Masses $m$ and $2m$ are connected by a massless rod of length $d$. If angular momentum about an axis passing through centre of mass and perpendicular to the rod is $L$, then the angular speed $(\omega)$ of the system is:
To determine the angular speed \((\omega)\) of the system, we'll follow these steps:
Determine the position of the center of mass (COM).
For two masses \(m\) and \(2m\) connected by a rod of length \(d\), the position of the COM from mass \(m\) is given by:
\(x_{\text{COM}} = \frac{m \times 0 + 2m \times d}{m + 2m} = \frac{2md}{3m} = \frac{2d}{3}\)
Calculate the moments of inertia about the COM.
The moment of inertia \((I)\) of the system about an axis passing through the COM and perpendicular to the rod is:
\(I = m \left(\frac{2d}{3}\right)^2 + 2m \left(\frac{d}{3}\right)^2\)
Simplifying this,
\(I = m \frac{4d^2}{9} + 2m \frac{d^2}{9} = \frac{4md^2}{9} + \frac{2md^2}{9} = \frac{6md^2}{9} = \frac{2md^2}{3}\)
Use the relation between angular momentum and angular speed.
The angular momentum \((L)\) is related to the moment of inertia and angular speed by the formula:
\(L = I \omega\)
Substituting the expression for \(I\), we have:
\(L = \left(\frac{2md^2}{3}\right) \omega\)
Solving for \(\omega\) gives:
\(\omega = \frac{3L}{2md^2}\)
Therefore, the angular speed of the system is \(\frac{3L}{2md^2}\), which matches the given correct answer.
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) 