91Ó°ÊÓ

The equation for the angular momentum of a rotating object about a fixed rotation axis is as follows:

\(L = I\omega \)

Here, \(I\) is the moment of inertia of the object and \(\omega \) is the angular velocity.

Given data:

The mass of the rod is\(M\).

The length of the rod is\(l\).

Mass \(m\) is attached to each end of the rod.

The expression for the moment of inertia of the rod is as follows:

\({I_1} = \frac{1}{{12}}M{l^2}\)

The expression for the moment of inertia of the mass on one end of the rod is as follows:

\({I_2} = m{R^2}\)

The expression for the moment of inertia of the mass on another end of the rod is as follows:

\({I_3} = m{R^2}\)

The distance between the masses on either end of the rotation axis is equal to half its length. That is:

\(R = \frac{l}{2}\)

The moment of inertia of a system is equal to the sum of the moments of inertia of the individual components of the system. Therefore, we can write:

\(\begin{aligned}{c}I &= {I_1} + {I_2} + {I_3}\\I &= \frac{1}{{12}}M{l^2} + m{R^2} + m{R^2}\\I &= \frac{1}{{12}}M{l^2} + 2m{R^2}\\I &= \frac{1}{{12}}M{l^2} + 2m{\left( {\frac{l}{2}} \right)^2}\end{aligned}\)

Solve further as:

\(\begin{aligned}{l}I &= \frac{1}{{12}}M{l^2} + \frac{1}{2}m{l^2}\\I &= \frac{1}{{12}}\left( {M + 6m} \right){l^2}\\I &= \frac{1}{2}\left( {\frac{1}{6}M + m} \right){l^2}\end{aligned}\)

The angular momentum of the system about the axis can be calculated as:

\(\begin{aligned}{l}L &= I\omega \\L &= \left( {\frac{1}{2}\left( {\frac{1}{6}M + m} \right){l^2}} \right)\omega \end{aligned}\)

Thus, the angular momentum of the system about the axis is \(\left( {\frac{1}{2}\left( {\frac{1}{6}M + m} \right){l^2}} \right)\omega \).