| Exam Board | OCR MEI |
|---|---|
| Module | M1 (Mechanics 1) |
| Marks | 21 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Newton's laws and connected particles |
| Type | Particle on rough horizontal, string over pulley |
| Difficulty | Standard +0.3 This is a standard connected particles question with straightforward application of Newton's second law. Part (i) is routine F=ma, parts (ii)-(iv) involve standard pulley system analysis with clear setup, and part (v) uses basic SUVAT equations. While multi-part and requiring careful bookkeeping, all techniques are textbook-standard with no novel insight required, making it slightly easier than average. |
| Spec | 3.02h Motion under gravity: vector form3.02i Projectile motion: constant acceleration model3.03k Connected particles: pulleys and equilibrium3.03o Advanced connected particles: and pulleys3.03r Friction: concept and vector form3.03t Coefficient of friction: F <= mu*R model |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Mark | Guidance |
| N2L: \(F - 11.2 = 8 \times 2\) | M1 | Use of N2L (allow \(F = mga\)). Allow 11.2 omitted; no extra forces |
| All correct | A1 | |
| \(F = 27.2\) N | A1 | Cao |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Mark | Guidance |
| The string is inextensible | E1 | Allow 'light inextensible' but not other irrelevant reasons given as well (e.g. smooth pulley) |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Mark | Guidance |
| Force diagram | B1 | One diagram with all forces present; no extras; correct arrows and labels; accept use of words |
| Both diagrams correct with a common label | B1 |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Mark | Guidance |
| For either box or sphere, \(F = ma\) | M1 | Allow omitted force and sign errors but not extra forces. Need correct mass. Allow use of mass not weight |
| Box N2L: \(105 - T - 11.2 = 8a\) | A1 | Correct and in any form |
| Sphere N2L \(\uparrow\): \(T - 58.8 = 6a\) | A1 | Correct and in any form. [box and sphere equations with consistent signs] |
| Adding \(35 = 14a\) | M1 | Eliminating 1 variable from 2 equations in 2 variables |
| \(a = 2.5\) m s\(^{-2}\) | E1 | |
| Substitute \(a = 2.5\) giving \(T = 58.8 + 15\) | M1 | Attempt to substitute in either box or sphere equation |
| \(T = 73.8\) N | A1 |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Mark | Guidance |
| \(105 - 11.2 - 58.8 = 14a\) | M1 | For box and sphere, \(F = ma\). Must be correct mass. Allow use of mass not weight |
| \(a = 2.5\) | A1 | |
| Method made clear | E1 | |
| For either box or sphere, \(F = ma\) | M1 | Allow omitted force and sign errors but not extra forces. Need correct mass |
| Box N2L: \(105 - T - 11.2 = 8a\) or Sphere N2L \(\uparrow\): \(T - 58.8 = 6a\) | A1 | Correct and in any form |
| Substitute \(a = 2.5\) in either equation | M1 | Attempt to substitute in either box or sphere equation |
| \(T = 73.8\) N | A1 | [If AG used in either equation award M1 A1 for that equation as above and M1 A1 for finding \(T\). For full marks, both values must be shown to satisfy the second equation.] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Mark | Guidance |
| \(g\) downwards | B1 | Accept \(\pm g\), \(\pm 9.8\), \(\pm 10\), \(\pm 9.81\) |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Mark | Guidance |
| Taking \(\uparrow\) +ve, \(s = -1.8\), \(u = 3\) and \(a = -9.8\), so \(-1.8 = 3T - 4.9T^2\) | M1 | Some attempt to use \(s = ut + 0.5at^2\) with \(a = \pm 9.8\) etc. \(s = \pm 1.8\) and \(u = \pm 3\). Award for \(a = g\) even if answer to (A) wrong |
