Edexcel M1 2014 June — Question 7 16 marks

Exam BoardEdexcel
ModuleM1 (Mechanics 1)
Year2014
SessionJune
Marks16
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicPulley systems
TypeHeavier particle hits ground, lighter continues upward - inclined plane involved
DifficultyStandard +0.3 This is a standard M1 pulley system question with connected particles. Part (a) requires routine application of F=ma to both particles with given answer to show. Parts (b)-(d) involve straightforward kinematics after Q hits ground. All techniques are standard textbook exercises requiring no novel insight, though the multi-part nature and careful tracking of motion phases makes it slightly above average difficulty for M1.
Spec3.02d Constant acceleration: SUVAT formulae3.03k Connected particles: pulleys and equilibrium3.03l Newton's third law: extend to situations requiring force resolution3.03o Advanced connected particles: and pulleys

7. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{edcc4603-f006-4c4f-a4e5-063cab41da98-12_486_1257_230_347} \captionsetup{labelformat=empty} \caption{Figure 3}
\end{figure} Two particles \(P\) and \(Q\), of mass 2 kg and 3 kg respectively, are connected by a light inextensible string. Initially \(P\) is held at rest on a fixed smooth plane inclined at \(30 ^ { \circ }\) to the horizontal. The string passes over a small smooth fixed pulley at the top of the plane. The particle \(Q\) hangs freely below the pulley and 0.6 m above the ground, as shown in Figure 3. The part of the string from \(P\) to the pulley is parallel to a line of greatest slope of the plane. The system is released from rest with the string taut. For the motion before \(Q\) hits the ground,
    1. show that the acceleration of \(Q\) is \(\frac { 2 g } { 5 }\),
    2. find the tension in the string. On hitting the ground \(Q\) is immediately brought to rest by the impact.
  1. Find the speed of \(P\) at the instant when \(Q\) hits the ground. In its subsequent motion \(P\) does not reach the pulley.
  2. Find the total distance moved up the plane by \(P\) before it comes to instantaneous rest.
  3. Find the length of time between \(Q\) hitting the ground and \(P\) first coming to instantaneous rest.

Question 7:
Part (a):
AnswerMarks Guidance
AnswerMarks Guidance
\(3g - T = 3a\)M1 Eqn of motion for \(Q\): must have the correct terms but condone sign errors
A1Correct equation
\(T - 2g\cos60 = 2a \quad (T - g = 2a)\)M1 Eqn of motion for \(P\): must have the correct terms but condone sign errors. Weight must be resolved
A1Correct equation
Allow M1A1 for \(3g - 2g\cos60 = 5a\) in place of either of these two equations
\(2g = 5a \quad a = \frac{2g}{5}\) ✱DM1 Use an exact method to solve for \(a\) (i.e. not the equation solver on their calculator). Dependent on the first 2 M marks or the M for the combined equation
A1Given answer derived correctly from exact working
\(T = 2 \times \frac{2g}{5} + g = \frac{9g}{5}\)M1 Use given acceleration to solve for \(T\)
A1(8)Accept 18 or 17.6
Part (b):
AnswerMarks Guidance
AnswerMarks Guidance
\(v^2 = 2 \times \frac{2g}{5} \times 0.6 = \frac{2.4g}{5}\)M1 Use the given acceleration to find the speed
\(v = \frac{2}{5}\sqrt{3g}\) oe involving \(g\)A1(2) Accept 2.2 or 2.17
Part (c):
AnswerMarks Guidance
AnswerMarks Guidance
String slack: accel of \(P\) (up plane) \(= -g\cos60 = -\frac{1}{2}g\)B1
\(0 = \frac{2.4g}{5} - gs\)M1 Use of \(v^2 = u^2 + 2as\) or equivalent for their acceleration \(\neq \frac{2g}{5}\)
\(s = \frac{2.4g}{5} \times \frac{1}{g} = \frac{2.4}{5} = 0.48\)A1
Total dist \(= 1.08\) mA1ft(4) \(0.6 +\) their \(0.48\)
Part (d):
AnswerMarks Guidance
AnswerMarks Guidance
\(0 = \frac{2}{5}\sqrt{3g} - \frac{g}{2}t \quad (0 = 2.17 - 4.9t)\)M1 Use of \(v = u + at\) or equivalent with their acceleration \(\neq \frac{2g}{5}\) to find \(t\)
\(t = \frac{4\sqrt{3g}}{5g} = 0.4426...\)
\(= 0.44\) or \(0.443\)A1(2) only
Total: [16]
# Question 7:

