To solve this problem, we need to understand how the intensity of light behaves when a plane polarized light passes through a polarizer. The intensity of light passing through a polarizer is given by Malus's Law, which states that:
\(I = I_0 \cos^2(\theta - \phi)\)
where:
We are given four different angles of the polarizer \((\theta = 8^{\circ}, 38^{\circ}, 188^{\circ}, 218^{\circ})\) where the intensity \(I\) is the same. According to Malus's Law, the calculated intensities being the same implies:
\(\cos^2(8^{\circ} - \phi) = \cos^2(38^{\circ} - \phi) = \cos^2(188^{\circ} - \phi) = \cos^2(218^{\circ} - \phi)\)
This means that the values inside the cosine function are equal modulo \(180^{\circ}\). Therefore, we have:
Evaluating these congruences for consistent intensity, we check each possible solution:
This is possible if the angle \(\phi\) is such that it adjusts for a consistent \(30^\circ\) difference, suggesting symmetrical matching around:
Thus, the angle between the direction of polarization and the x-axis is \(203^\circ\).