Edexcel M2 Specimen — Question 8 15 marks

Exam BoardEdexcel
ModuleM2 (Mechanics 2)
SessionSpecimen
Marks15
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMomentum and Collisions 1
TypeCollision followed by wall impact
DifficultyStandard +0.3 This is a standard M2 collision problem requiring conservation of momentum and Newton's restitution law, followed by a wall collision and a meeting-time calculation. All techniques are routine for M2 students, though the algebra in part (c) requires careful tracking of multiple steps. Slightly easier than average due to the structured parts guiding students through the solution.
Spec6.03a Linear momentum: p = mv6.03b Conservation of momentum: 1D two particles6.03i Coefficient of restitution: e6.03j Perfectly elastic/inelastic: collisions6.03k Newton's experimental law: direct impact

8. A small ball A of mass 3 m is moving with speed u in a straight line on a smooth horizontal table. The ball collides directly with another small ball B of mass m moving with speed \(u\) towards \(A\) along the same straight line. The coefficient of restitution between \(A\) and \(B\) is \(\frac { 1 } { 2 }\). The balls have the same radius and can be modelled as particles.
  1. Find
    1. the speed of A immediately after the collision,
    2. the speed of B immediately after the collision. A fter the collision \(B\) hits a smooth vertical wall which is perpendicular to the direction of motion of \(B\). The coefficient of restitution between \(B\) and the wall is \(\frac { 2 } { 5 }\).
  2. Find the speed of B immediately after hitting the wall.
    (2) The first collision between A and B occurred at a distance 4a from the wall. The balls collide again \(T\) seconds after the first collision.
  3. Show that \(T = \frac { 112 a } { 15 u }\).

Question 8:
Part (a)(i):
AnswerMarks Guidance
WorkingMarks Notes
Conservation of Momentum: \(3mu - mu = 3mv + mw\) → \(2u = 3v + w\) (1)M1# A1
N.L.R.: \(\frac{1}{2}(u+u) = w - v\) → \(u = w - v\) (2)M1# A1
\((1)-(2)\): \(u = 4v\) → \(v = \frac{1}{4}u\)DM1# A1 (7)
Part (a)(ii):
AnswerMarks Guidance
WorkingMarks Notes
In (2): \(u = w - \frac{1}{4}u\) → \(w = \frac{5}{4}u\)A1 (7 total)
Part (b):
AnswerMarks Guidance
WorkingMarks Notes
\(B\) to wall N.L.R.: \(\dfrac{5}{4}u \times \dfrac{2}{5} = V\)M1
\(V = \dfrac{1}{2}u\)A1ft (2)
Part (c):
AnswerMarks Guidance
WorkingMarks Notes
\(B\) to wall: time \(= 4a \div \dfrac{5}{4}u = \dfrac{16a}{5u}\)B1ft
Distance travelled by \(A = \dfrac{1}{4}u \times \dfrac{16a}{5u} = \dfrac{4}{5}a\)B1ft
Collide when speed of approach \(= \dfrac{1}{2}ut + \dfrac{1}{4}ut\), distance to cover \(= 4a - \dfrac{4}{5}a\)M1$
\(\therefore t = \dfrac{4a - \frac{4}{5}a}{\frac{3}{4}u} = \dfrac{16a}{5} \times \dfrac{4}{3u} = \dfrac{64a}{15u}\)DM1$ A1
Total time \(= \dfrac{16a}{5u} + \dfrac{64a}{15u} = \dfrac{112a}{15u}\) *A1 (6) [15]
# Question 8:

## Part (a)(i):
| Working | Marks | Notes |
|---------|-------|-------|
| Conservation of Momentum: $3mu - mu = 3mv + mw$ → $2u = 3v + w$ (1) | M1# A1 | |
| N.L.R.: $\frac{1}{2}(u+u) = w - v$ → $u = w - v$ (2) | M1# A1 | |
| $(1)-(2)$: $u = 4v$ → $v = \frac{1}{4}u$ | DM1# A1 | (7) |

## Part (a)(ii):
| Working | Marks | Notes |
|---------|-------|-------|
| In (2): $u = w - \frac{1}{4}u$ → $w = \frac{5}{4}u$ | A1 | (7 total) |

## Part (b):
| Working | Marks | Notes |
|---------|-------|-------|
| $B$ to wall N.L.R.: $\dfrac{5}{4}u \times \dfrac{2}{5} = V$ | M1 | |
| $V = \dfrac{1}{2}u$ | A1ft | (2) |

## Part (c):
| Working | Marks | Notes |
|---------|-------|-------|
| $B$ to wall: time $= 4a \div \dfrac{5}{4}u = \dfrac{16a}{5u}$ | B1ft | |
| Distance travelled by $A = \dfrac{1}{4}u \times \dfrac{16a}{5u} = \dfrac{4}{5}a$ | B1ft | |
| Collide when speed of approach $= \dfrac{1}{2}ut + \dfrac{1}{4}ut$, distance to cover $= 4a - \dfrac{4}{5}a$ | M1$ | |
| $\therefore t = \dfrac{4a - \frac{4}{5}a}{\frac{3}{4}u} = \dfrac{16a}{5} \times \dfrac{4}{3u} = \dfrac{64a}{15u}$ | DM1$ A1 | |
| Total time $= \dfrac{16a}{5u} + \dfrac{64a}{15u} = \dfrac{112a}{15u}$ * | A1 | (6) **[15]** |
8. A small ball A of mass 3 m is moving with speed u in a straight line on a smooth horizontal table. The ball collides directly with another small ball B of mass m moving with speed $u$ towards $A$ along the same straight line. The coefficient of restitution between $A$ and $B$ is $\frac { 1 } { 2 }$. The balls have the same radius and can be modelled as particles.
\begin{enumerate}[label=(\alph*)]
\item Find
\begin{enumerate}[label=(\roman*)]
\item the speed of A immediately after the collision,
\item the speed of B immediately after the collision.

A fter the collision $B$ hits a smooth vertical wall which is perpendicular to the direction of motion of $B$. The coefficient of restitution between $B$ and the wall is $\frac { 2 } { 5 }$.
\end{enumerate}\item Find the speed of B immediately after hitting the wall.\\
(2)

The first collision between A and B occurred at a distance 4a from the wall. The balls collide again $T$ seconds after the first collision.
\item Show that $T = \frac { 112 a } { 15 u }$.
\end{enumerate}

\hfill \mbox{\textit{Edexcel M2  Q8 [15]}}