| Exam Board | Edexcel |
|---|---|
| Module | Paper 3 (Paper 3) |
| Year | 2024 |
| Session | June |
| Marks | 12 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Projectiles |
| Type | Deriving trajectory equation |
| Difficulty | Moderate -0.3 This is a standard A-level mechanics projectile question requiring derivation of the trajectory equation from parametric equations, then using it to find range and maximum height. Part (a) involves routine application of kinematic equations and elimination of parameter t. Parts (b)-(c) are straightforward calculus/algebra. Parts (d)-(e) test conceptual understanding. All techniques are standard textbook material with no novel problem-solving required, making it slightly easier than average. |
| Spec | 3.02i Projectile motion: constant acceleration model |
| Answer | Marks | Guidance |
|---|---|---|
| \[x = 35\cos\theta \cdot t\] | M1 | 3.3 |
| A1 | 1.1b |
| Answer | Marks | Guidance |
|---|---|---|
| \[y = 35\sin\theta \cdot t - \frac{1}{2}gt^2\] | M1 | 3.4 |
| A1 | 1.1b |
| Answer | Marks | Guidance |
|---|---|---|
| \[y = 35\sin\theta \cdot \frac{x}{35\cos\theta} - \frac{1}{2}g\left(\frac{x}{35\cos\theta}\right)^2\] | DM1 | 3.1b |
| \[y = \frac{3}{4}x - \frac{1}{160}x^2\] | A1* | 1.1b |
| Answer | Marks |
|---|---|
| \(x = 0, y = 0 \Rightarrow c = 0\) | M1A1 |
| \(x = 0, \frac{dy}{dx} = 2ax + b = \frac{3}{4} \Rightarrow b = \frac{3}{4}\) | M1A1 |
| \(x = 120, y = 0 \Rightarrow 0 = 120^2a + 120 \cdot \frac{3}{4} \Rightarrow a = -\frac{1}{160}\) | DM1 |
| \[y = \frac{3}{4}x - \frac{1}{160}x^2\] | A1* |
| Answer | Marks | Guidance |
|---|---|---|
| AND \(OA = 35\cos\theta \cdot t = \frac{35\cos\theta \cdot 70\sin\theta}{g}\) | M1 | 3.1b |
| Answer | Marks | Guidance |
|---|---|---|
| \(OA = 120\) (m) | A1 | 1.1b |
| Answer | Marks | Guidance |
|---|---|---|
| N.B. OR use the calculator to input the equation of the path which then gives \(y_{\max} = \frac{45}{2}\) (when \(x = 60\)) with no working. | M1 | 3.1b |
| \(H = 22.5\) Accept 23 | A1 | 1.1b |
| Answer | Marks | Guidance |
|---|---|---|
| \(H\) is greater (or \(K\) is smaller), as air resistance would slow the particle down or equivalent. | B1 | 3.5a |
| Answer | Marks | Guidance |
|---|---|---|
| e.g. the inaccuracy of using \(9.8 \text{ m s}^{-2}\) for \(g\) | B1 | 3.5b |
| Answer | Marks |
|---|---|
| M1 | Correct terms but condone \(\sin/\cos\) confusion and sign errors. Available if they use \(s\) instead of \(x\) |
| A1 | Correct equation in \(x\) and \(t\). N.B. they may have the wrong value for \(\cos\theta\) |
| M1 | Correct terms but condone \(\sin/\cos\) confusion and sign errors. Available if they use a different letter for \(y\) provided it's not the same as they've used for \(x\). N.B. M0 if they subsequently use a value for \(y\) e.g. 0 |
| A1 | Correct equation in \(y\) and \(t\). N.B. they may have the wrong value for \(\sin\theta\). They may have \(t\) in terms of \(x\), from their first equation. |
| DM1 | Dependent on the two previous M marks for eliminating \(t\) to give an equation in \(y\) and \(x\) only. |
| A1* | Given answer correctly obtained, with at least one further line of working with trig ratios and \(g = 9.8\) explicitly seen or \(4.9\) or equivalent used for \(0.5g\). Allow \(y = \frac{3x}{4} - \frac{x^2}{160}\) and with \(y\) on the RHS |
| Answer | Marks |
|---|---|
| M1 | ALT 1: Use of \(y = 0\) in equation of path and solve for \(x\). ALT 2: Use calculus to find the \(x\)-coordinate of the max point and double it. ALT 3: Any other complete suvat method to |
# Question 5
## 5(a)
Using horizontal motion, $s = ut$, with 35 resolved
$$x = 35\cos\theta \cdot t$$ | M1 | 3.3
| A1 | 1.1b
Using vertical motion, $s = ut + \frac{1}{2}at^2$, with 35 resolved
$$y = 35\sin\theta \cdot t - \frac{1}{2}gt^2$$ | M1 | 3.4
| A1 | 1.1b
Eliminate $t$:
$$y = 35\sin\theta \cdot \frac{x}{35\cos\theta} - \frac{1}{2}g\left(\frac{x}{35\cos\theta}\right)^2$$ | DM1 | 3.1b
$$y = \frac{3}{4}x - \frac{1}{160}x^2$$ | A1* | 1.1b
**N.B.** No marks available if they just quote the equation of the path.
**ALTERNATIVE:** they do (b) and/or (c) first using a suvat method
Assume $y = ax^2 + bx + c$
Use any three of $(0,0)$, $(120,0)$ from part (b), $(60,22.5)$ from part (c)
or $\frac{dy}{dx} = \frac{3}{4}$ at $x = 0$ to find $a$, $b$, and $c$.
$\text{M1A1, M1A1, DM1A1}^*$ for finding each of $a$, $b$ and $c$ and stating final answer in correct form.
**N.B.** If they realise that $c = 0$, and just use $y = ax^2 + bx$, that could score M1A1.
Enter marks on ePEN in the order in which $a$, $b$ and $c$ are found:
$x = 0, y = 0 \Rightarrow c = 0$ | M1A1
$x = 0, \frac{dy}{dx} = 2ax + b = \frac{3}{4} \Rightarrow b = \frac{3}{4}$ | M1A1
$x = 120, y = 0 \Rightarrow 0 = 120^2a + 120 \cdot \frac{3}{4} \Rightarrow a = -\frac{1}{160}$ | DM1
$$y = \frac{3}{4}x - \frac{1}{160}x^2$$ | A1*
**(6 marks)**
## 5(b)
**ALT 1**
$$0 = \frac{3}{4}x - \frac{1}{160}x^2$$ and solve for $x$
**ALT 2**
$$\frac{dy}{dx} = \frac{3}{4} - \frac{x}{80} = 0 \Rightarrow x = 60$$ and $OA = 2 \times 60$
**ALT 3**
A complete suvat method to find $OA$:
e.g. $0 = 35\sin\theta \cdot t - \frac{1}{2}gt^2$
or $0 = 35\sin\theta - \frac{1}{2}gt$
or $35\sin\theta = 35\sin\theta - gt$
to find $t = \frac{70\sin\theta}{g}$
AND $OA = 35\cos\theta \cdot t = \frac{35\cos\theta \cdot 70\sin\theta}{g}$ | M1 | 3.1b
**N.B.** OR use the calculator to input the equation of the path which then gives $y_{\max} = \frac{45}{2}$ when $x = 60$ with no working, so $OA = 2 \times 60$
$OA = 120$ (m) | A1 | 1.1b
**(2 marks)**
## 5(c)
**ALT 1**
$$H = \frac{3}{4} \cdot 60 - \frac{1}{160} \cdot 60^2$$
**ALT 2**
$$y = \frac{1}{160}(x^2 - 120x) = 22.5 - \frac{1}{160}(x - 60)^2$$ so $\max y = \frac{45}{2}$ or $22.5$
**ALT 3**
$$\frac{dy}{dx} = \frac{3}{4} - \frac{2x}{160} = 0 \Rightarrow x = 60$$ then find $y$ when $x = 60$
**ALT 4**
A complete suvat method:
e.g. $H = \frac{(35\sin\theta)^2}{2g}$
or $0 = 35\sin\theta - gt$ to find the time to top, $t = \frac{35\sin\theta}{g}$, or use half their time they found in (b)
AND $H = 35\sin\theta \cdot t - \frac{1}{2}g\left(\frac{35\sin\theta}{g}\right)^2$ or $\frac{35\sin\theta + 0}{2} \cdot \frac{35\sin\theta}{g}$
**N.B.** OR use the calculator to input the equation of the path which then gives $y_{\max} = \frac{45}{2}$ (when $x = 60$) with no working. | M1 | 3.1b
$H = 22.5$ Accept 23 | A1 | 1.1b
**(2 marks)**
## 5(d)
$H$ is greater (or $K$ is smaller), as air resistance would slow the particle down or equivalent. | B1 | 3.5a
**(1 mark)**
## 5(e)
e.g. the inaccuracy of using $9.8 \text{ m s}^{-2}$ for $g$ | B1 | 3.5b
**(1 mark)**
**(12 marks total)**
---
## Notes
**5a**
| M1 | Correct terms but condone $\sin/\cos$ confusion and sign errors. Available if they use $s$ instead of $x$
| A1 | Correct equation in $x$ and $t$. N.B. they may have the wrong value for $\cos\theta$
| M1 | Correct terms but condone $\sin/\cos$ confusion and sign errors. Available if they use a different letter for $y$ provided it's not the same as they've used for $x$. N.B. M0 if they subsequently use a value for $y$ e.g. 0
| A1 | Correct equation in $y$ and $t$. N.B. they may have the wrong value for $\sin\theta$. They may have $t$ in terms of $x$, from their first equation.
| DM1 | Dependent on the two previous M marks for eliminating $t$ to give an equation in $y$ and $x$ only.
| A1* | Given answer correctly obtained, with at least one further line of working with trig ratios and $g = 9.8$ explicitly seen or $4.9$ or equivalent used for $0.5g$. Allow $y = \frac{3x}{4} - \frac{x^2}{160}$ and with $y$ on the RHS
**5b**
| M1 | ALT 1: Use of $y = 0$ in equation of path and solve for $x$. ALT 2: Use calculus to find the $x$-coordinate of the max point and double it. ALT 3: Any other complete suvat method to
5.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{184043b7-1222-44fb-bc9f-3f484f72147b-12_270_1109_244_470}
\captionsetup{labelformat=empty}
\caption{Figure 4}
\end{center}
\end{figure}
At time $t = 0$, a small stone is projected with velocity $35 \mathrm {~ms} ^ { - 1 }$ from a point $O$ on horizontal ground.
The stone is projected at an angle $\alpha$ to the horizontal, where $\tan \alpha = \frac { 3 } { 4 }$\\
In an initial model
\begin{itemize}
\item the stone is modelled as a particle $P$ moving freely under gravity
\item the stone hits the ground at the point $A$
\end{itemize}
Figure 4 shows the path of $P$ from $O$ to $A$.\\
For the motion of $P$ from $O$ to $A$
\begin{itemize}
\item at time $t$ seconds, the horizontal distance of $P$ from $O$ is $x$ metres
\item at time $t$ seconds, the vertical distance of $P$ above the ground is $y$ metres
\begin{enumerate}[label=(\alph*)]
\item Using the model, show that
\end{itemize}
$$y = \frac { 3 } { 4 } x - \frac { 1 } { 160 } x ^ { 2 }$$
\item Use the answer to (a), or otherwise, to find the length $O A$.
Using the model, the greatest height of the stone above the ground is found to be $H$ metres.
\item Use the answer to (a), or otherwise, to find the value of $H$.
\begin{itemize}
\item The model is refined to include air resistance.
\end{itemize}
Using this new model, the greatest height of the stone above the ground is found to be $K$ metres.
\item State which is greater, $H$ or $K$, justifying your answer.
\item State one limitation of this refined model.
\begin{center}
\end{center}
\end{enumerate}
\hfill \mbox{\textit{Edexcel Paper 3 2024 Q5 [12]}}