Questions on rotational motion have been discussed on many occasions on this site. You can access them by clicking on the label ‘rotation’ below this post. Now, see the following questions involving rotation.
(a) [2gh/(I + mR)]1/2
(b) [2mgh/ (I + 2m)]1/2
(c) [2mgh/ (I + 2mR2)]1/2
(d) [2mgh/ (I + mR2)]1/2
(e) [2mgh/ (I + m)]1/2
The mass loses gravitational potential energy and gains kinetic energy. The wheel also gains kinetic energy so that we have
mgh = ½ mv2 + ½ Iω2 where v is the velocity of the mass after falling through the distance h and ω is the angular velocity of the wheel.
Since v =ωR the above equation becomes
mgh = ½ mω2R 2 + ½ Iω2
This yields ω = [2mgh/ (I + mR2)]1/2
(2) A simple pendulum has a spherical bob of mass 200 g. The string of the pendulum has negligible mass and it can withstand a maximum tension of 22 N. By holding the string in hand a student whirls the bob in a vertical circle of radius 1 m. The maximum possible angular velocity the bob can have throughout its motion (in radian per second) will be nearly
(a) 2
(b) 4
(c) 6
(d) 8
T – mg = mrω2, where m is the mass of the bob, T is the tension in the string, r is the radius of the circular path and ω is the angular velocity of revolution of the bob.
This gives ω = [(T – mg)/mr]1/2
= [(22 – 0.2×10)/(0.2×1)]1/2 = 10 radian/sec
We have substituted the maximum tension the string can withstand and hence the above angular velocity is the maximum value possible.
You will find some useful posts on rotational motion at AP Physics Resources: AP Physics B and C– Multiple Choice Questions on Circular Motion and Rotation
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