CAIE M1 2024 November — Question 5 9 marks

Exam BoardCAIE
ModuleM1 (Mechanics 1)
Year2024
SessionNovember
Marks9
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicSUVAT in 2D & Gravity
TypeTwo particles: same start time, different heights
DifficultyStandard +0.8 This is a multi-stage 2D kinematics problem requiring: (1) finding collision time and position using simultaneous SUVAT equations for two particles, (2) applying conservation of momentum to find P's post-collision velocity, and (3) using SUVAT again from collision point to ground. The collision condition (same position at same time) requires careful algebraic manipulation, and the momentum calculation with different masses adds complexity beyond standard single-particle projectile questions.
Spec3.02h Motion under gravity: vector form6.03b Conservation of momentum: 1D two particles6.03f Impulse-momentum: relation

5 Two particles, \(P\) and \(Q\), of masses \(2 m \mathrm {~kg}\) and \(m \mathrm {~kg}\) respectively, are held at rest in the same vertical line. The heights of \(P\) and \(Q\) above horizontal ground are 1 m and 2 m respectively. \(P\) is projected vertically upwards with speed \(2 \mathrm {~ms} ^ { - 1 }\). At the same instant, \(Q\) is released from rest.
  1. Find the speed of each particle immediately before they collide.
  2. It is given that immediately after the collision the downward speed of \(Q\) is \(3.5 \mathrm {~ms} ^ { - 1 }\). Find the speed of \(P\) at the instant that it reaches the ground.

Question 5(a):
AnswerMarks Guidance
AnswerMark Guidance
\([s_P \text{ up}=] \pm\left(2t - \frac{1}{2}gt^2\right)\) OR \([s_Q \text{ down}=] \pm\frac{1}{2}gt^2\)M1 For use of \(s = ut + \frac{1}{2}at^2\) at least once with \(a = \pm g\) and \(u = 0\) or \(u = \pm 2\). Seen anywhere
\(2t - \frac{1}{2}gt^2 + \frac{1}{2}gt^2 = 2 - 1 \Rightarrow t = \frac{1}{2}\)M1 Use \(s_P + s_Q = \pm(2-1)\) OR \(\pm 1\) ONLY with \(s_P\) and \(s_Q\) of the correct form
\(v_P = 2 - \frac{1}{2}g = -3\ \text{ms}^{-1}\) so speed \(= 3\ \text{ms}^{-1}\)A1 Must be positive
\(v_Q = -\frac{1}{2}g = -5\ \text{ms}^{-1}\) so speed \(= 5\ \text{ms}^{-1}\)A1 Must be positive. If A0A0, allow SCB1 if both are negative
Question 5(b):
AnswerMarks Guidance
AnswerMark Guidance
\(2m \times (3[v_P]) + m \times (5[v_Q]) = 2mv + m \times 3.5\)*M1 Use of conservation of momentum; 4 non-zero terms; using their \(\pm 3\ \text{ms}^{-1}\) and their \(\pm 5\ \text{ms}^{-1}\); allow sign errors and \(m\) missing ONLY. Do not allow with \(v_p = \pm 2\) or \(v_Q = 0\). Do not allow made up values for 3 and 5. Allow LHS to have only one term but only if getting \(v_P = 0\) in (a) from \(s_P = s_Q\)
\(v = 3.75\)A1 Allow \(v = -3.75\) from correct work
At \(t = \frac{1}{2}\): \(s_p = \pm\left(2 \times \frac{1}{2} - \frac{1}{2}g\left(\frac{1}{2}\right)^2\right) = \mp\frac{1}{4}\) OR \(s_p = \pm\left(-3 \times \frac{1}{2} + \frac{1}{2}g\left(\frac{1}{2}\right)^2\right) = \mp\frac{1}{4}\) OR \(s_p = \pm\left(\frac{(-3)^2 - 2^2}{2g}\right) = \pm\frac{1}{4}\) OR At \(t=\frac{1}{2}\): \(s_Q = \pm\frac{1}{2}g\left(\frac{1}{2}\right)^2 = \pm\frac{5}{4}\) OR \(s_Q = \pm\left(5 \times \frac{1}{2} - \frac{1}{2}g\left(\frac{1}{2}\right)^2\right) = \pm\frac{5}{4}\) OR \(s_Q = \pm\left(\frac{5^2 - 0^2}{2g}\right) = \pm\frac{5}{4}\); so height above ground \(= \frac{3}{4}\)*B1 This may be seen in part (a), but do not award the mark until stated/used in part (b)
Question 5(b):
AnswerMarks Guidance
AnswerMark Guidance
\(v^2 = (their\ 3.75)^2 + 2 \times (\pm g) \times \left(\pm \frac{3}{4}\right)\)DM1 Use of \(v^2 = u^2 + 2as\) using their \(v\) and \(a = \pm g\); their \(s\) is either \(\pm\left[1+\left(-\frac{1}{4}\right)\right]\) or \(\pm\left[2-\frac{5}{4}\right]\) OE. Dependent on previous M and B marks.
OR \(0^2 = (their\ 3.75)^2 - 2\times(\pm g)\times s \Rightarrow s = \frac{45}{64}\) AND \(v^2 = \left[0^2+\right]2\times(\pm g)\times\left[\left(\frac{3}{4}\right)+\frac{45}{64}\right]\)
\(v = 5.39\ \text{ms}^{-1}\)A1 Or \(\frac{\sqrt{465}}{4}\); AWRT 5.39; 5.390964...
## Question 5(a):

