Step 1: Understanding the Concept:
The moment of inertia of a solid sphere about its diameter is $I = \frac{2}{5} mR^2$. To find the moment of inertia about a tangent, we use the Parallel Axis Theorem.
Step 2: Formula Application:
Parallel Axis Theorem: $I_{tangent} = I_{cm} + md^2$.
Here, $I_{cm} = I = \frac{2}{5} mR^2$ and the distance $d$ between the diameter and the tangent is $R$.
Step 3: Explanation:
$I_{tangent} = \frac{2}{5} mR^2 + mR^2 = \frac{7}{5} mR^2$.
Since $I = \frac{2}{5} mR^2$, we can write $mR^2 = \frac{5}{2} I$.
Substituting this: $I_{tangent} = \frac{7}{5} \times \left( \frac{5}{2} I \right) = \frac{7}{2} I = 3.5I$.
Step 4: Final Answer:
The moment of inertia about the tangent is 3.5I.