A ball of mass m is dropped from a height h above the ground, as shown in Figure 8.6. (a) Neglecting air resistance, determine the speed of the ball when it is at a height y above the ground.
A ball of mass m is dropped from a height h above the ground, as shown in Figure 8.6. (a) Neglecting air resistance, determine the speed of the ball when it is at a height y above the ground.
Because the ball is in free fall, the only force act- ing on it is the gravitational force. Therefore, we apply the principle of conservation of mechanical energy to the ball – Earth system. Initially, the system has potential energy but no kinetic energy. As the ball falls, the total mechanical energy remains constant and equal to the initial potential en- ergy of the system. At the instant the ball is released, its kinetic energy is K_{i}=0 and the potential energy of the system is U_{i}=m g h . When the ball is at a distance y above the ground, its kinetic energy is K_{f}=\frac{1}{2} m v_{f}^{2} and the potential energy relative to the ground is U_{f}=m g y. Applying Equation 8.10, we obtain
K_{i}+U_{i} =K_{f}+U_{f} 0+m g h =\frac{1}{2} m v_{f}^{2}+m g y v_{f}^{2} =2 g(h-y) v_{f}=\sqrt{2 g(h-y)}The speed is always pasitive. If we had been asked to find the ball’s velocity, we would use the negative value of the square root as the y component to in dicate the downward motion.
(b) Determine the speed of the ball at y if at the instant of release it already has an initial speed v_{i} at the initial altitude h .
In this case, the initial energy includes kinetic energy equal to \frac{1}{2} m v_{i}^{2}, and Equation 8.10 gives \frac{1}{2} m v_{2}^{2}+m g h=\frac{1}{2} m v_{f}^{2}+m g y
v_{f}^{2} =v_{i}^{2}+2 g(h-y) v_{f} =\sqrt{v_{i}^{2}+2 g(h-y)}This result is consistent with the expression v_{y f}{ }^{2}=v_{y i}^{2}-2 g\left(y-y_{i}\right) from kinematics, where y_{i}=h . Furthermore, this result is valid even if the initial velocity is at an angle to the horizontal (the projectile situation) for two reasons: (1) energy is a scalar, and the kinetic energy depends only on the magnitude of the velocity; and (2) the change in the gravitational potential energy depends only on the change in position in the vertical direction.