A uniform cylinder of mass 100 kg and radius 50 cm is mounted so it is free to rotate about a fixed, horizontal axis that passes through the centers of its circular ends. A 10-kg block is hung from a massless cord that is wrapped around the cylinder’s circumference. When the block is released, the cord unwinds and the block accelerates downward. a) What is the block’s acceleration?
The equation of motion for the falling block (mass m) is
(tension in the cord is T):
m a = m g - T
The equation for the rotating cylinder (mass M, radius R, angular
acceleration A):
1/2 M R^2 A = T R
because 1/2MR^2 is the moment of inertia for a solid cylinder about
its axes and T R is the external torque.
When no slip occurs then R A = a, so this last equation
becomes
1/2 M a = T
So now we have two equations for the two unknowns a and T:
ma = m g - T
1/2 Ma = T
Substituting the second expression for T in the first allows us to
obtain the acceleration of the block, a:
m a = m g - 1/2 M a
(m + M/2) a = m g
a = m g /(m + M/2)
a = g/(1 + M/(2m))
a = 9.81 m/s^2 / ( 1 + 100kg/(2*10kg))
a = 1.64 ms^2
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