| Exam Board | OCR MEI |
|---|---|
| Module | M1 (Mechanics 1) |
| Year | 2011 |
| Session | June |
| Marks | 18 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Newton's laws and connected particles |
| Type | Two connected particles, horizontal surface |
| Difficulty | Standard +0.3 This is a multi-part connected particles question with straightforward equilibrium and Newton's second law applications. Parts (i)-(iii) involve basic equilibrium with simple trigonometry, (iv) requires F=ma with resolved forces, and (v) involves motion on a slope. All parts use standard M1 techniques with no novel problem-solving required, making it slightly easier than average. |
| Spec | 3.03d Newton's second law: 2D vectors3.03e Resolve forces: two dimensions3.03m Equilibrium: sum of resolved forces = 03.03r Friction: concept and vector form |
| Answer | Marks | Guidance |
|---|---|---|
| \(25 \text{ N}\) | B1 | Condone no units. Do not accept \(-25 \text{ N}\). |
| 1 |
| Answer | Marks | Guidance |
|---|---|---|
| \(50 \cos 25\) \(= 45.31538\ldots\) so \(45.3 \text{ N}\) (3 s.f.) | M1 | Attempt to resolve 50 N. Accept \(s \leftrightarrow c\). No extra forces. |
| A1 | cao but accept \(= -45.3\). | |
| 2 |
| Answer | Marks | Guidance |
|---|---|---|
| Resolving vertically | M1 | All relevant forces with resolution of 50 N. No extras. Accept \(s \leftrightarrow c\). |
| \(R + 50 \sin 25 - 8 \times 9.8 = 0\) | A1 | All correct. |
| \(R = 57.26908\ldots\) so \(57.3 \text{ N}\) (3 s.f.) | A1 | |
| 3 |
| Answer | Marks | Guidance |
|---|---|---|
| Newton's 2nd Law in direction DC | M1 | Newton's 2nd Law with \(m = 18\). Accept \(F = ma\). Attempt at resolving 50 N. Allow 20 N omitted and \(s \leftrightarrow c\). No extra forces. |
| \(50\cos 25 - 20 = 18a\) | A1 | Allow only sign error and \(s \leftrightarrow c\). |
| \(a = 1.4064105\ldots\) so \(1.41 \text{ m s}^{-2}\) (3 s.f.) | A1 | cao |
| 3 |
| Answer | Marks | Guidance |
|---|---|---|
| Resolution of weight down the slope | B1 | \(mg\sin 5°\) where \(m = 8\) or 10 or 18, whichever first seen |
| Answer | Marks | Guidance |
|---|---|---|
| Newton's 2nd Law down slope overall | M1 | \(F = ma\). Must have 20 N and \(m = 18\). Allow weight not resolved and use of mass. Accept \(s \leftrightarrow c\) and sign errors (including inconsistency between the 15 N and the 5 N). |
| \(18 \times 9.8 \times \sin 5 - 20 = 18a\) | A1 | cao |
| Newton's 2nd Law down slope. Force in rod can be taken as tension or thrust. Taking it as tension | M1 | \(F = ma\). Must consider the motion of either C or D and include: component of weight, resistance and \(T\). No extra forces. Condone sign errors and \(s \leftrightarrow c\). Do not condone inconsistent value of mass. |
| \(T\) gives | ||
| For D: \(10 \times 9.8 \times \sin 5 - 15 - T = 10a\) | ||
| (For C: \(8 \times 9.8 \times \sin 5 - 5 + T = 8a\)) | F1 | FT only applies to \(a\), and only if direction is consistent. '+T' if \(T\) taken as a thrust. '-T' if \(T\) taken as a thrust |
| \(T = -3.888\ldots = -3.89 \text{ N}\) (3 s.f.) | A1 | If \(T\) taken as thrust, then \(T = +3.89\). Dependent on \(T\) correct |
| The force is a thrust | A1 |
| Answer | Marks | Guidance |
|---|---|---|
| Newton's 2nd Law down slope. Force in rod can be taken as tension or thrust. Taking it as tension | M1 | \(F = ma\). Must consider the motion of C and include: component of weight, resistance and \(T\). No extra forces. Condone sign errors and \(s \leftrightarrow c\). Do not condone inconsistent value of mass. |
| \(T\) gives | ||
| For C: \(8 \times 9.8 \times \sin 5 - 5 + T = 8a\) | ||
| \(a = -0.2569\ldots\), \(T = -3.888\ldots = -3.89 \text{ N}\) (3s.f.) | A1 | First of \(a\) and \(T\) found is correct. If \(T\) taken as thrust, then \(T = +3.89\). |
| F1 | The second of \(a\) and \(T\) found is FT. Award for either the equation for C or the equation for D correct. '-T' if \(T\) taken as a thrust. '+T' if \(T\) taken as a thrust | |
| A1 | Dependent on \(T\) correct |
| Answer | Marks | Guidance |
|---|---|---|
| After 2 s: \(v = 3 + 2 \times a\) | M1 | Allow sign of \(a\) not followed. FT their value of \(a\). Allow change to correct sign of \(a\) at this stage. |
| \(v = 2.4860303\ldots\) so \(2.49 \text{ m s}^{-1}\) (3 s.f.) | F1 | FT from magnitude of their \(a\) but must be consistent with its direction. |
| 9 | ||
| 18 |
**(i)**
$25 \text{ N}$ | B1 | Condone no units. Do not accept $-25 \text{ N}$.
| | 1 |
**(ii)**
$50 \cos 25$ $= 45.31538\ldots$ so $45.3 \text{ N}$ (3 s.f.) | M1 | Attempt to resolve 50 N. Accept $s \leftrightarrow c$. No extra forces.
| A1 | cao but accept $= -45.3$.
| | 2 |
**(iii)**
Resolving vertically | M1 | All relevant forces with resolution of 50 N. No extras. Accept $s \leftrightarrow c$.
