Edexcel Paper 3 2018 June — Question 10 15 marks

Exam BoardEdexcel
ModulePaper 3 (Paper 3)
Year2018
SessionJune
Marks15
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicProjectiles
TypeProjectile passing through given point
DifficultyStandard +0.3 This is a standard projectile motion problem requiring systematic application of SUVAT equations and trajectory formulas. Part (a) uses maximum height formula (routine derivation), part (b) involves substituting into trajectory equation to find angle, part (c) is a standard modelling statement, and part (d) applies time of flight formula. All techniques are textbook exercises with no novel problem-solving required, making it slightly easier than average.
Spec3.02h Motion under gravity: vector form3.02i Projectile motion: constant acceleration model

10. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{65e4b254-fb7b-45c2-9702-32f034018193-32_435_1257_244_402} \captionsetup{labelformat=empty} \caption{Figure 4}
\end{figure} A boy throws a ball at a target. At the instant when the ball leaves the boy's hand at the point \(A\), the ball is 2 m above horizontal ground and is moving with speed \(U\) at an angle \(\alpha\) above the horizontal. In the subsequent motion, the highest point reached by the ball is 3 m above the ground. The target is modelled as being the point \(T\), as shown in Figure 4.
The ball is modelled as a particle moving freely under gravity.
Using the model,
  1. show that \(U ^ { 2 } = \frac { 2 g } { \sin ^ { 2 } \alpha }\). The point \(T\) is at a horizontal distance of 20 m from \(A\) and is at a height of 0.75 m above the ground. The ball reaches \(T\) without hitting the ground.
  2. Find the size of the angle \(\alpha\)
  3. State one limitation of the model that could affect your answer to part (b).
  4. Find the time taken for the ball to travel from \(A\) to \(T\).

Question 10:
Part (a):
AnswerMarks Guidance
\(0^2 = (U\sin\alpha)^2 - 2g \times (3-2)\)M1 3.3
\(U^2 = \frac{2g}{\sin^2\alpha}\)A1* 2.2a
Part (b):
AnswerMarks Guidance
\(20 = Ut\cos\alpha\)M1, A1 3.4, 1.1b
\(-\frac{5}{4} = Ut\sin\alpha - \frac{1}{2}gt^2\)M1, A1 3.4, 1.1b
\(-\frac{5}{4} = U\sin\alpha\left(\frac{20}{U\cos\alpha}\right) - \frac{1}{2}g\left(\frac{20}{U\cos\alpha}\right)^2\)M1(I) 3.1b
Sub for \(U^2\) using part (a)M1(II) 3.1b
\(-\frac{5}{4} = 20\tan\alpha - 100\tan^2\alpha\)A1(I) 1.1b
\((4\tan\alpha - 1)(100\tan\alpha + 5) = 0\)M1(III) 1.1b
\(\tan\alpha = \frac{1}{4} \Rightarrow \alpha = 14°\) or betterA1(II) 2.2a
Alternative method for (b):
AnswerMarks
Sub \(U\sin\alpha\) to give equation in \(t\) only: \(-\frac{5}{4} = \sqrt{2g}\,t - \frac{1}{2}gt^2\)M1(II), A1(I)
Solve for \(t\): \(t = \frac{5}{\sqrt{2g}}\) or \(1.1\) or \(1.13\)M1(III), M1(I)
Use \(20 = Ut\cos\alpha \Rightarrow \alpha = 14°\) or betterA1(II)
Part (c):
AnswerMarks Guidance
The target will have dimensions so there would be a range of possible values of \(\alpha\); or there will be air resistance; or the ball will have dimensions; or wind effects; or spin of the ballB1 3.5b
Part (d):
AnswerMarks Guidance
Find \(U\) using their \(\alpha\), e.g. \(U = \sqrt{\frac{2g}{\sin^2\alpha}}\)M1 3.1b
Use \(20 = Ut\cos\alpha\) (or vertical motion equation)A1 M1 1.1b
\(t = \frac{5}{\sqrt{2g}}\) or \(1.1\) or \(1.13\)B1 A1 1.1b
Alternative for (d):
AnswerMarks Guidance
\(A\) to top: \(s = vt - \frac{1}{2}at^2\) giving \(t_1 = \sqrt{\frac{2}{g}}\); top to \(T\): \(s = ut + \frac{1}{2}at^2\) giving \(t_2 = \frac{3}{\sqrt{2g}}\)M1, A1 M1 3.1b, 1.1b
Total time \(= \sqrt{\frac{2}{g}} + \frac{3}{\sqrt{2g}} = \frac{5}{\sqrt{2g}} = 1.1\) or \(1.13\) sB1 A1 1.1b
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# Question 10:

