OCR MEI M2 2006 January — Question 4 16 marks

Exam BoardOCR MEI
ModuleM2 (Mechanics 2)
Year2006
SessionJanuary
Marks16
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicAdvanced work-energy problems
TypeConnected particles pulley energy method
DifficultyStandard +0.3 This is a standard M2 connected particles problem requiring energy methods. Part (i) is straightforward work-energy calculation. Parts (ii) and (iii) involve routine application of energy conservation with gravitational PE changes, friction work, and kinetic energy - all standard textbook techniques with clear scaffolding. The multi-part structure and numerical complexity place it slightly above average difficulty, but no novel insight is required.
Spec6.02a Work done: concept and definition6.02b Calculate work: constant force, resolved component6.02i Conservation of energy: mechanical energy principle6.02j Conservation with elastics: springs and strings6.02l Power and velocity: P = Fv

4 A block of mass 20 kg is pulled by a light, horizontal string over a rough, horizontal plane. During 6 seconds, the work done against resistances is 510 J and the speed of the block increases from \(5 \mathrm {~m} \mathrm {~s} ^ { - 1 }\) to \(8 \mathrm {~m} \mathrm {~s} ^ { - 1 }\).
  1. Calculate the power of the pulling force. The block is now put on a rough plane that is at an angle \(\alpha\) to the horizontal, where \(\sin \alpha = \frac { 3 } { 5 }\). The frictional resistance to sliding is \(11 g \mathrm {~N}\). A light string parallel to the plane is connected to the block. The string passes over a smooth pulley and is connected to a freely hanging sphere of mass \(m \mathrm {~kg}\), as shown in Fig. 4. \begin{figure}[h]
    \includegraphics[alt={},max width=\textwidth]{c1785fde-a6ce-4f8b-9948-4b4dd973ce84-6_348_855_847_605} \captionsetup{labelformat=empty} \caption{Fig. 4}
    \end{figure} In parts (ii) and (iii), the sphere is pulled downwards and then released when travelling at a speed of \(4 \mathrm {~m} \mathrm {~s} ^ { - 1 }\) vertically downwards. The block never reaches the pulley.
  2. Suppose that \(m = 5\) and that after the sphere is released the block moves \(x \mathrm {~m}\) up the plane before coming to rest.
    (A) Find an expression in terms of \(x\) for the change in gravitational potential energy of the system, stating whether this is a gain or a loss.
    (B) Find an expression in terms of \(x\) for the work done against friction.
    (C) Making use of your answers to parts (A) and (B), find the value of \(x\).
  3. Suppose instead that \(m = 15\). Calculate the speed of the sphere when it has fallen a distance 0.5 m from its point of release.

Question 4:
Part (i)
AnswerMarks Guidance
AnswerMark Guidance
\(\dfrac{0.5 \times 20 \times 8^2 - 0.5 \times 20 \times 5^2 + 510}{6}\)M1 Use of \(P = \text{WD}/t\)
B1\(\Delta\)KE. Accept \(\pm 390\) soi
A1All correct including signs
\(= 150\) WA1
Part (ii)(A)
AnswerMarks Guidance
AnswerMark Guidance
\(20g \times \dfrac{3}{5}x - 5gx\)M1 Use of \(mgh\) on both terms
B1Either term (neglecting signs)
A1\(\pm 7gx\) in any form
\(7gx\) (68.6\(x\)) gainA1 cao
Part (ii)(B)
AnswerMarks Guidance
AnswerMark Guidance
\(11gx\)B1
Part (ii)(C)
AnswerMarks Guidance
AnswerMark Guidance
\(0.5 \times 25 \times 4^2 = 7gx + 11gx = 18gx\)M1 Use of work-energy equation. Allow 1 RHS term omitted.
B1KE term correct
\(x = 1.13378...\) so 1.13 m (3 s.f.)A1 cao. Except follow wrong sign for \(7gx\) only.
Part (iii)
AnswerMarks Guidance
AnswerMark Guidance
either
\(0.5 \times 35 \times v^2 - 0.5 \times 35 \times 16 = 15g \times 0.5 - 11g \times 0.5 - 12g \times 0.5\)M1 Use of work-energy. KE, GPE and WD against friction terms present.
B1\(\Delta\)GPE correct inc sign (1.5\(g\) J loss)
A1All correct
\(v^2 = 13.76\) so \(v = 3.70944...\) so \(3.71\ \text{m s}^{-1}\) (3 s.f.)A1 cao
or
\(15g - T = 15a \quad T - 12g - 11g = 20a\)M1 N2L in 1 or 2 equations. All terms present
so \(a = -2.24\)A1 cao
\(v^2 = 4^2 + 2 \times (-2.24) \times 0.5\)M1 Use of appropriate (sequence of) \(uvast\)
so \(3.71\ \text{m s}^{-1}\) (3 s.f.)A1 cao
# Question 4:

