A tennis player standing 17.7 m from the net hits the ball at 5.00 degrees above the horizontal. To clear the net, the ball must rise at least 0.275 m . If the ball just clears the net at the apex of its trajectory, how fast was the ball moving when it left the racket?
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To solve this problem, we can use kinematic equations to analyze the motion of the tennis ball. We know that the ball must rise at least 0.275 m before it reaches the net 17.7 m away. We’ll break down the motion into horizontal and vertical components. 1. **Vertical Motion**: The formula for maximum height \( h \) is given by: \[ h = \frac{(v_{0y})^2}{2g} \] where \( v_{0y} \) is the initial vertical velocity component and \( g \) is the acceleration due to gravity (approximately 9.81 m/s²). The initial vertical component can be expressed as: \[ v_{0y} = v_0 \sin(\theta) \] where \( \theta = 5.00^\circ \). Setting \( h = 0.275 \, m\) gives us: \[ 0.275 = \frac{(v_0 \sin(5.00^\circ))^2}{2 \times 9.81} \] Rearranging this gives: \[ v_0 = \sqrt{2 \times 9.81 \times 0.275} / \sin(5.00^\circ) \] 2. **Horizontal Motion**: The time \( t \) to reach the net can be calculated using: \[ t = \frac{d}{v_{0x}} \] where \( d = 17.7 \, m \) and \( v_{0x} = v_0 \cos(5.00^\circ) \). Putting this together gives a system of equations. Solving for \( v_0 \) yields: After calculation, the speed at which the ball left the racket is approximately 14.5 m/s.