Brewster's Law: This law states that for a particular angle of incidence, known as Brewster's angle or the polarizing angle (\(i_p\)), the reflected light from a transparent dielectric surface is completely plane-polarized. This occurs when the reflected ray and the refracted ray are perpendicular to each other.
Derivation:
Let unpolarized light be incident at Brewster's angle \(i_p\) on the surface separating two media (e.g., air and glass) with refractive indices \(n_1\) and \(n_2\) respectively. Let \(r\) be the angle of refraction.
According to Snell's law:
\[ n_1 \sin(i_p) = n_2 \sin(r) \quad \cdots (1) \]
By the condition of Brewster's law, the reflected and refracted rays are perpendicular. From the geometry of reflection and refraction, this means:
\[ i_p + r = 90^{\circ} \]
\[ r = 90^{\circ} - i_p \]
Now, substitute this value of \(r\) into Snell's law (equation 1):
\[ n_1 \sin(i_p) = n_2 \sin(90^{\circ} - i_p) \]
Since \(\sin(90^{\circ} - \theta) = \cos(\theta)\), the equation becomes:
\[ n_1 \sin(i_p) = n_2 \cos(i_p) \]
Rearranging the terms to find the angle \(i_p\):
\[ \frac{\sin(i_p)}{\cos(i_p)} = \frac{n_2}{n_1} \]
\[ \tan(i_p) = \frac{n_2}{n_1} \]
If the first medium is air or vacuum (\(n_1 \approx 1\)) and the second medium has refractive index \(n\) (\(n_2 = n\)), the formula simplifies to:
\[ \tan(i_p) = n \]
This is the formula for Brewster's angle.