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Search - velocity - List
[
Mathimatics-Numerical algorithms
]
velocity computing.rar
DL : 0
二分法解非线性方程---相变过程中的界面迁移速率
Date
: 2025-12-23
Size
: 1.19kb
User
:
[
Mathimatics-Numerical algorithms
]
velocity computing
DL : 0
二分法解非线性方程---相变过程中的界面迁移速率---- Dichotomy solution of nonlinear equations in the process of phase-change interface migration rate
Date
: 2025-12-23
Size
: 1kb
User
:
俞伟
[
Mathimatics-Numerical algorithms
]
PID-c-source-code
DL : 0
在使用单片机作为控制cpu时,请稍作简化,具体的PID参数必须由具体对象通过实验确定。由于单片机的处理速度和ram资源的限制,一般不采用浮点数运算,而将所有参数全部用整数,运算到最后再除以一个2的N次方数据(相当于移位),作类似定点数运算,可大大提高运算速度,根据控制精度的不同要求,当精度要求很高时,注意保留移位引起的“余数”,做好余数补偿。这个程序只是一般常用pid算法的基本架构,没有包含输入输出处理部分。-In the use of single-chip microcomputer as the control cpu, please make some simplification, the specific PID parameters must be determined through experiments at specific audiences. As the single-chip processing speed and ram resource constraints, generally do not use floating-point, and will use all parameters of all integers, computing the final 2 and then divided by a N-th power of data (equivalent to shift), similar fixed-point computation can be greatly enhanced speed of operation, according to the different requirements of control precision, when high precision, the attention to retain the shift caused by the balance , do a good job in the balance of compensation. This procedure is commonly used algorithm pid basic structure does not contain input and output part of treatment.
Date
: 2025-12-23
Size
: 1kb
User
:
王强
[
Mathimatics-Numerical algorithms
]
sjlb
DL : 0
卡尔曼滤波值计算方法 一飞行物,初始时刻距离雷达站距离 =30km,初始速度 =300米/秒,加速度 =20 ,过程噪声 ,测量 ,测量噪声 ,采样周期T=0.5s,求卡尔曼滤波值 及 -Kalman filter method of calculating the value of one flying objects, the initial moment of the distance from the radar station = 30km, initial velocity = 300 m/s, acceleration = 20, the process noise, measurement, measurement noise, sampling period T = 0.5s, for Carl Cayman filter values and
Date
: 2025-12-23
Size
: 1kb
User
:
阿杜
[
Mathimatics-Numerical algorithms
]
cavity
DL : 0
this program solves the steady-state navier-stokes eqn in 2d for the flow in a driven cavity problem. the function solved for is the streamfunction. the velocity may be obtained by differentiating the streamfunction.
Date
: 2025-12-23
Size
: 41kb
User
:
Maged
[
Mathimatics-Numerical algorithms
]
222
DL : 0
卫星位置和速度的Lagrange插值算法分析,介绍卫星位置和速度的算法-Satellite position and velocity analysis of the Lagrange interpolation algorithm on satellite position and velocity of the algorithm
Date
: 2025-12-23
Size
: 256kb
User
:
吴瑞祥
[
Mathimatics-Numerical algorithms
]
ch5soft
DL : 0
These codes require an ASCII input file called input.dat of the following form: Lower Limit on x Upper Limit on x Final Time Pressure for x<0 when t=0 Density for x<0 when t=0 Speed for x<0 when t=0 Pressure for x>0 when t=0 Density for x>0 when t=0 Speed for x>0 when t=0 These codes produce 8 ASCII output files: density.out. Density vs. x entropy.out. Entropy vs. x mach.out. Mach number vs. x massflux.out. Mass flux vs. x pressure.out. Pressure vs. x sound.out. Speed-of-sound vs. x velocity.out. Velocity vs. x waves.out. A description of the solution in terms of the three waves defined in the book (+,-,0). -These codes require an ASCII input file called input.dat of the following form: Lower Limit on x Upper Limit on x Final Time Pressure for x<0 when t=0 Density for x<0 when t=0 Speed for x<0 when t=0 Pressure for x>0 when t=0 Density for x>0 when t=0 Speed for x>0 when t=0 These codes produce 8 ASCII output files: density.out. Density vs. x entropy.out. Entropy vs. x mach.out. Mach number vs. x massflux.out. Mass flux vs. x pressure.out. Pressure vs. x sound.out. Speed-of-sound vs. x velocity.out. Velocity vs. x waves.out. A description of the solution in terms of the three waves defined in the book (+,-,0).
Date
: 2025-12-23
Size
: 39kb
User
:
mcastle
[
Mathimatics-Numerical algorithms
]
BreedPSO
DL : 0
基于杂交的粒子群算法求解无约束优化问题,主要是各粒子的位置和速度-Based on the hybrid particle swarm algorithm for unconstrained optimization problems, mainly the position and velocity of particles
Date
: 2025-12-23
Size
: 1kb
User
:
王国
[
Mathimatics-Numerical algorithms
]
INS
DL : 0
A good INS code. Can calc position velocity from the available data of IMU. The calc are made with treliable accuracy.
