Edexcel FM1 2023 June — Question 7 14 marks

Exam BoardEdexcel
ModuleFM1 (Further Mechanics 1)
Year2023
SessionJune
Marks14
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicOblique and successive collisions
TypeBall between two walls, successive rebounds
DifficultyChallenging +1.2 This is a standard Further Mechanics 1 collision question requiring systematic application of restitution laws and geometric relationships. Parts (a)-(b) involve routine resolution of velocities and applying e = (separation speed)/(approach speed) perpendicular to walls. Part (c) requires angle sum reasoning in triangle APQ. Part (d) is a straightforward deduction from the given result. While it's multi-part and requires careful bookkeeping, it follows predictable FM1 patterns without requiring novel insight—slightly above average difficulty due to the geometric coordination needed across multiple collisions.
Spec6.03k Newton's experimental law: direct impact6.03l Newton's law: oblique impacts

7. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{0da9cd5b-6f6f-4607-bd4f-c8ae164466ae-24_721_1367_280_349} \captionsetup{labelformat=empty} \caption{Figure 2}
\end{figure} A small smooth snooker ball is projected from the corner \(A\) of a horizontal rectangular snooker table \(A B C D\). The ball is projected so it first hits the side \(D C\) at the point \(P\), then hits the side \(C B\) at the point \(Q\) and then returns to \(A\). Angle \(A P D = \alpha\), Angle \(Q P C = \beta\), Angle \(A Q B = \gamma\) The ball moves along \(A P\) with speed \(U\), along \(P Q\) with speed \(V\) and along \(Q A\) with speed \(W\), as shown in Figure 2. The coefficient of restitution between the ball and side \(D C\) is \(e _ { 1 }\) The coefficient of restitution between the ball and side \(C B\) is \(e _ { 2 }\) The ball is modelled as a particle. \section*{Use the model to answer all parts of this question.}
  1. Show that \(\tan \beta = e _ { 1 } \tan \alpha\)
  2. Hence show that \(e _ { 1 } \tan \alpha = e _ { 2 } \cot \gamma\)
  3. By considering (angle \(A P Q\) + angle \(A Q P\) ) or otherwise, show that it would be possible for the ball to return to \(A\) only if \(e _ { 2 } > e _ { 1 }\) If instead \(e _ { 1 } = e _ { 2 }\), the ball would not return to \(A\).
    Given that \(e _ { 1 } = e _ { 2 }\)
  4. use the result from part (b) to describe the path of the ball after it hits \(C B\) at \(Q\), explaining your answer.

