Edexcel FM1 2024 June — Question 4 15 marks

Exam BoardEdexcel
ModuleFM1 (Further Mechanics 1)
Year2024
SessionJune
Marks15
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMomentum and Collisions 1
TypeCollision followed by wall impact
DifficultyStandard +0.3 This is a standard Further Mechanics 1 collision problem with straightforward application of conservation of momentum and Newton's restitution law. Part (a) is a routine 'show that' requiring two equations, part (b) requires comparing velocities (standard technique), and parts (c)-(d) are direct applications of impulse and energy formulas. While it's a multi-part question requiring careful algebra, it involves no novel insight—just systematic application of well-practiced methods from the FM1 syllabus.
Spec6.03b Conservation of momentum: 1D two particles6.03e Impulse: by a force6.03f Impulse-momentum: relation6.03k Newton's experimental law: direct impact

  1. A particle \(A\) of mass \(2 m\) is moving in a straight line with speed \(3 u\) on a smooth horizontal plane. Particle \(A\) collides directly with a particle \(B\) of mass \(m\) which is at rest on the plane.
The coefficient of restitution between \(A\) and \(B\) is \(e\), where \(e > 0\)
  1. Show that the speed of \(B\) immediately after the collision is \(2 u ( 1 + e )\). After the collision, \(B\) hits a smooth fixed vertical wall which is perpendicular to the direction of motion of \(B\).
  2. Show that there will be a second collision between \(A\) and \(B\). The coefficient of restitution between \(B\) and the wall is \(\frac { 1 } { 2 }\) Find, in simplified form, in terms of \(m\), \(u\) and \(e\),
  3. the magnitude of the impulse received by \(B\) in its collision with the wall,
  4. the loss in kinetic energy of \(B\) due to its collision with the wall.

Question 4:
Part (a):
AnswerMarks Guidance
Answer/WorkingMark Guidance
CLM appliedM1
\(2m \times 3u = 2mv_A + mv_B \Rightarrow (6u = 2v_A + v_B)\) or \(2m \times 3u = -2mv_A + mv_B \Rightarrow (6u = -2v_A + v_B)\)A1
Impact Law appliedM1
\(3ue = -v_A + v_B\) or \(3ue = v_A + v_B\)A1
Solve for \(v_B\)M1
\(v_B = 2u(1+e)\)A1* Given answer
Part (b):
AnswerMarks Guidance
Answer/WorkingMark Guidance
Solve for \(v_A\)M1
\(v_A = u(2-e)\) or \(v_A = u(e-2)\)A1
Complete and correct explanation: \(0 \leq e \leq 1 \Rightarrow v_A > 0 \Rightarrow A\) continues to move towards the wall \(\Rightarrow A\) will collide again with \(B\) or \(0 \leq e \leq 1 \Rightarrow v_A < 0 \Rightarrow A\) continues to move towards the wall \(\Rightarrow A\) will collide again with \(B\)A1
Part (c):
AnswerMarks Guidance
Answer/WorkingMark Guidance
Rebound speed or velocity of \(B = \pm\frac{1}{2} \times 2u(1+e)\)B1
\(\pm m[-u(1+e) - 2u(1+e)]\)M1
\(3(1+e)mu\)A1
Part (d):
AnswerMarks Guidance
Answer/WorkingMark Guidance
Attempt at KE loss of \(B\)M1
\(\frac{1}{2}m\left[(2u(1+e))^2 - (u(1+e))^2\right]\)A1
\(\frac{3mu^2(1+e)^2}{2}\)A1
## Question 4:

### Part (a):

| Answer/Working | Mark | Guidance |
|---|---|---|
| CLM applied | M1 | |
| $2m \times 3u = 2mv_A + mv_B \Rightarrow (6u = 2v_A + v_B)$ **or** $2m \times 3u = -2mv_A + mv_B \Rightarrow (6u = -2v_A + v_B)$ | A1 | |
| Impact Law applied | M1 | |
| $3ue = -v_A + v_B$ **or** $3ue = v_A + v_B$ | A1 | |
| Solve for $v_B$ | M1 | |
| $v_B = 2u(1+e)$ | A1* | Given answer |

### Part (b):

| Answer/Working | Mark | Guidance |
|---|---|---|
| Solve for $v_A$ | M1 | |
| $v_A = u(2-e)$ **or** $v_A = u(e-2)$ | A1 | |
| Complete and correct explanation: $0 \leq e \leq 1 \Rightarrow v_A > 0 \Rightarrow A$ continues to move towards the wall $\Rightarrow A$ will collide again with $B$ **or** $0 \leq e \leq 1 \Rightarrow v_A < 0 \Rightarrow A$ continues to move towards the wall $\Rightarrow A$ will collide again with $B$ | A1 | |

### Part (c):

| Answer/Working | Mark | Guidance |
|---|---|---|
| Rebound speed or velocity of $B = \pm\frac{1}{2} \times 2u(1+e)$ | B1 | |
| $\pm m[-u(1+e) - 2u(1+e)]$ | M1 | |
| $3(1+e)mu$ | A1 | |

### Part (d):

| Answer/Working | Mark | Guidance |
|---|---|---|
| Attempt at KE loss of $B$ | M1 | |
| $\frac{1}{2}m\left[(2u(1+e))^2 - (u(1+e))^2\right]$ | A1 | |
| $\frac{3mu^2(1+e)^2}{2}$ | A1 | |
\begin{enumerate}
  \item A particle $A$ of mass $2 m$ is moving in a straight line with speed $3 u$ on a smooth horizontal plane. Particle $A$ collides directly with a particle $B$ of mass $m$ which is at rest on the plane.
\end{enumerate}

The coefficient of restitution between $A$ and $B$ is $e$, where $e > 0$\\
(a) Show that the speed of $B$ immediately after the collision is $2 u ( 1 + e )$.

After the collision, $B$ hits a smooth fixed vertical wall which is perpendicular to the direction of motion of $B$.\\
(b) Show that there will be a second collision between $A$ and $B$.

The coefficient of restitution between $B$ and the wall is $\frac { 1 } { 2 }$\\
Find, in simplified form, in terms of $m$, $u$ and $e$,\\
(c) the magnitude of the impulse received by $B$ in its collision with the wall,\\
(d) the loss in kinetic energy of $B$ due to its collision with the wall.

\hfill \mbox{\textit{Edexcel FM1 2024 Q4 [15]}}