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1.
0.引 言 我们知道TVD格式能高效地捕捉激波,特别是在激波附近解不发生振荡,因此在流体力学数值计算中得到了广泛的应用.但在 1985年,J.Goodman和 R.Leveque证明了二维守恒型 TVD格式至多是一阶精度格式[6],而 MmB格式[1]的提出使构造二维高精度格式有了新的突破.另外,在传统理论下,差分格式的熵条件是很难证明的.文[2]提出了在多维空间变量下的高精度差分格式下收敛性的一般方法.证明中只须假设格式解的一致l∞估计和空间离散熵的弱估计,然后运用 Diperna的唯一性定理[5]…  相似文献   

2.
提高变型标准遗传算法收敛速度的混合法及其推广   总被引:1,自引:0,他引:1  
针对即使是全局收敛的变型标准遗传算法VCGA[1]有时也会发生收敛速度变慢的问题,提出了VCGA和最陡下降法相结合的混合法HVCSDA.该方法增强了VCGA在接近全局最优解时的微调能力.还将HVCSDA推广到一类修正的VCGA上.仿真实例表明了HVCSDA及其推广能有效地提高收敛速度.对30城市TSP的仿真结果为6.822,要好于用TABU得到的6.99的结果[6].  相似文献   

3.
徐川育 《信息与控制》1997,26(4):266-271
针对即使是全局收敛的变型标准遗传算法VCGA^[1]有时也会发生收敛速度变慢的问题,提出了VCGA和最陡下降法相结合的混合法HVCSDA。该方法增强了VCGA在接近全局最优解时的微调能力。还将HVCSDA推广到一类修正的VCGA上。仿真实例表明了HVCSDA及其推广能的效地提高收敛速度。对30城市TSP的仿真结果为6.822,要好于用TABU得到的6.99的结果[6]  相似文献   

4.
在UCDOS3.1的软件中提供了随机抓取VGA/TVGA图像的功能,但是,实际的使用效果不佳,对256色的VGA/TVGA图像,UCDOS3.1不能正确随机抓取。本文首先提出了一种有效地确定VGA/TVGA图像素存放方式的方法,然后介绍了随机抓取VGA/TVGA图像的技术,最后简单讨论了VGA/TVGA的图像特性。  相似文献   

5.
对流占优扩散问题的并行计算   总被引:1,自引:0,他引:1  
1.引言 在刻画流体运动的某些物理现象,以及研究热的传导、粒子的扩散等问题时,都会归结到求解对流扩散方程.用有限差分方法求解该方程,若采用显式方法,计算格式简单,但它们都是条件稳定的,时间步长必须取得非常小;若采用隐式方法,方法是无条件稳定的,但要解代数方程组,求解比较困难.D.J.EVANS和A.R.AHMAD在文[2]中提出了用显式交替方向法求解定态椭圆型方程,对Laplace方程做了数值实验.本文将这个方法推广到了时间依赖的问题,而且适用于对流占优扩散问题的求解.基于二阶迎风格式[1];本…  相似文献   

6.
《电脑》2002,(2)
ECS精英 K7S6A V1.0X主板最新BIOS 01/15/2002版新增支持 Athlon XP 2000+处理器,增加了 USB唤醒功能,修正了在安装Win98时,USB键盘不能使用热键的问题[182K]ECS精英 P6VXAT V1.0X主板最新 BIOS1.0b版修正了与 Tulatin1.2G CPU的兼容性问题 [202K]下载:www.ecs.com.twAsus华硕P45333主板(无板载网路及声音芯片)最新BIOS 1003C版[179K]华硕A7V266-E/AA主板(无板载网络及声音…  相似文献   

7.
EDSUNIGRAPHICSV10.4最新版本UGV10.4是目前最全面的CAD/CAE/CAM系统.拥有40多个应用软件,并能在各种平台上运行,如HP700系列、VAX和AXP系列、SGI、SUN和IBMRS/600系列的各种机器。与老版本相比,1...  相似文献   

8.
Burgers方程为Navier-Stokes方程组的简化形式,在计算数学和计算流体力学领域中有着广泛应用.本文设计了粘性Burgers方程的高阶精度半隐式加权紧致非线性格式(WCNS),并给出了稳定性分析.方程对流项和粘性项分别采用五阶精度WCNS格式和四阶中心差分格式计算.半离散系统采用三阶精度IMEX Runge...  相似文献   

