OCR M1 2012 January — Question 7 16 marks

Exam BoardOCR
ModuleM1 (Mechanics 1)
Year2012
SessionJanuary
Marks16
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicPulley systems
TypeThree or more connected particles
DifficultyStandard +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.
Spec3.02d 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

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 \(R\).
  1. (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 \(R\).
  2. 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.
  3. Calculate the greatest height of \(P\) above the surface.

Question 7:
Part (i)(a)
AnswerMarks Guidance
AnswerMarks 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)
AnswerMarks Guidance
AnswerMarks 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)
AnswerMarks Guidance
AnswerMarks 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)
AnswerMarks Guidance
AnswerMarks 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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# 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]}}