Question 7(a):
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(V\sin\beta = e_1 U\sin\alpha\)B1 3.4 – \(e_1 U\sin\alpha\) seen from a relevant equation or diagram
\(V\cos\beta = U\cos\alpha\)B1 3.4 – \(U\cos\alpha\) seen in a relevant equation or diagram
Eliminate \(U\) and \(V\) from two equationsM1 1.1b – A clear method using two equations to eliminate \(U\) and \(V\)
\(\tan\beta = e_1\tan\alpha\) *A1* 2.2a – Given answer correctly obtained. Must include both equations showing how to reach both \(\tan\beta\) and \(e_1\tan\alpha\). Accept \(\tan\beta = e_1\tan\alpha\) or \(e_1\tan\alpha = \tan\beta\)
Total(4)
Question 7(b):
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(\tan\gamma = e_2\tan(90°-\beta)\), so \(\tan\gamma = e_2\cot\beta\), \(\cot\gamma = \dfrac{\tan\beta}{e_2}\)B1 1.1b – Form correct expression for \(\tan\gamma\) or \(\cot\gamma\) in terms of \(e_2\) and \(\beta\) or \((90-\beta)\). May quote result from (a) or obtain again
\(\tan\gamma = e_2 \times \dfrac{1}{\tan\beta} = e_2 \times \dfrac{1}{e_1\tan\alpha}\)M1 3.1b – Use result from (a) to eliminate \(\tan\beta\) and form equation in \(\alpha\), \(\gamma\), \(e_1\), \(e_2\)
\(e_1\tan\alpha = e_2\cot\gamma\) *A1* 2.2a – Given answer correctly obtained. Must include replacement of \(\tan\beta\) and rearrangement. Accept \(e_1\tan\alpha = e_2\cot\gamma\) or \(e_2\cot\gamma = e_1\tan\alpha\)
Total(3)
Question 7(c):
AnswerMarks Guidance
Answer/WorkingMark Guidance
\((\text{angle } APQ + \text{angle } AQP) = (180°-\alpha-\beta)+\{180°-(90°-\beta)-\gamma\} = 270°-\alpha-\gamma\). Otherwise: angle \(PAQ = \alpha+\gamma-90°\)M1 1.1b – Clear attempt to find angle sum (condone slips) or another relevant starting point e.g. expression for angle \(PAQ\)
To return to \(A\): angle \(APQ\) + angle \(AQP < 180°\) since \(APQ\) is a triangle. Otherwise: angle \(PAQ > 0\)M1 3.1b – Clear statement to form inequality e.g. correct angle sum \(< 180°\) is acceptable, or angle \(PAQ > 0\)
\(270°-\alpha-\gamma < 180° \Rightarrow \alpha > 90°-\gamma\)A1 1.1b – Correct simplified inequality in correct form
\(\tan\alpha > \tan(90°-\gamma)\) – correct method using addition formulaeM1 1.1b – Correct method to form inequality in tan or cot
\(\dfrac{e_2\cot\gamma}{e_1} > \cot\gamma\)M1 1.1b – Using part (b) to eliminate the angles
\(e_2 > e_1\) *A1* 2.2a – Given answer correctly obtained
Total(6)
Question 7(d):
AnswerMarks Guidance
Answer/WorkingMark Guidance
From (b), \(\alpha = 90°-\gamma\), so it moves parallel to \(AP\), e.g. parallel to the initial velocityB1 2.4
Total(1)
Question 7:
Part (c) alt — Use of trig identity
AnswerMarks Guidance
Answer/WorkingMark Guidance
(angle \(APQ\) + angle \(AQP\)) \(= (180° - \alpha - \beta) + \{180° - (90° - \beta) - \gamma\} = 270 - \alpha - \gamma\)M1
To return to \(A\), (angle \(APQ\) + angle \(AQP\)) \(< 180°\), since \(APQ\) is a triangleM1
\(\tan(\alpha + \gamma) = \dfrac{\tan\alpha + \tan\gamma}{1 - \tan\alpha\tan\gamma}\) and \(\tan\alpha = \dfrac{e_2\cot\gamma}{e_1}\) or \(\tan\alpha = \dfrac{e_2}{e_1\tan\gamma}\), leads to \(\tan(\alpha+\gamma) = \dfrac{e_2 + e_1\tan^2\gamma}{e_1\tan\gamma - e_2\tan\gamma}\) oeA1
\(180 > (\alpha+\gamma) > 90 \Rightarrow \tan(\alpha+\gamma) < 0 \Rightarrow \dfrac{e_2 + e_1\tan^2\gamma}{e_1\tan\gamma - e_2\tan\gamma} < 0\)M1 Condone if '\(180 >\)' is not stated again
Since numerator \(> 0\), therefore \(e_1\tan\gamma - e_2\tan\gamma < 0\)M1
\(e_2 > e_1\) *A1
Part (d)
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(\alpha = 90° - \gamma\), so it moves parallel to \(AP\); or \(\alpha = 90° - \gamma\), so it moves parallel to the initial velocityB1 Use given information from (b) to make any equivalent statement with a correct reason and no incorrect statements. Do not accept 'it moves parallel to the initial speed'
# Question 7(a):

| Answer/Working | Mark | Guidance |
|---|---|---|
| $V\sin\beta = e_1 U\sin\alpha$ | B1 | 3.4 – $e_1 U\sin\alpha$ seen from a relevant equation or diagram |
| $V\cos\beta = U\cos\alpha$ | B1 | 3.4 – $U\cos\alpha$ seen in a relevant equation or diagram |
| Eliminate $U$ and $V$ from two equations | M1 | 1.1b – A clear method using **two equations** to eliminate $U$ and $V$ |
| $\tan\beta = e_1\tan\alpha$ * | A1* | 2.2a – Given answer correctly obtained. Must include both equations showing how to reach both $\tan\beta$ and $e_1\tan\alpha$. Accept $\tan\beta = e_1\tan\alpha$ or $e_1\tan\alpha = \tan\beta$ |
| **Total** | **(4)** | |

# Question 7(b):

| Answer/Working | Mark | Guidance |
|---|---|---|
| $\tan\gamma = e_2\tan(90°-\beta)$, so $\tan\gamma = e_2\cot\beta$, $\cot\gamma = \dfrac{\tan\beta}{e_2}$ | B1 | 1.1b – Form correct expression for $\tan\gamma$ or $\cot\gamma$ in terms of $e_2$ and $\beta$ or $(90-\beta)$. May quote result from (a) or obtain again |
| $\tan\gamma = e_2 \times \dfrac{1}{\tan\beta} = e_2 \times \dfrac{1}{e_1\tan\alpha}$ | M1 | 3.1b – **Use result from (a)** to eliminate $\tan\beta$ and form equation in $\alpha$, $\gamma$, $e_1$, $e_2$ |
| $e_1\tan\alpha = e_2\cot\gamma$ * | A1* | 2.2a – Given answer correctly obtained. Must include replacement of $\tan\beta$ and rearrangement. Accept $e_1\tan\alpha = e_2\cot\gamma$ or $e_2\cot\gamma = e_1\tan\alpha$ |
| **Total** | **(3)** | |

