Concept:
The moment of inertia of a body measures its resistance to rotational motion about a given axis. For composite systems, the total moment of inertia is obtained by adding the moments of inertia of individual parts.
For a solid sphere, the moment of inertia about its own central axis is:
\[
I_{\text{sphere}} = \frac{2}{5}MR^2
\]
When the axis of rotation does not pass through the center of mass of the body, we use the parallel axis theorem:
\[
I = I_{\text{cm}} + Md^2
\]
where
\(I_{\text{cm}}\) = moment of inertia about the center of mass
\(d\) = distance between the axis and the center of mass.
Step 1: Moment of inertia of each sphere about its center.
\[
I_{\text{cm}} = \frac{2}{5}MR^2
\]
Step 2: Distance between the spheres.
The distance between the centers is \(20\,\text{cm}\).
If the axis is taken through the midpoint between the spheres, each sphere is at a distance \(R\) from the axis.
Thus,
\[
d = R
\]
Step 3: Applying the parallel axis theorem.
\[
I = I_{\text{cm}} + Md^2
\]
\[
I = \frac{2}{5}MR^2 + MR^2
\]
\[
I = \frac{7}{5}MR^2
\]
This is the moment of inertia for one sphere about the given axis.
Step 4: Total moment of inertia of two spheres.
\[
I_{\text{total}} = 2 \times \frac{7}{5}MR^2
\]
\[
I_{\text{total}} = \frac{14}{5}MR^2
\]
Thus, the moment of inertia of the system is:
\[
\frac{14}{5}MR^2
\]