| Exam Board | OCR MEI |
|---|---|
| Module | M1 (Mechanics 1) |
| Year | 2010 |
| Session | June |
| Marks | 20 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Friction |
| Type | Practical friction scenarios |
| Difficulty | Standard +0.3 This is a multi-part mechanics question involving standard M1 topics (Newton's laws, friction, kinematics). Parts (i)-(iii) are straightforward applications of F=ma and vector resolution. Part (iv) is a 'show that' requiring kinematic equations and Newton's second law. Part (v) uses constant acceleration equations. While lengthy with multiple parts, each step uses routine M1 techniques without requiring novel insight, making it slightly easier than average. |
| Spec | 1.10a Vectors in 2D: i,j notation and column vectors3.03d Newton's second law: 2D vectors3.03e Resolve forces: two dimensions3.03m Equilibrium: sum of resolved forces = 03.03r Friction: concept and vector form |
| 4 | □ box P □ |
| \multirow[t]{10}{*}{4 | |
| 4 | |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| N2L i direction: \(150 = 250a\), \(a = 0.6\) so \(0.6 \text{ m s}^{-2}\) | M1 | Use of N2L. Allow \(F = mga\). |
| A1 | Accept no reference to direction |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| \(150 \text{ N}\) | B1 | |
| \(-\)i direction | B1 | Allow correct description or arrow. [Accept '\(-150\) in i direction' for B1 B1] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| For force only in direction perp to i: \(300\sin 40 = 450\sin\theta\) | M1 | Resolution of both terms attempted. Allow \(\sin \leftrightarrow \cos\) if in both terms. Allow 250 or \(250g\) present. |
| B1 | \(300\sin40\) or \(450\sin\theta\) | |
| \(\theta = 25.37300...\) so \(25.4°\) (3 s.f.) | A1 | Accept \(\pm\). Accept answer rounding to 25.5. Allow SC1 if seen in this part. |
| In i direction: \(300\cos 40 + 150 + 450\cos\theta\) | M1 | Proper resolution attempted of 450 and 300. Allow \(\sin \leftrightarrow \cos\) if in both terms. Accept use of their \(\theta\) or just \(\theta\). |
| A1 | Either resolution correct. Accept their \(\theta\) or just \(\theta\). Accept sin/cos consistent with use for cpt perpendicular to i. | |
| \(786.4017...\) so \(786\)i N (3 s.f.) | A1 | Accept no reference to direction cao. Allow SC1 WW |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Using \(s = ut + 0.5at^2\): \(1 = 0.5a \times 2^2\), \(a = 0.5\) | M1 | Appropriate (sequence of) suvat. [WW M0 A0] |
| A1 | ||
| Using N2L in i direction: \(786.4017... - F = 250\times0.5\) | M1 | Use of \(F = ma\) with their 786.4 and their \(a\). No extra forces. Allow sign errors. |
| \(661.4017...\) so \(661 \text{ N}\) (3 s.f.) | A1 | All correct using their 786.4 and \(a\) |
| E1 | Use of N2L clearly shown. (Accept 0.5 used WW) |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Using N2L in i direction either: \(125 - 200 = 250a_1\) or (starting again): \(786.4017... - (200 + 661.4017...) = 250a_1\) | M1 | Use of \(F = ma\) with their values. Allow 1 force missing. |
| so \(a_1 = -0.3\) | F1 | FT only their 786... and their 661 |
| Using \(v^2 = u^2 + 2a_1 s\): \(v^2 = 1.8^2 + 2\times(-0.3)\times1.65\) | M1 | Appropriate (sequence of) suvat with \(u \neq 0\). Must be 'new' \(a\) obtained by using N2L. |
| \(v = 1.5\) so \(1.5 \text{ m s}^{-1}\) | F1 | Only FT use of \(\pm\) their \(a_1\) |
| A1 | cao |
# Question 8:
## Part (i)
| Answer/Working | Mark | Guidance |
|---|---|---|
| N2L **i** direction: $150 = 250a$, $a = 0.6$ so $0.6 \text{ m s}^{-2}$ | M1 | Use of N2L. Allow $F = mga$. |
| | A1 | Accept no reference to direction |
## Part (ii)
| Answer/Working | Mark | Guidance |
|---|---|---|
| $150 \text{ N}$ | B1 | |
| $-$**i** direction | B1 | Allow correct description or arrow. [Accept '$-150$ in **i** direction' for B1 B1] |
