钢筋混凝土结构的微波成像正问题研究
详细信息    本馆镜像全文|  推荐本文 |  |   获取CNKI官网全文
摘要
随着电磁学理论的发展和计算机性能的不断提高,计算电磁学在最近几年得到了长足的发展。时域有限差分方法是计算电磁学里重要的研究方法,它将电场和磁场在时间顺序上交替抽样,将电磁场在空间上划分为Yee元胞,即将麦克斯韦方程离散以后构成显式差分方程,然后在时间上迭代求解。因而,由给定响应电磁问题的初始值,时域有限差分方法就可以逐步推进地求得以后各个时刻空间电磁场的分布。所以本文将采用时域有限差分方法解决实际问题。
     本文以微波在钢筋混凝土中的传播为研究对象开展正问题计算研究。依照时域有限并分法的基本思想,结合钢筋混凝土结构的微波检测原理,给出了具体的解题步骤。其中包括:计算测量钢筋混凝土结构的微波频段;对模型进行网格剖分;由麦克斯韦方程得到描述高频电磁场的差分方程对每个Yee氏单元进行差分计算;再根据入射平面波的加入条件,设定以0°角加载到总场边界;在空气的最外层用完全匹配层(PML)截断仿真区间来模拟无限大自由空间中钢筋混凝土的散射问题。本文在吸收边界的选取中,用MATLAB编写了两种吸收边界的程序来模拟波在自由空间中的传播,从理论比较到数值仿真的比较发现PML吸收边界法优于Mur吸收边界法。
     最后,建立了多个不同规格的钢筋混凝土模型。用3.0GHz频率的微波进行仿真,用Fortran语言编写程序,得到场强-位置关系图象,形象直观的显示了在混凝土内存在钢筋的情况。把该仿真结果与ANSYS的仿真结果进行归一化比较,曲线趋势比较一致。结果表明,整个问题的设计思路是正确的。用时域有限差分法实现钢筋混凝土中的微波场数值计算是可行的,而且方便快捷的。
With the development of the electromagnetic theory and the improvement of the computer performance, the computational electromagnetism has been developed fatherly in recent years. Finite Difference Time Domain (FDTD) method is an important method of computational electromagnetic research. It alternately samples chronological electric and magnetic fields, meshes the electric field into Yee unit, that is to say, disperses Maxwell's equations into the explicit differential equations, and gets the iterative solution. Therefore, with the initial value of given reply electromagnetic problem, the FDTD method is able to get the electromagnetic field distribution in space at anytime step by step. Here will take the FDTD method to solve practical problems.
     In this paper, microwave dissemination in the reinforced concrete as research subjects for questions compute and research. The specific problem-solving steps are given according to basic idea of FDTD and the microwave detection principle of the reinforced concrete structure. Including calculating the microwave frequency band of measuring reinforced concrete structure, meshing the model, differential equations describing high-frequency electromagnetic fields from Maxwell's equations to difference calculate for each Yee unit, loading the plane wave to the boundary of the total field with 0 degree according to the condition of its accession, and in the outer layer truncating the simulation region with PML, using this model to simulate the scatting of reinforced concrete in infinite space. In the selection of the absorbing boundary, this paper programming two absorbing boundaries to simulate propagation of wave in free space with MATLAB. From the theoretical comparison to the numerical simulation, it is found that the PML absorbing boundary condition is superior to Mur absorbing boundary condition.
     Finally, Variable specification reinforced concrete models are built and simulation is made on 3.0GHz microwave frequency by using Fortran programming language. By this way, electric field intensity-location relation image is received. It displays steel bar distributing situation in concrete intuitively. Compare with the normalized simulation result of ANSYS, the curves superposition degree is satisfying with small error. The results indicate that the whole design is reasonable. It is feasible and convenient to realize nondestructive testing for reinforced concrete structure by using FDTD method.
引文
[1]曾海宁,曾美玉,曾芳金.混凝土无损检测方法及应用展望.山西建筑,2007,3(28):88-89.
    [2]赵永辉,吴健生,万明浩.钢筋混凝土地层透视雷达无损检测技术.工程勘察,2002,64-66.
    [3]周燕小,坛陶里.混凝土内部雷达探测仪的工程应用.施工技术,1997,6,28-29.
    [4]#12
    [5]#12
    [6]#12
    [7]Zoughi R.Microwave and millimeter wave non - destructive testing[J],a succinct review.Mater.Eval.1995,53:461-462.
    [8]Nathan Ida.Microwave Nondestructive Testing,Kluwer Publishing Company,1992.
    [9]Zoughi R,Ganchev S I.Application of microwave nondestructive testing and evaluation to thick composites.Proceedings of the NDE,Applied to Process Control of Composite Fabrication,St.Louis,Missouri,1994.