9.
装机指南     
BlueMaster 《电脑》2002,(2):81-83
元旦都已经过去又好一阵子了,厂商在过年前还都准备再疯狂一把呢!你看这不,AMD推出了 Athlon XP 2000+,而 Intel推出了Northwood 的系列CPU,2.0GHz 和2.2GHz。令人兴奋不已,这只是高端的CPU方面,低端方面有Celeron1.3GHz和Duron1.3GHz的产品,加上新加入的1GHz的VIAC3这片市场里也是被折腾的热气腾腾的。而在其它产品方面nVidia已经放出了GeForce4的消息,而且VIA也已经把KT333的发布日公布于众了,支持 AGP8X,US…  相似文献   

10.
周强  闫大顺 《现代计算机》2000,(89):66-68,75
本文叙述了某合洗厂前配料生产微机监控系统的软、硬件组成及其。该系统采用WindowsGU CK ,ELPHI4.0YMYFA HW ;FCP ET XG KHTKGTT OVRNCAQ FCL RFSYPUGMUJ JQWWAA TGUTJTY  相似文献   

11.
In this paper, a new methodology has been proposed to solve two-dimensional (2D) Navier-Stokes (N-S) equations representing incompressible viscous fluid flows on irregular geometries. It is based on second order compact finite difference discretization of the fourth order streamfunction equation on computational plane. The important advantage of this formulation is not only to overcome the difficulties existing in the velocity-pressure and streamfunction-vorticity formulations, but also for being applicable to complex geometries beyond rectangular. We first apply the proposed scheme to a problem having analytical solution and then to the well-studied benchmark problem (problem of lid-driven cavity flow) in viscous fluid flow. Finally, we demonstrate the robustness of our proposed scheme on flow in a complex domain (e.g. constricted channel and dilated channel). It is seen to efficiently capture steady state solutions of the N-S equations with Dirichlet as well as Neumann boundary conditions. In addition to this, it captures viscous flows involving free and wall bounded shear layers which invariably contain spatial scale variations. Estimates of the error incurred show that the results are very accurate on a coarser grid. The results obtained using this scheme are in excellent agreement with analytical and numerical results whenever available and they clearly demonstrate the superior scale resolution of the proposed scheme.  相似文献   

12.
A new three-dimensional viscous aeroelastic solver is developed in the present work. A well validated full Navier-Stokes code is coupled with a nonlinear finite element plate model. Implicit coupling between the computational fluid dynamics and structural solvers is achieved using a subiteration approach. Computations of several benchmark static and dynamic plate problems are used to validate the finite element portion of the code. This coupled aeroelastic scheme is then applied to the problem of three-dimensional panel flutter. Inviscid and viscous supersonic results match previous computations using the same aerodynamic method coupled with a finite difference structural solver. For the case of subsonic flow, multiple solutions consisting of static, upward and downward deflections of the panel are discussed. The particular solution obtained is shown to be sensitive to the cavity pressure specified underneath the panel.  相似文献   

13.
An explicit-implicit time-dependent finite difference technique is presented which has been successfully implemented for the solution of the unsteady Navier-Stokes equations including multicomponent finite rate chemistry. Stability restrictions encountered in explicit schemes due to the variable relaxation times associated with the finite rate chemical reactions are eliminated. As a result, the stability of the coupled Navier-Stokes and species conservatiion finite difference equations is shown to be governed only by the hydrodynamic stability cri- terion. The viscous nonequilibrium flow about a blunt axisymmetric nosetip at high Mach number and low Reynolds number, where the viscous shock layer and shock transition zone are merged, was computed using this time-dependent numerical scheme. Solutions along the stagnation streamline are compared with corresponding solutions obtained by Dellinger using the thin layer approximation of the Navier-Stokes equations.  相似文献   

14.
This paper presents the development of a 2D high-order solver with spectral difference method for unsteady incompressible Navier-Stokes equations accelerated by a p-multigrid method. This solver is designed for unstructured quadrilateral elements. Time-marching methods cannot be applied directly to incompressible flows because the governing equations are not hyperbolic. An artificial compressibility method (ACM) is employed in order to treat the inviscid fluxes using the traditional characteristics-based schemes. The viscous fluxes are computed using the averaging approach (Sun et al., 2007; Kopriva, 1998) [29] and [12]. A dual time stepping scheme is implemented to deal with physical time marching. A p-multigrid method is implemented (Liang et al., 2009) [16] in conjunction with the dual time stepping method for convergence acceleration. The incompressible SD (ISD) method added with the ACM (SD-ACM) is able to accurately simulate 2D steady and unsteady viscous flows.  相似文献   

15.
A second-order residual-based compact scheme, initially developed for computing flows on Cartesian and curvilinear grids, is extended to general unstructured grids in a finite-volume framework. The scheme is applied to the computation of several inviscid and viscous compressible flows governed by the Euler and Navier-Stokes equations. Its efficiency and accuracy properties are compared with those of conventional second-order upwind schemes based on variable reconstruction.  相似文献   

