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Approximate Current on a Wire – A Differential Equation Method Adam Schreiber, Yuriy Goykhman, Chalmers Butler
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Outline Derivation Solution Method – Solve DE and Iterate Sample Data Discussion Conclusion
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Integral Equation Reference Integral Equation Method Break K(z-z’) into it’s real and imaginary parts K R (z-z’) resembles the delta function K I (z-z’) resembles sin(x)/x
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Justification of K R Approximation
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Approximation For 0.4 & 0.8 λ
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Differential Equation Second Order Differential Equation I(-h)=I(h)=0
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Pulse Test Evaluate the Differential Equation at m points Creates N equations in I(z) Changes intervals from (-h, h) to (z m - Δ/2, z m + Δ/2)
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Triangle Expansion Replaces I(z) with N unknowns We now have N equations with N unknowns
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MatrixEquation
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Solution Method Generate tri-diagonal matrix Find I 0 with J 0 = 0 Generate a new right hand side Find I p Repeat the above 2 steps till convergence Compare results with integral equation data
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0.4 Wavelength
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0.8 Wavelength
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1.0 Wavelength
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Error:
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Lengths without Convergence Region around 0.5 λ Region around 1.5 λ Odd multiples of 0.5 λ
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Reasons for Error Initial delta function approximation Accuracy of evaluating Almost singular matrices at non- convergent lengths
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Future Work Increase efficiency/speed Extend algorithm to bent/curved wires Improve numerical integration methods
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Conclusion Provides good approximations for current on wires, although not near lengths equal to odd multiples of 0.5 λ Can be adjusted to improve speed and increase accuracy Perhaps, method can be fixed for lengths near 0.5 λ
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Acknowledgements Clemson University NSF Dr.Butler Dr. Noneaker & Dr. Xu
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Psi R
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