(a) From the particle under constant velocity model in the $$x$$ direction, find the time at which the ball arrives at the goal:
$$x_{f}=x_{i}+v_{i}t\rightarrow t=\frac{x_{f}-x_{i}}{v_{xi}}=\frac{36.0-0}{(20m/s)\cos53.0^{0}}=2.99s$$
From the particle under constant acceleration model in the $$y$$ direction, find the height of the ball at this time
$$y_{f}=y_{i}+v_{yi}t+\frac{1}{2}a_{y}t^{2}$$
$$y_{f}=0+(20.0m/s)\sin53.0^{0}(2.99s)-\frac{1}{2}(9.80m/s^{2})(2.99s)^{2}$$
$$y_{f}=3.94m$$
Therefore, the ball clears the crossbar by
$$3.94 m − 3.05 m = 0.89 m$$
(b) Use the particle under constant acceleration model to find the time at which the ball is at its highest point in its trajectory
$$v_{yf}=v_{yi}-gt\rightarrow t=\frac{v_{yf}-v_{yf}}{g}=\frac{(20.0m/s)\sin53.0^{0}-0}{9.80m/s^{2}}=1.63s$$
Because this is earlier than the time at which the ball reaches the goal, the ball clears the goal on its way down.