CAIE M1 2005 November — Question 7 10 marks

Exam BoardCAIE
ModuleM1 (Mechanics 1)
Year2005
SessionNovember
Marks10
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicPulley systems
TypeTwo particles over pulley, vertical strings
DifficultyStandard +0.3 This is a standard M1 pulley problem requiring Newton's second law for connected particles, followed by routine kinematics (SUVAT) and energy calculations. The multi-part structure and need to track motion after disconnection adds slight complexity, but all techniques are textbook applications with no novel insight required.
Spec3.03k 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]{2026cad4-8494-4139-ad21-d8a17ac2b955-4_601_515_699_815} Two particles \(A\) and \(B\), of masses 0.3 kg and 0.2 kg respectively, are attached to the ends of a light inextensible string which passes over a smooth fixed pulley. Particle \(B\) is held on the horizontal floor and particle \(A\) hangs in equilibrium. Particle \(B\) is released and each particle starts to move vertically with constant acceleration of magnitude \(a \mathrm {~m} \mathrm {~s} ^ { - 2 }\).
  1. Find the value of \(a\). Particle \(A\) hits the floor 1.2 s after it starts to move, and does not rebound upwards.
  2. Show that \(A\) hits the floor with a speed of \(2.4 \mathrm {~m} \mathrm {~s} ^ { - 1 }\).
  3. Find the gain in gravitational potential energy by \(B\), from leaving the floor until reaching its greatest height.

Question 7:
Part (i)
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(0.3g - T = 0.3a\), \(T - 0.2g = 0.2a\)M1, A1 For applying Newton's second law to either particle
\(0.3g - 0.2g = 0.3a + 0.2a\)M1 For eliminating \(T\)
\(a = 2\)A1
Alternatively: \(a = \frac{m_1 - m_2}{m_1 + m_2}g\)M2, A2
Part (ii)
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(v = 2 \times 1.2\); Speed is \(2.4\ \text{ms}^{-1}\)B1
Part (iii)
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(s_1 = \frac{1}{2}(0 + 2.4) \times 1.2\)B1
\(2.4^2 = 2gs_2\) or PE gain while string is slack \(= \frac{1}{2} \times 0.2 \times 2.4^2\)M1 For using \(u^2 = 2gs\) or 'gain in PE = loss in KE'
\((s_1 + s_2) = 1.728\) or PE gain while string is slack \(= 0.576\) JA1 May be implied by final answer
Total PE gain \(= 0.2g \times 1.728\) (or PE gain while string is taut \(= 0.2g \times 1.44\))M1 For using PE gain \(= mg(s_1 + s_2)\) (or PE gain while string is taut \(= mgs_1\), in the case where PE gain while string is slack is calculated separately)
Total PE gain \(= 3.456\) JA1
## Question 7:

### Part (i)
| Answer/Working | Mark | Guidance |
|---|---|---|
| $0.3g - T = 0.3a$, $T - 0.2g = 0.2a$ | M1, A1 | For applying Newton's second law to either particle |
| $0.3g - 0.2g = 0.3a + 0.2a$ | M1 | For eliminating $T$ |
| $a = 2$ | A1 | |
| Alternatively: $a = \frac{m_1 - m_2}{m_1 + m_2}g$ | M2, A2 | |

### Part (ii)
| Answer/Working | Mark | Guidance |
|---|---|---|
| $v = 2 \times 1.2$; Speed is $2.4\ \text{ms}^{-1}$ | B1 | |

### Part (iii)
| Answer/Working | Mark | Guidance |
|---|---|---|
| $s_1 = \frac{1}{2}(0 + 2.4) \times 1.2$ | B1 | |
| $2.4^2 = 2gs_2$ or PE gain while string is slack $= \frac{1}{2} \times 0.2 \times 2.4^2$ | M1 | For using $u^2 = 2gs$ or 'gain in PE = loss in KE' |
| $(s_1 + s_2) = 1.728$ or PE gain while string is slack $= 0.576$ J | A1 | May be implied by final answer |
| Total PE gain $= 0.2g \times 1.728$ (or PE gain while string is taut $= 0.2g \times 1.44$) | M1 | For using PE gain $= mg(s_1 + s_2)$ (or PE gain while string is taut $= mgs_1$, in the case where PE gain while string is slack is calculated separately) |
| Total PE gain $= 3.456$ J | A1 | |
7\\
\includegraphics[max width=\textwidth, alt={}, center]{2026cad4-8494-4139-ad21-d8a17ac2b955-4_601_515_699_815}

Two particles $A$ and $B$, of masses 0.3 kg and 0.2 kg respectively, are attached to the ends of a light inextensible string which passes over a smooth fixed pulley. Particle $B$ is held on the horizontal floor and particle $A$ hangs in equilibrium. Particle $B$ is released and each particle starts to move vertically with constant acceleration of magnitude $a \mathrm {~m} \mathrm {~s} ^ { - 2 }$.\\
(i) Find the value of $a$.

Particle $A$ hits the floor 1.2 s after it starts to move, and does not rebound upwards.\\
(ii) Show that $A$ hits the floor with a speed of $2.4 \mathrm {~m} \mathrm {~s} ^ { - 1 }$.\\
(iii) Find the gain in gravitational potential energy by $B$, from leaving the floor until reaching its greatest height.

\hfill \mbox{\textit{CAIE M1 2005 Q7 [10]}}