CAIE Further Paper 3 2021 November — Question 7 11 marks

Exam BoardCAIE
ModuleFurther Paper 3 (Further Paper 3)
Year2021
SessionNovember
Marks11
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicImpulse and momentum (advanced)
TypeTwo wall collisions sequence
DifficultyChallenging +1.8 This is a challenging Further Maths mechanics problem requiring systematic application of coefficient of restitution in 2D, resolving velocities parallel and perpendicular to walls, and connecting energy loss to restitution. Part (a) is standard technique, part (b) requires geometric insight about the symmetry of rebounds, and part (c) involves simultaneous equations linking energy, angles, and restitution. The multi-step reasoning and need to synthesize several concepts places it well above average difficulty.
Spec6.03k Newton's experimental law: direct impact6.03l Newton's law: oblique impacts

\includegraphics{figure_7} The smooth vertical walls \(AB\) and \(CB\) are at right angles to each other. A particle \(P\) is moving with speed \(u\) on a smooth horizontal floor and strikes the wall \(CB\) at an angle \(\alpha\). It rebounds at an angle \(\beta\) to the wall \(CB\). The particle then strikes the wall \(AB\) and rebounds at an angle \(\gamma\) to that wall (see diagram). The coefficient of restitution between each wall and \(P\) is \(e\).
  1. Show that \(\tan \beta = e \tan \alpha\). [3]
  2. Express \(\gamma\) in terms of \(\alpha\) and explain what this result means about the final direction of motion of \(P\). [4]
As a result of the two impacts the particle loses \(\frac{8}{9}\) of its initial kinetic energy.
  1. Given that \(\alpha + \beta = 90°\), find the value of \(e\) and the value of \(\tan \alpha\). [4]

Question 7:

AnswerMarks Guidance
7(a)ucosα=vcosβ M1
eusinα=vsinβM1
Divide: tanβ=etanαA1 AG. Must see divide OE.
3

AnswerMarks Guidance
7(b)vsinβ=wcosγ (=eusinα) M1
evcosβ=wsinγ (=eucosα)M1
Divide: tanγ=1/tanα: γ=90°−α*A1
After second rebound, direction of motion is parallel to initial path.DB1
4

AnswerMarks
7(c)( )
Final KE = 1 m ( eusinα)2 +( eucosα)2  = 1 me2u2 
 
AnswerMarks Guidance
2  2 M1 Energy expression in terms of u.
1 1 1 1
So me2u2 = × mu2 giving e=
AnswerMarks
2 9 2 3A1
( 90−α)=etanα
AnswerMarks
Part (a) gives tanM1
So tanα= 3A1
4
Question 7:
--- 7(a) ---
7(a) | ucosα=vcosβ | M1
eusinα=vsinβ | M1
Divide: tanβ=etanα | A1 | AG. Must see divide OE.
3
--- 7(b) ---
7(b) | vsinβ=wcosγ (=eusinα) | M1
evcosβ=wsinγ (=eucosα) | M1
Divide: tanγ=1/tanα: γ=90°−α | *A1
After second rebound, direction of motion is parallel to initial path. | DB1
4
--- 7(c) ---
7(c) | ( )
Final KE = 1 m ( eusinα)2 +( eucosα)2  = 1 me2u2 
 
2  2  | M1 | Energy expression in terms of u.
1 1 1 1
So me2u2 = × mu2 giving e=
2 9 2 3 | A1
( 90−α)=etanα
Part (a) gives tan | M1
So tanα= 3 | A1
4
\includegraphics{figure_7}

The smooth vertical walls $AB$ and $CB$ are at right angles to each other. A particle $P$ is moving with speed $u$ on a smooth horizontal floor and strikes the wall $CB$ at an angle $\alpha$. It rebounds at an angle $\beta$ to the wall $CB$. The particle then strikes the wall $AB$ and rebounds at an angle $\gamma$ to that wall (see diagram). The coefficient of restitution between each wall and $P$ is $e$.

\begin{enumerate}[label=(\alph*)]
\item Show that $\tan \beta = e \tan \alpha$. [3]
\item Express $\gamma$ in terms of $\alpha$ and explain what this result means about the final direction of motion of $P$. [4]
\end{enumerate}

As a result of the two impacts the particle loses $\frac{8}{9}$ of its initial kinetic energy.

\begin{enumerate}[label=(\alph*)]
\setcounter{enumi}{2}
\item Given that $\alpha + \beta = 90°$, find the value of $e$ and the value of $\tan \alpha$. [4]
\end{enumerate}

\hfill \mbox{\textit{CAIE Further Paper 3 2021 Q7 [11]}}