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    Please use this identifier to cite or link to this item: http://tkuir.lib.tku.edu.tw:8080/dspace/handle/987654321/35647

    Title: 應用時域有限差分法於平面天線結構的分析
    Other Titles: Application of fdtd method to the analysis of planar antenna structure
    Authors: 涂志明;Tu, Chih-ming
    Contributors: 淡江大學電機工程學系碩士班
    李慶烈;Li, Ching-lieh
    Keywords: 有限時域差分法;透明源;平面天線;遞回損失;輻射場型;FDTD;transparent source;planar antenna;S11;radiation pattern
    Date: 2008
    Issue Date: 2010-01-11 06:57:07 (UTC+8)
    Abstract: 本論文探討有限時域差分法(Finite Difference Time Domain ,FDTD)應用於平面天線結構的分析。首先,對於激發源的設置方式,本論文探討由微帶線饋入的結構中,以更新方程式建立穩定的入射電場,並對於兩種不同的激發方式進行比較,一是在微帶線與完美匹配層(PML)的介面處激發,叧一是在微帶線上某處做激發,比較二種激發方式的異同。
    當要進一步分析天線的S11參數,其過程需經二次(two passes)的計算,第一次(first pass)的計算只模擬天線的傳輸線結構部分,以在觀測點處獲取記錄入射波隨時間的波形變化,第二次(second pass)的計算則是對包含天線的完整結構進行分析,此次的目的在觀測點處記錄反射波隨時間的波形變化,再由傅立葉轉換進而得到兩者的比值(即S11值)。
    In this thesis the method of finite difference time domain (FDTD) is
    applied for the analysis of several structures of the planar antenna. First of all,
    about the establishment of the stimulating sources to excite the antenna
    structures, two modeling methods are examined and compared in this thesis
    for the microstrip feed line structures by using the FDTD updating equations
    in order to set up steady incidence electric field. One is set up the
    stimulating source at interface of the perfectly matched layer (PML) and the
    microstrip line, while the other is to set up the stimulating source at a certain
    place of the microstrip line. The similarities and differences of the above two
    stimulating sources are examined.

    The profound theory for the FDTD method to calculate the radiated far
    field of the antennas is based the equivalent principle of the electric magnetic
    field. In this thesis, the frequently-used formulas employed for the near-field
    to far-field transformation in either frequency domain and time domain is
    exhaustively reviewed. The needed coordinate transformation from spherical
    coordinate to rectangular coordinate is carried out in order to execute the
    integration to sum up the far field contribution in the free space in terms of
    the equivalent magnetic currents and the equivalent electric currents.
    The calculation of the S11 parameter of the antenna is regularly required,
    the course needs to pass for twice calculation (two passes) usually. The first
    pass is to analyze the structure of the transmission line part only such that at
    an observation point the incident wave is calculated and saved for later usage.
    The second pass is to analyze the structure of the whole structure that include
    antenna. The purpose of this time is to calculate the reflection wave from the
    antenna at the same observation point. The Fouries transforms for both the
    incident and reflected waves are then performed, while the ratio of the two
    results in value of the S11 parameter.
    Finally, in this thesis the above-mentioned FDTD method is applied to
    calculate the S11 and the far field patterns of three kinds of plane antennas.
    Then, the simulated results are compared with those obtained with the
    commercial EM softwares HFSS and IE3D, and with the measured results. It
    is found that when the planar substrate of the antennas extends into the PML
    to model an infinite substrate, the results could match quite well with those
    obtained by using the software IE3D which justify the effectiveness of
    applying the FDTD method for the planar antennas structures.
    Appears in Collections:[電機工程學系暨研究所] 學位論文

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