## Part (a):
| Answer | Marks | Guidance |
|--------|-------|----------|
| $3g - T = 3a$ | M1 | Eqn of motion for $Q$: must have the correct terms but condone sign errors |
| | A1 | Correct equation |
| $T - 2g\cos60 = 2a \quad (T - g = 2a)$ | M1 | Eqn of motion for $P$: must have the correct terms but condone sign errors. Weight must be resolved |
| | A1 | Correct equation |
| Allow M1A1 for $3g - 2g\cos60 = 5a$ in place of either of these two equations | | |
| $2g = 5a \quad a = \frac{2g}{5}$ ✱ | DM1 | Use an exact method to solve for $a$ (i.e. not the equation solver on their calculator). Dependent on the first 2 M marks or the M for the combined equation |
| | A1 | Given answer derived correctly from exact working |
| $T = 2 \times \frac{2g}{5} + g = \frac{9g}{5}$ | M1 | Use given acceleration to solve for $T$ |
| | A1(8) | Accept 18 or 17.6 |

## Part (b):
| Answer | Marks | Guidance |
|--------|-------|----------|
| $v^2 = 2 \times \frac{2g}{5} \times 0.6 = \frac{2.4g}{5}$ | M1 | Use the given acceleration to find the speed |
| $v = \frac{2}{5}\sqrt{3g}$ oe involving $g$ | A1(2) | Accept 2.2 or 2.17 |

## Part (c):
| Answer | Marks | Guidance |
|--------|-------|----------|
| String slack: accel of $P$ (up plane) $= -g\cos60 = -\frac{1}{2}g$ | B1 | |
| $0 = \frac{2.4g}{5} - gs$ | M1 | Use of $v^2 = u^2 + 2as$ or equivalent for their acceleration $\neq \frac{2g}{5}$ |
| $s = \frac{2.4g}{5} \times \frac{1}{g} = \frac{2.4}{5} = 0.48$ | A1 | |
| Total dist $= 1.08$ m | A1ft(4) | $0.6 +$ their $0.48$ |

## Part (d):
| Answer | Marks | Guidance |
|--------|-------|----------|
| $0 = \frac{2}{5}\sqrt{3g} - \frac{g}{2}t \quad (0 = 2.17 - 4.9t)$ | M1 | Use of $v = u + at$ or equivalent with their acceleration $\neq \frac{2g}{5}$ to find $t$ |
| $t = \frac{4\sqrt{3g}}{5g} = 0.4426...$ | | |
| $= 0.44$ or $0.443$ | A1(2) | only |

**Total: [16]**
7.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{edcc4603-f006-4c4f-a4e5-063cab41da98-12_486_1257_230_347}
\captionsetup{labelformat=empty}
\caption{Figure 3}
\end{center}
\end{figure}

Two particles $P$ and $Q$, of mass 2 kg and 3 kg respectively, are connected by a light inextensible string. Initially $P$ is held at rest on a fixed smooth plane inclined at $30 ^ { \circ }$ to the horizontal. The string passes over a small smooth fixed pulley at the top of the plane. The particle $Q$ hangs freely below the pulley and 0.6 m above the ground, as shown in Figure 3. The part of the string from $P$ to the pulley is parallel to a line of greatest slope of the plane. The system is released from rest with the string taut.

For the motion before $Q$ hits the ground,
\begin{enumerate}[label=(\alph*)]
\item \begin{enumerate}[label=(\roman*)]
\item show that the acceleration of $Q$ is $\frac { 2 g } { 5 }$,
\item find the tension in the string.

On hitting the ground $Q$ is immediately brought to rest by the impact.
\end{enumerate}\item Find the speed of $P$ at the instant when $Q$ hits the ground.

In its subsequent motion $P$ does not reach the pulley.
\item Find the total distance moved up the plane by $P$ before it comes to instantaneous rest.
\item Find the length of time between $Q$ hitting the ground and $P$ first coming to instantaneous rest.
\end{enumerate}

\hfill \mbox{\textit{Edexcel M1 2014 Q7 [16]}}