(组)的奇异摄动问题出发,解分解为外部解加边界修正解(以下简称为修正解).外部解的边界条件有:给定(原边界条件)、待定(用原边界条件和修正解)和延拓类.修正解的边界条件有:给定(用原边界条件和外部解延拓)渐近(在边界层外缘)和待定  相似文献   

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In this article, we show large time behavior of weak solutions to the Cauchy problem of the Navier-Stokes equations with damping α|u|β-1u (α0).  相似文献   

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In this paper we study a generalization of self-similar solutions. We show that just as for the solutions to the Navier-Stokes equations these supposedly singular solution reduce to the zero solution.In this paper we study a generalization of self-similar solutions. We show that just as for the solutions to the Navier-Stokes equations these supposedly singular solution reduce to the zero solution.  相似文献   

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1. IntroductionLet us consider the unsteady incompressible Navier--Stokes equatinns (qSE)on a twedimensional reginn n with boundary On. Here w is the velocity vector; interms of its Caxtesian,components w = (u, v)"; p is the Pressure. The initial conditionis given assatisheng (1.2). We are concerned mainly with the solid wall boundary conditiollbut we will also briefly discuss the outflow boundary conditinn. Note the convectionterm can ajBo be written in conservative form (w' glad)w = div(…  相似文献   

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不可压Navier-Stokes方程的隐式投影法   总被引:3,自引:1,他引:2  
起的解的小尺度以外,还有解的约束条件,即(1.1)。为了分辨小尺度,需用足够小的网格;而为了保证计算效率,时间步△_t需适当地大,从而必须用隐式格式。但是,由于解的约束条件,隐式格式的实现有困难,为此可用所谓的投影法,如[1]-[3]。前两者基于全隐式或Crank-Nicholson(CN)隐式和所谓的全投影;后者基于CN和压力修正投影。当然可以同时迭代u,v,p而得出每时间层的解,如[4]中的Peyret以及[5]中的Spolding-  相似文献   

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鞠立力  张林波 《计算数学》1998,20(3):325-336
1.CNMTZ格式和压力Poisson、方程的快速解法为后面讨论的方便,本节中我们简要介绍一下[1,2]提出的求解上述方程的CNMTZ算法以及相应的压力Poisson方程的快速算法.考虑原始变量非定常不可压N—S方程(INSE)和满足方程(2的初始条件W(;队0),W在边界*0上给定并满足这里,V=(。,V厂是速度场,p是压力.方程(1)(2)进行空间离散后可以写成以下形式:其中力(W,t)包括动量方程中的对流项、扩散项和非齐次项的空间差分近似及相应的边界条件,G和D分别为梯度和散度算子的离散形式.它的CNMT格式的PC投影法如下:其…  相似文献   

14.
Navier-Stokes方程的非奇异解分支的谱Galerkin逼近   总被引:3,自引:0,他引:3  
No error estimate of the spectral Galerkin approximation for the steady-state Navier-Stokes equations was given without assuming that the data of the externalforce field and the boundary conditions are small enough. In this paper, under the condition that the solutions of the Navier-Stokes equations are nonsingular,we proved the existence and convergence of the spectral Galerkin approximation solutions and gave the error estimate. At last, this approximation method wasapplied to simulate the spherical Couette flow.  相似文献   

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This paper studies a two-dimensional modified Navier-stokes equations. The author shows the existence and uniqueness of weak solutions for this equation by Galerkin method in bounded domains. The result is further extended to the case of unbounded channel-like domains.  相似文献   

16.
The compressible Navier-Stokes equations driven by a time-periodic external force are considered in this article. We establish the existence of weak time-periodic solutions and improve the result from [3] in the following sense: we extend the class of pressure functions, that is, we consider lower exponent γ.  相似文献   

17.
具有无界时滞的微分方程解的振动性   总被引:3,自引:0,他引:3  
具有无界时滞的微分方程解的振动性刘正荣(云南大学数学系和云南省应用数学研究所,昆明650091)俞元洪(中国科学院应用数学研究所,北京100080)基金项目:国家自然科学基金资助项目1992年3月25日收到.一、引言考虑泛函微分方程i=1其中,.关于...  相似文献   

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1引言不可压Navier-Stokes方程作为流体力学的基本方程,其数值计算一直是科学与工程计算关心的问题.本文考虑定常问题: -ε△u (u·▽)u ▽p = f x∈Ω,▽·u=0 x∈Ω, (1) u =0 x∈(?)Ω.这里ε=1/Re是Reynolds数的倒数,u=(u1,u2,…,ud)为待求流速场,p是待求压力场,f=(f1,f2,…,fd)是给定的体力.Ωv(?) Rd(d=2,3)是有界区域,且具有分片Lipschitz连续边界(?)Ω.  相似文献   

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成圣江 《计算数学》1984,6(1):63-69
定常不可压流体的Navier-Stokes方程有限元解要想获得收敛速度是H~1模以h~2阶收敛于0,必须使用二阶近似有限元子空间X_h~((2))×M_h~((2)[2]),这就要求解对应于这一有限元子空间的非线性方程组。直接求解这一方程组工作量很大。根据[1]所提出的加速收敛方法,先用一阶近似有限元子空间X~_h((1))×M_h~((1)[2])求得初次近似u_h,它按H~1模以h一次幂收敛于0,然后以u_h代入Navier-Stokes方程中的迁移项,将它化成Stokes方程。对这一线性方程的对应变分形式,采用密网格的有限元子空同X'_h~((1))×M'_h~((1)),求得第二次近似u_h,它按H~1模以h~2阶速度收敛于真解。最后讨论了非线性迭代过程与精确化之间的关系。  相似文献   

20.
We give blow-up criteria of strong solutions of Navier-Stokes equations with its initial data in Besov spaces and consider the regularity of Leray-Hopf solutions of the equation.  相似文献   

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