| \(4.9T^2 - 3T - 1.8 = 0\) | E1 | Clearly shown. No need to show +ve required |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Mark | Guidance |
| Time to reach \(3\) m s\(^{-1}\) given by \(3 = 0 + 2.5t\) so \(t = 1.2\) | B1 | |
| Remaining time is root of quadratic | M1 | Quadratic solved and +ve root added to time to break |
| Time is \(0.98513\ldots\) s | B1 | Allow \(0.98\). [Award for answer seen WW] |
| Total \(2.1851\ldots\) so \(2.19\) s (3 s.f.) | A1 | Cao |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Mark | Guidance |
| (i) \(F + 11.2 = 8 \times 2\) so \(F = 4.8\) | — | The same scheme as above |
| (iii) | — | The 11.2 N force may be in either direction, otherwise the same scheme |
| (iv) Method (1): Box N2L \(\rightarrow\) \(105 - T + 11.2 = 8a\); sphere as before. Method (2): \(105 + 11.2 - 58.8 = 14a\); giving \(a = 4.1\) and \(T = 83.4\) | — | Allow 2.5 substituted in box equation to give \(T = 96.2\). If the sign convention gives as positive the direction of the sphere descending, \(a = -4.1\). Allow substituting \(a = 2.5\) in the equations to give \(T = 43.8\) (sphere) or \(136.2\) (box) |
| (v) | — | In (C) allow use of \(a = 4.1\) to give time to break as \(0.73117\ldots\) s and total time as \(1.716\ldots\) s |
## Question 2(i):
| Answer | Mark | Guidance |
|--------|------|----------|
| N2L: $F - 11.2 = 8 \times 2$ | M1 | Use of N2L (allow $F = mga$). Allow 11.2 omitted; no extra forces |
| All correct | A1 | |
| $F = 27.2$ N | A1 | Cao |
**Total: [3]**
---
## Question 2(ii):
| Answer | Mark | Guidance |
|--------|------|----------|
| The string is inextensible | E1 | Allow 'light inextensible' but not other irrelevant reasons given as well (e.g. smooth pulley) |
**Total: [1]**
---
## Question 2(iii):
| Answer | Mark | Guidance |
|--------|------|----------|
| Force diagram | B1 | One diagram with all forces present; no extras; correct arrows and labels; accept use of words |
| Both diagrams correct with a common label | B1 | |
**Total: [2]**
---
## Question 2(iv):
**Method (1):**
| Answer | Mark | Guidance |
|--------|------|----------|
| For either box or sphere, $F = ma$ | M1 | Allow omitted force and sign errors but not extra forces. Need correct mass. Allow use of mass not weight |
| Box N2L: $105 - T - 11.2 = 8a$ | A1 | Correct and in any form |
| Sphere N2L $\uparrow$: $T - 58.8 = 6a$ | A1 | Correct and in any form. [box and sphere equations with consistent signs] |
| Adding $35 = 14a$ | M1 | Eliminating 1 variable from 2 equations in 2 variables |
| $a = 2.5$ m s$^{-2}$ | E1 | |
| Substitute $a = 2.5$ giving $T = 58.8 + 15$ | M1 | Attempt to substitute in either box or sphere equation |
| $T = 73.8$ N | A1 | |
**Method (2):**
| Answer | Mark | Guidance |
|--------|------|----------|
| $105 - 11.2 - 58.8 = 14a$ | M1 | For box and sphere, $F = ma$. Must be correct mass. Allow use of mass not weight |
| $a = 2.5$ | A1 | |
| Method made clear | E1 | |
| For **either** box **or** sphere, $F = ma$ | M1 | Allow omitted force and sign errors but not extra forces. Need correct mass |
| Box N2L: $105 - T - 11.2 = 8a$ **or** Sphere N2L $\uparrow$: $T - 58.8 = 6a$ | A1 | Correct and in any form |
| Substitute $a = 2.5$ in either equation | M1 | Attempt to substitute in either box or sphere equation |
| $T = 73.8$ N | A1 | [If AG used in either equation award M1 A1 for that equation as above and M1 A1 for finding $T$. For full marks, both values must be shown to satisfy the second equation.] |
**Total: [7]**
---
## Question 2(v)(A):
| Answer | Mark | Guidance |
|--------|------|----------|
| $g$ downwards | B1 | Accept $\pm g$, $\pm 9.8$, $\pm 10$, $\pm 9.81$ |
**Total: [1]**
---
