Concept:
For a body rolling without slipping down an incline, acceleration depends on both translational and rotational motion.
Step 1: General formula.
For rolling motion:
\[
a = \frac{g \sin \theta}{1 + \frac{I}{mR^2}}
\]
Step 2: Moment of inertia of solid sphere.
\[
I = \frac{2}{5} mR^2
\]
Step 3: Substitute in formula.
\[
a = \frac{g \sin \theta}{1 + \frac{2}{5}} = \frac{g \sin \theta}{\frac{7}{5}} = \frac{5}{7} g \sin \theta
\]
Step 4: For $\theta = 30^\circ$.
\[
a = \frac{5}{7} g \sin 30^\circ
\]
Step 5: Evaluating the options.
- $\frac{g}{2}$ $\rightarrow$ Incorrect
- $\frac{5g}{7}$ $\rightarrow$ Missing $\sin \theta$ (incorrect)
- $\frac{5g}{7} \sin 30^\circ$ $\rightarrow$ Correct
- $\frac{2g}{7} \sin 30^\circ$ $\rightarrow$ Incorrect
Step 6: Conclusion.
Thus, acceleration is $\frac{5g}{7} \sin 30^\circ$.