Express \(\vec{C}\) as a Unit Vector:
Let \(\vec{C} = C_1\vec{i} + C_2\vec{j} + C_3\vec{k}\) such that:
\[ C_1^2 + C_2^2 + C_3^2 = 1. \]
Using the Angle Condition with \(2\vec{i} + 2\vec{j} - \vec{k}\):
The dot product \(\vec{C} \cdot (2\vec{i} + 2\vec{j} - \vec{k})\) is given by:
\[ \vec{C} \cdot (2\vec{i} + 2\vec{j} - \vec{k}) = |\vec{C}||2\vec{i} + 2\vec{j} - \vec{k}|\cos 60^\circ. \]
Since \(\vec{C}\) is a unit vector: \[ 2C_1 + 2C_2 - C_3 = \frac{3}{2}. \]
Using the Angle Condition with \(\vec{i} - \vec{k}\):
The dot product \(\vec{C} \cdot (\vec{i} - \vec{k})\) is given by:
\[ \vec{C} \cdot (\vec{i} - \vec{k}) = |\vec{C}||\vec{i} - \vec{k}|\cos 45^\circ. \]
Simplifying gives: \[ C_1 - C_3 = 1. \]
Solving the Equations:
From \(C_1 - C_3 = 1\) and \(2C_1 + 2C_2 - C_3 = \frac{3}{2}\), we find: \[ C_1 = \frac{\sqrt{2}}{3}, \quad C_2 = -\frac{1}{3\sqrt{2}}, \quad C_3 = \frac{\sqrt{2}}{3} - \frac{1}{2}. \]
Vector Addition:
Adding \(\vec{C}\) to \(\left(\frac{1}{2}\vec{i} + \frac{1}{3\sqrt{2}}\vec{j} - \frac{\sqrt{2}}{3}\vec{k}\right)\):
\[ \vec{C} + \left(\frac{1}{2}\vec{i} + \frac{1}{3\sqrt{2}}\vec{j} - \frac{\sqrt{2}}{3}\vec{k}\right) = \frac{\sqrt{2}}{3}\vec{i} - \frac{1}{2}\vec{k}. \]
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).

Method used for separation of mixture of products (B and C) obtained in the following reaction is: 