Challenging +1.2 This is a standard M3 energy conservation problem with elastic strings. It requires setting up initial and final geometries, calculating extensions using trigonometry, applying elastic potential energy formula (λx²/2l), and using conservation of energy. While it involves multiple steps and careful geometric reasoning with the 30° and 60° angles, the approach is methodical and follows standard M3 techniques without requiring novel insight. The algebraic manipulation to reach the given answer is moderately involved but straightforward.
Two light elastic strings, each of length \(l\) m and modulus of elasticity \(\lambda\) N, are attached to a particle \(P\) of mass \(m\) kg. The other ends of the strings are attached to fixed points \(A\) and \(B\) on the same horizontal level, where \(AB = 2l\) m. \(P\) is held vertically below the mid-point of \(AB\), with each string taut and inclined at \(30°\) to the horizontal, and released from rest. Given that \(P\) comes to instantaneous rest when each string makes an angle of \(60°\) with the horizontal, show that \(\lambda = \frac{3mg}{6 - 2\sqrt{3}}\).
\includegraphics{figure_1}
[10 marks]
Two light elastic strings, each of length $l$ m and modulus of elasticity $\lambda$ N, are attached to a particle $P$ of mass $m$ kg. The other ends of the strings are attached to fixed points $A$ and $B$ on the same horizontal level, where $AB = 2l$ m. $P$ is held vertically below the mid-point of $AB$, with each string taut and inclined at $30°$ to the horizontal, and released from rest. Given that $P$ comes to instantaneous rest when each string makes an angle of $60°$ with the horizontal, show that $\lambda = \frac{3mg}{6 - 2\sqrt{3}}$.
\includegraphics{figure_1}
[10 marks]
\hfill \mbox{\textit{Edexcel M3 Q4 [10]}}