2008 Paper 3 Q11

Year: 2008
Paper: 3
Question Number: 11

Course: zNo longer examinable
Section: Moments of inertia

Difficulty: 1700.0 Banger: 1500.0

Problem

A circular wheel of radius \(r\) has moment of inertia \(I\) about its axle, which is fixed in a horizontal position. A light string is wrapped around the circumference of the wheel and a particle of mass \(m\) hangs from the free end. The system is released from rest and the particle descends. The string does not slip on the wheel. As the particle descends, the wheel turns through \(n_1\) revolutions, and the string then detaches from the wheel. At this moment, the angular speed of the wheel is \(\omega_0\). The wheel then turns through a further \(n_2\) revolutions, in time \(T\), before coming to rest. The couple on the wheel due to resistance is constant. Show that \[ \frac12 \omega_0 T = 2 \pi n_2\] and \[ I =\dfrac {mgrn_1T^2 -4\pi mr^2n_2^2}{4\pi n_2(n_1+n_2)}\;. \]

No solution available for this problem.

Examiner's report
— 2008 STEP 3, Question 11
~8% attempted (inferred) Inferred ~8% from 'under a twelfth'

Under a twelfth tried this. A number of different correct approaches were successfully applied, and there were very few partially correct solutions.

Most candidates attempted five, six or seven questions, and scored the majority of their total score on their best three or four. Those attempting seven or more tended not to do well, pursuing no single solution far enough to earn substantial marks.

Source: Cambridge STEP 2008 Examiner's Report · 2008-full.pdf
Rating Information

Difficulty Rating: 1700.0

Difficulty Comparisons: 0

Banger Rating: 1500.0

Banger Comparisons: 0

Show LaTeX source
Problem source
A circular wheel of radius $r$ has moment of inertia $I$ about
its
axle, which is fixed in a horizontal position. A light string is
wrapped around the circumference of the wheel and a particle of 
mass $m$ hangs from the free end. The system is released from rest
and the particle descends.
The string does not slip on the wheel.
As the particle descends, the wheel turns through
$n_1$ revolutions, and the string then detaches from the wheel. At this
moment, the angular speed of the wheel is $\omega_0$.  The wheel then
turns through a further
 $n_2$ revolutions, in time $T$, before coming to rest.
The couple on the wheel due to resistance is constant.
Show that
\[ \frac12 \omega_0 T = 2 \pi n_2\]
and
\[
I =\dfrac {mgrn_1T^2 -4\pi mr^2n_2^2}{4\pi n_2(n_1+n_2)}\;.
\]