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Navier_Stokes_simulation
- 求解navier stokes方程进行流体仿真，很好的计算程序，提供给大家学习使用。-Solving navier stokes equations of fluid simulation, a good computer program, available to everyone to learn to use.
cfdsolutions-code-141
- 用于cfd流体仿真，求解navier stokes 方程，是很好的学习代码，供各位好好学习和使用。-Cfd fluid simulation for solving navier stokes equations, is a good learning code for you to learn and use.
Fluid-MATLAB-PDE-simulation-code
- 运用MATLAB的偏微分方程求解工具对流体进行动力学仿真-Using the MATLAB partial differential equation solution tool to carry on the dynamics simulation to the fluid
zhoucheng
- 基于HS边界润滑条件和雷诺方程流体润滑模型的求解程序-Solution procedure of fluid lubrication model based on HS boundary lubrication condition and Reynolds equation
CUDA.tar
- 利用格子波尔兹曼方法求解三维流体问题，利用CUDA加速迭代过程。是单个CPU运算速度的20倍。(Here we use the Lattice Boltzmann Method to solve a problem of 3D fluid dynamics with the help of CUDA. It is 20 times the speed of a single CPU operation.)
对流边界
- 墙角在对流边界情况下的温度场模拟计算程序。用户输入墙角两侧的流体主流温度，对流换热表面传热系数，设定墙角以及计算网格尺寸后，程序可以通过迭代求解墙体的温度场并以矩阵和三维图像的形式输出。(A simulation program for the temperature field of the wall corner under the convective boundary condition. After entering the
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- 二维不可压缩黏性流体泊松流动问题的数值解与计算程序，二维泊松流动问题是有解析解的二维不可压缩黏性流动。对它采用算法和压力迭代解法进行数值求解。(The numerical solution and calculation program for the two dimensional incompressible viscous fluid Poisson flow problem, the two-dimensional Poisso
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- 二维不可压缩黏性流体库页特流动问题的有限体积算法与计算程序，二维库页特流动是一个不可压缩黏性流动的典型流动，并有解析解，可以用来检验数值算法计算精度和可靠性。对它采用有限体积算法一阶迎风型离散格式进行数值求解。(The finite volume algorithm and calculation program of a two-dimensional incompressible viscous fluid reservoir fl
3DMHDcode
- 磁流体通道3D模型仿真，给定流场条件和边界条件，采用泊松方程迭代求解通道电磁场分布。(Magnetic fluid channel 3D model simulation, given the flow field conditions and boundary conditions, using Poisson equation iterative solution channel electromagnetic field dist
lattice boltzmann method for single phase flow
- 本程序系对格子Boltzmann方法中经典的D2Q9模型进行编程求解。该程序模拟了单相流体在单通道中的流动情况，在流动通道中可以添加不渗透固体，从而用于模拟流体扰流的情况。进一步可以增加不渗透固体的数量，达到模拟流体在多孔介质中的二维流动。该程序适用于初学者对LBM方法编程求解的理解，经二次开发后可以用于油气勘探开发领域。(This program solves the classical D2Q9 model of lattice B