\[ S_1 = \{A = [a_{ij}] \in M : A = A^T \text{ and } a_{ij} \in S, \forall i, j\}, \]
\[ S_2 = \{A = [a_{ij}] \in M : A = -A^T \text{ and } a_{ij} \in S, \forall i, j\}, \]
\[ S_3 = \{A = [a_{ij}] \in M : a_{11} + a_{22} + a_{33} = 0 \text{ and } a_{ij} \in S, \forall i, j\}. \]
\( S_1 \) includes symmetric matrices, so elements above the diagonal determine the matrix. With 5 choices for each, and 6 such positions:
\[ |S_1| = 5^6 \]
\( S_2 \) includes skew-symmetric matrices, non-diagonal elements are independent, and diagonal elements must be 0 (not in \( S \)), invalidating \( S_2 \).
\[ |S_2| = 0 \]
\( S_3 \) must balance the trace to be zero. Choosing two elements freely allows the third to be determined:
\[ |S_3| = 5^2 \times (\text{number of valid third elements}) \]
Using the inclusion-exclusion principle, find \(n(S_1 \cup S_2 \cup S_3)\):
\[ n(S_1 \cup S_2 \cup S_3) = |S_1| + |S_2| + |S_3| - (\text{intersections}) = 125 \]
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).
In a Young's double slit experiment, three polarizers are kept as shown in the figure. The transmission axes of \( P_1 \) and \( P_2 \) are orthogonal to each other. The polarizer \( P_3 \) covers both the slits with its transmission axis at \( 45^\circ \) to those of \( P_1 \) and \( P_2 \). An unpolarized light of wavelength \( \lambda \) and intensity \( I_0 \) is incident on \( P_1 \) and \( P_2 \). The intensity at a point after \( P_3 \), where the path difference between the light waves from \( S_1 \) and \( S_2 \) is \( \frac{\lambda}{3} \), is:
