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时域有限差分法在汽车电磁兼容性分析中的应用与研究
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摘要
时域有限差分法(FDTD)作为一种典型的全波时域分析方法备受关注,并迅速的发展。它直接将有限差分式代替Maxwell时域场旋度方程中的微分式,能直接反应电磁波的时域特性,并充分而形象的描绘电磁波的传播和与目标的相互作用过程,得到复杂物理过程的清晰物理图像。随着汽车上的电子产品越来越多,使其电磁兼容问题变得极为复杂,对汽车电磁兼容性的研究也变得尤为重要。为了在汽车设计及其生产初期能够发现自身或与环境的不兼容性,避免进行二次修改造成的损失与降低成本,提高解决问题的效率,把数学建模和数字仿真技术应用到汽车EMC研究上具有很高的价值,并为汽车电磁兼容性检验和防护设计提供理论依据。
     本文在前人研究的基础上,分析了空间和时间离散间隔对数值色散及数值稳定性的要求,通过对空间PML构造及PML中分裂场的特性分析,提出一种简化形式的PML参数设置方法去简化计算机编程,提高计算效率。通过对实测点火系特征频率的提取构造得到更符合实际点火系辐射特性的双重调制激励源,并模拟了在此激励源激励下的点火系、暖风电机产生的辐射场的传播。最后对辐射场对受扰设备的耦合干扰进行了分析,并对缝隙处的场值进行了计算,配合实验进行了一些比较和研究,得到了比较满意的检测结果。
A lot of respects of modern technology are relevant to electric magnetic field, especially in the high-frequency electric magnetic field. As the electrical products on the automobile is getting more and more, its electromagnetic compatibility (EMC) problems become more complex. Many automobile manufacturers have attached great importance to the automotive EMC Research. Automotive Electromagnetic Compatibility Study is to ensure that when the car is in the process of running, the electrical and electronic equipment on the car does not influence each other, and can work compatibly. The entire automobile can resist external interference, and don't release the interference which exceeds the allowed scope to other equipment outside or in the environment. The purpose of EMC test is to analyze and estimate the incompatible phenomenon that may exist in advance, Pre-test, Preventive designation and solve the present problem before designing finished. On the basis research of FDTD in this paper, for the Prediction of EMC in Automotive electrical equipment,we compare the outcome results of forecasts with actual test results or actual project experiences. To check their consistency and use it provide a certain extent theoretical guidance for the designation and production. This article reads as follows:
     1、Electromagnetic problems in the finite difference time domain method.
     The FDTD method is first proposed by K.S.Yee in 1966.Since it is established directly on all electromagnetic field problems which is to meet on the basis of Maxwell's equations. Therefore its solving train of thought is clear, easily realized and developed continually. The FDTD method is a time-domain approach, and any one distribution of the field which been interested in can be got. The computer animation simulation of Electromagnetic wave propagation can be achieved. Through the use of pulse excitation with Fourier transformation, we can get the contained response of effective spectrum of pulse through calculating, compared with the frequency domain methods which will save a substantial amount of computing time. The way to solve these problems is universal, and the only difference with other numerical methods lies in its geometry and electromagnetic parameters. The electromagnetic compatibility issues are major concerned in all the spectrum of radiation equipments. It is precisely because of broadband characteristics of equipment radiation that led to the interference to other equipments. In order to access the spectrum of researched problem promptly, The FDTD method is a good algorithm. It can get all value of electromagnetic fields at any time. With Fourier transformation, their spectral response can be got. FDTD method regards Yee grids as discrete modules for the space field and turns Maxwell's curl equation into the difference equation to solve in the time frame step by step. It is concise to understand, and can combine with the computer to deal with very complicated electromagnetic problems. In the second chapter the basic principles of FDTD method is introduced, Derivate the FDTD differential formulas of the one-dimensional and three-dimensional circumstances in Cartesian coordinate system. And present how to deal with the equivalent parameters in cube cellular simplely.
