| Exam Board | OCR MEI |
|---|---|
| Module | M4 (Mechanics 4) |
| Year | 2015 |
| Session | June |
| Marks | 12 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Moments |
| Type | Potential energy with elastic strings/springs |
| Difficulty | Challenging +1.8 This is a challenging M4 question requiring setup of potential energy for a rod-spring system with geometric constraints, differentiation to find equilibrium positions, and stability analysis via second derivative test. The geometry (horizontal spring to vertical rail) requires careful coordinate work, and the multi-step nature with proof verification elevates it above standard mechanics questions, though the techniques themselves are syllabus-standard for Further Maths M4. |
| Spec | 6.02e Calculate KE and PE: using formulae6.02g Hooke's law: T = k*x or T = lambda*x/l6.04e Rigid body equilibrium: coplanar forces |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| \(V = mga\sin\theta\) with datum level through A | B1 | |
| \(+ \frac{1}{2}\frac{mg}{a}(2a\cos\theta)^2\) | M1* | Genuine attempt at extension + substitution into \(\frac{1}{2}kx^2\) |
| \(V = mga(\sin\theta + 1 + \cos 2\theta) = mga(\sin\theta + 2\cos^2\theta)\) | A1 | |
| \(\frac{dV}{d\theta} = mga\cos\theta - 4mga\cos\theta\sin\theta\) | M1 dep* | Differentiates their \(V\) of the correct form |
| \(= mga\cos\theta(1 - 4\sin\theta)\) | E1 | |
| [5] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| \(mga\cos\theta(1 - 4\sin\theta) = 0\) | M1 | |
| \(\cos\theta = 0 \Rightarrow \theta = \frac{1}{2}\pi, -\frac{1}{2}\pi\) | A1 | |
| \(\sin\theta = \frac{1}{4} \Rightarrow \theta = \sin^{-1}\frac{1}{4}\) | A1 | For this root and rejection of \(\pi - \arcsin(0.25)\); accept either no reason given for rejection or \(\sin\theta = 1/4\) only and the interval for \(\theta\) stated |
| \(\frac{d^2V}{d\theta^2} = -mga\sin\theta - 4mga\cos 2\theta\) | M1 | May use \(\frac{dV}{d\theta} = mga(\cos\theta - 2\sin 2\theta)\) giving \(-mga(\sin\theta + 4\cos 2\theta)\) or \(-mga(\sin\theta + 4 - 8\sin^2\theta)\) |
| When \(\theta = \frac{1}{2}\pi\), \(\frac{d^2V}{d\theta^2} = -mga + 4mga > 0\) so stable | A1 | For all A marks accept (as a minimum) correct \(V''\) with corresponding sign of \(V''\) + correct conclusion |
| When \(\theta = -\frac{1}{2}\pi\), \(\frac{d^2V}{d\theta^2} = mga + 4mga > 0\) so stable | A1 | |
| When \(\theta = \sin^{-1}\frac{1}{4}\), \(\frac{d^2V}{d\theta^2} = -\frac{1}{4}mga - \frac{7}{2}mga < 0\) so unstable | A1 | |
| [7] |
# Question 2:
## Part (i):
| Answer | Marks | Guidance |
|--------|-------|----------|
| $V = mga\sin\theta$ with datum level through A | B1 | |
| $+ \frac{1}{2}\frac{mg}{a}(2a\cos\theta)^2$ | M1* | Genuine attempt at extension + substitution into $\frac{1}{2}kx^2$ |
| $V = mga(\sin\theta + 1 + \cos 2\theta) = mga(\sin\theta + 2\cos^2\theta)$ | A1 | |
| $\frac{dV}{d\theta} = mga\cos\theta - 4mga\cos\theta\sin\theta$ | M1 dep* | Differentiates their $V$ of the correct form |
| $= mga\cos\theta(1 - 4\sin\theta)$ | E1 | |
| **[5]** | | |
## Part (ii):
| Answer | Marks | Guidance |
|--------|-------|----------|
| $mga\cos\theta(1 - 4\sin\theta) = 0$ | M1 | |
| $\cos\theta = 0 \Rightarrow \theta = \frac{1}{2}\pi, -\frac{1}{2}\pi$ | A1 | |
| $\sin\theta = \frac{1}{4} \Rightarrow \theta = \sin^{-1}\frac{1}{4}$ | A1 | For this root and rejection of $\pi - \arcsin(0.25)$; accept either no reason given for rejection or $\sin\theta = 1/4$ only and the interval for $\theta$ stated |
| $\frac{d^2V}{d\theta^2} = -mga\sin\theta - 4mga\cos 2\theta$ | M1 | May use $\frac{dV}{d\theta} = mga(\cos\theta - 2\sin 2\theta)$ giving $-mga(\sin\theta + 4\cos 2\theta)$ or $-mga(\sin\theta + 4 - 8\sin^2\theta)$ |
| When $\theta = \frac{1}{2}\pi$, $\frac{d^2V}{d\theta^2} = -mga + 4mga > 0$ so stable | A1 | For all A marks accept (as a minimum) correct $V''$ with corresponding sign of $V''$ + correct conclusion |
| When $\theta = -\frac{1}{2}\pi$, $\frac{d^2V}{d\theta^2} = mga + 4mga > 0$ so stable | A1 | |
| When $\theta = \sin^{-1}\frac{1}{4}$, $\frac{d^2V}{d\theta^2} = -\frac{1}{4}mga - \frac{7}{2}mga < 0$ so unstable | A1 | |
| **[7]** | | |
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2 Fig. 2 shows a system in a vertical plane. A uniform rod AB of length $2 a$ and mass $m$ is freely hinged at A . The angle that AB makes with the horizontal is $\theta$, where $- \frac { 2 } { 3 } \pi < \theta < \frac { 2 } { 3 } \pi$. Attached at B is a light spring BC of natural length $a$ and stiffness $\frac { m g } { a }$. The other end of the spring is attached to a small light smooth ring C which can slide freely along a vertical rail. The rail is at a distance of $a$ from A and the spring is always horizontal.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{8ea28e6f-528c-4e3c-9562-6c964043747e-2_737_703_1356_680}
\captionsetup{labelformat=empty}
\caption{Fig. 2}
\end{center}
\end{figure}
(i) Find the potential energy, $V$, of the system and hence show that $\frac { \mathrm { d } V } { \mathrm {~d} \theta } = m g a \cos \theta ( 1 - 4 \sin \theta )$.\\
(ii) Hence find the positions of equilibrium of the system and investigate their stability.
\hfill \mbox{\textit{OCR MEI M4 2015 Q2 [12]}}