Step 1: Understanding the Concept:
The moment of inertia of a solid sphere about an axis through its centre is \(\dfrac25MR^2\). For a parallel axis at distance \(d\) from the centre, \(I = I_{cm} + Md^2\).
Step 2: Apply the theorem:
With \(d = \dfrac R3\):
\[ I = \frac25MR^2 + M\left(\frac R3\right)^2 = \frac25MR^2 + \frac19MR^2 \]
Step 3: Add the fractions:
\[ \frac25 + \frac19 = \frac{18 + 5}{45} = \frac{23}{45} \]
\[ I = \frac{23}{45}MR^2 \]
Step 4: Check:
Option (C), \(\dfrac{23}{45}MR^2\), is the value that results.
Final Answer:
I = 2/5 MR^2 + M(R/3)^2 = 23 MR^2 / 45.
\[ \boxed{\text{(C) }\dfrac{23}{45}MR^2} \]