     2、The numerical dispersion and stability conditions.
     Using FDTD method makes Maxwell's curl equation approximate and receive a group of coupling differential equations, only when the solution of differential equations is convergence or stability, the results of FDTD method can be meaningful. Convergence means that when the dispersed interval tends to zero, the solving of differential equations tends to the solving of original equation at the space point of all times consistent and arbitrary. Stability is such a basic condition, in such conditions the numerical solution of differential equations with time step will not unlimited increase. So as to ensure that the error between the numerical solution of differential equations and the original equation is strict bounded. In the third chapter we mainly discuss the constraints for time and discrete intervals of space as the stability and convergence of discrete Maxwell's equations, and the numerical dispersion analysis of space intervals.
     3、The Simplified absorbing boundary conditions of PML.
     From the beginning of simple interpolation border to later widely used Mur absorbing boundary, and the development of PML absorbing boundary in recent years. Its absorption is getting better and better. Because of the constraints of computer's capacity, the calculation of FDTD is only in a limited region. It is impossible to calculate the infinite structure directly. Therefore, we must set appropriate absorpting boundary conditions at the truncation department. To use the limited space grids to simulate open unlimited space or long unlimited transmission structure. Then to simulate a open domain of electromagnetic scattering process. Chapter IV presents the MUR absorbing boundary conditions and PML absorbing boundary conditions. On the basis of understanding of the parameter settings in the two-dimensional of PML. It is easy to extent to set parameters of 3D case. The simplification of PML application and programming realization are presented based on the PML structure and computing characteristics of the split fields in FDTD calculation. So that make the parameter settings of absorption boundary conditions in the program of MATLAB of FDTD method become clear and simple. Through calculating the split fields in FDTD, we get radiation field of 3D line source in the simplification of the PML, and contrast the PML and Mur method which used on the modulation excitation source to calculat the input impedance of shielding. At last the feasibility of simplified setting is drawn.
     4、Excitation source technology and the construction of excitation source in automotive.
     Practical electromagnetic issues always contain excitation source. So select a reasonable excitation source can avoid the harmful effects of the cut-off frequency component and can be effective in raising the calculation efficiency of FDTD method. Significant savings of time and computer memory space. In order to introduce the appropriate excitation source into numerical calculation of FDTD method. So simulate the problem of EMC correctly is very important. In the fifth chapter is a variety of excitation source technology. Through collecting the acquisition and experimental testing of the characteristic spectrum of vehicle ignition system, we get the actual amplitude and frequency points of interference which exceed the safety threshold. On the basis of proposing switch function, we applicate them into the amplitude and frequency of switch function to get correct modulation excitation source's simulation of interference which caused by the actual ignition system.
     5、The FDTD analysis of Electromagnetic radiation inside the automotive.
     The existence of major electromagnetic environment of vehicles is analyzed. According to Chapter IV from the radiation of electromagnetic interference of the actual data collection, we get the double modulation Time-harmonic field excitation source. We calculate the the radiation field of ignition System using FDTD method, and Simulate the spreading of radiation through different aperture size in different frequency radiation field. And extract the data of designated point in modulation field in order to compare with the experimental results. At the same time, we analysed the interference source of inductive load through modeling. And get the output map of inductive load in different response. Using the modulated excitation source to simulate the radiation of heater machine through the heater-hole of automotive in the method of FDTD analysis. Finally, calculated the value of radiation field in the gap through FDTD method, and analysed the interference of sensitive equipments' radiation field by means of the coupling. To provide a theoretical calculation basis of taking measures for minimizing the interference by the disturbance.
引文
[1]廖传书,戴焯.汽车电子产品的电磁环境[J].汽车电器,1995,(3):7-9.
    [2]张玉.电磁场并行计算.西安电子科技大学出版社[M].西安:2006.
    [3]陈淑凤等.电磁兼容试验技术[M].北京:北京邮电大学出版社,2001.3
    [4]GB/T 4365-1995,电磁兼容术语[S].
