DSP28335控制的有霍尔无刷直流电机闭环程序

采用COMSOL软件，对平面变压器的仿真过程进行叙述，让大家了解平面变压器的仿真流程，是个很好的指导教材Solved with COMSOL Multiphysics 5.0Results and discussionThe magnetostatic analysis yields an inductance of 0. 1l mH and a dc resistance of0. 29 mQ2. Figure 2 shows the magnetic flux density norm and the electric potentialdistributionvolume: Coil potentiaL()Volume: Magnetic flux density norm (t▲0.07▲2.88×10-42.51.50.03050.01V656×107v0igure 2: Magnetic flux density norm and electric potential distribution for themagnetostatic analysisIn the static (DC) limit, the potential drop along the winding is purely resistive andcould in principle be computed separately and before the magnetic flux density iscomputed. When increasing the frequency, inductive effects start to limit the currentand skin effect makes it increasingly difficult to resolve the current distribution in thewinding. At sufficiently high frequency, the current is mainly flowing in a thin layernear the conductor surface. When increasing the frequency further. capacitive effectscome into play and current is flowing across the winding as displacement currentdensity. When going through the resonance frequency, the device goes from behavingas an inductor to become predominantly capacitive. At the self resonance, the resistivelosses peak due to the large internal currents Figure 4 shows the surface current3 MODELING OF A 3D INDUCTORSolved with COMSOL Multiphysics 5.0distribution atl MHz. Typical for high frequency the currents are displaced towardsthe edges of the conductor.freq(1)=1.0000E6_Surfaee: Surface-current density norm (A/)▲18618Q16010￥1.02Figure 3: Surface current density at I MHz (below the resonance frequency)Figure 4 shows how the resistive part of the coil impedance peaks at the resonancefrequency near 6MHz whereas Figure 5 shows how the reactive part of the coiimpedance changes sign and goes from inductive to capacitive when passing throughthe resonance4 MODELING OFA3DINDUCTORSolved with COMSOL Multiphysics 5.0Global: Lumped port impedance(Q2)d port impedance7.5G6.583275655545352510.10.20.30.40.509igure 4: Real part of the electric potential distribution5 MODELING OF A INDUCTORSolved with COMSOL Multiphysics 5.0Global: Lumped port impedance(Q2)35000Lumped port impedance200001000050000500010000-1500020000250000.10.20.30.40.50.60.70.809Figure 5: The reactive part of the coil impedance changes sign hen passing through theresonance frequency, going from inductive to capacitiveModel library path: ACDC_Module/Inductive_ Devices_and_coils/inductor 3dFrom the file menu. choose newNEWI In the new window click model wizardMODEL WIZARDI In the model wizard window click 3D2 In the Select physics tree, select AC/DC> Magnetic Fields(mf)3 Click Add4 Click StudyMODELING OF A3D NDUCTORSolved with COMSOL Multiphysics 5.05 In the Select study tree, select Preset Studies>StationaryGEOMETRYThe main geometry is imported from file. Air domains are typically not part of a CaDgeometry so they usually have to be added later. For convenience three additionaldomains have been defined in the CAd file. These are used to define a narrow feed gapwhere an excitation can be appliedport l(impl)I On the model toolbar, click Import2 In the Settings window for Import, locate the Import section3 Click Browse4 Browse to the models model library folder and double-click the filenductor 3d. mphbinSphere /(sphl)I On the Geometry toolbar, click Sphere2 In the Settings window for Sphere, locate the Size section3 In the Radius text field, type 0.2ick to expand the Layers section. In the table, enter the