Concept:
The moment of inertia \( I \) of a uniform solid disc about its central axis is given by: \[ I = \frac{1}{2} M R^2 \] For a disc with density \( \rho \), radius \( R \), and thickness \( t \): \[ M = \rho \times \text{Volume} = \rho \pi R^2 t \] Substituting this into the formula for the moment of inertia: \[ I = \frac{1}{2} \rho \pi R^4 t \] Thus, for discs of the same material: \[ I \propto R^4 t \]
Step 1: Use the condition of equal moments of inertia.
Given that the moments of inertia of both discs are equal: \[ I_1 = I_2 \quad \Rightarrow \quad R_1^4 t_1 = R_2^4 t_2 \]
Step 2: Substitute the given radius ratio.
We are given the radius ratio as \( \frac{R_1}{R_2} = \frac{1}{2} \). Therefore: \[ \left(\frac{R_1}{R_2}\right)^4 = \frac{1}{16} \] Substitute this into the equation: \[ \frac{1}{16} \cdot t_1 = t_2 \]
Step 3: Find the required ratio.
Rearranging the equation to find the ratio of thicknesses: \[ \frac{t_1}{t_2} = 16 \]
Final Answer: \[ \boxed{\frac{t_1}{t_2} = 16}\]
A thin uniform rod (\(X\)) of mass \(M\) and length \(L\) is pivoted at a height \( \left(\dfrac{L}{3}\right) \) as shown in the figure. The rod is allowed to fall from a vertical position and lie horizontally on the table. The angular velocity of this rod when it hits the table top is ________. (\(g\) = gravitational acceleration) 