$60^\circ$
To determine the angle of incidence such that the reflected and refracted rays are perpendicular, we can utilize the concept of Brewster's angle. When the reflected and refracted rays are perpendicular, the angle of incidence is known as Brewster's angle.
Brewster's angle, denoted as \( \theta_B \), can be calculated using the formula:
\[\tan \theta_B = \frac{n_2}{n_1}\]
Where:
In this problem:
Substituting the given values into the Brewster's angle formula:
\[\tan \theta_B = \frac{2\sqrt{3}}{2} = \sqrt{3}\]
The angle whose tangent is \( \sqrt{3} \) is \( 60^\circ \), as:
\[\tan 60^\circ = \sqrt{3}\]
Therefore, the angle of incidence \( \theta_B \) is \( 60^\circ \).
Thus, the correct answer is: \( 60^\circ \)
A beam of unpolarised light of intensity \( I_0 \) is passed through a polaroid A and then through another polaroid B which is oriented so that its principal plane makes an angle of 45° relative to that of A. The intensity of emergent light is:
Two polaroide $A$ and $B$ are placed in such a way that the pass-axis of polaroids are perpendicular to each other Now, another polaroid $C$ is placed between $A$ and $B$ bisecting angle between them If intensity of unpolarized light is $I _0$ then intensity of transmitted light after passing through polaroid $B$ will be: