| Exam Board | Edexcel |
|---|---|
| Module | Paper 3 (Paper 3) |
| Year | 2022 |
| Session | June |
| Marks | 12 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Projectiles |
| Type | Basic trajectory calculations |
| Difficulty | Moderate -0.5 This is a standard A-level mechanics projectile question requiring routine application of range and maximum height formulas. Parts (a) and (b) involve straightforward substitution into standard equations (R = U²sin(2α)/g and H = U²sin²α/2g), while parts (c) and (d) test conceptual understanding of air resistance. The 'show that' format guides students to the answer, and the mathematics involves only basic algebraic manipulation with no novel problem-solving required. |
| Spec | 3.02i Projectile motion: constant acceleration model |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Using horizontal motion (whole motion): \(U\cos\alpha \times t = 120\) OR (half way): \(U\cos\alpha \times t = 60\) | M1, A1 | 3.3, 1.1b |
| Using vertical motion: \(U\sin\alpha \times t - \frac{1}{2}gt^2 = 0\) OR \(0 = U\sin\alpha - gt\) | M1, A1 | 3.4, 1.1b |
| Attempt to solve problem by eliminating \(t\) | DM1 | 3.1b |
| \(U^2 \sin\alpha\cos\alpha = 588\) | A1* | 2.2a |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Using vertical motion OR conservation of energy | M1 | 3.4 |
| \(0^2 = (U\sin\alpha)^2 - 2g\times10\) OR \(\frac{1}{2}mU^2 - \frac{1}{2}m(U\cos\alpha)^2 = mg\times10\) | A1 | 1.1b |
| Alternative 1: If \(t\) is time to top: use of \(10 = \frac{1}{2}gt^2\) oe (\(t = \frac{10}{7}\)) to obtain equation in \(U\) and \(\alpha\) only; \(U\sin\alpha = 14\) or \(U\cos\alpha = 42\) | M1, A1 | |
| Alternative 2: use of \(10 = U\sin\alpha\cdot t - \frac{1}{2}gt^2\) with \(t = \frac{60}{U\cos\alpha}\) substituted; \(10 = U\sin\alpha \times \frac{60}{U\cos\alpha} - \frac{1}{2}g\left(\frac{60}{U\cos\alpha}\right)^2\) | M1, A1 | |
| Attempt to solve by eliminating \(\alpha\): e.g. \(U\sin\alpha = 14 \Rightarrow U\cos\alpha = 42\), square and add; OR \(U^2\sin^2\alpha = 20g = 196\) and \(U^2\sin\alpha\cos\alpha = 588\), divide to give \(\tan\alpha = \frac{1}{3}\) then \(\sin^2\alpha = \frac{1}{10}\) | DM1 | 3.1b |
| \(U^2 = 1960\) | A1* | 2.2a |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| \(V\) less than calculated, since air resistance has to be overcome, or just 'because of air resistance' isw | B1 | 3.5a |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| e.g. wind effects, more accurate value of \(g\), spin of ball, size of ball, shape of ball, dimensions of ball, not a particle, variable acceleration, surface area of ball, humidity. Allow wind resistance and rotational resistance. (Ignore any mention of air resistance or drag) | B1 | 3.5c |
## Question 5:
**Part 5(a):**
| Answer/Working | Mark | Guidance |
|---|---|---|
| Using horizontal motion (whole motion): $U\cos\alpha \times t = 120$ OR (half way): $U\cos\alpha \times t = 60$ | M1, A1 | 3.3, 1.1b |
| Using vertical motion: $U\sin\alpha \times t - \frac{1}{2}gt^2 = 0$ OR $0 = U\sin\alpha - gt$ | M1, A1 | 3.4, 1.1b |
| Attempt to solve problem by eliminating $t$ | DM1 | 3.1b |
| $U^2 \sin\alpha\cos\alpha = 588$ | A1* | 2.2a |
**Notes 5a:**
- N.B. Could score 2/6 for any one of the 4 given equations if there is no corresponding second equation or the attempt is incorrect
- M1: Complete method to give equation in $U$, $\alpha$ and $t$ only, condone sin/cos confusion and sign errors, each term that needs to be resolved must be resolved
- A1: Correct equation
- DM1: Eliminate $t$, dependent on first and second M1s
- A1*: Given answer correctly obtained, with no wrong working seen. Allow $588 = U^2\sin\alpha\cos\alpha$ but nothing else
---
**Part 5(b):**
| Answer/Working | Mark | Guidance |
|---|---|---|
| Using vertical motion OR conservation of energy | M1 | 3.4 |
| $0^2 = (U\sin\alpha)^2 - 2g\times10$ OR $\frac{1}{2}mU^2 - \frac{1}{2}m(U\cos\alpha)^2 = mg\times10$ | A1 | 1.1b |
| **Alternative 1:** If $t$ is time to top: use of $10 = \frac{1}{2}gt^2$ oe ($t = \frac{10}{7}$) to obtain equation in $U$ and $\alpha$ only; $U\sin\alpha = 14$ or $U\cos\alpha = 42$ | M1, A1 | |
| **Alternative 2:** use of $10 = U\sin\alpha\cdot t - \frac{1}{2}gt^2$ with $t = \frac{60}{U\cos\alpha}$ substituted; $10 = U\sin\alpha \times \frac{60}{U\cos\alpha} - \frac{1}{2}g\left(\frac{60}{U\cos\alpha}\right)^2$ | M1, A1 | |
| Attempt to solve by eliminating $\alpha$: e.g. $U\sin\alpha = 14 \Rightarrow U\cos\alpha = 42$, square and add; OR $U^2\sin^2\alpha = 20g = 196$ and $U^2\sin\alpha\cos\alpha = 588$, divide to give $\tan\alpha = \frac{1}{3}$ then $\sin^2\alpha = \frac{1}{10}$ | DM1 | 3.1b |
| $U^2 = 1960$ | A1* | 2.2a |
**Notes 5b:**
- N.B. Just stating $\sin^2\alpha = \frac{1}{10}$ with no working is DM0A0
- N.B. Verification (starting with $U^2 = 1960$ and working backwards) is not acceptable
---
**Part 5(c):**
| Answer/Working | Mark | Guidance |
|---|---|---|
| $V$ less than calculated, since air resistance has to be overcome, or just 'because of air resistance' isw | B1 | 3.5a |
**Notes 5c:**
- B1: Clear statement isw
---
**Part 5(d):**
| Answer/Working | Mark | Guidance |
|---|---|---|
| e.g. wind effects, more accurate value of $g$, spin of ball, size of ball, shape of ball, dimensions of ball, not a particle, variable acceleration, surface area of ball, humidity. Allow wind resistance and rotational resistance. (Ignore any mention of air resistance or drag) | B1 | 3.5c |
**Notes 5d:**
- B1: B0 if there is an incorrect extra e.g. mass or weight
5.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{414946db-64d7-44b8-801d-2c7805ee9cc6-16_303_1266_237_404}
\captionsetup{labelformat=empty}
\caption{Figure 3}
\end{center}
\end{figure}
A golf ball is at rest at the point $A$ on horizontal ground.\\
The ball is hit and initially moves at an angle $\alpha$ to the ground.\\
The ball first hits the ground at the point $B$, where $A B = 120 \mathrm {~m}$, as shown in Figure 3.\\
The motion of the ball is modelled as that of a particle, moving freely under gravity, whose initial speed is $U \mathrm {~m} \mathrm {~s} ^ { - 1 }$
Using this model,
\begin{enumerate}[label=(\alph*)]
\item show that $U ^ { 2 } \sin \alpha \cos \alpha = 588$
The ball reaches a maximum height of 10 m above the ground.
\item Show that $U ^ { 2 } = 1960$
In a refinement to the model, the effect of air resistance is included.\\
The motion of the ball, from $A$ to $B$, is now modelled as that of a particle whose initial speed is $V \mathrm {~m} \mathrm {~s} ^ { - 1 }$
This refined model is used to calculate a value for $V$
\item State which is greater, $U$ or $V$, giving a reason for your answer.
\item State one further refinement to the model that would make the model more realistic.
\end{enumerate}
\hfill \mbox{\textit{Edexcel Paper 3 2022 Q5 [12]}}