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Lindsey Yue edited section_Reflection_Coefficients_The_reflection__.tex
almost 8 years ago
Commit id: ae6104ab9c21a048d36266700f4472281afcc111
deletions | additions
diff --git a/section_Reflection_Coefficients_The_reflection__.tex b/section_Reflection_Coefficients_The_reflection__.tex
index 02f17c7..ee4d32b 100644
--- a/section_Reflection_Coefficients_The_reflection__.tex
+++ b/section_Reflection_Coefficients_The_reflection__.tex
...
\mathbf{H}_{0\mathrm{i}} e^{-2 \pi i \left( \mathbf{w}'_{\mathrm{i}} \cdot \mathbf{r} - i \mathbf{w}''_{\mathrm{i}} \cdot \mathbf{r} \right)} \times \mathbf{\hat{n}} + \mathbf{H}_{0\mathrm{r}} e^{-2 \pi i \left( \mathbf{w}'_{\mathrm{r}} \cdot \mathbf{r} - i \mathbf{w}''_{\mathrm{r}} \cdot \mathbf{r} \right)} \times \mathbf{\hat{n}} = \mathbf{H}_{0\mathrm{t}} e^{-2 \pi i \left( \mathbf{w}'_{\mathrm{t}} \cdot \mathbf{r} - i \mathbf{w}''_{\mathrm{t}} \cdot \mathbf{r} \right)} \times \mathbf{\hat{n}}
\end{equation}
%
With the coordinate origin on the boundary, at the point $\mathbf{r}=0$, Eqs.\ \ref{eq:eboundary}
and \ref{eq:hboundary} become
%
\begin{equation}
\left(\mathbf{E}_{0\mathrm{i}} + \mathbf{E}_{0\mathrm{r}} \right) \times \mathbf{\hat{n}} = \mathbf{E}_{0\mathrm{t}} \times \mathbf{\hat{n}}
...
%
\begin{equation}
\left( \mathbf{H}_{0\mathrm{i}} + \mathbf{H}_{0\mathrm{r}} \right) \times \mathbf{\hat{n}} = \mathbf{H}_{0\mathrm{t}} \times \mathbf{\hat{n}}
\end{equation}
%
These equations can then be broken into parallel and perpendicular components.
%
\begin{equation}
\left[ \left( E_{\parallel\mathrm{i}} + E_{\parallel\mathrm{r}} \right) \mathbf{\hat{e}}_{\parallel} + \left( E_{\perp\mathrm{i}} + E_{\perp\mathrm{r}} \right) \mathbf{\hat{e}}_{\perp}\right] \times \mathbf{\hat{n}} = \left[ E_{\parallel\mathrm{t}} \mathbf{\hat{e}}_{\parallel} + E_{\perp\mathrm{t}} \mathbf{\hat{e}}_{\perp} \right] \times \mathbf{\hat{n}}
\end{equation}