| Exam Board | OCR |
|---|---|
| Module | M1 (Mechanics 1) |
| Year | 2012 |
| Session | January |
| Marks | 16 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Pulley systems |
| Type | Three or more connected particles |
| Difficulty | Standard +0.3 This is a standard three-particle pulley system requiring systematic application of Newton's second law to each particle, followed by a kinematics calculation. While it involves multiple connected parts and careful bookkeeping of forces, the techniques are routine for M1 students who have practiced pulley problems. The multi-stage nature (descent, then after R hits) adds modest complexity but follows predictable patterns. |
| Spec | 3.02d Constant acceleration: SUVAT formulae3.03k Connected particles: pulleys and equilibrium3.03l Newton's third law: extend to situations requiring force resolution6.02i Conservation of energy: mechanical energy principle |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| \(0.45a = 0.45g - 2.52\) | M1 | N2L for R. 2 vertical forces. Accept \(+/-0.45a = 0.45g +/- 2.52\) |
| \(a = 4.2 \text{ ms}^{-2}\) | A1 [2] | Accept \(-4.2\) |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| \(0.05 \times 4.2 = 0.05g + 2.52 - T\) | M1 | N2L for Q, 3 vertical forces, \(0.05 \times 4.2 = 0.05g +/- 2.52 +/- T\); accn not 9.8; \(0.5g\) is TWO vertical forces \((0.45g + 0.05g)\) not MR |
| \(T = 0.05 \times 9.8 + 2.52 - 0.05 \times 4.2\) | A1 ft | ft cv\((a(\mathbf{i}))\). Any equivalent form of equation |
| \(T = 2.8 \text{ N}\) | A1 [3] | |
| ACCEPT COMBINED Q AND R METHOD: \((0.45+0.05) \times 4.2 = 0.45g + 0.05g +/-T\) giving \(T = 2.8\text{ N}\) | M1, A1ft, A1 |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| \(\pm 4.2m = T - mg\) OR \(\pm 4.2 = (0.05g + 0.45g - mg)/(0.05 + 0.45 + m)\) | M1 | N2L for P, difference of 2 vertical forces, accn cv\((a(\mathbf{i}))\); \(\pm\text{cv}(a(\mathbf{i})) = (\text{wt } P + \text{wt } Q - \text{wt } R)/\text{sum of masses}\) |
| \(4.2m = 2.8 - mg\) OR \(9.8m + 4.2m = 2.8\) | A1 ft | ft cv\((T(\mathbf{ib}))\). Any equivalent form of equation with cv\((a(\mathbf{i}))\) |
| \(m = 0.2\) | A1 [3] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| BEFORE R STRIKES SURFACE | ||
| \(v = 4.2 \times 0.5\) | M1* | Find speed when R hits surface, using \(a(\mathbf{i})\) |
| \(v = 2.1\) | A1 | |
| \(s = 2.1^2/(2 \times 4.2) = 4.2 \times 0.5^2/2\) | M1 | Distance R falls (0.525 m). Accept \(+/-4.2 \times 0.5^2/2\) |
| AFTER R STRIKES SURFACE | ||
| \(+/-0.2a = T - 0.2g\) OR \(+/-0.05a = 0.05g - T\) | M1 | N2L for either P (with cv\((m)\)) or Q |
| \(+/-0.2a = T - 0.2g\) AND \(+/-0.05a = 0.05g - T\) | A1 | Correct equations for both P and Q. OR combination \(0.05g(-T+T) - 0.2g = +/-(0.2a + 0.05a)\) |
| \(a = +/-5.88\) | A1 | |
| \(S = 2.1^2/(2 \times 5.88)\) | D*M1 | Distance P rises after R hits ground (0.375), \(a\) not \(a(\mathbf{i})\) or 9.8 |
| TOTAL JOURNEY Distance \(= (0.375 + 0.525) = 0.9\text{ m}\) | A1 [8] |
# Question 7:
## Part (i)(a)
| Answer | Marks | Guidance |
|--------|-------|----------|
| $0.45a = 0.45g - 2.52$ | M1 | N2L for R. 2 vertical forces. Accept $+/-0.45a = 0.45g +/- 2.52$ |