| Answer | Mark | Guidance |
|--------|------|----------|
| $[s_P \text{ up}=] \pm\left(2t - \frac{1}{2}gt^2\right)$ OR $[s_Q \text{ down}=] \pm\frac{1}{2}gt^2$ | M1 | For use of $s = ut + \frac{1}{2}at^2$ at least once with $a = \pm g$ and $u = 0$ or $u = \pm 2$. Seen anywhere |
| $2t - \frac{1}{2}gt^2 + \frac{1}{2}gt^2 = 2 - 1 \Rightarrow t = \frac{1}{2}$ | M1 | Use $s_P + s_Q = \pm(2-1)$ OR $\pm 1$ ONLY with $s_P$ and $s_Q$ of the correct form |
| $v_P = 2 - \frac{1}{2}g = -3\ \text{ms}^{-1}$ so speed $= 3\ \text{ms}^{-1}$ | A1 | Must be positive |
| $v_Q = -\frac{1}{2}g = -5\ \text{ms}^{-1}$ so speed $= 5\ \text{ms}^{-1}$ | A1 | Must be positive. If A0A0, allow SCB1 if both are negative |

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## Question 5(b):

| Answer | Mark | Guidance |
|--------|------|----------|
| $2m \times (3[v_P]) + m \times (5[v_Q]) = 2mv + m \times 3.5$ | *M1 | Use of conservation of momentum; 4 non-zero terms; using their $\pm 3\ \text{ms}^{-1}$ and their $\pm 5\ \text{ms}^{-1}$; allow sign errors and $m$ missing ONLY. Do not allow with $v_p = \pm 2$ or $v_Q = 0$. Do not allow made up values for 3 and 5. Allow LHS to have only one term but only if getting $v_P = 0$ in (a) from $s_P = s_Q$ |
| $v = 3.75$ | A1 | Allow $v = -3.75$ from correct work |
| At $t = \frac{1}{2}$: $s_p = \pm\left(2 \times \frac{1}{2} - \frac{1}{2}g\left(\frac{1}{2}\right)^2\right) = \mp\frac{1}{4}$ OR $s_p = \pm\left(-3 \times \frac{1}{2} + \frac{1}{2}g\left(\frac{1}{2}\right)^2\right) = \mp\frac{1}{4}$ OR $s_p = \pm\left(\frac{(-3)^2 - 2^2}{2g}\right) = \pm\frac{1}{4}$ OR At $t=\frac{1}{2}$: $s_Q = \pm\frac{1}{2}g\left(\frac{1}{2}\right)^2 = \pm\frac{5}{4}$ OR $s_Q = \pm\left(5 \times \frac{1}{2} - \frac{1}{2}g\left(\frac{1}{2}\right)^2\right) = \pm\frac{5}{4}$ OR $s_Q = \pm\left(\frac{5^2 - 0^2}{2g}\right) = \pm\frac{5}{4}$; so height above ground $= \frac{3}{4}$ | *B1 | This may be seen in part (a), but do not award the mark until stated/used in part (b) |

## Question 5(b):

| Answer | Mark | Guidance |
|--------|------|----------|
| $v^2 = (their\ 3.75)^2 + 2 \times (\pm g) \times \left(\pm \frac{3}{4}\right)$ | **DM1** | Use of $v^2 = u^2 + 2as$ using their $v$ and $a = \pm g$; their $s$ is either $\pm\left[1+\left(-\frac{1}{4}\right)\right]$ or $\pm\left[2-\frac{5}{4}\right]$ OE. Dependent on previous M and B marks. |
| OR $0^2 = (their\ 3.75)^2 - 2\times(\pm g)\times s \Rightarrow s = \frac{45}{64}$ AND $v^2 = \left[0^2+\right]2\times(\pm g)\times\left[\left(\frac{3}{4}\right)+\frac{45}{64}\right]$ | | |
| $v = 5.39\ \text{ms}^{-1}$ | **A1** | Or $\frac{\sqrt{465}}{4}$; AWRT 5.39; 5.390964... |

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5 Two particles, $P$ and $Q$, of masses $2 m \mathrm {~kg}$ and $m \mathrm {~kg}$ respectively, are held at rest in the same vertical line. The heights of $P$ and $Q$ above horizontal ground are 1 m and 2 m respectively. $P$ is projected vertically upwards with speed $2 \mathrm {~ms} ^ { - 1 }$. At the same instant, $Q$ is released from rest.
\begin{enumerate}[label=(\alph*)]
\item Find the speed of each particle immediately before they collide.
\item It is given that immediately after the collision the downward speed of $Q$ is $3.5 \mathrm {~ms} ^ { - 1 }$.

Find the speed of $P$ at the instant that it reaches the ground.
\end{enumerate}

\hfill \mbox{\textit{CAIE M1 2024 Q5 [9]}}