Solution :
When solid sphere rolls on inclined plane, then it has both rotational as well as translational kinetic energy
Total kinetic energy $$K = {K_{{\text{rot}}}} + {K_{{\text{trans}}}} = \frac{1}{2}I{\omega ^2} + \frac{1}{2}m{v^2}$$
For sphere, moment of inertia about its diameter $$I = \frac{2}{5}m{r^2}$$
$$\eqalign{
& \therefore K = \frac{1}{2}\left( {\frac{2}{5}m{r^2}} \right){\omega ^2} + \frac{1}{2}m{v^2} \cr
& = \frac{1}{5}m{r^2}{\omega ^2} + \frac{1}{2}m{v^2} \cr
& = \frac{1}{5}m{v^2} + \frac{1}{2}m{v^2}\,\,\left( {{\text{as}}\,v = r\omega } \right) \cr
& = \frac{7}{{10}}m{v^2} \cr} $$

On reaching sphere at $$O,$$ it has only kinetic energy
$$\eqalign{
& \therefore PE = {\text{Total}}\,KE \cr
& mgh = \frac{7}{{10}}m{v^2} \cr
& \Rightarrow v = \sqrt {\frac{{10gh}}{7}} \cr} $$