16.
We propose here a new approach to optimally control incompressible viscous flow past a circular cylinder for drag minimization by rotary oscillation. The flow at Re = 15000 is simulated by solving 2D Navier-Stokes equations in stream function-vorticity formulation. High accuracy compact scheme for space discretization and four stage Runge-Kutta scheme for time integration makes such simulation possible. While numerical solution for this flow field has been reported using a fast viscous-vortex method, to our knowledge, this has not been done at such a high Reynolds number by computing the Navier-Stokes equation before. The importance of scale resolution, aliasing problem and preservation of physical dispersion relation for such vortical flows of the used high accuracy schemes [Sengupta TK. Fundamentals of computational fluid dynamics. Hyderabad, India: University Press; 2004] is highlighted.For the dynamic problem, a novel genetic algorithm (GA) based optimization technique has been adopted, where solutions of Navier-Stokes equations are obtained using small time-horizons at every step of the optimization process, called a GA generation. Then the objective functions is evaluated that is followed by GA determined improvement of the decision variables. This procedure of time advancement can also be adopted to control such flows experimentally, as one obtains time-accurate solution of the Navier-Stokes equation subject to discrete changes of decision variables. The objective function - the time-averaged drag - is optimized using a real-coded genetic algorithm [Deb K. Multi-objective optimization using evolutionary algorithms. Chichester, UK: Wiley; 2001] for the two decision variables, the maximum rotation rate and the forcing frequency of the rotary oscillation. Various approaches to optimal decision variables have been explored for the purpose of drag reduction and the collection of results are self-consistent and furthermore match well with the experimental values reported in [Tokumaru PT, Dimotakis PE. Rotary oscillation control of a cylinder wake. J Fluid Mech 1991;224:77].  相似文献   

17.
A new high spectral accuracy compact difference scheme is proposed here. This has been obtained by constrained optimization of error in spectral space for discretizing first derivative for problems with non-periodic boundary condition. This produces a scheme with the highest spectral accuracy among all known compact schemes, although this is formally only second-order accurate. Solution of Navier-Stokes equation for incompressible flows are reported here using this scheme to solve two fluid flow instability problems that are difficult to solve using explicit schemes. The first problem investigates the effect of wind-shear past bluff-body and the second problem involves predicting a vortex-induced instability.  相似文献   

18.
In this paper we review fourth-order approximations of the biharmonic operator in one, two and three dimensions. In addition, we describe recent developments on second and fourth order finite difference approximations of the two dimensional Navier-Stokes equations. The schemes are compact both for the biharmonic and the Laplacian operators. For the convective term the fourth order scheme invokes also a sixth order Pade approximation for the first order derivatives, using an approximation suggested by Carpenter-Gottlieb-Abarbanel (J. Comput. Phys. 108:272–295, 1993). We also introduce the derivation of a pure streamfunction formulation for the Navier-Stokes equations in three dimensions.  相似文献   

19.
Direct numerical simulations of compressible turbulent flow over wavy wall geometries have been carried out by solving N–S equations on general curvilinear coordinates. A 6th order WENO scheme with minimized dispersion and controllable dissipation is employed to compute the inviscid fluxes, a 4th order central difference scheme is applied to compute the viscous fluxes, and a 6th order conservative compact scheme is used for computing the geometrical metrics. An implicit LU-SGS method is used for time integration to improve computational efficiency over the explicit schemes such as the Runge–Kutta approach. The validity and applicability of the present algorithm is confirmed by comparing our results with laboratory experimental measurements and DNS results in the literature.  相似文献   

20.
This paper deals with the formulation of a higher-order compact (HOC) scheme on non-uniform grids in complex geometries to simulate two-dimensional (2D) steady incompressible viscous flows governed by the Navier-Stokes (N-S) equations. The proposed scheme which is spatially fourth-order accurate is then tested on three nonlinear problems, namely (i) a problem governed by N-S equations with a constructed analytical solution, (ii) lid-driven cavity flow problem, and (iii) constricted channel flow problem. In the process, we have also expanded the scope of fourth-order 9-point compact schemes to geometries beyond rectangular. It is seen to efficiently capture steady-state solutions of the N-S equations with Dirichlet as well as Neumann boundary conditions. In addition to this, it captures viscous flows involving free and wall bounded shear layers which invariably contain spatial scale variations. Our results are in excellent agreement with analytical and numerical results whenever available and they clearly demonstrate the superior scale resolution of the proposed scheme.  相似文献   

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