Janine,
You can solve this problem using Conservation of Energy and the Work - Energy theorem. To apply to this problem first note that the height (or distance) that the ball has to reach after being thrown is (10 m - 1.5 m) = 8.5 m.
In the instant after the ball was thrown it will have an initial velocity v which means it will have initial kinetic energy
Ki = ½·mv². It's initial potential energy U = mgh, if taken with respect to its initial height 1.5 m above the floor is
Ui = 0. At the top of its trajectory 8.5 m above the height from which it was thrown, it velocity will drop to zero as it momentarily stops rising and, reversing its motion, begins to fall. At his point it kinetic energy K = 0, since v= 0, but its potential energy U = mgh is now (0.1 kg)(9.8 m/s²)(8.5 m) = 8.33 J. Since energy is conserved:
Ki + Ui = K(top) + U(top)
Since Ui and K(top) are both = 0
Ki = ½·mv² = U(top) = mgh ⇒ ½·mv = 8.33 J
Solving for vi = sqrt[2(mgh)/m] = [2·gh]½ (notice m cancels, so we the mass of the ball has no bearing on its final velocity and we didn't really need to explicitly calculate the value of U above.
vi = [2·9.8 m/s²·8.5 m]½ = 12.9 m/s (Initial velocity)
For the speed when it hit's the floor simply reverse the process this time with initial velocity = 0 and height = 10 m, since it has to fall the full distance from the ceiling to the floor. In the instance before it hits the floor h = 0, so
mgh = ½·mvf² ⇒ vf = [2·9.8 m/s²·10 m]½ = 14 m/s². (Final velocity)
Janine T.
09/08/14