## Part (a):
| $0^2 = (U\sin\alpha)^2 - 2g \times (3-2)$ | M1 | 3.3 | Any complete method for equation in $U$, $g$, $\alpha$ only |
|---|---|---|---|
| $U^2 = \frac{2g}{\sin^2\alpha}$ | A1* | 2.2a | Given answer |

## Part (b):
| $20 = Ut\cos\alpha$ | M1, A1 | 3.4, 1.1b | Using horizontal motion $s = ut$ |
| $-\frac{5}{4} = Ut\sin\alpha - \frac{1}{2}gt^2$ | M1, A1 | 3.4, 1.1b | Using vertical motion $s = ut + \frac{1}{2}at^2$; M0 if $s = \pm2$ or $\pm3$ used, allow $s = \pm1.25$, $\pm0.75$, $\pm2.25$, $\pm2.75$ |
| $-\frac{5}{4} = U\sin\alpha\left(\frac{20}{U\cos\alpha}\right) - \frac{1}{2}g\left(\frac{20}{U\cos\alpha}\right)^2$ | M1(I) | 3.1b | Sub for $t$ using $20 = Ut\cos\alpha$ |
| Sub for $U^2$ using part (a) | M1(II) | 3.1b | |
| $-\frac{5}{4} = 20\tan\alpha - 100\tan^2\alpha$ | A1(I) | 1.1b | Correct quadratic in $\tan\alpha$ or $\cot\alpha$ |
| $(4\tan\alpha - 1)(100\tan\alpha + 5) = 0$ | M1(III) | 1.1b | Solve 3-term quadratic by factorisation, formula, or calculator |
| $\tan\alpha = \frac{1}{4} \Rightarrow \alpha = 14°$ or better | A1(II) | 2.2a | No restriction on accuracy since $g$'s cancel |

### Alternative method for (b):
| Sub $U\sin\alpha$ to give equation in $t$ only: $-\frac{5}{4} = \sqrt{2g}\,t - \frac{1}{2}gt^2$ | M1(II), A1(I) | | |
|---|---|---|---|
| Solve for $t$: $t = \frac{5}{\sqrt{2g}}$ or $1.1$ or $1.13$ | M1(III), M1(I) | | |
| Use $20 = Ut\cos\alpha \Rightarrow \alpha = 14°$ or better | A1(II) | | |

## Part (c):
| The target will have dimensions so there would be a range of possible values of $\alpha$; **or** there will be air resistance; **or** the ball will have dimensions; **or** wind effects; **or** spin of the ball | B1 | 3.5b | B0 if any incorrect extras, but ignore extra consequences |

## Part (d):
| Find $U$ using their $\alpha$, e.g. $U = \sqrt{\frac{2g}{\sin^2\alpha}}$ | M1 | 3.1b | |
|---|---|---|---|
| Use $20 = Ut\cos\alpha$ (or vertical motion equation) | A1 M1 | 1.1b | Treat as M1 |
| $t = \frac{5}{\sqrt{2g}}$ or $1.1$ or $1.13$ | B1 A1 | 1.1b | Treat as A1; $t = 1.1$ or $1.10$ since depends on $g = 9.8$ |

### Alternative for (d):
| $A$ to top: $s = vt - \frac{1}{2}at^2$ giving $t_1 = \sqrt{\frac{2}{g}}$; top to $T$: $s = ut + \frac{1}{2}at^2$ giving $t_2 = \frac{3}{\sqrt{2g}}$ | M1, A1 M1 | 3.1b, 1.1b | |
|---|---|---|---|
| Total time $= \sqrt{\frac{2}{g}} + \frac{3}{\sqrt{2g}} = \frac{5}{\sqrt{2g}} = 1.1$ or $1.13$ s | B1 A1 | 1.1b | |

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10.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{65e4b254-fb7b-45c2-9702-32f034018193-32_435_1257_244_402}
\captionsetup{labelformat=empty}
\caption{Figure 4}
\end{center}
\end{figure}

A boy throws a ball at a target. At the instant when the ball leaves the boy's hand at the point $A$, the ball is 2 m above horizontal ground and is moving with speed $U$ at an angle $\alpha$ above the horizontal.

In the subsequent motion, the highest point reached by the ball is 3 m above the ground. The target is modelled as being the point $T$, as shown in Figure 4.\\
The ball is modelled as a particle moving freely under gravity.\\
Using the model,
\begin{enumerate}[label=(\alph*)]
\item show that $U ^ { 2 } = \frac { 2 g } { \sin ^ { 2 } \alpha }$.

The point $T$ is at a horizontal distance of 20 m from $A$ and is at a height of 0.75 m above the ground. The ball reaches $T$ without hitting the ground.
\item Find the size of the angle $\alpha$
\item State one limitation of the model that could affect your answer to part (b).
\item Find the time taken for the ball to travel from $A$ to $T$.
\end{enumerate}

\hfill \mbox{\textit{Edexcel Paper 3 2018 Q10 [15]}}