following settingsLayer nameThickness(m)ayer0.055 Click the Build All Objects buttonForm Union(fin)i On the Geometry toolbar, click Build AllClick the Zoom Extents button on the Graphics toolbar7 MODELING OF A 3D INDUCTORSolved with COMSOL Multiphysics 5.03 Click the Wireframe Rendering button on the Graphics toolbarThe geometry should now look as in the figure below0.1-0.10.20.0.0.1y0.0.2Next, define selections to be used when setting up materials and physics Start bdefining the domain group for the inductor winding and continue by adding otheruseful selectionsDEFINITIONSExplicitI On the Definitions toolbar, click Explicit2 In the Settings window for Explicit, in the Label text field, type Winding3 Select Domains 7,8 and 14 onlyI On the Definitions toolbar, click Explicit2 In the Settings window for Explicit, in the Label text field, type Gap3 Select domain 9 onlI On the Definitions toolbar, click Explicit8 MODELING OF A3DINDUCTORSolved with COMSOL Multiphysics 5.02 In the Settings window for Explicit, in the Label text field, type core3 Select Domain 6 onlyExplicit 4I On the Definitions toolbar, click Explicit2 In the Settings window for Explicit, in the Label text field, type InfiniteElements3 Select Domains 1-4 and 10-13 onlyExplicit 5I On the Definitions toolbar, click Explicit2 In the Settings window for Explicit, in the Label text field, type Non-conducting3 Select Domains 1-6 and 9-13 onlyI On the Definitions toolbar, click Explicit2 In the Settings window for Explicit, in the Label text field, type Non-conductingwithout Ie3 Select Domains 5, 6, and 9 only.Infinite Element Domain /(iel)Use infinite elements to emulate an infinite open space surrounding the inductorI On the definitions toolbar click Infinite element domain2 In the Settings window for Infinite Element Domain, locate the Domain Selectionsection3 From the Selection list. choose Infinite Elements4 Locate the Geometry section From the Type list, choose SphericalNext define the material settingsADD MATERIALI On the Model toolbar, click Add Material to open the add Material window2 Go to the Add material window3 In the tree, select AC/DC>Copper.4 Click Add to Component in the window toolbar9 MODELING OF A 3D INDUCTORSolved with COMSOL Multiphysics 5.0MATERIALSCopper(mat/)I In the Model Builder window, under Component I(comp l)>Materials click Copper(matD)2 In the Settings window for Material, locate the Geometric Entity Selection section3 From the Selection list, choose windingADD MATERIALI Go to the Add Material window2 In the tree. select built-In>Air3 Click Add to Component in the window toolbarMATERIALSAir(mat2I In the Model Builder window, under Component I(comp l)>Materials click Air(mat2)2 In the Settings window for Material, locate the Geometric Entity Selection section3 From the Selection list, choose Non-conductingThe core material is not part of the material library so it is entered as a user-definedmateriaMaterial 3(mat3)I In the Model Builder window, right-click Materials and choose Blank Material2 In the Settings window for Material, in the Label text field, type Core3 Locate the geometric Entity Selection section4 From the selection list choose Core5 Locate the Material Contents section. In the table, enter the following settingsPropertName Value Unit Property groupElectrical conductivity sigma0S/IBasicRelative permittivity epsilonrBasicRelative permeability mur1e3Basic6 On the model toolbar. click Add Material to close the Add Material windowMAGNETIC FIELDS (MF)Select Domains 1-8 and 10-14 only0MODELING OF A 3D INDUCTOR

