To determine the intensity of transmitted light through the second polaroid \(P_2\) when unpolarized light \(I_0\) is incident on the first polaroid \(P_1\), we use Malus's Law and the properties of polaroids. Let's solve the problem step-by-step:
This is because a polaroid only allows the component of light polarized in its axis to pass through, reducing the intensity by half.
Since \(\cos(45^\circ) = \frac{\sqrt{2}}{2}\), we have:
\(I_2 = \frac{I_1}{2} = \frac{I_0}{4}\).Similarly, because \(\cos(45^\circ) = \frac{\sqrt{2}}{2}\), we find:
\(I_3 = \frac{I_2}{2} = \frac{I_0}{8}\).Thus, the intensity of the light transmitted through \(P_2\) is \(\frac{I_0}{8}\), which matches the correct answer.
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: