Let
be the initial velocity of the ball. Then it has components

The position vector
of the ball at time
has components

where
is the acceleration due to gravity. When the ball is 90.0 m away from home plate, we're told that it clears (presumably) a barrier of some kind that is 7.50 m tall, so that for some time
we get

Solving for this
gives

Substituting this into the second equation gives