## Part (iii)
| Answer/Working | Mark | Guidance |
|---|---|---|
| For force only in direction perp to **i**: $300\sin 40 = 450\sin\theta$ | M1 | Resolution of both terms attempted. Allow $\sin \leftrightarrow \cos$ if in both terms. Allow 250 or $250g$ present. |
| | B1 | $300\sin40$ or $450\sin\theta$ |
| $\theta = 25.37300...$ so $25.4°$ (3 s.f.) | A1 | Accept $\pm$. Accept answer rounding to 25.5. Allow SC1 if seen in this part. |
| In **i** direction: $300\cos 40 + 150 + 450\cos\theta$ | M1 | Proper resolution attempted of 450 **and** 300. Allow $\sin \leftrightarrow \cos$ if in both terms. Accept use of **their** $\theta$ or just $\theta$. |
| | A1 | Either resolution correct. Accept **their** $\theta$ or just $\theta$. Accept sin/cos consistent with use for cpt perpendicular to **i**. |
| $786.4017...$ so $786$**i** N (3 s.f.) | A1 | Accept no reference to direction cao. Allow SC1 WW |
## Part (iv)
| Answer/Working | Mark | Guidance |
|---|---|---|
| Using $s = ut + 0.5at^2$: $1 = 0.5a \times 2^2$, $a = 0.5$ | M1 | Appropriate (sequence of) suvat. [WW M0 A0] |
| | A1 | |
| Using N2L in **i** direction: $786.4017... - F = 250\times0.5$ | M1 | Use of $F = ma$ with **their** 786.4 and **their** $a$. No extra forces. Allow sign errors. |
| $661.4017...$ so $661 \text{ N}$ (3 s.f.) | A1 | All correct using **their** 786.4 and $a$ |
| | E1 | Use of N2L clearly shown. (Accept 0.5 used WW) |
## Part (v)
| Answer/Working | Mark | Guidance |
|---|---|---|
| Using N2L in **i** direction **either**: $125 - 200 = 250a_1$ **or** (starting again): $786.4017... - (200 + 661.4017...) = 250a_1$ | M1 | Use of $F = ma$ with **their** values. Allow 1 force missing. |
| so $a_1 = -0.3$ | F1 | FT only **their** 786... and **their** 661 |
| Using $v^2 = u^2 + 2a_1 s$: $v^2 = 1.8^2 + 2\times(-0.3)\times1.65$ | M1 | Appropriate (sequence of) suvat with $u \neq 0$. Must be 'new' $a$ obtained by using N2L. |
| $v = 1.5$ so $1.5 \text{ m s}^{-1}$ | F1 | Only FT use of $\pm$ **their** $a_1$ |
| | A1 | cao |
8 A cylindrical tub of mass 250 kg is on a horizontal floor. Resistance to its motion other than that due to friction is negligible.
The first attempt to move the tub is by pulling it with a force of 150 N in the $\mathbf { i }$ direction, as shown in Fig. 8.1.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{6cca1e5e-82b0-487d-8048-b9db7745dea6-5_319_1358_511_392}
\captionsetup{labelformat=empty}
\caption{Fig. 8.1}
\end{center}
\end{figure}
(i) Calculate the acceleration of the tub if friction is ignored.
In fact, there is friction and the tub does not move.\\
(ii) Write down the magnitude and direction of the frictional force opposing the pull.
Two more forces are now added to the 150 N force in a second attempt to move the tub, as shown in Fig. 8.2.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{6cca1e5e-82b0-487d-8048-b9db7745dea6-5_502_935_1411_607}
\captionsetup{labelformat=empty}
\caption{Fig. 8.2}
\end{center}
\end{figure}
Angle $\theta$ is acute and chosen so that the resultant of the three forces is in the $\mathbf { i }$ direction.\\
(iii) Determine the value of $\theta$ and the resultant of the three forces.
With this resultant force, the tub moves with constant acceleration and travels 1 metre from rest in 2 seconds.\\
(iv) Show that the magnitude of the friction acting on the tub is 661 N , correct to 3 significant figures.
When the speed of the tub is $1.8 \mathrm {~m} \mathrm {~s} ^ { - 1 }$, it comes to a part of the floor where the friction on the tub is 200 N greater. The pulling forces stay the same.\\
(v) Find the velocity of the tub when it has moved a further 1.65 m .
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\hfill \mbox{\textit{OCR MEI M1 2010 Q8 [20]}}