Step 1: Concept Identification:
This problem applies Malus's Law to determine light intensity through three polarizers (P1, P2, P3). P3 is oriented perpendicular to P1.
Step 2: Governing Equation:
Malus's Law: \( I = I_{inc} \cos^2\theta \), where \( \theta \) is the angle between transmission axes and \( I_{inc} \) is incident intensity.Let \( \theta_1, \theta_2, \theta_3 \) be the angles of P1, P2, and P3 respectively.
Step 3: Intensity Analysis:
Initial unpolarized light intensity: \( I_0 \).P1 transmits \( I_1 = I_0/2 \). Set \( \theta_1 = 0 \).P3 is crossed with P1, so \( \theta_3 = \pi/2 \).P2's axis is at angle \( \theta \) relative to P1, so \( \theta_2 = \theta \).Intensity progression:1. After P1: \( I_1 = I_0/2 \).2. After P2: Incident intensity \( I_1 \) at angle 0. Angle between P1 and P2 is \( \theta \). \( I_2 = I_1 \cos^2(\theta) = \left(\frac{I_0}{2}\right) \cos^2(\theta) \)3. After P3: Incident intensity \( I_2 \) at angle \( \theta \). P3 axis is at \( \pi/2 \). Angle between P2 and P3 is \( (\pi/2 - \theta) \). \( I_3 = I_2 \cos^2(\pi/2 - \theta) = I_2 \sin^2(\theta) \) Substituting \( I_2 \): \( I_3 = \left(\frac{I_0}{2}\right) \cos^2(\theta) \sin^2(\theta) \)To maximize \( I_3 \), use \( \sin(2\theta) = 2\sin\theta\cos\theta \):\( I_3 = \frac{I_0}{2} \left(\frac{\sin(2\theta)}{2}\right)^2 = \frac{I_0}{8} \sin^2(2\theta) \)\( I_3 \) is maximum when \( \sin^2(2\theta) = 1 \).This occurs when \( \sin(2\theta) = \pm 1 \), leading to \( 2\theta = \pi/2, 3\pi/2, \dots \), and thus \( \theta = \pi/4, 3\pi/4, \dots \).The relevant angle is \( \pi/4 \).
Step 4: Conclusion:
Maximum transmitted intensity occurs when the angle between P1 and P2 is \( \pi/4 \).
