On the Inviscid Limit Problem of the Vorticity Equations for Viscous Incompressible Flows in the Half‐Plane

We consider the Navier‐Stokes equations for viscous incompressible flows in the half‐plane under the no‐slip boundary condition. By using the vorticity formulation we prove the local‐in‐time convergence of the Navier‐Stokes flows to the Euler flows outside a boundary layer and to the Prandtl flows in the boundary layer in the inviscid limit when the initial vorticity is located away from the boundary. © 2014 Wiley Periodicals, Inc.     

The Free-boundary Problem for Gravity-driven Unidirectional Viscous Flows

If a layer of viscous fluid drains steadily under gravity, whilein contact with an upward-moving vertical cylinder of a generalcross section with boundary C_B its velocity w(x, y) satisfiesa Poisson equation w_xx+w_yy = g/v = constant. There are two boundaries,the given curve C_B on which w takes a prescribed constant value,and a free boundary C_p marking the edge of the layer, whoseshape we wish to determine. In order to do this, we need twoboundary conditions on C_F; one is the zero-stress conditionw/n = 0, and we assume that the other is that w is constantaround C_F. The latter condition is shown to be equivalent toa requirement that the volume flux in the layer is maximal.The properties of the resulting free-boundary problem are discussed,and numerical solutions obtained for some special cases. Forexample, a solution for the case when C_B is a 270? corner showsthat the layer thickness at the corner is reduced to 76% ofthe thickness on the flat part of the boundary. The presentanalysis is relevant to industrial coating problems, such asedge effects in continuous galvanizing of sheet steel.     

A New Viscous Regularization of the Riemann Problem for Burgers' Equation

This paper gives a new viscous regularization of the Riemann problem for Burgers' equation u_t + (\frac{u²}{2})_z = 0 with Riemann initial data u = u_(x ≤ 0), u = u_+(x > 0} at t = 0. The regularization is given by u_t + (\frac{u²}{2})_z = εe^tu_{zz} with appropriate initial data. The method is different from the classical method, through comparison of three viscous equations of it. Here it is also shown that the difference of the three regularizations approaches zero in appropriate integral norms depending on the data as ε → 0_+ for any given T > 0.     

Feedback Optimal Control Problem for a Network Model of Viscous Fluid Flows

Mathematical Notes - We study a feedback optimal control problem for a three-dimensional model of a stationary flow of a non-Newtonian fluid (with variable viscosity) in a pipeline network with...     

Comparison of Inviscid and Viscous Two‐Phase Calculations of Cavitating Pump Flow

In cavitating flows there is a strong interaction between the fine dispersed vapor bubbles and turbulence. Therefore in two‐phase flow calculations the prediction of turbulence is a matter of great difficulties and uncertainties. To get an idea of the influence of turbulence modelling on the calculated result, viscous and inviscid two‐phase calculations of cavitating pump flow were performed. In the inviscid calculations the influence of cavitation is isolated from turbulence effects. In the viscous calculations the effect of turbulence is modelled with a k – ϵ turbulence model. The results show that the influence of viscous effects on the flow field is weak in comparison to cavitation. However, in contrast to the steady cavitation behaviour predicted by the viscous calculations, the inviscid calculations show unsteady behaviour of the cavitation (as can be seen in the experiment).     

求解超声速无粘绕流的杂交型有限元格式

本文从一维双曲型标量方程出发,以一个普通二阶有限元格式及由其单边对角化导出的一阶单调型格式为基础,构造出一种具有单调性的杂交型有限元格式.为了向二维Euler方程组情形推广,所采用的开关函数是基于流场梯度的局部函数,并专门考虑了相邻单元的影响.二维情形的算例表明新格式可以明显抑制激波附近的振荡.     

A Series Solution of the Unsteady Von Kármán Swirling Viscous Flows

A new analytic technique is applied to solve the unsteady viscous flow due to an infinite rotating disk, governed by a set of two fully coupled nonlinear partial differential equations deduced directly from the exact Navier-Stokes equations. The system of coupled nonlinear partial differential equations is replaced by a sequence of uncoupled systems of linear ordinary differential equations. Different from all other previous analytic results, our series solution is accurate and valid for all time in the whole spatial region. Accurate expressions for skin friction coefficients are given, which are valid for all time. Such kind of series solutions have not been reported, to the best of our knowledge.      

无穷直线上的Riemann边值问题解的稳定性

讨论了无穷直线X上的R iem ann边值问题[1]的解当X轴发生光滑摄动时解的存在性和稳定性问题,并给出了相应的误差估计.     

