OCR MEI M4 2008 June — Question 4 24 marks

Exam BoardOCR MEI
ModuleM4 (Mechanics 4)
Year2008
SessionJune
Marks24
PaperDownload PDF ↗
TopicSimple Harmonic Motion
TypeSmall oscillations: rigid body compound pendulum
DifficultyChallenging +1.2 This is a multi-part Further Maths mechanics question involving energy methods and small oscillations. While it requires understanding of elastic potential energy, rotational systems, and equilibrium analysis, the mathematical steps are fairly guided (showing a given result, using a provided graph). The conceptual demand is moderate for FM students, and the calculations follow standard energy differentiation techniques without requiring particularly novel insights.
Spec3.03n Equilibrium in 2D: particle under forces6.02i Conservation of energy: mechanical energy principle6.02j Conservation with elastics: springs and strings

4 A uniform smooth pulley can rotate freely about its axis, which is fixed and horizontal. A light elastic string AB is attached to the pulley at the end B . The end A is attached to a fixed point such that the string is vertical and is initially at its natural length with B at the same horizontal level as the axis. In this position a particle P is attached to the highest point of the pulley. This initial position is shown in Fig. 4.1. The radius of the pulley is \(a\), the mass of P is \(m\) and the stiffness of the string AB is \(\frac { m g } { 10 a }\). \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{636e1d23-3bbb-469f-8fc9-1f64da865126-3_451_517_607_466} \captionsetup{labelformat=empty} \caption{Fig. 4.1}
\end{figure} \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{636e1d23-3bbb-469f-8fc9-1f64da865126-3_456_451_607_1226} \captionsetup{labelformat=empty} \caption{Fig. 4.2}
\end{figure}
  1. Fig. 4.2 shows the system with the pulley rotated through an angle \(\theta\) and the string stretched. Write down the extension of the string and hence find the potential energy, \(V\), of the system in this position. Show that \(\frac { \mathrm { d } V } { \mathrm {~d} \theta } = m g a \left( \frac { 1 } { 10 } \theta - \sin \theta \right)\).
  2. Hence deduce that the system has a position of unstable equilibrium at \(\theta = 0\).
  3. Explain how your expression for \(V\) relies on smooth contact between the string and the pulley. Fig. 4.3 shows the graph of the function \(\mathrm { f } ( \theta ) = \frac { 1 } { 10 } \theta - \sin \theta\). \begin{figure}[h]
    \includegraphics[alt={},max width=\textwidth]{636e1d23-3bbb-469f-8fc9-1f64da865126-3_538_1342_1706_404} \captionsetup{labelformat=empty} \caption{Fig. 4.3}
    \end{figure}
  4. Use the graph to give rough estimates of three further values of \(\theta\) (other than \(\theta = 0\) ) which give positions of equilibrium. In each case, state with reasons whether the equilibrium is stable or unstable.
  5. Show on a sketch the physical situation corresponding to the least value of \(\theta\) you identified in part (iv). On your sketch, mark clearly the positions of P and B .
  6. The equation \(\mathrm { f } ( \theta ) = 0\) has another root at \(\theta \approx - 2.9\). Explain, with justification, whether this necessarily gives a position of equilibrium.

4 A uniform smooth pulley can rotate freely about its axis, which is fixed and horizontal. A light elastic string AB is attached to the pulley at the end B . The end A is attached to a fixed point such that the string is vertical and is initially at its natural length with B at the same horizontal level as the axis. In this position a particle P is attached to the highest point of the pulley. This initial position is shown in Fig. 4.1.

The radius of the pulley is $a$, the mass of P is $m$ and the stiffness of the string AB is $\frac { m g } { 10 a }$.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{636e1d23-3bbb-469f-8fc9-1f64da865126-3_451_517_607_466}
\captionsetup{labelformat=empty}
\caption{Fig. 4.1}
\end{center}
\end{figure}

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{636e1d23-3bbb-469f-8fc9-1f64da865126-3_456_451_607_1226}
\captionsetup{labelformat=empty}
\caption{Fig. 4.2}
\end{center}
\end{figure}

(i) Fig. 4.2 shows the system with the pulley rotated through an angle $\theta$ and the string stretched. Write down the extension of the string and hence find the potential energy, $V$, of the system in this position. Show that $\frac { \mathrm { d } V } { \mathrm {~d} \theta } = m g a \left( \frac { 1 } { 10 } \theta - \sin \theta \right)$.\\
(ii) Hence deduce that the system has a position of unstable equilibrium at $\theta = 0$.\\
(iii) Explain how your expression for $V$ relies on smooth contact between the string and the pulley.

Fig. 4.3 shows the graph of the function $\mathrm { f } ( \theta ) = \frac { 1 } { 10 } \theta - \sin \theta$.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{636e1d23-3bbb-469f-8fc9-1f64da865126-3_538_1342_1706_404}
\captionsetup{labelformat=empty}
\caption{Fig. 4.3}
\end{center}
\end{figure}

(iv) Use the graph to give rough estimates of three further values of $\theta$ (other than $\theta = 0$ ) which give positions of equilibrium. In each case, state with reasons whether the equilibrium is stable or unstable.\\
(v) Show on a sketch the physical situation corresponding to the least value of $\theta$ you identified in part (iv). On your sketch, mark clearly the positions of P and B .\\
(vi) The equation $\mathrm { f } ( \theta ) = 0$ has another root at $\theta \approx - 2.9$. Explain, with justification, whether this necessarily gives a position of equilibrium.

\hfill \mbox{\textit{OCR MEI M4 2008 Q4 [24]}}