蚁群算法单路径和多路径路由31节点网络拓扑下寻找单个最短路径和前三条最短路径

家用防盗报警器的Verilog源代码及原理图

一款安卓的表白软件，进入软件，背景图片，告白文字逐渐一个一个的显示出来，并伴随着音乐的播放。另外，里面是四份图片告白音乐随机出现，并有一张爱心小图片在界面上不断的飞来飞去。

使用主元分析法PCA对两片点云数据作粗略的拼接配准，可以作为ICP算法的预处理步骤。尝试规定了PCA主元向量的朝向。附带ply文件格式的bunny多视角数据。

设一个时隙 Aloha 系统的时隙长度为 1，所有节点的数据包均等长且等于时隙长度。网络中的节点数为 m，各节点数据包以泊松过程到达。 1 假定每个节点的数据包到达强度均为 λ /m，在不同的 λ 下，仿真时隙Aloha 数据包传送的成功概率，绘制呼入强度和成功概率的曲线，和理论结果进行对照。 仿真思路： 1） 生成一个二项分布列来模拟数据包的到达过程 2） 因为数据包以泊松过程到达，所以二项分布的 P 定为（1- m eλ− ） 3） 对生成的数列求和，只有当其和恰等于 1 即有且仅有一个数据包到达时，才可以成功发送，这时成功个数计数+1 4） 2.选取合理的引,,qa,m,采用延时的下界,仿真时隙Aoha系统数据传输过程,统计在不冋同η下,到达率及离开率,绘制它们随n的分布情况,和理论值进行对照qn:等待重传的节点在每一时隙内重传数据包的概率qa:每个发送节点有新数据包到达的概率m:系统内总的节点数n:每个时隙开始时等待重传的节点数仿真思路:1)用二项分布模拟数据包的到达及发送过程2)生成两个数列:一个表示等待重传的节点以q,重传的情况;一个表示新到达的数据包情况因为题日说明采用延时的下界,即不缓冲,每个节点最多容纳一个数据包,有包则扔。所以第一个数列前n项令为1,后一个前n项令为0,之后两个数列可以进行简单加和3)发送成功率:对两个数列相加之后求和,如果sum等于1,说明此时隙内到达和发送的总数为1,只有在这种情况下发送才有可能成功,计数加1到达率:在每N次实验中,对“表示到达的数列”求和,统计4)对n做循环以表示到达率和离开率随n的变化情况;每个n下进行N次实验,数理统计3/8仿真结果0.40.35*0.30.250.20.150.10.0550607080901001/曲线为理论曲线:Ps=G exp(-G)and G=(m-n)a+n gr2/仿真值基木与理论曲线吻合在仿真的过程中,合理选取个参数值对能否得到埋想的曲线起了重要的作用下图分别为qr=0.02,0.05,0.08s时的曲线。可以看到,随着qr的增加,曲线向左移,导致第二个交叉点也左移,这个时候重传的延时将会减小。反之,曲线右移。当q,增加到一定程度的时候,系统只有一个稳定点了。4/840.350.30.20.1501020304050607080901c03仿真时隙Aoha系统下的伪贝叶斯算法,通过仿真结果眼正在n的估计误差较大的情况下的收敛特性及到达率小于1/e下的稳定性。仿真思路:1、伪贝叶斯算法的主要思路是对新数据包和积压节点等同对待:当有新数据包到达的时候,暂不发送,下一时刻与以前的积压节点一起以4r发送。所以修改2中的仿真模型:1)依旧是一列表到达,一列表上一时隙的积压节点2)对两列加和,统计其中为1的个数,设为d3)以qr为概率,d为长度,生成又一个二项分布数列 depart,表示发送的情况4)对depa求和,如果 depart的和为一,说明恰发送成功,n(k+1)=d-1,否则n(k+1)=n(k)5)循环,进行数理统计2、仿真收敛特性和稳定特性哩论值:根据给岀的伪贝叶斯算法的具体步骤,由给出的n(k),不断模拟生成n(k+1)5/8仿真值:由仿真模型及给出的n(k),生成n(k+1)观察两种方式得到曲线的走向3、给出不同的值,观察n(k+1)随时间变化的情况判断标准如果要保持系统的稳定,至少n(k+1)应该保持在一个恒定的状态,或者逐渐趋于零。如果n(k+1)不断增加,则系统最终将趋于饱和,无法再接纳新的数据包,此时系统不稳定。仿真结果:1、验证在n的佔计误差较大的情况下的收敛特性:1)n=170;估计nt=20;m=100:20.2:N=100016030040050060070080g001CC08002)n=50;估计nt=180;m=1000=-1-02:N=80结果说明可以看出,当估计值与系统本身的积压数据包数有很大差别的时候,无论是大还是小,最终都可以趋于实际值,从而收敛特性得到验证。1)同时可以看到,改变的值:当λ增大的时候,收敛地更快;2)当n不变的时候,改变m的值,如果n/m变大,那么发生碰撞的几率就变大,也会导致估计的n值更快地趋向理论n值这些都是于课堂分析的理论情况相吻合的6/82、验证系统的稳定性下图分别为A=02:=10.1:=1:4=1+02:=0.3时候的情况。可以看到,当λ

这是图像处理课程的作业，对图片进行边缘检测和特征提取，这是我自己实现的MATLAB源代码。

【实例简介】自己编写的Buck变换器双闭环控制的比较规范的程序。开发环境为CCS，适用的DSP型号为TI公司的TMS320F28335，针对其他型号的DSP程序也可以借鉴。程序实现同步bbuck电路的电压电流双闭环控制，电压外环和电流内环均采用PI调节器。为了提升控制系统的动态性能，采用双更新模式，采样频率为开关频率的两倍。 该程序编写规范，注释率较高，可以作为电力电子变换器闭环控制的参考程序，很多编程思路都可以借鉴到其他类型的电力电子变换器的闭环控制程序中。

【实例简介】PSASP版本为6.24，原始数据请搜索“ieee 标准测试系统原始数据”

关于移动机器人路径规划的ppt，参考了大量文献，涵盖了几乎可以看到的所有成熟路径规划算法并且加入了很多作者本人的理解。希望对需要的朋友有所帮助。-on mobile robot path planning ppt reference to the vast body of literature, cover almost all can see the maturity path planning algorithm and to the many authors I understand. Hope to a friend in need of help.