Edexcel M2 2004 June — Question 7 17 marks

Exam BoardEdexcel
ModuleM2 (Mechanics 2)
Year2004
SessionJune
Marks17
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicWork done and energy
TypeMotion on rough inclined plane
DifficultyStandard +0.3 This is a standard M2 work-energy and projectile motion question with straightforward application of well-practiced techniques. Part (a) uses work-energy principle with given values, parts (b-d) are routine projectile motion calculations with a given angle. All steps are textbook exercises requiring no novel insight, making it slightly easier than average.
Spec3.02i Projectile motion: constant acceleration model6.02i Conservation of energy: mechanical energy principle

7. \begin{figure}[h]
\captionsetup{labelformat=empty} \caption{Figure 2} \includegraphics[alt={},max width=\textwidth]{8e694174-b9a9-4018-8896-31a3b4f0d344-5_424_1324_264_383}
\end{figure} In a ski-jump competition, a skier of mass 80 kg moves from rest at a point \(A\) on a ski-slope. The skier's path is an arc \(A B\). The starting point \(A\) of the slope is 32.5 m above horizontal ground. The end \(B\) of the slope is 8.1 m above the ground. When the skier reaches \(B\), she is travelling at \(20 \mathrm {~m} \mathrm {~s} ^ { - 1 }\), and moving upwards at an angle \(\alpha\) to the horizontal, where \(\tan \alpha = \frac { 3 } { 4 }\), as shown in Fig. 2. The distance along the slope from \(A\) to \(B\) is 60 m . The resistance to motion while she is on the slope is modelled as a force of constant magnitude \(R\) newtons. By using the work-energy principle,
  1. find the value of \(R\). On reaching \(B\), the skier then moves through the air and reaches the ground at the point \(C\). The motion of the skier in moving from \(B\) to \(C\) is modelled as that of a particle moving freely under gravity.
  2. Find the time for the skier to move from \(B\) to \(C\).
  3. Find the horizontal distance from \(B\) to \(C\).
  4. Find the speed of the skier immediately before she reaches \(C\). END

Question 7:
Part (a)
AnswerMarks Guidance
Answer/WorkingMarks Guidance
Work-Energy: \(R \times 60 = 80 \times 9.8 \times 24.4 - \frac{1}{2} \times 80 \times 20^2\)M1 A2(1,0)
\((= 19129.6 - 16000 = 3129.6)\)
\(R = 52\) (N)M1 A1 accept 52.2
Part (b)
AnswerMarks Guidance
Answer/WorkingMarks Guidance
\(-8.1 = 20\sin\alpha \times t - \frac{1}{2}gt^2\)M1 A2(1,0)
\(4.9t^2 - 12t - 8.1 = 0\)M1
\(t = 3\) (s)A1
Part (c)
AnswerMarks Guidance
Answer/WorkingMarks Guidance
\(20\cos\alpha \times 3 = 16 \times 3 = 48\) (m)M1 A1ft ft their \(t\)
Part (d)
AnswerMarks Guidance
Answer/WorkingMarks Guidance
Energy: \(\frac{1}{2}mv^2 - \frac{1}{2}m \times 20^2 = m \times 9.8 \times 8.1\)M1 A2(1,0)
\(v = \sqrt{558.56} \approx 24\) \((\text{ms}^{-1})\)M1 A1 accept 23.6
Alternative for (d):
AnswerMarks Guidance
Answer/WorkingMarks Guidance
\(\uparrow\) \(v_y = 12 - 3g = -17.4\); \(\rightarrow\) \(v_x = 16\)M1 A1, A1
\(v = \sqrt{17.4^2 + 16^2} \approx 24\) \((\text{ms}^{-1})\)M1 A1 accept 23.6
## Question 7:

### Part (a)

| Answer/Working | Marks | Guidance |
|---|---|---|
| Work-Energy: $R \times 60 = 80 \times 9.8 \times 24.4 - \frac{1}{2} \times 80 \times 20^2$ | M1 A2(1,0) | |
| $(= 19129.6 - 16000 = 3129.6)$ | | |
| $R = 52$ (N) | M1 A1 | accept 52.2 |

### Part (b)

| Answer/Working | Marks | Guidance |
|---|---|---|
| $-8.1 = 20\sin\alpha \times t - \frac{1}{2}gt^2$ | M1 A2(1,0) | |
| $4.9t^2 - 12t - 8.1 = 0$ | M1 | |
| $t = 3$ (s) | A1 | |

### Part (c)

| Answer/Working | Marks | Guidance |
|---|---|---|
| $20\cos\alpha \times 3 = 16 \times 3 = 48$ (m) | M1 A1ft | ft their $t$ |

### Part (d)

| Answer/Working | Marks | Guidance |
|---|---|---|
| Energy: $\frac{1}{2}mv^2 - \frac{1}{2}m \times 20^2 = m \times 9.8 \times 8.1$ | M1 A2(1,0) | |
| $v = \sqrt{558.56} \approx 24$ $(\text{ms}^{-1})$ | M1 A1 | accept 23.6 |

**Alternative for (d):**

| Answer/Working | Marks | Guidance |
|---|---|---|
| $\uparrow$ $v_y = 12 - 3g = -17.4$; $\rightarrow$ $v_x = 16$ | M1 A1, A1 | |
| $v = \sqrt{17.4^2 + 16^2} \approx 24$ $(\text{ms}^{-1})$ | M1 A1 | accept 23.6 |
7.

\begin{figure}[h]
\begin{center}
\captionsetup{labelformat=empty}
\caption{Figure 2}
  \includegraphics[alt={},max width=\textwidth]{8e694174-b9a9-4018-8896-31a3b4f0d344-5_424_1324_264_383}
\end{center}
\end{figure}

In a ski-jump competition, a skier of mass 80 kg moves from rest at a point $A$ on a ski-slope. The skier's path is an arc $A B$. The starting point $A$ of the slope is 32.5 m above horizontal ground. The end $B$ of the slope is 8.1 m above the ground. When the skier reaches $B$, she is travelling at $20 \mathrm {~m} \mathrm {~s} ^ { - 1 }$, and moving upwards at an angle $\alpha$ to the horizontal, where $\tan \alpha = \frac { 3 } { 4 }$, as shown in Fig. 2. The distance along the slope from $A$ to $B$ is 60 m . The resistance to motion while she is on the slope is modelled as a force of constant magnitude $R$ newtons. By using the work-energy principle,
\begin{enumerate}[label=(\alph*)]
\item find the value of $R$.

On reaching $B$, the skier then moves through the air and reaches the ground at the point $C$. The motion of the skier in moving from $B$ to $C$ is modelled as that of a particle moving freely under gravity.
\item Find the time for the skier to move from $B$ to $C$.
\item Find the horizontal distance from $B$ to $C$.
\item Find the speed of the skier immediately before she reaches $C$.

END
\end{enumerate}

\hfill \mbox{\textit{Edexcel M2 2004 Q7 [17]}}