The moment of inertia of a solid sphere about its diameter is given by the formula:
\( I_{\text{sphere}} = \frac{2}{5}mr^2 \)
where: - \( m \) is the mass of the sphere, - \( r \) is the radius of the sphere.
The parallel axis theorem states that the moment of inertia of a body about an axis parallel to and a distance \( d \) away from an axis through its center of mass is given by:
\( I = I_{\text{cm}} + md^2 \)
where: - \( I_{\text{cm}} \) is the moment of inertia about the center of mass axis, - \( d \) is the distance from the center of mass to the new axis.
The distance between the center of a sphere and the midpoint of the rod is:
\( d = \frac{40}{2} \, \text{cm} = 20 \, \text{cm} = 0.2 \, \text{m} \)
The radius of each sphere is \( r = 10 \, \text{cm} = 0.1 \, \text{m} \). Using the parallel axis theorem, the moment of inertia of one sphere about the midpoint of the rod is:
\( I_{\text{one}} = \frac{2}{5}mr^2 + md^2 \)
Substitute the values into the equation:
\( I_{\text{one}} = \frac{2}{5}(2)(0.1)^2 + (2)(0.2)^2 = 0.008 + 0.08 = 0.088 \, \text{kg-m}^2 \)
Since there are two identical spheres, the total moment of inertia of the system is:
\( I_{\text{sys}} = 2 \times I_{\text{one}} = 2 \times 0.088 = 0.176 \, \text{kg-m}^2 = 176 \times 10^{-3} \, \text{kg-m}^2 \)
The moment of inertia of the system is \( \mathbf{176 \times 10^{-3} \, \text{kg-m}^2} \).