diode

在倒立摆摆角及摆速很小的时候，实现基于sugeno模型的倒立摆模糊控制(Monotonously in inverted pendulum angle and velocity very young to realize sugeno Model Based Fuzzy Control of Inverted Pendulum)

说明：  数学实验：使用MATLAB书的源码 实验1 矩阵运算与Matlab命令 1.1 知识要点与背景:日常矩阵及其运算 1.2 实验与观察:矩阵和Matlab语言 1.3 应用、思考与练习 实验2 函数的可视化与Matlab作图 2.1 实验与观察:函数的可视化 2.2 应用、思考与练习 实验3 函数式——直接确定型模型 3.1 知识要点与背景:函数——直接确定型模型 3.2 实验与观察:插值与拟合 3.3 应用、思考与练习 实验4 微分、积分和微分方程 4.1 知识要点与背景:微积分学基本定理 4.2 实验与观察(I):数值微积分 4.3 实验与观察(II):Matlab符号微积分简介 4.4 应用、思考与练习 实验5 用导数作定性分析 5.1 知识要点:函数作图——用导数定性描述函数 5.2 实验与观察:微分方程的定性解图示 5.3 应用、思考与练习(Mathematical Experiment: Using MATLAB source book)

建设和测试模式，尤其是那些将以往的重大知识的过程，涉及到当前正在很差综合多个步骤。我们已经开发锑管道建立一个有效的工作流，基于开放源代码，公众标准与现代软件的做法(The process of constructing and testing models, particularly those that incorporate significant prior knowledge, involves multiple steps that are currently very poorly integrated. We have developed SB-Pipeline to create an effective workflow based on open-source code, public standards and modern software practice.)

基于卡尔曼滤波器的永磁同步电机的二阶电阻辨识(Kalman filter based on permanent magnet synchronous motor of the second-order Resistance Identification)

m file matlab traitement d image

电网优化，能够用于分布式电源的选址定容，也可以用于电网的网架优化计算等等(Power network optimization)

用matlab编写的程序，可以画出waterfall形式的图形。(using Matlab prepared by the procedure could paint waterfall forms of graphics.)

in this package are the programs needed to solve any eigenvalue problem.

面阵阵列天线二维方向图仿真，代码简单易懂(The two-dimensional surface bursts columns antenna pattern simulation, the code is easy to understand)

基于MATLAB利用Particle-in-cell模型,对梯形管内壁等离子体离子注入过程,进行了二维数值模拟.计算结果表明在中心电极附近出现了“阳极鞘层”,该鞘层内部不存在离子,而且在鞘层边缘离子密度最高.在上下管壁上的离子注入剂量呈现“m”形分布.通过对注入过程中等离子体密度分布和不同时间段管壁不同位置离子注入剂量的跟踪,发现“阳极鞘层”扩展行为是导致“m”形分布的原因.由于梯形管形状的不对称性,“阳极鞘层”的边缘向梯形长底方向扩展较快.在注入初始时刻离子注入的能量很低,随着时间延长离子能量逐渐升高,这是由离子初始位置决定的.可见梯形管自身形状决定了鞘层形状和最终的离子注入能量和剂量分布.(Based on MATLAB use Particle-in-cell model, the trapezoidal pipe wall plasma ion implantation process, the numerical simulation of two-dimensional calculation results show that in the vicinity of the center electrode to a "anode sheath," which does not exist inside the plasma sheath, and the highest in the sheath edge ion density ion implantation dose showing the upper and lower walls of the "m"-shaped distribution through the process of injecting the plasma density distribution and the wall at different locations in different time periods ion implantation dose tracking, found that "anode sheath "extension behavior is leading to" m "-shaped distribution of the reasons due to the asymmetry of the trapezoidal shape of the tube," Edge anode sheath "extension to the end of a long trapezoid direction quickly in the initial moment of implantation energy ion implantation is low ion energy with time gradually increased, which is determined by the initial position of the ion. visible trapezoida)