\(\cdot 10.53\) In a tire-throwing competition, a man holding a
\(23.5-\mathrm{kg}\) car tire quickly swings the tire through three full turns
and releases it, much like a discus thrower. The tire starts from rest and is
then accelerated in a circular path. The orbital radius \(r\) for the tire's
center of mass is \(1.10 \mathrm{~m},\) and the path is horizontal to the
ground. The figure shows a top view of the tire's circular path, and the dot
at the center marks the rotation axis. The man applies a constant torque of
\(20.0 \mathrm{~N} \mathrm{~m}\) to accelerate the tire at a constant angular
acceleration. Assume that all of the tire's mass is at a radius \(R=0.350
\mathrm{~m}\) from its center.
a) What is the time, \(t_{\text {throw }}\) required for the tire to complete
three full revolutions?
b) What is the final linear speed of the tire's center of mass (after three
full revolutions)?
c) If, instead of assuming that all of the mass of the tire is at a distance
\(0.350 \mathrm{~m}\) from its center, you treat the tire as a hollow disk of
inner radius \(0.300 \mathrm{~m}\) and outer radius \(0.400 \mathrm{~m},\) how
does this change your answers to parts (a) and (b)?