Challenging +1.2 This is a standard Further Maths mechanics question on small oscillations with elastic strings. It requires setting up forces using Hooke's law, applying Newton's second law, and using binomial approximation for small oscillations—all routine techniques for FP2/FM students. The geometry is straightforward (symmetric setup) and the question guides students through both parts explicitly. While it involves multiple steps and some algebraic manipulation, it follows a well-established template that students practice extensively.
2
\includegraphics[max width=\textwidth, alt={}, center]{71a3b842-9d31-4c25-b894-ca6d1f47d84b-2_293_875_525_635}
Two light elastic strings, each of natural length \(a\) and modulus of elasticity \(2 m g\), are attached to a particle \(P\) of mass \(m\). The strings join the particle to the points \(A\) and \(B\) which are fixed and at a distance \(4 a\) apart on a smooth horizontal surface. The particle is at rest at the mid-point \(O\) of \(A B\). The particle is now displaced a small distance in a direction perpendicular to \(A B\), on the surface, and released from rest. At time \(t\), the displacement of \(P\) from \(O\) is \(x\) (see diagram). Show that
$$\ddot { x } = - \frac { 4 g x } { a } \left( 1 - \frac { 1 } { 2 } \left( 1 + \frac { x ^ { 2 } } { 4 a ^ { 2 } } \right) ^ { - \frac { 1 } { 2 } } \right) .$$
Given that \(\frac { x } { a }\) is so small that \(\left( \frac { x } { a } \right) ^ { 2 }\) and higher powers may be neglected, show that the motion of \(P\) is approximately simple harmonic and state the period of the motion.
2\\
\includegraphics[max width=\textwidth, alt={}, center]{71a3b842-9d31-4c25-b894-ca6d1f47d84b-2_293_875_525_635}
Two light elastic strings, each of natural length $a$ and modulus of elasticity $2 m g$, are attached to a particle $P$ of mass $m$. The strings join the particle to the points $A$ and $B$ which are fixed and at a distance $4 a$ apart on a smooth horizontal surface. The particle is at rest at the mid-point $O$ of $A B$. The particle is now displaced a small distance in a direction perpendicular to $A B$, on the surface, and released from rest. At time $t$, the displacement of $P$ from $O$ is $x$ (see diagram). Show that
$$\ddot { x } = - \frac { 4 g x } { a } \left( 1 - \frac { 1 } { 2 } \left( 1 + \frac { x ^ { 2 } } { 4 a ^ { 2 } } \right) ^ { - \frac { 1 } { 2 } } \right) .$$
Given that $\frac { x } { a }$ is so small that $\left( \frac { x } { a } \right) ^ { 2 }$ and higher powers may be neglected, show that the motion of $P$ is approximately simple harmonic and state the period of the motion.
\hfill \mbox{\textit{CAIE FP2 2012 Q2 [7]}}