    [10]Weedon W H,Chew W C,Mayes P E.A step frequency radar imaging system for microwave nondestructive evaluation,Progress in Electromagnetics Research.2000,18:121-146.
    [11]Ghodgaonkar Deepak K,et al.Microwave nondestructive testing of Malaysian timber for grading applications,Proceedings of the 14th WCNDT,New Delhi,1996.
    [12]张丽霞.电磁场有限元分析中并行计算的研究:(硕士学位论文).天津:河北工业大学 2006.
    [13]曾新,苏杰.微波无损检测技术及应用.仪器仪表用户,2003,2.
    [14]龚杏.微波断层成像重建算法研究:(博士学位论文).杭州:浙江大学 2001.
    [15]李志平,何国瑜.基于STOLT插值聚焦的二维近场微波成像.电波科学学报,2007,22(1):12-17
    [16]李杰.微波成像算法研究:(硕士学位论文).西北工业大学,2002,1.
    [17]Cadall N,Munson D C.J r.A simulation study of the ω- k SAR algorithm for the highly squinted case with application to runway imaging[C].In Proc.IEEE Int.Conf.Acoust.Speech and Signal Processing Istanbul,Turkey.2000,5:3025-3028.
    [18]倪光正,钱秀英.电磁场数值计算.北京:高等教育出版社,1996,3(9):183-191.
    [19]倪光正.工程电磁场原理.北京:高等教育出版社,2004.
    [20]杜平安,甘娥忠,于亚婷.有限元法-原理、建模及应用.北京:国防工业出版社,2006.
    [21]何红雨.电磁场数值计算法与MATLAB实现:(硕士学位论文).上海:华北师范大学,2004.
    [22]魏学旺.电磁波在钢筋混凝土墙中的反射与透射研究:(硕士学位论文).汕头:汕头大学,2007.
    [23]R.Dalke,C.L.Holloway,P.Mckenna,M.Johansson,and A.S.Ali,"Effects of reinforced concrete structures on RFcommunications",IEEE Transactions on Electromanetic compatibility,2000,42(4):117-121.
    [24]Elodie Richalot,Matthieu Bonilla,Man-Fai Wong,"Electromagnetic propagateion into Reinforced-Concrete Walls",IEEE Transations on Microwave Theory and Techniques,2000,48(3):121-124.
    [25]R.Paknys,"Reflection and transmitsion by reinforced concrete-numerical and asymptotic analysis",IEEE Trans.Antennas Propagat,2003,51(10):489-494.
    [26]Daniel Pena,Rodolfo Feict,"Measurement and modeling of propagateion losses in brick and concrete walls for the 900-MHz band",IEEE Trans.Antennas Propagat,2003,51(1):1521-1527.
    [27]秦卫平,丁胜高,张业荣.时域分析钢筋混凝土砖墙对电磁脉冲短径传播的影响,南京邮电学院学报,2005,25(6),12-16.
    [28]倪光正,杨仕友,钱秀英.工程电磁场数值计算.机械工业出版社,2006.
    [29]苏俊宏.屯磁场数值分析方法讨论.西安工业学院学报,1994,14(3):191-197.
    [30]Nannapaneni Narayana Rao(著),周建华游佰强(译).工程电磁学基础.北京:机械工业出版社 2006,459-483.
    [31]何红雨.电磁场数值计算法与MATLAB实现.武汉:华中科技大学出版社,2004.
    [32]贺昌辉.矩量法分析目标的近场电磁散射:(硕士学位论文).武汉:华中师范大学,2006.
    [33]王涛.电磁场计算中的时域有限差分法的研究:(硕士学位论文).长春:吉林大学,2003.
    [34]金建铭,王建国,葛德彪.电磁场有限元方法.西安:电子科技大学出版社,1997.8-22.
    [35]范瑾.应用于电磁散射分析的有限元算法研究:(硕士学位论文).西安:西北工业大学,2006.
    [36]Schroeder W,Wolff L The Origin of Spurious Modes in Numerical Solutions of Electromagnetic Field Eigenvalue Problems.IEEE Trans M T T,1994,42(4):644-653.
    [37]Sony B,Albert H,Baudrand H.Elimination of Spurious Solutions in the Caculation of Eigenmodes by Moment Method.IEEE Trans M T T,1996,44(1):154-15.
    [39]王增和,王培章,卢春兰.电磁场与电磁波.北京:电子工业出版社,2001.
    [40]李书芳,李莉,张阳安等.电磁场与电磁波.北京:科学出版社,2004.
    [41]矩量法分析目标的近场电磁散射:(硕士学位论文).武汉:华中科技大学.2006.
