A 170-kg merry-go-round in the shape of a uniform, solid, horizontal disk of radius 1.50 m is set in motion by wrapping a rope about the rim of the disk and pulling on the rope. What constant force would have to be exerted on the rope to bring the merry-go-round from rest to an angular speed of 0.600 rev/s in 2.00 s? (State the magnitude of the force.)
Given
mass of the horizontal disc (merry-go-round) m = 170 kg
radius R = 1.50 m
angular speed is w = 0.6 rev/s = 0.6*2pi rad/s = 3.76991 rad/s
time t =2 s
the angular speed is w = 3.76991 rad/s
so the angular acceleration alpha = W/t = 3.76991/2 rad/s2 = 1.884955 rad/s2
due to the force applied by the rope on the rim of the disc the torque will act on it
by definition torque T = R X F = R*F sin theta
here theta = 90 degrees
and from rotational motion the torque T = I*alpha
I is moment of inertia of the disc I = 0.5*M*R^2
I = 0.5*170*1.5^2 kg m2 = 191.25 kg m2
equating the torques
R*F sin theta = I*alpha
1.5*F sin90 = 191.25*1.884955
solving for F
F = 240.332 N
constant force would have to be exerted on the rope to bring the merry-go-round from rest to an angular speed of 0.600 rev/s in 2.00 s is 240.332 N
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