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Robust adaptive beamforming波束成形的必读书
本书可以说是做方向合成图和波束成形必须要看的书，国外的书看的就是好
- 2020-12-12下载
- 积分：1
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alShaders-win-1.0.0rc20-ai5.0.0.0
arnold渲染器的材质资源alShaders,这个是最新版的，希望各位喜欢
- 2020-12-11下载
- 积分：1
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仿宋gb2312.ttf
【实例简介】微软word仿宋gb2312字体，新版的word一般不带的，可以用这个
- 2021-12-02 00:43:56下载
- 积分：1
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模糊自适应PID控制器matlab仿真程序
内涵matlab仿真程序，关于运用模糊自适应的PId程序实例。
- 2020-07-03下载
- 积分：1
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心率检测系统的设计论文
心率检测系统的设计论文，ti杯电子设计大赛优秀论文右手接至低通前置放大电路滤波器输左手入端共模电压右腿驱动屏蔽动右腿退导联屏蔽线图2前置放人电路框图1)前賢放大调理针对心电信号高增益,高输入阻抗,高垬模抑訇比,低噪声,低漂移和合适带宽的采集要求,采用仪表放大器,以获得良好的综合性能。所以采用仪用放大器AD620只要用只外接电阻便可设置放大器的增益,增益G为494人R2)右腿驱动电路将右腿连接到一个辅助的运算放大器的输出端,把混杂于原始心电信号中的共模噪声提取出来,经过一级倒相放大后,再返回到人体,使它们相互叠加,从而减小人体共模干扰的绝对值,提高信噪比。本电路采用高精度运算放大器O217。通过这个负反馈结构,可大大抑制测量过程屮前置敚大器输入端共模电压的影响。此外,右腿驱动电路还可以提供电气上的安全性。3)屏蔽驱动电路屏蔽驱动器是一个同相电压跟随器,将放大器的输出端和屏蔽相连,将屏蔽线和地隔开,并且对于50Ⅳz的共模干扰信号来说,从人体输入的两路信号是相等的导联线和屏蔽线之间的电压差为0,从而消除了其间的电容,提高了输入电路的阻抗,降低人与地之间的漏电流。如图3所小220kTT1点2R图3带屏蔽驱动、右腿驱动的前置放大调理电路经过前置放大器后心电信号被放大的倍数为49.4KG=1+51IK∥(24.9K+24.9K)(2)高通滤波电路的设计电极与皮肤表面之间容易产生直流偏压,为了消除这部分的干扰,需要采取高通滤波电路图4所示予以滤除,其截止频率为≈0.5Hz2丌√RR,CC22x√22X×47K×101×10U4BQPZITT图4二阶高通滤波电路(3)低通滤波电路的设计噪声来源一类是各种电子设备辐射出的高频噪声,一类是市电的50z噪声。通常情况下后者影响尤为明显。对这些噪声的滤波需要用到滤波器。低通滤波器(电路图如图5)通常情况下截止频率选择在100Hz以下。低通截止频率为2兀√RR1CC42√24K×24K×0.047×Dm≈100H2T745TQP2171图5二阶低通滤波电路(4)50Hz陷波电路的设计为了去除人体或测试系统中产生的工频50Hz干扰34,需用带阻滤波器加以抑制。我们采用心电测量没备当前普煸采用的双T陷波电路滤除工频干扰,其参数计R算公式为:2可C其中f为滤去频率,如图6所小。USD图650Hz陷波电路(5)后置放大电路及抬升电路的设计因为wsP430F169模数转换器的范围为0~2.5V,所以要对采集的心电信号进行拾升如此在实现后置放大的过程中,既要考虑信号中平的提升,又要实现信号的放大。放大器芯片用INA217。具体电路如图7所示图7后置放大发抬升电路放大倍数为:G=110K10KRIK抬升电路有对放大信号拾升了1.25V(6)电源电路的设计电源电路的设计是由电平转换器760,线性调节器MX8511,电压基准REF3025及电池盒组成,如图8所示电源电路图8电源电路31.3元件的布局和PCB板的设计在PCB板中,包含多种类型的电路,为了避免各部分电路中信号相互耦合而生千扰,对不同类型的电路部分进行分离布局是PCB板设计的一个基本原则。各部分之间不仅应保持相当距离,还要分开走线。电源系统的布线包括电源线VDD和地线vSs的布线,是系统抗干扰的个重要部分。VDD和wSS应尽可能扩大面积,以防止因电磁能量较强而产生电磁干扰能量的发射,这也是保证高频信号到地之间具有低阻抗的措施3.2软件设计软件设计的关键是对MSP430F169的控制以及LCD显示。所有软件均采用C语言绽写。软件实现的功能是QRS波检测并算出心率,LCD显小波形以及SD卡存储3.2.1软件流程系统软件部分流程图9如下所示,开关按键按下后,屏幕显示L0GO图(江苏省TⅠ杯电子设计大赛),通过对各模块的初始化后,由中断定时服务实现对心电信号QRS波检测,心率计算,波形回放。系统初始化A/D采集LCG0显示N按键显示模块初始化
- 2020-12-01下载
- 积分：1
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winhex 模板
一共所括102个模板文件AFP_Structured_Fields.tplBMP.tplBoot Sector FAT.tplBoot Sector FAT32.tplBoot Sector NTFS.tplCDFS Directory Entry Ascii.tplCDFS Directory Entry Unicode.tplCDFS Path Tables Ascii.tplCDFS Path Tables Unicode.tplCDFS Volume Descriptor.tplCDFS路径表.tplDalet BWF file header.txtDalet
- 2020-12-05下载
- 积分：1
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小波去除音频信号中的噪声，观察频谱
对声音信号加入随机噪声，用小波去除噪声，观察去噪前后的时域和频谱图，可听前后声音的变化。
- 2020-12-05下载
- 积分：1
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matlab车牌识别完整源程序
完整的车牌识别源码，实用化的程序，很好的算法，对搞车牌识别的研究很有帮助。
- 2020-06-25下载
- 积分：1
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希尔伯特--变换的MATLAB程序.rar
【实例简介】希尔伯特变换,用MATLAB程序实现希尔伯特变换，各种例程
- 2021-11-28 00:36:53下载
- 积分：1
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平面变压器3D仿真资料
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
- 2020-12-10下载
- 积分：1
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