Let the initial velocity be \( V_0 \) and the height be \( H \). The ball is projected upwards, and it reaches the ground with a speed of \( 3V_0 \).
We can use the equation of motion for vertical displacement and velocity. The equation relating velocity, acceleration, and displacement is:
\[
v^2 = u^2 + 2a s
\]
where:
- \( v \) is the final velocity,
- \( u \) is the initial velocity,
- \( a \) is the acceleration (which is \( -g \), the acceleration due to gravity, as the ball is moving upwards),
- \( s \) is the displacement (which in this case is \( H \)).
At the point when the ball reaches the ground, we have:
- Final velocity \( v = 3V_0 \),
- Initial velocity \( u = V_0 \),
- Displacement \( s = H \),
- Acceleration \( a = -g \).
Using the equation:
\[
(3V_0)^2 = (V_0)^2 + 2(-g)H
\]
Simplifying:
\[
9V_0^2 = V_0^2 - 2gH
\]
\[
9V_0^2 - V_0^2 = 2gH
\]
\[
8V_0^2 = 2gH
\]
\[
H = \frac{4V_0^2}{g}
\]
Thus, the height \( H \) is \( \frac{4V_0^2}{g} \).
Now, we need to find the time taken by the ball to reach the ground. The time \( t \) can be found from the equation:
\[
v = u + at
\]
Using the same values for \( v = 3V_0 \), \( u = V_0 \), and \( a = -g \), we get:
\[
3V_0 = V_0 - g t
\]
Solving for \( t \):
\[
3V_0 - V_0 = g t
\]
\[
2V_0 = g t
\]
\[
t = \frac{2V_0}{g}
\]
Thus, the time taken by the ball to reach the ground is \( \frac{2V_0}{g} \).
So, the correct answer is (B) \( \frac{V_0}{g} \), \( \frac{3V_0^2}{2g} \).