An electromagnetic wave travels from vacuum into a non-magnetic medium. We are given the incident electric field amplitude, $E_0$, and the transmitted electric field amplitude, $E_t = 2E_0/3$. We need to find the refractive index, $n$, of the medium.
The transmission coefficient ($t$) relates the transmitted electric field amplitude to the incident electric field amplitude:
$t = \frac{E_t}{E_0}$Substituting the given values:
$t = \frac{2E_0/3}{E_0} = \frac{2}{3}$For an electromagnetic wave normally incident from vacuum (refractive index $n_1 = 1$) onto a non-magnetic medium (refractive index $n_2 = n$), the transmission coefficient ($t$) is given by the formula:
$t = \frac{2n_1}{n_1 + n_2}$Since the wave is incident from vacuum, $n_1 = 1$. Let the refractive index of the medium be $n$. The formula becomes:
$t = \frac{2(1)}{1 + n} = \frac{2}{1 + n}$Now, we equate the two expressions for the transmission coefficient:
Therefore:
$\frac{2}{3} = \frac{2}{1 + n}$By comparing the denominators (since the numerators are equal):
$3 = 1 + n$Solving for $n$:
$n = 3 - 1 = 2$The refractive index of the medium is 2.
A monochromatic plane wave is incident normally from a dielectric medium $A$ onto another dielectric medium $B$. The indices of refraction satisfy $n_A < n_B$. One-fourth of the incident energy is reflected back into medium $A$. Let $E$ be the resultant electric field due to the superposition of the incident wave and the reflected wave. Then, the ratio of the two time-averages $\langle \vec{E}^2 \rangle_{\text{min}}/\langle \vec{E}^2 \rangle_{\text{max}}$ is
A beam of unpolarized light in a medium with dielectric constant $\epsilon_1$ is reflected from a plane interface formed with another medium of dielectric constant $\epsilon_2 = 3\epsilon_1$. The two media have identical magnetic permeability. If the angle of incidence is $60^\circ$, then the reflected light