    [5]GJB 72-85,电磁干扰和电磁兼容性名词术语[S].
    [6]张林昌,戴焯.汽车电子产品的电磁环境[J].汽车电器,1995,(3):7-9.
    [7]廖传书,戴焯.汽车电子产品的电磁环境[J].汽车电器,1995,(3):7-91.
    [8]马兴义,杨立群.Matlab6应用开发指南[M].北京:机械工业出版社,2002.
    [9]吕英华.计算电磁学的数值方法[M].清华大学出版社,北京:2006.
    [10]Yee K S.Numerical solution of initial boundary value problems involving Maxwell equations in isotropic media.IEEE Trans[J].Antennas Propagat,May 1996,AP-14(3):302-307.
    [11]Mur G.Absorbing boundary conditions for the finite-difference approximation of the time-domain electromagnetic field equations[J].IEEE Trans Electromagn.Compat.,Nov.1981,EMC-23(4):377-382.
    [12]高本庆.时域有限差分法[M].北京:国防工业出版社,1995.
    [13]王飞,裴永祥.有限差分法的MATLAB编程[C].新疆师范大学学报,2003,Vol.22,No4.
    [14]王长清,祝西里.电磁场计算中的时域有限差分方法[M].北京:北京大学出版社,1994.
    [15]MinLi,Kuang_ping Ma,David M.Hockanson,Numerical and Experimental Corroboratio of an FDTD Thin_slot Model for Slots Near Comers of Shielding Enclosures[J].IEEE Trans.EMC,1997,39(3):225-232.
    [16]Jean_Pierre Berenger.A Perfectly Matched Layer for the Absorption of Electromagnetic Waves[J].J.Computational Physics,1994,114:185-200.
    [17]Jean_Pierre Berenger.Three_Dimensional Perfectly Matched Layer for the Absorption of Electromagnetic Waves[J].J.Computational Physics,1996,127:363-379.
    [18]FangJ,Wu Z.Generalized PML for the Absorption of Propagating and Evanescent Waves[J].IEEETrans.Microwave Theory and Techniques,1996,44(12):2216-2222.
    [19]Berenger J P.A Perfectly Matched Layer for the Absorption of Electromagnetic Waves[J].Toumal of Computational Physics 1994,114:185-200.
    [20]Katzeta D S.Validation and Extension to Three Dimensions of the Berenger PML Absorbing Boundary Condition for FDTD meshes[J].IEEE Microwave and Guided Wave Letters,1994,4(8):268-270.
    [21]Berenger J P.Three-Dimensional Perfectly Matched Layer for the Absorption Boundary Condition for FDTD mutation Physics[J],1996,127:363-379.
    [22]蔡仁刚.电磁兼容原理、设计和预测技术[M].北京:北京航空航天大学出版社,1997.
    [23]金建铭等.电磁场有限元方法[M].西安:西安电子科技大学出,1998,1:76-82.
    [24]戴焯等.汽车点火系电磁兼容性设计[J].汽车研究与开发,1994,4.
    [25]谢处方等.电磁场与电磁波[M].北京:高等教育出版社,1979:348-351.
    [26]张智星.MATLAB程序设计与应用[M].北京:清华大学出版社,2002.
    [27]周梅初.汽车电磁干扰的产生、抑制和测试[J].长沙:国防科技大学出版社,1992.
    [28]徐立,武建刚.电动汽车电磁辐射骚扰测量技术研究与实践[J].汽车工程,2006,Vol.28(5):427-429.
    [29]韦绍秋.汽车电磁干扰的产生与排除[R].大众科技,2005,No.2:33-35.
    [30]K.S.Yee.Numerical Solution of Initial Boundary Value Problems Involving Maxwell's Equations in Isotropic Media[J]. IEEE Trans, on Antennas and propagation, 1966, AP-14(8):302-307.