On the Rayleigh-Taylor Instability for Two Uniform Viscous Incompressible Flows

The authors study the Rayleigh-Taylor instability for two incompressible immis- cible fluids with or without surface tension, evolving with a free interface in the presence of a uniform gravitational field in Eulerian coordinates. To deal with the free surface, instead of using the transformation to Lagrangian coordinates, the perturbed equations in Eule- rian coordinates are transformed to an integral form and the two-fluid flow is formulated as a single-fluid flow in a fixed domain, thus offering an alternative approach to deal with the jump conditions at the free interface. First, the linearized problem around the steady state which describes a denser immiscible fluid lying above a light one with a free interface separating the two fluids, both fluids being in （unstable） equilibrium is analyzed. By a general method of studying a family of modes, the smooth （when restricted to each fluid domain） solutions to the linearized problem that grow exponentially fast in time in Sobolev spaces are constructed, thus leading to a global instability result for the linearized problem. Then, by using these pathological solutions, the global instability for the corresponding nonlinear problem in an appropriate sense is demonstrated.     

Derivation of Inviscid Quasi-geostrophic Equation from Rotational Compressible Magnetohydrodynamic Flows

In this paper, we consider the compressible models of magnetohydrodynamic flows giving rise to a variety of mathematical problems in many areas. We derive a rigorous quasi-geostrophic equation governed by magnetic field from the rotational compressible magnetohydrodynamic flows with the well-prepared initial data. It is a first derivation of quasi-geostrophic equation governed by the magnetic field, and the tool is based on the relative entropy method. This paper covers two results: the existence of the unique local strong solution of quasi-geostrophic equation with the good regularity and the derivation of a quasi-geostrophic equation.     

初-边值问题驻波解的渐近稳定性

本文考虑一带有人工粘性的二维定常等熵无旋平面流方程组的初-边值问题. 在一定的假设下,我们证明其驻波解是渐近稳定的.     

非线性退化波方程的Riemann问题

研究了弹性力学中一退化波方程的Riemann问题．其应力函数非凸非凹,从而使得激波条件退化．通过引入广义激波条件下的退化激波,构造性地得到了各种情形下Riemann问题的整体解．     

The Numerical Calculation of Viscous Stratified Flows

The calculation of steady low Reynolds number flows with strongstable thermal stratification is analysed. It is shown how thebehaviour of an iterative method depends on the Rayleigh number.Time dependent calculations are also considered, and an apparentlynew time step limitation is derived. It is shown that the iterativemethod is more efficient than the time dependent calculationas a means of finding the steady state.     

Monotone Mappings and Flows of Viscous Media

We establish solvability of the boundary-value problems describing stationary and periodic flows of viscoplastic media. In the case of stationary flows we study the question of convergence of the Galerkin method. For the problem of periodic flows we prove a version of the second Bogolyubov theorem.     

黎曼曲面上Riemann边值问题的一点注记

本文给出了紧黎曼曲面上关于Ｒｉｅｍａｎｎ边值问题的Ａｂｅｌ定理，由此定理可得经典Ａｂｅｌ定理，并且解决了非紧黎曼曲面上关于Ｒｉｅｍａｎｎ边值问题的ＣｏｕｓｉｎＩ，ＩＩ问题。     

Two-Dimensional Riemann Problem for Scalar Conservation Laws

Using the generalized characteristic analysis method, we study the two-dimensional Riemann problem for scalar conservation laws, which is nonconvex along the y direction, and interactions of its elementary waves, give the classification of initial discontinuities and construct all Riemann solutions, which Riemann data are two or three pieces of constants. All kinds of Guckenheimer structure appear in the solutions and the necessary and sufficient condition of appearance of it is given.     

Riemann问题的间断有限元

用时空全离散间断零次有限元对Riemarm问题进行了数值求解，没有出现振荡，很好的模拟了稀疏波的逐渐稀疏化和激波的剧烈变化。     

气体动力学燃烧模型的广义Riemann问题

考察了在(x,t)平面上原点(t＞0)的邻域内气体动力学燃烧模型的广义Riemann问题．在改进的熵条件下构造了此问题的唯一解．它们是自相似ZND燃烧模型的极限．发现对某些情形,广义Riemann问题的解与相应的Riemann问题的解有本质的不同．特别地,扰动会使得相应Riemann问题的强爆轰波转化为由预压激波点燃的弱爆燃波．在一些情形,尽管相应的Riemann解中不含燃烧波,扰动后燃烧波会出现．这反映了未燃气体的不稳定性．