# Question 7(c):

| Answer/Working | Mark | Guidance |
|---|---|---|
| $(\text{angle } APQ + \text{angle } AQP) = (180°-\alpha-\beta)+\{180°-(90°-\beta)-\gamma\} = 270°-\alpha-\gamma$. Otherwise: angle $PAQ = \alpha+\gamma-90°$ | M1 | 1.1b – Clear attempt to find angle sum (condone slips) or another relevant starting point e.g. expression for angle $PAQ$ |
| To return to $A$: angle $APQ$ + angle $AQP < 180°$ since $APQ$ is a triangle. Otherwise: angle $PAQ > 0$ | M1 | 3.1b – Clear statement to form inequality e.g. correct angle sum $< 180°$ is acceptable, or angle $PAQ > 0$ |
| $270°-\alpha-\gamma < 180° \Rightarrow \alpha > 90°-\gamma$ | A1 | 1.1b – Correct simplified inequality in correct form |
| $\tan\alpha > \tan(90°-\gamma)$ – correct method using addition formulae | M1 | 1.1b – Correct method to form inequality in tan or cot |
| $\dfrac{e_2\cot\gamma}{e_1} > \cot\gamma$ | M1 | 1.1b – Using part (b) to eliminate the angles |
| $e_2 > e_1$ * | A1* | 2.2a – Given answer correctly obtained |
| **Total** | **(6)** | |

# Question 7(d):

| Answer/Working | Mark | Guidance |
|---|---|---|
| From (b), $\alpha = 90°-\gamma$, so it moves parallel to $AP$, e.g. parallel to the initial velocity | B1 | 2.4 |
| **Total** | **(1)** | |

## Question 7:

**Part (c) alt — Use of trig identity**

| Answer/Working | Mark | Guidance |
|---|---|---|
| (angle $APQ$ + angle $AQP$) $= (180° - \alpha - \beta) + \{180° - (90° - \beta) - \gamma\} = 270 - \alpha - \gamma$ | M1 | |
| To return to $A$, (angle $APQ$ + angle $AQP$) $< 180°$, since $APQ$ is a triangle | M1 | |
| $\tan(\alpha + \gamma) = \dfrac{\tan\alpha + \tan\gamma}{1 - \tan\alpha\tan\gamma}$ and $\tan\alpha = \dfrac{e_2\cot\gamma}{e_1}$ or $\tan\alpha = \dfrac{e_2}{e_1\tan\gamma}$, leads to $\tan(\alpha+\gamma) = \dfrac{e_2 + e_1\tan^2\gamma}{e_1\tan\gamma - e_2\tan\gamma}$ oe | A1 | |
| $180 > (\alpha+\gamma) > 90 \Rightarrow \tan(\alpha+\gamma) < 0 \Rightarrow \dfrac{e_2 + e_1\tan^2\gamma}{e_1\tan\gamma - e_2\tan\gamma} < 0$ | M1 | Condone if '$180 >$' is not stated again |
| Since numerator $> 0$, therefore $e_1\tan\gamma - e_2\tan\gamma < 0$ | M1 | |
| $e_2 > e_1$ * | A1 | |

**Part (d)**

| Answer/Working | Mark | Guidance |
|---|---|---|
| $\alpha = 90° - \gamma$, so it moves parallel to $AP$; or $\alpha = 90° - \gamma$, so it moves parallel to the initial velocity | B1 | Use given information from (b) to make any equivalent statement with a correct reason and no incorrect statements. Do not accept 'it moves parallel to the initial speed' |
7.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{0da9cd5b-6f6f-4607-bd4f-c8ae164466ae-24_721_1367_280_349}
\captionsetup{labelformat=empty}
\caption{Figure 2}
\end{center}
\end{figure}

A small smooth snooker ball is projected from the corner $A$ of a horizontal rectangular snooker table $A B C D$.

The ball is projected so it first hits the side $D C$ at the point $P$, then hits the side $C B$ at the point $Q$ and then returns to $A$.

Angle $A P D = \alpha$, Angle $Q P C = \beta$, Angle $A Q B = \gamma$\\
The ball moves along $A P$ with speed $U$, along $P Q$ with speed $V$ and along $Q A$ with speed $W$, as shown in Figure 2.

The coefficient of restitution between the ball and side $D C$ is $e _ { 1 }$\\
The coefficient of restitution between the ball and side $C B$ is $e _ { 2 }$\\
The ball is modelled as a particle.

\section*{Use the model to answer all parts of this question.}
\begin{enumerate}[label=(\alph*)]
\item Show that $\tan \beta = e _ { 1 } \tan \alpha$
\item Hence show that $e _ { 1 } \tan \alpha = e _ { 2 } \cot \gamma$
\item By considering (angle $A P Q$ + angle $A Q P$ ) or otherwise, show that it would be possible for the ball to return to $A$ only if $e _ { 2 } > e _ { 1 }$

If instead $e _ { 1 } = e _ { 2 }$, the ball would not return to $A$.\\
Given that $e _ { 1 } = e _ { 2 }$
\item use the result from part (b) to describe the path of the ball after it hits $C B$ at $Q$, explaining your answer.
\end{enumerate}

\hfill \mbox{\textit{Edexcel FM1 2023 Q7 [14]}}