Consider a well which has a swinging bucket of nugatory size dangling from a massless rope- forming a simple pendulum. The rope's initial length is 20 metres, but I begin to winch the rope upwards at a regular rate to a length of 2 metres, which takes one minute. During this time, how many full swings (or oscillations, assuming I start winching when the bucket is at a point of equilibrium) does the bucket complete?
Ignore friction/air resistance, and assume .
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The period of a simple pendulum is 2 π g L seconds (where g = 9 . 8 ). The frequency of our pendulum is thus 2 π 9 . 8 L 1 . In order to find the total oscillations of such a pendulum in a minute, we need to find the area under the graph of frequency against time between 0 and 60 seconds (since oscillations = frequency × time). However, length ( L ) is not constant, so more work needs to be done. L varies from 20 to 2 metres over 60 seconds, so we can express L in terms of t : L = 2 0 − 0 . 3 t . Substituting this expression for L , we can integrate the new expression for the frequency of the pendulum from 0 to 60 seconds to find the area under the graph, and thus the total oscillations: ∫ 0 6 0 2 π 9 . 8 2 0 − 0 . 3 t 1 d t , which can be rearranged to 2 π 9 . 8 ∫ 0 6 0 ( 2 0 − 0 . 3 t ) − 0 . 5 d t . Using the chain rule, this can be written as [ 2 2 π 9 . 8 ∗ 3 1 0 ∗ ( 2 0 − 0 3 t ) 2 1 ] 0 6 0 , which works out as ≈ 1 0 . 1 oscillations, so our answer is 1 0 .