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Meshless_SPH
无网格算法中的光滑粒子水动力学sph算法源程序(溃坝)(Meshless algorithm smoothed particle hydrodynamics sph algorithm source (dam))
- 2021-01-21 21:38:45下载
- 积分:1
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leifing
用谱方法计算流体力学一些流动现象的整体稳定性,利用自然梯度算法,包括四元数的各种计算。( Spectral methods of computational fluid dynamics flow of some of the overall stability of the phenomenon, Use of natural gradient algorithm, Including quaternion various calculations.)
- 2017-01-03 17:25:25下载
- 积分:1
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uve_pls
对一维光谱实现偏最小二乘回归进行UVE变量选择(UVE variable selection on the spectrum)
- 2021-04-19 15:18:51下载
- 积分:1
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Fractional Fourier Transform
分数傅里叶变换和分数余弦变换,动态展示实部,虚部和模值(Computation of the Fractional Fourier Transform)
- 2019-04-26 17:22:14下载
- 积分:1
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HEAT
matlab编写的流体计算和传热程序(很不错的哦)(matlab prepared and heat transfer fluid calculation procedures)
- 2013-10-15 19:44:22下载
- 积分:1
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test1_1
说明: 研究舍入误差的例程,可以帮助初学计算方法的人。(Of rounding error in the routine that can help beginners who calculation.)
- 2011-04-11 23:55:26下载
- 积分:1
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断裂力学中的数值计算方法及工程应用-算例程序
说明: 金属断裂的数值计算提供理论依据及实际详例解读(The numerical calculation of metal fracture provides theoretical basis and interpretation of practical examples)
- 2019-03-15 13:45:02下载
- 积分:1
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3803
关于非线性离散系统辨识,小波包分析提取振动信号中的特征频率,有小波分析的盲信号处理。( Nonlinear discrete system identification, Wavelet packet analysis to extract vibration signal characteristic frequency, There Wavelet Analysis Blind Signal Processing.)
- 2017-05-08 17:46:22下载
- 积分:1
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poisson-process-simulation
模拟应用随机过程中时齐泊松和非时齐泊松过程的matlab源代码(matlab code for poisson process)
- 2012-04-11 16:19:44下载
- 积分:1
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comsol14
下面我们将给出一些基于Galerkin有限元法的微型泵模拟结果,模拟过程在商业软件COMSOL Multiphysics 3.2中实现。数值求解采用压力修正算法——SIMPLE,它首先假设一个压力场,然后通过求解不可压缩流动的Navier-Stokes方程得到速度场。这些速度不需要满足Possion型连续方程,所以对压力场的修正也带来速度场的修正,最终满足质量守恒。求解速度场的同时计算电势场方程。这会得到Lorentz力,然后将其反馈回N-S方程并作为体积力处理。连续耦合Lorentz力和速度场直到Newton迭代收敛。
(Below we will give some micro-pump simulation results based on the Galerkin finite element method, the simulation process in the commercial software COMSOL Multiphysics 3.2. The numerical solution of pressure correction algorithm- the SIMPLE, it begins by assuming a pressure field, and then by solving the incompressible Navier-Stokes equations, the velocity field. These velocities do not need to satisfy the continuity equation of Possion type pressure field correction to bring the amendment of the velocity field, and ultimately to meet the conservation of mass. Solving the velocity field at the same time to calculate the potential field equations. This will be the Lorentz force, and then fed back to the NS equations and processing as a volume force. Continuous coupling of the Lorentz force and the velocity field until the Newton iteration convergence.)
- 2012-06-03 12:26:50下载
- 积分:1