matlab 计算李雅普诺夫指数的方法集合

【实例简介】采用TI公司的浮点数字信号控制器TMS320F28335 DSP为控制电路核心，采用CPLD自行设计驱动的4.3’’彩色液晶TFT LCD非常直观地完成了输出信号波形、频谱特性的在线实时显示，以及输入电压、电流、功率，输出电压、电流、功率，效率，频率，相位差，失真度参数的正确显示，具有开机自检、输入电压欠压及输出过流保护，在过流、欠压故障排除后能自动恢复，里面包含了原理图、PCB、及所用的程序，保证可用，有需要设计，或者毕业设计的，可以下载，直接使用。

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

深入理解RNN和LSTM，对LSTM的解剖深刻，每一个公式意义说明详细。

资源名称 CASIA汉语情感语料库共包括四个专业发音人，六种情绪，共9,600句不同发音，包括300句相同文本和100句不同文本，可供各种分析实验使用本数据集包含部分数据用途 为研究情感语音所设计的语料

imdb 电影评分数据集 包含评分数据等

基于QT(+MySQL)的学生信息管理系统的开发

现在图片一般都有很多去雾算法对图片进行处理，但是对图片增加雾的代码却少之又少，本代码就是用matlab代码实现了对图片的加雾处理。

提出了一种基于级联混沌系统的图像加密算法。实验结果表明，这种加密算法具有高度的安全性和有效性。关键词： 图像加密算法；混沌；级联混沌 目前混沌加密己成为密码学研究的热点之一，但已有的大部分混沌加密算法都是基于单个混沌系统的。事实表明，一些混沌映射可通过相空间重构的方法精确预测出来[1]。另外，由于计算机精度的限制，单混沌系统输出的时间序列并不能达到理论上的完全随机，而可通过多个混沌系统的级联使1382002GDCTK LP(M/K)(NIL). PS DCT(M/K)(N/L)],i=h,j=G[0,1GSm=88(k=1,2,,M/8Sign(nn)ⅠB.IBIlByDCT2,,M/K,j=1,2,,N/L),IB=j+(-1)(N[O,1,,31L). IPⅠP3.3K L)SteplIBi= pImmage3.2.3Outl mageInl mageStep2.(1k(k=1,Out/ mageyhSkm DCtep2.(1)rk yk(= 1,g km10.88 DCTJPE GPGDCTIPEJPEG3.2.43.3JPEGMPEG, JPEGx0=0.60773).2en aDCTx0=0.60773)Huffman[2,8]JPEG1d.2d0=0.60772SG3DCT3a,3b3 cJPEG90DCTDCTa Lena原图b加密图像c解密恢复的图像d密钥错误解密的图像1994-2012 China academic journ图Hlec图像筐國咖密解密铺果. All rights reserved.htt:ww. cnkinet139B enn原图b加密图像c解密恢复的图像d密钥错误解密的图像图2图像域加密与解密结果a随机噪声b均匀噪声C JPEG压缩图3加密图像的失真对解密图像的影响[4] C Shi, B Bhargava. Light -w eight M PEG video encr yption agorithm Al. In: Pr oc ee dings of the Int ernat ional ConferenceDelhi, India, 1998. 55 6[5 Josef Scharinger. Fast en cry pt ion of image dat a usin g ch aot iKolm og or ov flows[A]. In: Proceedings of E lectronicImaging 97, Security and Watermarking of Multimed ia Conten ts, S an Jos e,1997,3022:278289[6 Qi Don gxu, Zou Jiancheng. et al. New scramble tr ans form a-tion and applic at ion in inform at ion hiding[ J]. Ch inese Science(E),20,030(5):440447( in chinese)E),2000,30(5):440447)[1 Li Y uh uan. Comb inat orial Mathem at ics[ M I. Beijing: Beijing [7] Hui Xiang, et aL. D igital water ark ing sys tems w ith ch icNormal College press, 1998( in Chinese)sequences[ A]. In: Proceedings of Electronic Imaging99, Se-M,1998)cu rity and Waterm ark ing of Multimedia Contents, SPIE, San[2] Wu M insh eng, Wang Jiesheng. L iu Shen quan. Perm ut at ionJose,1999,3657:449457transformation of image[ J]. Chinese Journal of Computers, [8] Yi Kaixiang, Sun Xin, Shi jiaoy ing. Chaotic sequences bas ed1998,21(6):514519 in chines e)image encry pt ion alg or ith m[ J]. Journ al of Computer-A idedDes ign Com puler Graph ics, 2000, 12(9):672 676(in Chi-1998,21(6):514519leseWei, Qi Don gxu. Digit al image tran format ion and in-format ion hiding and dis guisin g techn ology[ J]. Chin ese Jour2000,12(9):672nal of Computers, 1998, 21(9):838 843( in Chinese676)1998,21(9):838843)o1994-2012ChinaAcademicJournalElectronicPublishingHouse.Allrightsreservedhttp://www.cnki.net

结构计算和量子力学-分子动力学模拟软件包

经典的串口收发调试工具，实现了利用C# SerialPort串口控件进行(二进制，十进制，十六进制)数据的收发和显示处理； 已经经过测试调试，可用！-----No.2