Let \( \vec{a} = \hat{i} + \alpha \hat{j} + \beta \hat{k} \), \( \alpha, \beta \in \mathbb{R} \). Let a vector \( \vec{b} \) be such that the angle between \( \vec{a} \) and \( \vec{b} \) is \( \frac{\pi}{4} \) and \( |\vec{b}|^2 = 6 \),
If \( \vec{a} \times\vec{b} = 3\sqrt{2} \), then the value of \( \left( \alpha^2 + \beta^2 \right) | \vec{a} \times \vec{b} |^2 \) is equal to
Using \(\vec{a} \times \vec{b} = |\vec{a}||\vec{b}| \cos \theta\):
\(3\sqrt{2} = |\vec{a}| \times 6 \times \frac{\sqrt{2}}{2} \Rightarrow |\vec{a}| = 1.\)
Since \(|\vec{a}|^2 = 1\), we have \(1 + \alpha^2 + \beta^2 = 1 \Rightarrow \alpha^2 + \beta^2 = 5.\)
For \(|\vec{a} \times \vec{b}| = |\vec{a}||\vec{b}| \sin \theta\):
\(|\vec{a} \times \vec{b}| = 1 \times 6 \times \frac{\sqrt{2}}{2} = 3\sqrt{2}.\)
Thus, \((\alpha^2 + \beta^2)|\vec{a} \times \vec{b}|^2 = 5 \times 18 = 90.\)
To solve the problem, let's break it down step-by-step using vector algebra and trigonometry principles.
Therefore, the value of \((\alpha^2 + \beta^2) |\vec{a} \times \vec{b}|^2\) is 90.
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:
