| Exam Board | OCR |
|---|---|
| Module | M4 (Mechanics 4) |
| Year | 2004 |
| Session | June |
| Marks | 11 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Moments |
| Type | Potential energy with elastic strings/springs |
| Difficulty | Challenging +1.8 This is a sophisticated M4 mechanics problem requiring energy methods to find equilibrium positions and stability analysis. Students must recognize geometric constraints (horizontal string from symmetry), derive potential energy expressions for both gravitational and elastic components, differentiate to find equilibrium, and apply second derivative test for stability. The combination of rotating rod, elastic string, and sliding ring creates a non-trivial system requiring careful geometric reasoning and calculus, placing it well above average difficulty but within reach of strong Further Maths students. |
| Spec | 6.02i Conservation of energy: mechanical energy principle6.04e Rigid body equilibrium: coplanar forces |
| Answer | Marks | Guidance |
|---|---|---|
| e.g. \(R\) has no weight/mass; There is no friction; There is no vertical force at \(R\); String has minimum length/elastic energy | B1 | For any one contributory reason Total: 1 |
| Answer | Marks | Guidance |
|---|---|---|
| \(V = \frac{1}{2}\left(\frac{mg}{a}\right)(2a\sin\theta)^2 + mga\cos\theta\) | B2 | Give B1 for correct EE or PE |
| \(= mga(2\sin^2\theta + \cos\theta)\) | ||
| \(\frac{dV}{d\theta} = mga(4\sin\theta\cos\theta - \sin\theta)\) | B1 ft, B1 ft | Diffn of \(\sin^2\theta\) (or \(\cos^2\theta\)); Diffn of \(\cos\theta\) (or \(\sin\theta\)) |
| For equilibrium, \(mga\sin\theta(4\cos\theta - 1) = 0\) | M1 | |
| \(\theta = 1.32\) (or \(75.5°\)) | A1 | Allow \(\cos^{-1}\frac{1}{4}\), \(76°\); Ignore \(\theta=0\) if stated Total: 6 |
| Answer | Marks | Guidance |
|---|---|---|
| \(\frac{d^2V}{d\theta^2} = mga\cos\theta(4\cos\theta - 1) - 4mga\sin^2\theta\) | B2 ft | Give B1 if just one error; Only B1 ft if work is simpler |
| Answer | Marks | Guidance |
|---|---|---|
| \(\frac{d^2V}{d\theta^2} = -4mga\sin^2\theta \quad (= -\frac{15}{4}mga) < 0\) | M1 | |
| Equilibrium is unstable | A1 | Fully correct working only Total: 4 |
| OR When \(\theta < 1.32\), \(\frac{dV}{d\theta} > 0\) | B1 ft | |
| When \(\theta > 1.32\), \(\frac{dV}{d\theta} < 0\) | B1 ft | |
| \(V\) has a maximum; Equilibrium is unstable | M1, A1 | Fully correct working, and convincing demonstration of signs above |
# Question 6(i):
e.g. $R$ has no weight/mass; There is no friction; There is no vertical force at $R$; String has minimum length/elastic energy | B1 | For any one contributory reason **Total: 1**
## Question 6(ii):
$V = \frac{1}{2}\left(\frac{mg}{a}\right)(2a\sin\theta)^2 + mga\cos\theta$ | B2 | Give B1 for correct EE or PE
$= mga(2\sin^2\theta + \cos\theta)$ | |
$\frac{dV}{d\theta} = mga(4\sin\theta\cos\theta - \sin\theta)$ | B1 ft, B1 ft | Diffn of $\sin^2\theta$ (or $\cos^2\theta$); Diffn of $\cos\theta$ (or $\sin\theta$)
For equilibrium, $mga\sin\theta(4\cos\theta - 1) = 0$ | M1 |
$\theta = 1.32$ (or $75.5°$) | A1 | Allow $\cos^{-1}\frac{1}{4}$, $76°$; Ignore $\theta=0$ if stated **Total: 6**
SR If done by taking moments, M1A1 for $\frac{mg(2a\sin\theta)}{a}(2a\cos\theta) = mg(a\sin\theta)$; A1 for $\theta = 1.32$ (Max 3 out of 6)
## Question 6(iii):
$\frac{d^2V}{d\theta^2} = mga\cos\theta(4\cos\theta - 1) - 4mga\sin^2\theta$ | B2 ft | Give B1 if just one error; Only B1 ft if work is simpler
When $\cos\theta = \frac{1}{4}$:
$\frac{d^2V}{d\theta^2} = -4mga\sin^2\theta \quad (= -\frac{15}{4}mga) < 0$ | M1 |
Equilibrium is unstable | A1 | Fully correct working only **Total: 4**
OR When $\theta < 1.32$, $\frac{dV}{d\theta} > 0$ | B1 ft |
When $\theta > 1.32$, $\frac{dV}{d\theta} < 0$ | B1 ft |
$V$ has a maximum; Equilibrium is unstable | M1, A1 | Fully correct working, and convincing demonstration of signs above
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6\\
\includegraphics[max width=\textwidth, alt={}, center]{fb9e4e4a-953b-4e52-858e-438b4009e79c-3_428_595_221_806}
A uniform rod $A B$, of mass $m$ and length $2 a$, is free to rotate in a vertical plane about a fixed horizontal axis through $A$. A light elastic string has natural length $a$ and modulus of elasticity $m g$; one end is attached to $B$ and the other end is attached to a light ring $R$ which can slide along a smooth vertical wire. The wire is in the same vertical plane as $A B$, and is at a distance $a$ from $A$. The rod $A B$ makes an angle $\theta$ with the upward vertical, where $0 < \theta < \frac { 1 } { 2 } \pi$ (see diagram).\\
(i) Give a reason why the string $R B$ is always horizontal.\\
(ii) By considering potential energy, find the value of $\theta$ for which the system is in equilibrium.\\
(iii) Determine whether this position of equilibrium is stable or unstable.
\hfill \mbox{\textit{OCR M4 2004 Q6 [11]}}