I am solving a boundary value problem and stuck at simple algebra part. I've four equation as:
- $E_i+E_r=E_++E_-$
- $E_i-E_r=n(E_+-E_-)$
- $E_t=E_+e^{i\phi}+E_-e^{-i\phi}$
- $n(E_+e^{i\phi}-E_-e^{-i\phi})=E_t$
Here n and $\phi$ are constants. And I am trying to express $E_t$ and $E_r$ in terms of $E_i$ separately. Any kind of idea will be highly appreciated.
Thank you in advance.
Step 1: Use equations 1 and 2 to express $E_+$ and $E_-$ in terms of $E_i, E_r$ and $n$: $$ E_+ = \frac1{2n} (E_i -E_r + n(E_r + E_i))\\ E_- = \frac1{2n} (E_r -E_i + n(E_r + E_i)) $$ Step 2: Substitute for $E_+$ and $E_-$ in equations 3 and 4: $$ 3: E_t = \frac1{2n} \left( e^{i\phi} (E_r-E_i+n(E_r+E_i)) + e^{-i\phi} (E_r-E_i-n(E_r+E_i)) \right) \\E_t= \frac1n\left[ (n\cos\phi +i\sin\phi)E_i + (n\cos\phi -i\sin\phi)E_r) \right]$$ and$$ 4:E_t = (\cos\phi + ni\sin\phi)E_i -(\cos\phi -ni\sin\phi)E_r $$ Step 3: Equate those two expressions for $E_t$ and thus have one equation to solve for $E_r$ in terms of $n,\phi,E_i$: $$ E_r = -E_i \frac{(n^2-1\sin\phi}{(n^2+1)\sin\phi+2in\cos\phi} $$ Step 4: substitute $E_r$ into either of the $E_t$ expressions and simplify to get $$ E_t = E_i\frac{2in}{2in\cos\phi+(n^2+1)\sin\phi} $$ Don't be scared by the fact that the expressions imply complex values; i fact, in a general medium, the index of reflection $n$ is also complex.
Do be scared by the fact that in the first edition of Jackson, problem 7.5 is different, asking for the transmission coefficient when a plane wave strikes a thin or thick "excellent conductor." If I remember correctly, the solution to that problem is more difficult.