    [31] Allen Taflove, Radar Cross Section of General Three-Dimensional Scatters[J]. IEEE Trans. On Electromagnetic Compatibility, 1983, EMC-25(4):433-440.
    [32] Raymond Luebbers, Li.Chen. FDTD Calculation of Radiation Patterns, Imhedence. And Gain for a Monopole Antenna on a Conducting Box[J]. IEEE Trans. on Antennas and Propagation, 1992, AP-40 (12): 1577-1583.
    [33] Allen Taflove, A Hybrid Moment Method/Finite-Difference Time-Domain Approach to Elcetromagnetic Coupling and Apertures Penetration into Complex Geometries [J]. IEEE Trans. On Antennas and Propagation, 1982 AP-30(4): 617-627.
    [34] Q Mur, Absorbing Boundary Conditions for the Finite-Difference Approximation of theTime-Domain Electromagnetic Field Equations[J], IEEE Trans, on Electromagnetic Compatibility 1981 EMC-23(4):377-382.
    [35] K. S. Yee. Numerical solution of initial boundary value problems involving Maxwell's equations in isotropic media[J]. IEEE Transactions on Antennas and Propagation, 1966, Vol.14: 302-307.
    
    [36] J. J. P. Berenger, Perfectly Matched Layer for the FDTD Solution of Wave-Structure Interactions Problems[J], IEEE Trans, on Antennas and Propagation, 1996 AP-44(I).
    [37] Xu Li, Allen Taflove and Vadim Beckman. Modified FDTD Near-to-Far-Field Transformation for Improved Backscattering Calculation of Strongly Forward-Scattering Objects[J]. IEEE Antennas and Wireless propagation Letters, 2005, Vol.4:35-38.
    [38] Gedney S D.An Anisotropic Perfectly Matched Layers Absorbing Medium for the Truncation of FDTD lattices [J]. IEEE Trans Antennas and Propagat, 1996,44( 12): 1630-1639.
    [39] Gedney S D.An Anisotropic Perfectly Matched Layers Absorbing Medium for the Truncation of FDTD lattices[J].IEEE Trans Antennas and Propagat,1996,44(12):1630-1639.
    [40]沙奇林,莎莉.现代汽车电器电子系统[M].武汉:中国地质大学出版社,1993.
    [41]金建铭.电磁场有限元法[M].西安:西安电子科技大学出版社,1998.
    [42]徐立.汽车电子部件的电磁抗扰度技术要求[J].电子质量,2006,No.11:77-80.
    [43]南利平,吕洪国。电磁兼容性(EMC)的预测试[S].国外电子测量技术,1998,No.3:38-39.
    [44]吕飞燕,沙斐.用FDTD法分析开孔金属板的屏蔽效能[J].北方交通大学学报,2003,Vol.27,No.3.
    [45]俞恢春,罗宇翔.车载电子设备的EMC测试[J].测试与计量.
    [46][美]DeitelHM.C程序设计教程[M].薛万明译.北京:机械工业出社,2000.
    [47]法尹雷,殷晓星.电磁耦合问题的区域分解算[J).微波学报,2000,Vol.16(5):467-474.
    [48]葛德彪,闰玉波.电磁波时域有限差分法[M].西安:西安电子科技大学出社.2002.
    [49]高攸纲.电磁兼容总论[M]。北京:北京邮电大学出版社,2001.
    [50]白同云,吕晓德.电磁兼容设计[M].北京:北京邮电大学出版社,2001.
    [51]肖小军。电磁兼容(EMC)技术的发展动态[J]。湖南电力,2000,20(2):28-30.
    [52]Eva Part-Enander,Anders Sjoberg.The MATLAB 5Handbook[M].Beijing:China Machine Press,2000.1-6.
    [53]楼顺天,于卫等.MATLAB程序设计语言[M].西安:西安电子科技大学出版社,1998.1-10.
    [54]盛振华.电磁场与微波技术[M].北京:电子工业出版社,1998。
    [55]罗延钟.有限差分法[J].物化探电子计算技术,1982,6(1):75-88.
