The movement equations are given by
\begin{align*}
\begin{cases}
\displaystyle y(t) = v_{0}\sin(\theta)t - \frac{gt^{2}}{2}\\\\
\displaystyle x(t) = v_{0}\cos(\theta)t
\end{cases}
\end{align*}
When the ball reaches the ground, we have $y(t) = 0$, that is to say
\begin{align*}
y(t) = v_{0}\sin(\theta)t - \frac{gt^{2}}{2} = 0 \Longleftrightarrow t_{1} = 0\quad\vee\quad t_{2} = \frac{2v_{0}\sin(\theta)}{g}
\end{align*}
Finally, the displacement on the $x$-axis is given by
\begin{align*}
x(t_{2}) = \frac{v^{2}_{0}\sin(2\theta)}{g}
\end{align*}
Then plug in the given values in order to obtain the numerical answer.