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Input Impedance of a Vertical Electric Dipole above earth Thomas Ng, RHIT Advisor: Prof. Xiao-Bang Xu SURE Program 2004 Clemson University July 27, 2004
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Outline Why is this hard ? Why is this interesting ? How do we do it ?
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Historical Overview Marconi’s Wireless Telegraph 1901 Sommerfeld’s Formulation 1909 Sommerfeld-Type Integrals Lossy Earth Air Dipole h R Observation
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Sommerfeld Integrals No analytic solution Oscillate Rapidly Decay Slowly Infinite
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Applications Design and development of communications systems Efficiency and cost considerations Scattering Problems Mine Detection
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Impedance Problem Induced EMF Method Sinusoidal Current Approximation Lossy Earth, ε r Air Half- Wavelength Dipole h 2*l z0z0 z1z1 z2z2
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Impedance Problem
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Complex Image Technique
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CIT Results
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Exact Image Theory Laplace Transforms performed on reflection coefficients Change order of integration
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Exact Image Theory Eliminates bad behavior of Sommerfeld Integral
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Impedance Problem Superposition Induced EMF Method
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Comparing Results: Z in
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Comparing Results: Time
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Conclusions Varying ground conditions affect input impedance There are different ways to avoid Sommerfeld-type Integrals Accuracy and Computation Time tradeoff
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Future Work More accurate expression for antenna current Investigate EIT method more completely
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Acknowledgements Prof. Xiao Bang Xu Prof. Daniel L. Noneaker
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Questions ?
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References Shubair and Chow Sarabandi and Casciato Kraus Balanis Collins Chow, Yang, Fang, and Howard Askun and Mitra Frohmberg
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Complex Image Technique z=0 2*l h dqdq d1d1 d2d2 Original antenna Real quasi-dynamic image Complex Images d q = l+h d 1 = l+h-j*b 1 d 2 = l+h-j*b 2
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Exact Image Theory Verification of Infinitesimal Dipole Results
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