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Evanescent Field due to Total Internal Reflection

Note that if $ c_1 < c_2 \vert\sin(\theta_1^+)\vert$, the horizontal component of the wavenumber in medium 2 becomes imaginary:

But what does it mean?

\begin{eqnarray*}
p(t,\underline{x}) &=&
\cos\left(\omega t - \underline{k}^T\...
...{-k_x x}\right\}}}\\ [5pt]
&=& e^{-k_x x} \cos(\omega t - k_y y)
\end{eqnarray*}


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Download Scattering.pdf
Download Scattering_2up.pdf
Download Scattering_4up.pdf

``Scattering at an Impedance Discontinuity'', by Julius O. Smith III, (From Lecture Overheads, Music 420).
Copyright © 2007-05-14 by Julius O. Smith III
Center for Computer Research in Music and Acoustics (CCRMA),   Stanford University
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