    [56]洪伟.电磁场边值问题的区域分解算法[M].科学出版社,北京:2005.
    [57]李宝全。电磁兼容测试工作与对策[J].标准化报道,1998,(3):41-45.
    [58]白同云,吕晓燕.电磁兼容设计[M].北京邮电大学出版社,2001.
    [59]Hirtenfelder,F.Markel,Predicting vehicle EMC/EMI performance with finite element software[J],Mechatronics,1993,p 639.
    [60]刘建鹏.汽车电磁辐射抗扰度试验信号解析[J].安全与电磁兼容,2005,Nol.6:13-15.
    [61]朱元丽,朱元清等.电磁干扰与电磁兼容设计[M].电脑开发与应用,2000,(1):14-17.
    [62]戴焯,廖传书.汽车点火系统电磁兼容性设计[J].设计与计算,2004.
    [63]仇雅莉.汽车点火系统故障诊断[J]。湖南交通科技,2004,Vol.30No.3
    [64]Kronberger,Rainer Hassmann,Gerd-Hinrich Schulz,Measurement and analysis of vehicle influences on the radiation pattern of SDARS-antennas[J],IEEE Antennas and Propagation Society,AP-S International Symposium,2002,Vol.4:740-743.
    [65]Imayakumar,A.Satyamurthy,S.Devarpiran,EMI- EMC studies on EMP protection system for fighting vehicles,Proceedings of the International Conference on Electromagnetic Interference and Compatibility,1999,p:35-38.
    [66]张子俊,高本庆.柱坐标系下FDTD算法的吸收边界条件[J].微波学报,1995,11(3):170-175.
    [67]ALLen Taflove,Susan C.Hagness.Computational Electrodynamics:The Finite-Difference Tune-Domain Method[J].London:Artech House.2000.
    [68]Qin Chen,Yong-Zhen Huang,Wei-Hua Guo and Li-Juan Yu.Analysis of Modes in a Freestanding Micro square Resonator by 3-D Finite-Difference Time-Domain Simulation[J].IEEE Journal of Quantum Electronics,2005:1-5.
    [69]M.J.Cyan,D.C.L.Wong,I.J.Craddock,S.Yu,J.Rorison,and C.J.Railton.Calculation of Losses in 2-D Photonic Crystal Membrane Wave Using the 3-D FDTD Method[J].IEEE Photonics Technology Letters,January 2005,Vol.17,No.l:58-60.
    [70]Antonio Soriano,Enrique A.Navarro,Dominique L.Paul,Jorge A.Ports,Juan A.Morente,and Ian J.Craddock.Finite Difference Time Domain Simulation of the Earth-Ionosphere Resonant Cavity:Schumann Resonances[J].IEEE Transactions on Antennas and Propagation,April 2005,Vo1.53,No.4:1535-1541.
    [71]Mur G.Absorbing Boundary Condition for the Finite-Difference Approximation of the Time-Domain Electromagnetic Field Equations[J].IEEE Trans.on EMC,1981,Vol.23,No.4:377-3 82.
    [72]Chen Z.H.and Hong W.Application of FD-MEI to electromagnetic scattering from transversally anisotropic inhomogeneous cylinders[J].IEEE Trans.on EMC,1998,Vol.40,No.2:103-110.
    [73]鲁述,徐鹏根.电磁场边值问题解析方法[M].武汉:武汉大学出版社,2005.102-104.
    [74]张子俊,高本庆。柱坐标系下FDTD算法的吸收边界条件[J]。微波学报,1995,11(3):170-175.
    [75]王秉中.计算电磁学[M].北京:科学出版社,2002.153-161.
    [76]甘甫烷,周佩白等.时域有限差分总场吸收边界条件的计算与验证[J],高压电器.2001,Vol.37,No.3:15.
    [77]熊彬,阮百尧.MATLAB在有限差分法中的应用[J],桂林工学院学报.2001,Vol.21.No.2.

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