Note that we use the boundary condition (last slide), together with
the relations between E and B following from their
positions in the expression for the Poynting vector (one before the
last slide below). That is how n1 and n2 enter
below
Here we work with the s-polarization, or the TE-polarization
1-work-with_B_and_E_transm.png
2a-s-polarized-derivation.png
The same as above - a bit more complicated manipulations
2b-P-polarized-derivation.png
- s-polarization, or the
TE-polarization geometry
4-summary-T_and_R.png
TRANSMISSION AND REFLECTION COEFFICIENTS
and Transmittance
and Reflectance
5-transmittance_reflectance_a.png
5-transmittance_reflectance_a.png
Transmittance and
Reflectance - relation summary
5-transmittance_reflectance_note.png
5-transmittance_reflectance_note.png
The relations between B and E (or less consistently here between
H and E) from the energy and transport. This relation naturally exists only
in the electromagnetic wave, not generally
6-energy-momentum-densities.png
6-energy-momentum-densities.png
Boundary conditions
on an interface (two media)