## Question 2(v)(B):
| Answer | Mark | Guidance |
|--------|------|----------|
| Taking $\uparrow$ +ve, $s = -1.8$, $u = 3$ and $a = -9.8$, so $-1.8 = 3T - 4.9T^2$ | M1 | Some attempt to use $s = ut + 0.5at^2$ with $a = \pm 9.8$ etc. $s = \pm 1.8$ and $u = \pm 3$. Award for $a = g$ even if answer to (A) wrong |
| $4.9T^2 - 3T - 1.8 = 0$ | E1 | Clearly shown. No need to show +ve required |
**Total: [2]**
---
## Question 2(v)(C):
| Answer | Mark | Guidance |
|--------|------|----------|
| Time to reach $3$ m s$^{-1}$ given by $3 = 0 + 2.5t$ so $t = 1.2$ | B1 | |
| Remaining time is root of quadratic | M1 | Quadratic solved and +ve root added to time to break |
| Time is $0.98513\ldots$ s | B1 | Allow $0.98$. [Award for answer seen WW] |
| Total $2.1851\ldots$ so $2.19$ s (3 s.f.) | A1 | Cao |
**Total: [4]**
---
*With the 11.2 N resistance acting to the right:*
| Answer | Mark | Guidance |
|--------|------|----------|
| **(i)** $F + 11.2 = 8 \times 2$ so $F = 4.8$ | — | The same scheme as above |
| **(iii)** | — | The 11.2 N force may be in either direction, otherwise the same scheme |
| **(iv)** Method (1): Box N2L $\rightarrow$ $105 - T + 11.2 = 8a$; sphere as before. Method (2): $105 + 11.2 - 58.8 = 14a$; giving $a = 4.1$ and $T = 83.4$ | — | Allow 2.5 substituted in box equation to give $T = 96.2$. If the sign convention gives as positive the direction of the sphere descending, $a = -4.1$. Allow substituting $a = 2.5$ in the equations to give $T = 43.8$ (sphere) or $136.2$ (box) |
| **(v)** | — | In (C) allow use of $a = 4.1$ to give time to break as $0.73117\ldots$ s and total time as $1.716\ldots$ s |
**Overall Total: [20]**
2 A box of mass 8 kg slides on a horizontal table against a constant resistance of 11.2 N .
\begin{enumerate}[label=(\roman*)]
\item What horizontal force is applied to the box if it is sliding with acceleration of magnitude $2 \mathrm {~ms} ^ { - 2 }$ ?
Fig. 7 shows the box of mass 8 kg on a long, rough, horizontal table. A sphere of mass 6 kg is attached to the box by means of a light inextensible string that passes over a smooth pulley. The section of the string between the pulley and the box is parallel to the table. The constant frictional force of 11.2 N opposes the motion of the box. A force of 105 N parallel to the table acts on the box in the direction shown, and the acceleration of the system is in that direction.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{0fbef619-ad15-4e46-be35-e17fed9952c0-2_372_878_870_683}
\captionsetup{labelformat=empty}
\caption{Fig. 7}
\end{center}
\end{figure}
\item What information in the question indicates that while the string is taut the box and sphere have the same acceleration?
\item Draw two separate diagrams, one showing all the horizontal forces acting on the box and the other showing all the forces acting on the sphere.
\item Show that the magnitude of the acceleration of the system is $2.5 \mathrm {~m} \mathrm {~s} ^ { - 2 }$ and find the tension in the string.
The system is stationary when the sphere is at point P . When the sphere is 1.8 m above P the string breaks, leaving the sphere moving upwards at a speed of $3 \mathrm {~m} \mathrm {~s} ^ { - 1 }$.
\item (A) Write down the value of the acceleration of the sphere after the string breaks.\\
(B) The sphere passes through P again at time $T$ seconds after the string breaks. Show that $T$ is the positive root of the equation $4.9 T ^ { 2 } - 3 T - 1.8 = 0$.\\
( $C$ ) Using part ( $B$ ), or otherwise, calculate the total time that elapses after the sphere moves from P before the sphere again passes through P .
\end{enumerate}
\hfill \mbox{\textit{OCR MEI M1 Q2 [21]}}