Step 1: Concept
Conservation of Energy: $mgh = \frac{1}{2}mv^2 + \frac{1}{2}I\omega^2$.
Step 2: Analysis
For a solid sphere, $I = \frac{2}{5}mr^2$. For pure rolling, $\omega = v/r$.
$mgh = \frac{1}{2}mv^2 + \frac{1}{2}(\frac{2}{5}mr^2)(\frac{v^2}{r^2}) = \frac{1}{2}mv^2 + \frac{1}{5}mv^2$.
Step 3: Calculation
$mgh = (\frac{1}{2} + \frac{1}{5})mv^2 = \frac{7}{10}mv^2$
$v^2 = \frac{10gh}{7} \implies v = \sqrt{\frac{10gh}{7}}$.
Step 4: Conclusion
Hence, the speed at the bottom is $(\frac{10gh}{7})^{1/2}$.
Final Answer: (B)