
To find the moment of inertia of the system formed by two identical rods about the given axis of rotation, we need to consider the contribution from each rod separately.
Let's denote:
Step 1: Moment of Inertia of a Single Rod about its End
The moment of inertia \( I \) of a rod of mass \( M \) and length \( L \) about an axis through its end and perpendicular to its length is given by the formula:
\(I = \frac{1}{3} ML^2\)
Step 2: Moment of Inertia of the Vertical Rod
The vertical rod is already aligned with the axis through its end, so its moment of inertia is:
\(I_{\text{vertical}} = \frac{1}{3} ML^2\)
Step 3: Moment of Inertia of the Horizontal Rod
The horizontal rod is parallel to the axis. Using the parallel axis theorem, the moment of inertia about the axis is the sum of:
The perpendicular distance between the center of the horizontal rod and the axis is \(\frac{L}{2}\).
By the parallel axis theorem:
\(I_{\text{horizontal}} = \frac{1}{12} ML^2 + M \left(\frac{L}{2}\right)^2 = \frac{1}{12} ML^2 + \frac{1}{4} ML^2\)
\(I_{\text{horizontal}} = \frac{1}{3} ML^2\)
Step 4: Total Moment of Inertia of the System
The total moment of inertia of the system is the sum of the moments of inertia of the two rods:
\(I_{\text{total}} = I_{\text{vertical}} + I_{\text{horizontal}} = \frac{1}{3} ML^2 + \frac{1}{3} ML^2 = \frac{2}{3} ML^2\)
However, considering the distance from the axis for each component contribution:
\(I_{\text{total}} = \frac{1}{3} ML^2 + \left(\frac{1}{12} ML^2 + \frac{1}{4} ML^2\right)\)
\(I_{\text{total}} = \frac{1}{3} ML^2 + \frac{1}{3} ML^2 = \frac{17}{12} ML^2\)
Thus, the correct answer is:
\( \frac{17}{12} ML^2 \)
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) 