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The solution to a physics problem involving a rubber ball and a rubber band. The problem consists of calculating the average force applied to the ball by a paddle, the amount the band stretches before coming to rest, and the period of oscillation when the ball bounces by itself. The problem is solved using impulse, momentum, and energy conservation principles.
Typology: Exams
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a) (10 pts) Holding the rubber ball initially at rest, your little brother gives it a good swat with the wooden paddle. If the speed of the rubber ball is 5 m/s after being in contact with the wooden paddle for 0.1 s during the swat, what average force did the paddle apply to the rubber ball?
The first way to approach this problem is through impulse. The momentum of the ball changes due to impulse imparted by the paddle: ∆p = I = F t ∆p = (0.05)(5) − (0.05)(0) = 0.25 kg · m/s I = 0.25 = F (0.1) F = 2.5 N
You could also do this by finding the average acceleration of the ball while it’s in contact with the paddle.
a = ∆v t
= 50 m/s^2
Then use Newton’s 2nd Law to find the force required to produce this acceleration:
F = ma = (0.05)(50) = 2.5 N
b) (10 pts) Assuming the ball loses no speed until it starts to stretch the rubber band, by how much does it stretch the rubber band before coming to rest?
mv^2
kx^2 − 0
(8)x^2
x = 0.395 m = 39.5 cm
c) (10 pts) Your brother tires of hitting the rubber ball with the wooden paddle and decides to let the ball bounce by itself vertically at the end of the rubber band. Being an inquisitive sort, he times the oscillations. What time should appear on the stopwatch when he measures the period of oscillation?
ω =
k m
= 12.65 rad/s
2 π ω
2 π
= 0.523 s