CAIE FP2 2012 June — Question 2 7 marks

Exam BoardCAIE
ModuleFP2 (Further Pure Mathematics 2)
Year2012
SessionJune
Marks7
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicSimple Harmonic Motion
TypeSmall oscillations with elastic strings/springs
DifficultyChallenging +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.
Spec4.10f Simple harmonic motion: x'' = -omega^2 x

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.

Question 2:
AnswerMarks Guidance
Answer/WorkingMarks Guidance
\(AP = \sqrt{4a^2 + x^2}\)B1 Find \(AP\) (or \(BP\)) in terms of \(x\) and \(a\)
\(T = 2mg(AP - a)/a\)B1 Hooke's Law for one string
\(md^2x/dt^2 = -2Tx/AP\)M1 Equation of motion at general point
\(d^2x/dt^2 = -(4gx/a)(1 - a/AP)\)M1 Combine to find \(d^2x/dt^2\)
\(= -(4gx/a)\{1 - \frac{1}{2}(1 + x^2/4a^2)^{-\frac{1}{2}}\}\) A.G.A1 M.R. Vertical motion loses only this A1; Motion along \(AB\) loses all marks
Neglect \((x/a)^2\): \(d^2x/dt^2 = -(4gx/a)\cdot\frac{1}{2} = -2gx/a\)B1
\(2\pi\sqrt{a/(2g)}\) or \(\pi\sqrt{2a/g}\)B1 Period using \(2\pi/\omega\) (AEF)
Total: 7 marks
## Question 2:

| Answer/Working | Marks | Guidance |
|---|---|---|
| $AP = \sqrt{4a^2 + x^2}$ | B1 | Find $AP$ (or $BP$) in terms of $x$ and $a$ |
| $T = 2mg(AP - a)/a$ | B1 | Hooke's Law for one string |
| $md^2x/dt^2 = -2Tx/AP$ | M1 | Equation of motion at general point |
| $d^2x/dt^2 = -(4gx/a)(1 - a/AP)$ | M1 | Combine to find $d^2x/dt^2$ |
| $= -(4gx/a)\{1 - \frac{1}{2}(1 + x^2/4a^2)^{-\frac{1}{2}}\}$ **A.G.** | A1 | **M.R.** Vertical motion loses only this A1; Motion along $AB$ loses all marks |
| Neglect $(x/a)^2$: $d^2x/dt^2 = -(4gx/a)\cdot\frac{1}{2} = -2gx/a$ | B1 | |
| $2\pi\sqrt{a/(2g)}$ or $\pi\sqrt{2a/g}$ | B1 | Period using $2\pi/\omega$ (AEF) |

**Total: 7 marks**

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\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]}}