OCR M3 2010 June — Question 7 17 marks

Exam BoardOCR
ModuleM3 (Mechanics 3)
Year2010
SessionJune
Marks17
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 2
TypeCollision/impulse during circular motion
DifficultyChallenging +1.2 This is a standard M3 circular motion problem combining collision mechanics, energy conservation, and projectile motion. While it requires multiple techniques (coefficient of restitution, energy methods, tension in circular motion, projectile analysis), each step follows predictable M3 patterns with clear signposting. The algebra is straightforward and the 'show that' parts provide targets to work towards, reducing problem-solving demand.
Spec6.03i Coefficient of restitution: e6.03k Newton's experimental law: direct impact6.05d Variable speed circles: energy methods6.05e Radial/tangential acceleration

\includegraphics{figure_7} A particle \(P\) is attached to a fixed point \(O\) by a light inextensible string of length \(0.7\) m. A particle \(Q\) is in equilibrium suspended from \(O\) by an identical string. With the string \(OP\) taut and horizontal, \(P\) is projected vertically downwards with speed \(6\) m s\(^{-1}\) so that it strikes \(Q\) directly (see diagram). \(P\) is brought to rest by the collision and \(Q\) starts to move with speed \(4.9\) m s\(^{-1}\).
  1. Find the speed of \(P\) immediately before the collision. Hence find the coefficient of restitution between \(P\) and \(Q\). [3]
  2. Given that the speed of \(Q\) is \(v\) m s\(^{-1}\) when \(OQ\) makes an angle \(\theta\) with the downward vertical, find an expression for \(v^2\) in terms of \(\theta\), and show that the tension in the string \(OQ\) is \(14.7m(1 + 2\cos\theta)\) N, where \(m\) kg is the mass of \(Q\). [6]
  3. Find the radial and transverse components of the acceleration of \(Q\) at the instant that the string \(OQ\) becomes slack. [4]
  4. Show that \(V^2 = 0.8575\), where \(V\) m s\(^{-1}\) is the speed of \(Q\) when it reaches its greatest height (after the string \(OQ\) becomes slack). Hence find the greatest height reached by \(Q\) above its initial position. [4]

\includegraphics{figure_7}

A particle $P$ is attached to a fixed point $O$ by a light inextensible string of length $0.7$ m. A particle $Q$ is in equilibrium suspended from $O$ by an identical string. With the string $OP$ taut and horizontal, $P$ is projected vertically downwards with speed $6$ m s$^{-1}$ so that it strikes $Q$ directly (see diagram). $P$ is brought to rest by the collision and $Q$ starts to move with speed $4.9$ m s$^{-1}$.

\begin{enumerate}[label=(\roman*)]
\item Find the speed of $P$ immediately before the collision. Hence find the coefficient of restitution between $P$ and $Q$. [3]
\item Given that the speed of $Q$ is $v$ m s$^{-1}$ when $OQ$ makes an angle $\theta$ with the downward vertical, find an expression for $v^2$ in terms of $\theta$, and show that the tension in the string $OQ$ is $14.7m(1 + 2\cos\theta)$ N, where $m$ kg is the mass of $Q$. [6]
\item Find the radial and transverse components of the acceleration of $Q$ at the instant that the string $OQ$ becomes slack. [4]
\item Show that $V^2 = 0.8575$, where $V$ m s$^{-1}$ is the speed of $Q$ when it reaches its greatest height (after the string $OQ$ becomes slack). Hence find the greatest height reached by $Q$ above its initial position. [4]
\end{enumerate}

\hfill \mbox{\textit{OCR M3 2010 Q7 [17]}}