    [42]孔金瓯.电磁波理论.北京:高等教育出版社,2002.
    [43]葛德彪,闫玉波.电磁波时域有限差分方法,西安:电子科技大学出版社,2002.
    [44]高本庆.时域有限差分法FDTD Method.北京:国防工业出版社,1995.
    [45]郭春波.时域有限差分法的MATLAB仿真,现代电子技术,2003,11,16-20.
    [46]李军,武振波,武哲.稳定因子对FDTD数值计算的影响.北京航空航天大学学报,2004,30(1):70-73.
    [47]李伟,赵春晖,徐娜.基于MATLAB的时域有限差分法(FDTD)的研究.牡丹江大学学报,2007,16(7):91-102.
    [48]杨芳.电磁波作用下人体的电场应力分布:(硕士学位论文),硝安:西安电科技大学,2002
    [49]C.D.Taylor,D.H.lam and T.H.shumpert,"Electromagnetic Pulse Scattering in Time-Varying Inhomogeneous Media",IEEE Trams.Antennas Propagat.,Vol.AP-17,No.5,pp.585-589,1969.
    [50]A.Taflove and M.E.Brodwin,"Numerical Solution of Steady-State Electromagnetic Scattering Problems Using the Time-Dependent Max well's Equations",IEEE Trans.On Microwave Theory tech.,Vol.Mtt-23,pp.623-630,1975.
    [51]易春.基于时域有限差分(FDTD)法的电磁场通用仿真软件设计:(硕士学位论文),成都:电子科技大学,2002.
    [52]葛德彪,石守元,朱之伟.一种新的FDTD入射场设置方法.微波学报,1995,11(3):187-191.
    [53]张清河.时域有限差分(FDTD)法中的吸收边界条件.三峡大学学报,2006,26(5):464-467.
    [54]R.J.Luebbers.F.Hunsberger.K.S.Kunz et al.A frequency-dependent finite- difference time-domain formulation for dispersive materials.IEEE Trans.on EMC,Vol.32.No.3.199..pp222-227;
    [55]赵辉.基于MATLAB交互式软件包实现对FDTD算法的改进.电气电子教学学报,2005,27(1):39-41.
    [56]郝彬,王江爱,姚纪欢.三维FDTD中完全匹配层的应用.宝鸡文理学院学报,1999,19(3):47-51.
    [57]陈彬,方大纲.完全匹配层PML吸收边界条件的理论分析.微波学报,1996,12(2):109-115.
    [58]Bernger J P.A perfectly matched layer for the absorption of electrom agnetic waves.J ComputPhys,1995,144(2):185-200.
    [59]李黎,李永东,刘纯亮.完全匹配层产生数值反射的原因分析.真空电子技术,2004,3,59-61.
    [60]方大纲,陈彬.完全匹配层(PML)的研究进展.南京理工大学学报,1996,20(6):572-576.
    [61]Berenger J P.Three-dimensional perfectly matched layer for the absorption of electron agnetic-waves.J ComputPhys,1996,127(2):363-379.
    [62]宋铮,沈爱国,邢军.PML吸收边界条件在微带天线计算中的应用.微波学报,2002,18(3):43-48.
    [63]钟选明,廖成,杨丹.一种有效的吸收边界条件及其应用.微波学报,2002,18(3):14-17.
    [64]马比武,高攸纲:时域有限差法中几种吸收边界条件的比较与数值验证.长沙大学学报,1999,13(4):1-4.
    [65]胡来平,刘占军.FDTD方法中的吸收边界条件.现代电子技术,2003,9,30-32.
    [66]彭国伦.Fortran95程序设计.北京:中国电力出版社,2007,9.
    [67]刘卫国.MATLAB程序设计与应用.北京:高等教育出版社 2006.
    [68]阎照文.ANSYS10.0工程电磁分析技术与实例详解.北京:中国水利水电出版社,2006,294-300.
    [69]张秋菊,时域有限差分电磁仿真软件的三维网格剖分及其设计:(硕士学位论文),成都:电子科技大学,2005,2.
    [70]郑木生.基于MATLAB语言实现电磁场中的FDTD算法编程.现代电子技术,2005,8,45-46.
    [71]薛晓春,刘波.在FDTD计算中对连接边界条件及其编程思想的改进.数值计算与计算机应用,2004,212-218.
    [72]武志刚,时域有限差分法通用类库的研制:(硕士学位论文),武汉:华中科技大学,2004.

© 2004-2018 中国地质图书馆版权所有 京ICP备05064691号 京公网安备11010802017129号

地址:北京市海淀区学院路29号 邮编:100083

电话:办公室:(+86 10)66554848;文献借阅、咨询服务、科技查新:66554700