| $a = 4.2 \text{ ms}^{-2}$ | A1 **[2]** | Accept $-4.2$ |
## Part (i)(b)
| Answer | Marks | Guidance |
|--------|-------|----------|
| $0.05 \times 4.2 = 0.05g + 2.52 - T$ | M1 | N2L for Q, 3 vertical forces, $0.05 \times 4.2 = 0.05g +/- 2.52 +/- T$; accn not 9.8; $0.5g$ is TWO vertical forces $(0.45g + 0.05g)$ not MR |
| $T = 0.05 \times 9.8 + 2.52 - 0.05 \times 4.2$ | A1 ft | ft cv$(a(\mathbf{i}))$. Any equivalent form of equation |
| $T = 2.8 \text{ N}$ | A1 **[3]** | |
| ACCEPT COMBINED Q AND R METHOD: $(0.45+0.05) \times 4.2 = 0.45g + 0.05g +/-T$ giving $T = 2.8\text{ N}$ | M1, A1ft, A1 | |
## Part (ii)
| Answer | Marks | Guidance |
|--------|-------|----------|
| $\pm 4.2m = T - mg$ OR $\pm 4.2 = (0.05g + 0.45g - mg)/(0.05 + 0.45 + m)$ | M1 | N2L for P, difference of 2 vertical forces, accn cv$(a(\mathbf{i}))$; $\pm\text{cv}(a(\mathbf{i})) = (\text{wt } P + \text{wt } Q - \text{wt } R)/\text{sum of masses}$ |
| $4.2m = 2.8 - mg$ OR $9.8m + 4.2m = 2.8$ | A1 ft | ft cv$(T(\mathbf{ib}))$. Any equivalent form of equation with cv$(a(\mathbf{i}))$ |
| $m = 0.2$ | A1 **[3]** | |
## Part (iii)
| Answer | Marks | Guidance |
|--------|-------|----------|
| **BEFORE R STRIKES SURFACE** | | |
| $v = 4.2 \times 0.5$ | M1* | Find speed when R hits surface, using $a(\mathbf{i})$ |
| $v = 2.1$ | A1 | |
| $s = 2.1^2/(2 \times 4.2) = 4.2 \times 0.5^2/2$ | M1 | Distance R falls (0.525 m). Accept $+/-4.2 \times 0.5^2/2$ |
| **AFTER R STRIKES SURFACE** | | |
| $+/-0.2a = T - 0.2g$ OR $+/-0.05a = 0.05g - T$ | M1 | N2L for either P (with cv$(m)$) or Q |
| $+/-0.2a = T - 0.2g$ AND $+/-0.05a = 0.05g - T$ | A1 | Correct equations for both P and Q. OR combination $0.05g(-T+T) - 0.2g = +/-(0.2a + 0.05a)$ |
| $a = +/-5.88$ | A1 | |
| $S = 2.1^2/(2 \times 5.88)$ | D*M1 | Distance P rises after R hits ground (0.375), $a$ not $a(\mathbf{i})$ or 9.8 |
| **TOTAL JOURNEY** Distance $= (0.375 + 0.525) = 0.9\text{ m}$ | A1 **[8]** | |
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7\\
\includegraphics[max width=\textwidth, alt={}, center]{2b3457b6-1fe9-4e67-91d4-a8bc4a5b1709-4_369_508_246_781}
Particles $P$ and $Q$, of masses $m \mathrm {~kg}$ and 0.05 kg respectively, are attached to the ends of a light inextensible string which passes over a smooth pulley. $Q$ is attached to a particle $R$ of mass 0.45 kg by a light inextensible string. The strings are taut, and the portions of the strings not in contact with the pulley are vertical. $P$ is in contact with a horizontal surface when the particles are released from rest (see diagram). The tension in the string $Q R$ is 2.52 N during the descent of $R$.
\begin{enumerate}[label=(\roman*)]
\item (a) Find the acceleration of $R$ during its descent.\\
(b) By considering the motion of $Q$, calculate the tension in the string $P Q$ during the descent of $R$.
\item Find the value of $m$.\\
$R$ strikes the surface 0.5 s after release and does not rebound. During their subsequent motion, $P$ does not reach the pulley and $Q$ does not reach the surface.
\item Calculate the greatest height of $P$ above the surface.
\end{enumerate}
\hfill \mbox{\textit{OCR M1 2012 Q7 [16]}}