## Part (i)

| Answer | Mark | Guidance |
|--------|------|----------|
| $\dfrac{0.5 \times 20 \times 8^2 - 0.5 \times 20 \times 5^2 + 510}{6}$ | M1 | Use of $P = \text{WD}/t$ |
| | B1 | $\Delta$KE. Accept $\pm 390$ soi |
| | A1 | All correct including signs |
| $= 150$ W | A1 | |

## Part (ii)(A)

| Answer | Mark | Guidance |
|--------|------|----------|
| $20g \times \dfrac{3}{5}x - 5gx$ | M1 | Use of $mgh$ on both terms |
| | B1 | Either term (neglecting signs) |
| | A1 | $\pm 7gx$ in any form |
| $7gx$ (68.6$x$) gain | A1 | cao |

## Part (ii)(B)

| Answer | Mark | Guidance |
|--------|------|----------|
| $11gx$ | B1 | |

## Part (ii)(C)

| Answer | Mark | Guidance |
|--------|------|----------|
| $0.5 \times 25 \times 4^2 = 7gx + 11gx = 18gx$ | M1 | Use of work-energy equation. Allow 1 RHS term omitted. |
| | B1 | KE term correct |
| $x = 1.13378...$ so 1.13 m (3 s.f.) | A1 | cao. Except follow wrong sign for $7gx$ only. |

## Part (iii)

| Answer | Mark | Guidance |
|--------|------|----------|
| **either** | | |
| $0.5 \times 35 \times v^2 - 0.5 \times 35 \times 16 = 15g \times 0.5 - 11g \times 0.5 - 12g \times 0.5$ | M1 | Use of work-energy. KE, GPE and WD against friction terms present. |
| | B1 | $\Delta$GPE correct inc sign (1.5$g$ J loss) |
| | A1 | All correct |
| $v^2 = 13.76$ so $v = 3.70944...$ so $3.71\ \text{m s}^{-1}$ (3 s.f.) | A1 | cao |
| **or** | | |
| $15g - T = 15a \quad T - 12g - 11g = 20a$ | M1 | N2L in 1 or 2 equations. All terms present |
| so $a = -2.24$ | A1 | cao |
| $v^2 = 4^2 + 2 \times (-2.24) \times 0.5$ | M1 | Use of appropriate (sequence of) $uvast$ |
| so $3.71\ \text{m s}^{-1}$ (3 s.f.) | A1 | cao |
4 A block of mass 20 kg is pulled by a light, horizontal string over a rough, horizontal plane. During 6 seconds, the work done against resistances is 510 J and the speed of the block increases from $5 \mathrm {~m} \mathrm {~s} ^ { - 1 }$ to $8 \mathrm {~m} \mathrm {~s} ^ { - 1 }$.
\begin{enumerate}[label=(\roman*)]
\item Calculate the power of the pulling force.

The block is now put on a rough plane that is at an angle $\alpha$ to the horizontal, where $\sin \alpha = \frac { 3 } { 5 }$. The frictional resistance to sliding is $11 g \mathrm {~N}$. A light string parallel to the plane is connected to the block. The string passes over a smooth pulley and is connected to a freely hanging sphere of mass $m \mathrm {~kg}$, as shown in Fig. 4.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{c1785fde-a6ce-4f8b-9948-4b4dd973ce84-6_348_855_847_605}
\captionsetup{labelformat=empty}
\caption{Fig. 4}
\end{center}
\end{figure}

In parts (ii) and (iii), the sphere is pulled downwards and then released when travelling at a speed of $4 \mathrm {~m} \mathrm {~s} ^ { - 1 }$ vertically downwards. The block never reaches the pulley.
\item Suppose that $m = 5$ and that after the sphere is released the block moves $x \mathrm {~m}$ up the plane before coming to rest.\\
(A) Find an expression in terms of $x$ for the change in gravitational potential energy of the system, stating whether this is a gain or a loss.\\
(B) Find an expression in terms of $x$ for the work done against friction.\\
(C) Making use of your answers to parts (A) and (B), find the value of $x$.
\item Suppose instead that $m = 15$. Calculate the speed of the sphere when it has fallen a distance 0.5 m from its point of release.
\end{enumerate}

\hfill \mbox{\textit{OCR MEI M2 2006 Q4 [16]}}