OCR M3 2010 January — Question 5 11 marks

Exam BoardOCR
ModuleM3 (Mechanics 3)
Year2010
SessionJanuary
Marks11
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicHooke's law and elastic energy
TypeWork-energy with multiple stages
DifficultyStandard +0.8 This is a two-part M3 question combining elastic string energy conservation with pulley mechanics. Part (i) requires straightforward energy conservation with elastic PE, gravitational PE, and KE. Part (ii) involves finding maximum speed by differentiating or recognizing equilibrium position. The second problem adds complexity with variable geometry on a cylinder, requiring careful setup of energy equations with changing heights and arc lengths. While requiring multiple techniques and careful bookkeeping, these are standard M3 applications without requiring novel insight.
Spec6.02h Elastic PE: 1/2 k x^26.02i Conservation of energy: mechanical energy principle6.02j Conservation with elastics: springs and strings6.05e Radial/tangential acceleration

5 A light elastic string of natural length 1.6 m has modulus of elasticity 120 N . One end of the string is attached to a fixed point \(O\) and the other end is attached to a particle \(P\) of weight 1.5 N . The particle is released from rest at the point \(A\), which is 2.1 m vertically below \(O\). It comes instantaneously to rest at \(B\), which is vertically above \(O\).
  1. Verify that the distance \(A B\) is 4 m .
  2. Find the maximum speed of \(P\) during its upward motion from \(A\) to \(B\). \begin{figure}[h]
    \includegraphics[alt={},max width=\textwidth]{08760a55-da6c-41f2-a88a-289ecc227f69-4_351_442_303_479} \captionsetup{labelformat=empty} \caption{Fig. 1}
    \end{figure} \begin{figure}[h]
    \includegraphics[alt={},max width=\textwidth]{08760a55-da6c-41f2-a88a-289ecc227f69-4_394_648_260_1018} \captionsetup{labelformat=empty} \caption{Fig. 2}
    \end{figure} A light inextensible string of length \(0.8 \pi \mathrm {~m}\) has particles \(P\) and \(Q\), of masses 0.4 kg and 0.58 kg respectively, attached to its ends. The string passes over a smooth horizontal cylinder of radius 0.8 m , which is fixed with its axis horizontal and passing through a fixed point \(O\). The string is held at rest in a vertical plane perpendicular to the axis of the cylinder, with \(P\) and \(Q\) at opposite ends of the horizontal diameter of the cylinder through \(O\) (see Fig. 1). The string is released and \(Q\) begins to descend. When \(O P\) has rotated through \(\theta\) radians, with \(P\) remaining in contact with the cylinder, the speed of each particle is \(v \mathrm {~m} \mathrm {~s} ^ { - 1 }\) (see Fig. 2).

5 A light elastic string of natural length 1.6 m has modulus of elasticity 120 N . One end of the string is attached to a fixed point $O$ and the other end is attached to a particle $P$ of weight 1.5 N . The particle is released from rest at the point $A$, which is 2.1 m vertically below $O$. It comes instantaneously to rest at $B$, which is vertically above $O$.\\
(i) Verify that the distance $A B$ is 4 m .\\
(ii) Find the maximum speed of $P$ during its upward motion from $A$ to $B$.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{08760a55-da6c-41f2-a88a-289ecc227f69-4_351_442_303_479}
\captionsetup{labelformat=empty}
\caption{Fig. 1}
\end{center}
\end{figure}

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{08760a55-da6c-41f2-a88a-289ecc227f69-4_394_648_260_1018}
\captionsetup{labelformat=empty}
\caption{Fig. 2}
\end{center}
\end{figure}

A light inextensible string of length $0.8 \pi \mathrm {~m}$ has particles $P$ and $Q$, of masses 0.4 kg and 0.58 kg respectively, attached to its ends. The string passes over a smooth horizontal cylinder of radius 0.8 m , which is fixed with its axis horizontal and passing through a fixed point $O$. The string is held at rest in a vertical plane perpendicular to the axis of the cylinder, with $P$ and $Q$ at opposite ends of the horizontal diameter of the cylinder through $O$ (see Fig. 1). The string is released and $Q$ begins to descend. When $O P$ has rotated through $\theta$ radians, with $P$ remaining in contact with the cylinder, the speed of each particle is $v \mathrm {~m} \mathrm {~s} ^ { - 1 }$ (see Fig. 2).\\

\hfill \mbox{\textit{OCR M3 2010 Q5 [11]}}