Edexcel M2 2014 June — Question 5 9 marks

Exam BoardEdexcel
ModuleM2 (Mechanics 2)
Year2014
SessionJune
Marks9
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMomentum and Collisions 1
TypeMultiple wall bounces or returns
DifficultyStandard +0.3 This is a standard M2 mechanics question involving coefficient of restitution and impulse-momentum theorem. Part (a) requires straightforward application of impulse = change in momentum with the restitution formula. Part (b) involves setting up distance equations for the two journeys (O to wall, wall to O) using the reduced speed after impact. While it requires careful bookkeeping of the speeds and distances, it follows a well-practiced template for collision problems with no novel insight required. Slightly easier than average due to the structured setup and standard techniques.
Spec6.03j Perfectly elastic/inelastic: collisions6.03k Newton's experimental law: direct impact

5. A particle of mass \(m \mathrm {~kg}\) lies on a smooth horizontal surface. Initially the particle is at rest at a point \(O\) midway between a pair of fixed parallel vertical walls. The walls are 2 m apart. At time \(t = 0\) the particle is projected from \(O\) with speed \(u \mathrm {~m} \mathrm {~s} ^ { - 1 }\) in a direction perpendicular to the walls. The coefficient of restitution between the particle and each wall is \(\frac { 2 } { 3 }\). The magnitude of the impulse on the particle due to the first impact with a wall is \(\lambda m u \mathrm {~N} \mathrm {~s}\).
  1. Find the value of \(\lambda\). The particle returns to \(O\), having bounced off each wall once, at time \(t = 3\) seconds.
  2. Find the value of \(u\).

Question 5:
Part (a):
AnswerMarks Guidance
Answer/WorkingMarks Guidance
Speed after impact \(= \frac{2}{3}u\)B1 Allow for velocity \(= -\frac{2u}{3}\)
Impulse \(=\) change in momentum \(= \pm\left(m \cdot \frac{2}{3}u - m(-u)\right) = \frac{5}{3}mu\)M1 Need to consider momentum before and after collision and use change of direction
\(\lambda = \frac{5}{3}\)A1 cso
Part (b):
AnswerMarks Guidance
Answer/WorkingMarks Guidance
Speed after second collision \(= e^2u = \frac{4}{9}u\)B1 Allow negative
Total time taken \(= \frac{1}{u} + \frac{2}{eu} + \frac{1}{e^2u} = \frac{1}{u} + \frac{3}{u} + \frac{9}{4u}\)M1 Use of time \(= \frac{\text{distance}}{\text{speed}}\) to find total time in terms of \(u\). At least one term dealt with correctly
A2\(-1\) each error
Alt M1A2: Ratio of times \(\frac{1}{3}:1:\frac{3}{4}\)M1, A2 Or equivalent. \(-1\) each error
\(\frac{4}{u} + \frac{9}{4u} = \frac{25}{4u} = 3\), \(\quad u = \frac{25}{12}\) o.e.DM1 Use total time \(= 3\) and solve for \(u\)
A1Accept 2.08 and 2.1 (or better)
## Question 5:

### Part (a):

| Answer/Working | Marks | Guidance |
|---|---|---|
| Speed after impact $= \frac{2}{3}u$ | B1 | Allow for velocity $= -\frac{2u}{3}$ |
| Impulse $=$ change in momentum $= \pm\left(m \cdot \frac{2}{3}u - m(-u)\right) = \frac{5}{3}mu$ | M1 | Need to consider momentum before and after collision and use change of direction |
| $\lambda = \frac{5}{3}$ | A1 | cso |

### Part (b):

| Answer/Working | Marks | Guidance |
|---|---|---|
| Speed after second collision $= e^2u = \frac{4}{9}u$ | B1 | Allow negative |
| Total time taken $= \frac{1}{u} + \frac{2}{eu} + \frac{1}{e^2u} = \frac{1}{u} + \frac{3}{u} + \frac{9}{4u}$ | M1 | Use of time $= \frac{\text{distance}}{\text{speed}}$ to find total time in terms of $u$. At least one term dealt with correctly |
| | A2 | $-1$ each error |
| **Alt M1A2:** Ratio of times $\frac{1}{3}:1:\frac{3}{4}$ | M1, A2 | Or equivalent. $-1$ each error |
| $\frac{4}{u} + \frac{9}{4u} = \frac{25}{4u} = 3$, $\quad u = \frac{25}{12}$ o.e. | DM1 | Use total time $= 3$ and solve for $u$ |
| | A1 | Accept 2.08 and 2.1 (or better) |

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5. A particle of mass $m \mathrm {~kg}$ lies on a smooth horizontal surface. Initially the particle is at rest at a point $O$ midway between a pair of fixed parallel vertical walls. The walls are 2 m apart. At time $t = 0$ the particle is projected from $O$ with speed $u \mathrm {~m} \mathrm {~s} ^ { - 1 }$ in a direction perpendicular to the walls. The coefficient of restitution between the particle and each wall is $\frac { 2 } { 3 }$. The magnitude of the impulse on the particle due to the first impact with a wall is $\lambda m u \mathrm {~N} \mathrm {~s}$.
\begin{enumerate}[label=(\alph*)]
\item Find the value of $\lambda$.

The particle returns to $O$, having bounced off each wall once, at time $t = 3$ seconds.
\item Find the value of $u$.
\end{enumerate}

\hfill \mbox{\textit{Edexcel M2 2014 Q5 [9]}}