Date
: 2025-12-23
Size
: 2kb
User
:
KASHIF
[
Mathimatics-Numerical algorithms
]
SIMPLE
DL : 0
流体计算中压力与速度耦合求解的算法。 是目前比较常用的方法之一。-Calculation of fluid pressure and velocity coupling solution algorithms. Is more commonly used methods.
Date
: 2025-12-23
Size
: 47kb
User
:
ze
[
Mathimatics-Numerical algorithms
]
simple3
DL : 1
SIMPLE算法自1972年问世以来在世界各国计算流体力学及计算传热学界得到了广泛的应用,这种算法提出不久很快就成为计算不可压流场的主要方法,随后这一算法以及其后的各种改进方案成功的推广到可压缩流场计算中,已成为一种可以计算任何流速的流动的数值方法。-SIMPLE algorithm since its inception in 1972, countries in the world of computational fluid dynamics and computational heat transfer in academia has been widely used, this method quickly became the calculations presented the near incompressible flow the main method, then the algorithm and the subsequent to promote the success of various programs to improve the compressible flow calculation, has become a flow velocity can be calculated to any numerical method.
Date
: 2025-12-23
Size
: 6kb
User
:
刘士博
[
Mathimatics-Numerical algorithms
]
siganjigou
DL : 0
程序是关于四杆机构的运动学计算,包括位移速度,加速度-Program is on the four-bar kinematics calculations, including the displacement velocity, acceleration
Date
: 2025-12-23
Size
: 91kb
User
:
林哲
[
Mathimatics-Numerical algorithms
]
Double-Diff-Free-P.-M.--AHM
DL : 0
This is a Fortran code simulating the heat and mass transfer in porous media by solving the non-Darcy flow by applying the streamfunction-vorticity method to calculate the velocity field without any need to calculate the pressure field and using the local thermal non-equilibuiriam model (LTNE) in order to calculate the temperature field for both solid and fluid phase.
Date
: 2025-12-23
Size
: 3kb
User
:
ahmed
[
Mathimatics-Numerical algorithms
]
datachange
DL : 0
将promax处理软件中导出的速度谱转换为解释软件可读的通用格式-Processing software will promax derived velocity spectrum into a common format readable interpretation software
Date
: 2025-12-23
Size
: 1kb
User
:
曹盛
[
Mathimatics-Numerical algorithms
]
Cpp-openlb
DL : 0
这个算例采用格子Boltzmann方法模拟不稳定绕柱流的情况。在固体边界出采用反弹格式进行处理。-this example examines an unsteady flow past a cylinder placed in a channel. The cylinder is offset somewhat from the center of the flow to make the steady-state symmetrical flow unstable. At the inlet, a Poiseuille profile is imposed on the velocity, where as the outlet implements an outflow condition: grad_x p = 0. At Reynolds numbers around 100, an unstable periodic pattern is created, the Karman vortex street.
Date
: 2025-12-23
Size
: 4kb
User
:
李学斌
[
Mathimatics-Numerical algorithms
]
ewrwre
DL : 0
竖直管路内流动液氢条件中弹状氢气泡运动速度.-Vertical pipe flow of liquid hydrogen in the hydrogen bubble-like conditions of shot velocity.
Date
: 2025-12-23
Size
: 182kb
User
:
you
[
Mathimatics-Numerical algorithms
]
houbolt-newmark
DL : 0
采用huobolt和newmark写的求解动力方程的程序,能算速度,加速度,位移等。用C++编写的。-Using huobolt and newmark written procedure for solving dynamic equations can be calculated velocity, acceleration, displacement and so on. Written in C++.
Date
: 2025-12-23
Size
: 704kb
User
:
caden
[
Mathimatics-Numerical algorithms
]
d4ef13.ZIP
DL : 0
带速度项电磁场控制方程的无网格解法With the velocity of the meshless method for electromagnetic field equations-With the velocity of the meshless method for electromagnetic field equations
Date
: 2025-12-23
Size
: 321kb
User
:
nn112233
[
Mathimatics-Numerical algorithms
]
xy7z.ZIP
DL : 0
惯性导航平台辨识的离心机方法With the velocity of the meshless method for electromagnetic field equations-With the velocity of the meshless method for electromagnetic field equations
Date
: 2025-12-23
Size
: 481kb
User
:
nn112233
[
Mathimatics-Numerical algorithms
]
ProjectCode
DL : 0
The objective is to find out the time at which the rocket reaches a speed of 1000m/s (3600km/hr). Analysis We know the following: * Initial mass of the rocket and fuel, 160000kg, or 160 metric tons. * Fuel combustion exhaust velocity relative to the rocket is assumed to be constant at 2200m/s * Fuel combustion rate is a constant 2680kg/sec2 * Gravitational acceleration is 9.8m/sec2 The following formula is used to calculate the upward velocity of the rocket while the fuel is providing thrust: V = u*loge(m0/(m0-qt))-g*t Now substituting the values in the formula we get: 1000 = 2200*log(160000 / (160000 – 9.8*t)) – 9.8*t which is too difficult to solve analytically so we use Bisection root-finding method. The source code is for a program that solves this problem with the given parameters.
Date
: 2025-12-23
Size
: 37kb
User
:
slabo
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