Set up the system in matrix form:
The system of equations can be represented in matrix form as: \[ \begin{pmatrix} 1 & \sqrt{2} \sin \alpha & \sqrt{2} \cos \alpha \\ 1 & \cos \alpha & \sin \alpha \\ 1 & \sin \alpha & -\cos \alpha \end{pmatrix} \begin{pmatrix} x \\ y \\ z \end{pmatrix} = \begin{pmatrix} 0 \\ 0 \\ 0 \end{pmatrix} \]
Condition for a Non-Trivial Solution:
For the system to have a non-trivial solution, the determinant of the matrix must be zero: \[ \text{det} \begin{pmatrix} 1 & \sqrt{2} \sin \alpha & \sqrt{2} \cos \alpha \\ 1 & \cos \alpha & \sin \alpha \\ 1 & \sin \alpha & -\cos \alpha \end{pmatrix} = 0 \]
Calculate the Determinant:
Expanding the determinant: \[ \text{det} = 1 \times (\cos \alpha \times (-\cos \alpha) - \sin \alpha \times \sin \alpha) - \sqrt{2} \sin \alpha \times (1 \times -\cos \alpha - 1 \times \sin \alpha) + \sqrt{2} \cos \alpha \times (1 \times \sin \alpha - 1 \times \cos \alpha) \]
Simplifying this determinant leads to an equation in terms of \(\alpha\) that must be solved for \(\alpha\).
Solve for \(\alpha\):
Solving the resulting trigonometric equation, we find that \(\alpha = \frac{5\pi}{24}\).
\[ \alpha + \frac{\pi}{8} = n\pi \pm \frac{\pi}{3} \] For \(n = 0\), \[ x = \frac{\pi}{3} - \frac{\pi}{8} = \frac{5\pi}{24}. \]
If the system of equations \[ (\lambda - 1)x + (\lambda - 4)y + \lambda z = 5 \] \[ \lambda x + (\lambda - 1)y + (\lambda - 4)z = 7 \] \[ (\lambda + 1)x + (\lambda + 2)y - (\lambda + 2)z = 9 \] has infinitely many solutions, then \( \lambda^2 + \lambda \) is equal to:
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:
