Edexcel M3 2004 June — Question 2 7 marks

Exam BoardEdexcel
ModuleM3 (Mechanics 3)
Year2004
SessionJune
Marks7
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicHooke's law and elastic energy
TypeParticle at midpoint of string between two horizontal fixed points: vertical motion
DifficultyStandard +0.8 This is a multi-step energy conservation problem requiring: (1) geometric analysis to find string extensions at two positions using tan α = 4/3, (2) elastic potential energy calculations for two strings, (3) gravitational potential energy change, and (4) algebraic manipulation to find λ. While the energy method is standard M3 content, the symmetric two-string geometry and the need to carefully track extensions at both positions elevates this above routine exercises.
Spec6.02h Elastic PE: 1/2 k x^26.02i Conservation of energy: mechanical energy principle

2. \begin{figure}[h]
\captionsetup{labelformat=empty} \caption{Figure 1} \includegraphics[alt={},max width=\textwidth]{b9e9b91c-7e6d-4b84-9f0e-180b626887c2-2_460_549_651_792}
\end{figure} Two light elastic strings each have natural length \(a\) and modulus of elasticity \(\lambda\). A particle \(P\) of mass \(m\) is attached to one end of each string. The other ends of the strings are attached to points \(A\) and \(B\), where \(A B\) is horizontal and \(A B = 2 a\). The particle is held at the mid-point of \(A B\) and released from rest. It comes to rest for the first time in the subsequent motion when \(P A\) and \(P B\) make angles \(\alpha\) with \(A B\), where \(\tan \alpha = \frac { 4 } { 3 }\), as shown in Fig. 1. Find \(\lambda\) in terms of \(m\) and \(g\).

2.

\begin{figure}[h]
\begin{center}
\captionsetup{labelformat=empty}
\caption{Figure 1}
  \includegraphics[alt={},max width=\textwidth]{b9e9b91c-7e6d-4b84-9f0e-180b626887c2-2_460_549_651_792}
\end{center}
\end{figure}

Two light elastic strings each have natural length $a$ and modulus of elasticity $\lambda$. A particle $P$ of mass $m$ is attached to one end of each string. The other ends of the strings are attached to points $A$ and $B$, where $A B$ is horizontal and $A B = 2 a$. The particle is held at the mid-point of $A B$ and released from rest. It comes to rest for the first time in the subsequent motion when $P A$ and $P B$ make angles $\alpha$ with $A B$, where $\tan \alpha = \frac { 4 } { 3 }$, as shown in Fig. 1.

Find $\lambda$ in terms of $m$ and $g$.\\

\hfill \mbox{\textit{Edexcel M3 2004 Q2 [7]}}