Edexcel M2 2009 June — Question 7 11 marks

Exam BoardEdexcel
ModuleM2 (Mechanics 2)
Year2009
SessionJune
Marks11
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicAdvanced work-energy problems
TypeRough inclined plane work-energy
DifficultyStandard +0.3 This is a standard M2 work-energy problem with friction on an inclined plane. Part (a) requires straightforward application of the work-energy principle with given values, while part (b) involves recognizing that friction reverses direction on the return journey. The trigonometry is simple (given tan α), and the problem follows a familiar textbook pattern with no novel insights required. Slightly easier than average due to clear structure and standard technique.
Spec3.03v Motion on rough surface: including inclined planes6.02i Conservation of energy: mechanical energy principle

7. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{8e220b8a-46f1-4b9b-88a4-f032c7fbda50-11_501_1018_116_468} \captionsetup{labelformat=empty} \caption{Figure 4}
\end{figure} A particle \(P\) of mass 2 kg is projected up a rough plane with initial speed \(14 \mathrm {~m} \mathrm {~s} ^ { - 1 }\), from a point \(X\) on the plane, as shown in Figure 4. The particle moves up the plane along the line of greatest slope through \(X\) and comes to instantaneous rest at the point \(Y\). The plane is inclined at an angle \(\alpha\) to the horizontal, where \(\tan \alpha = \frac { 7 } { 24 }\). The coefficient of friction between the particle and the plane is \(\frac { 1 } { 8 }\).
  1. Use the work-energy principle to show that \(X Y = 25 \mathrm {~m}\). After reaching \(Y\), the particle \(P\) slides back down the plane.
  2. Find the speed of \(P\) as it passes through \(X\).

Question 7:
Part (a):
AnswerMarks Guidance
Answer/WorkingMarks Guidance
KE at \(X = \frac{1}{2}mv^2 = \frac{1}{2} \times 2 \times 14^2\)B1
GPE at \(Y = mgd\sin\alpha\left(= 2 \times g \times d \times \frac{7}{25}\right)\)B1
Normal reaction \(R = mg\cos\alpha\)B1 M1
Friction \(= \mu \times R = \frac{1}{8} \times 2g \times \frac{24}{25}\)M1A1
Work-Energy: \(\frac{1}{2}mv^2 - mgd\sin\alpha = \mu \times R \times d\) or equivalent
\(196 = \frac{14gd}{25} + \frac{6gd}{25} = \frac{20gd}{25}\)A1
\(d = 25\text{ m}\)
Subtotal: (7)
Part (b):
AnswerMarks Guidance
Answer/WorkingMarks Guidance
Work done \(= \mu \times R \times 2d = \frac{1}{8} \times 2g \times \frac{24}{25} \times 2d\)
Return to \(X\): \(\frac{1}{2}mv^2 = \frac{1}{2}m14^2 - \frac{1}{8} \times 2g \times \frac{24}{25} \times 50\)M1A1
\(v = 8.9 \text{ ms}^{-1}\) (accept \(8.85 \text{ ms}^{-1}\))DM1A1
OR: \(2a = 2g\sin\alpha - F_{\max} = 2g \times \frac{7}{25} - \frac{6g}{25} = \frac{8g}{25}\)M1A1
\(v^2 = (0+)2 \times a \times s = 8g;\ v = 8.9\) (accept \(8.85 \text{ ms}^{-1}\))DM1;A1
Subtotal: (4) Total: [11]
## Question 7:

### Part (a):

| Answer/Working | Marks | Guidance |
|---|---|---|
| KE at $X = \frac{1}{2}mv^2 = \frac{1}{2} \times 2 \times 14^2$ | B1 | |
| GPE at $Y = mgd\sin\alpha\left(= 2 \times g \times d \times \frac{7}{25}\right)$ | B1 | |
| Normal reaction $R = mg\cos\alpha$ | B1 M1 | |
| Friction $= \mu \times R = \frac{1}{8} \times 2g \times \frac{24}{25}$ | M1A1 | |
| Work-Energy: $\frac{1}{2}mv^2 - mgd\sin\alpha = \mu \times R \times d$ or equivalent | | |
| $196 = \frac{14gd}{25} + \frac{6gd}{25} = \frac{20gd}{25}$ | A1 | |
| $d = 25\text{ m}$ | | |

**Subtotal: (7)**

### Part (b):

| Answer/Working | Marks | Guidance |
|---|---|---|
| Work done $= \mu \times R \times 2d = \frac{1}{8} \times 2g \times \frac{24}{25} \times 2d$ | | |
| Return to $X$: $\frac{1}{2}mv^2 = \frac{1}{2}m14^2 - \frac{1}{8} \times 2g \times \frac{24}{25} \times 50$ | M1A1 | |
| $v = 8.9 \text{ ms}^{-1}$ (accept $8.85 \text{ ms}^{-1}$) | DM1A1 | |
| OR: $2a = 2g\sin\alpha - F_{\max} = 2g \times \frac{7}{25} - \frac{6g}{25} = \frac{8g}{25}$ | M1A1 | |
| $v^2 = (0+)2 \times a \times s = 8g;\ v = 8.9$ (accept $8.85 \text{ ms}^{-1}$) | DM1;A1 | |

**Subtotal: (4) Total: [11]**

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7.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{8e220b8a-46f1-4b9b-88a4-f032c7fbda50-11_501_1018_116_468}
\captionsetup{labelformat=empty}
\caption{Figure 4}
\end{center}
\end{figure}

A particle $P$ of mass 2 kg is projected up a rough plane with initial speed $14 \mathrm {~m} \mathrm {~s} ^ { - 1 }$, from a point $X$ on the plane, as shown in Figure 4. The particle moves up the plane along the line of greatest slope through $X$ and comes to instantaneous rest at the point $Y$. The plane is inclined at an angle $\alpha$ to the horizontal, where $\tan \alpha = \frac { 7 } { 24 }$. The coefficient of friction between the particle and the plane is $\frac { 1 } { 8 }$.
\begin{enumerate}[label=(\alph*)]
\item Use the work-energy principle to show that $X Y = 25 \mathrm {~m}$.

After reaching $Y$, the particle $P$ slides back down the plane.
\item Find the speed of $P$ as it passes through $X$.
\end{enumerate}

\hfill \mbox{\textit{Edexcel M2 2009 Q7 [11]}}