资源列表
1D_Wave_Equation_Cavity_FDTD.m
- 1D Wave Equation Cavity FDTD in Rectangular Coordinates
tls-(2)
- tls 算法 解决带系数矩阵的问题比LS算法在误差校正方面更有优势-tls algorithm to solve the problem with the coefficient matrix more advantages than the LS algorithm in terms of error correction
PMSM_SMO
- This model for Permanent magnet synchronous motor by using SVPWM This is done using vector control technique PMSM is made sensorless with the help of sliding modle observer-This is model for Permanent magnet synchronous motor by using SVPWM Thi
dyzj
- 基于S变换的短时电能质量扰动检测方法，从S变换的结果S模矩阵及S复矩阵中提取出所需数据并以此来对各种扰动情况下的电压暂降的幅值、相位跳变、持续时间和谐波含量进行分析-Disturbance detection method based on the results of short-term power quality S transform from S Mode S transform matrix and complex matrix S to extract the required d
principal--stress
- 本程序可计算主应力大小和方向。主应力就是两个垂直方向的作用力的合力所产生的力在单位截面上的力。-This program can calculate principal stress size and direction. Two vertical principal stress is the force by the force of the force in the direction of force on cross section in the unit.
shishi
- 运用matlab软件进行6自由度并联机构工作仿真程序,-Using matlab software work parallel mechanism simulation program,
MATLAB-Wavelet-Analysis
- 《MATLAB小波分析（第2版）》张德丰源代码下载-" MATLAB Wavelet Analysis (2nd Edition)" Zhang Defeng Source Codes
lab2old.mdl
- Quadrocopter model in Simulink with basic PID controller
Finite_element_1d
- 演示一维有限元方法程序。并附有L2误差收敛阶数随着网格变细的误差图形-Presentation of one-dimensional finite element method program. Together with L2 error convergence order fining error with grid graphics
Stationary_Series2_MA
- 演示MA序列的特征值、自协方差函数和谱密度。程序是开放的，可以修改参数-MA eigenvalues demo sequence, since covariance function and spectral density. The program is open, you can modify the parameters
Stationary_Series1_AR1
- 演示AR序列的特征值、自协方差函数和谱密度。程序是开放的，可以修改参数-Eigenvalues demo AR sequence autocovariance function and spectral density. The program is open, you can modify the parameters
runge_stable_domain
- 演示龙格库塔方法的绝对稳定区域，从1阶到4阶，且阶数可以调整。另外，区域的左右边界可以计算出来-Absolutely stable region demonstrates Runge-Kutta methods, from an order to the fourth order, and the order can be adjusted. Further, around the boundary region can be calculated