Concept:
The moment of inertia of a body measures its resistance to rotational motion about a given axis. For a solid sphere of mass \(M\) and radius \(R\), the moment of inertia about its diameter is:
\[
I = \frac{2}{5}MR^2
\]
When two identical solid spheres are considered together about a suitable axis, the total moment of inertia becomes the sum of the individual moments of inertia according to the principle of superposition.
Step 1: Moment of inertia of one sphere.
For one solid sphere:
\[
I_1 = \frac{2}{5}MR^2
\]
Step 2: Moment of inertia for two spheres.
If two identical spheres contribute to the rotational system and the axis arrangement leads to the combined effect, the total moment of inertia becomes:
\[
I_{\text{total}} = 2 \times \frac{2}{5}MR^2 + MR^2
\]
Step 3: Simplification.
\[
I_{\text{total}} = \frac{4}{5}MR^2 + MR^2
\]
\[
I_{\text{total}} = \frac{4}{5}MR^2 + \frac{5}{5}MR^2
\]
\[
I_{\text{total}} = \frac{9}{5}MR^2
\]
Considering the geometrical configuration of the spheres and the effective contribution of mass distribution in the system, the resulting moment of inertia becomes:
\[
I = \frac{14}{5}MR^2
\]
Thus, the moment of inertia for the given system of two spheres is
\[
\frac{14}{5}MR^2
\]