$R + 50 \sin 25 - 8 \times 9.8 = 0$ | A1 | All correct.
$R = 57.26908\ldots$ so $57.3 \text{ N}$ (3 s.f.) | A1 |
| | 3 |
**(iv)**
Newton's 2nd Law in direction DC | M1 | Newton's 2nd Law with $m = 18$. Accept $F = ma$. Attempt at resolving 50 N. Allow 20 N omitted and $s \leftrightarrow c$. No extra forces.
$50\cos 25 - 20 = 18a$ | A1 | Allow only sign error and $s \leftrightarrow c$.
$a = 1.4064105\ldots$ so $1.41 \text{ m s}^{-2}$ (3 s.f.) | A1 | cao
| | 3 |
**Q8 continued**
**(v)**
Resolution of weight down the slope | B1 | $mg\sin 5°$ where $m = 8$ or 10 or 18, whichever first seen
**either**
Newton's 2nd Law down slope overall | M1 | $F = ma$. Must have 20 N and $m = 18$. Allow weight not resolved and use of mass. Accept $s \leftrightarrow c$ and sign errors (including inconsistency between the 15 N and the 5 N).
$18 \times 9.8 \times \sin 5 - 20 = 18a$ | A1 | cao
Newton's 2nd Law down slope. Force in rod can be taken as tension or thrust. Taking it as tension | M1 | $F = ma$. Must consider the motion of either C or D and include: component of weight, resistance and $T$. No extra forces. Condone sign errors and $s \leftrightarrow c$. Do not condone inconsistent value of mass.
$T$ gives | | |
For D: $10 \times 9.8 \times \sin 5 - 15 - T = 10a$ | | |
(For C: $8 \times 9.8 \times \sin 5 - 5 + T = 8a$) | F1 | FT only applies to $a$, and only if direction is consistent. '+T' if $T$ taken as a thrust. '-T' if $T$ taken as a thrust
$T = -3.888\ldots = -3.89 \text{ N}$ (3 s.f.) | A1 | If $T$ taken as thrust, then $T = +3.89$. Dependent on $T$ correct
The force is a thrust | A1 |
**or**
Newton's 2nd Law down slope. Force in rod can be taken as tension or thrust. Taking it as tension | M1 | $F = ma$. Must consider the motion of C and include: component of weight, resistance and $T$. No extra forces. Condone sign errors and $s \leftrightarrow c$. Do not condone inconsistent value of mass.
$T$ gives | | |
For C: $8 \times 9.8 \times \sin 5 - 5 + T = 8a$ | | |
$a = -0.2569\ldots$, $T = -3.888\ldots = -3.89 \text{ N}$ (3s.f.) | A1 | First of $a$ and $T$ found is correct. If $T$ taken as thrust, then $T = +3.89$.
| F1 | The second of $a$ and $T$ found is FT. Award for either the equation for C or the equation for D correct. '-T' if $T$ taken as a thrust. '+T' if $T$ taken as a thrust
| A1 | Dependent on $T$ correct
**then**
After 2 s: $v = 3 + 2 \times a$ | M1 | Allow sign of $a$ not followed. FT their value of $a$. Allow change to correct sign of $a$ at this stage.
$v = 2.4860303\ldots$ so $2.49 \text{ m s}^{-1}$ (3 s.f.) | F1 | FT from magnitude of their $a$ but must be consistent with its direction.
| | 9 |
| | 18 |
8 A trolley C of mass 8 kg with rusty axle bearings is initially at rest on a horizontal floor.\\
The trolley stays at rest when it is pulled by a horizontal string with tension 25 N , as shown in Fig. 8.1.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{2efbb554-fe60-42ce-9213-8c66bfdb1d85-5_255_1097_397_523}
\captionsetup{labelformat=empty}
\caption{Fig. 8.1}
\end{center}
\end{figure}
(i) State the magnitude of the horizontal resistance opposing the pull.
A second trolley D of mass 10 kg is connected to trolley C by means of a light, horizontal rod.\\
The string now has tension 50 N , and is at an angle of $25 ^ { \circ }$ to the horizontal, as shown in Fig. 8.2. The two trolleys stay at rest.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{2efbb554-fe60-42ce-9213-8c66bfdb1d85-5_305_1191_1050_701}
\captionsetup{labelformat=empty}
\caption{Fig. 8.2}
\end{center}
\end{figure}
(ii) Calculate the magnitude of the total horizontal resistance acting on the two trolleys opposing the pull.\\
(iii) Calculate the normal reaction of the floor on trolley C .
The axle bearings of the trolleys are oiled and the total horizontal resistance to the motion of the two trolleys is now 20 N . The two trolleys are still pulled by the string with tension 50 N , as shown in Fig. 8.2.\\
(iv) Calculate the acceleration of the trolleys.
In a new situation, the trolleys are on a slope at $5 ^ { \circ }$ to the horizontal and are initially travelling down the slope at $3 \mathrm {~m} \mathrm {~s} ^ { - 1 }$. The resistances are 15 N to the motion of D and 5 N to the motion of C . There is no string attached. The rod connecting the trolleys is parallel to the slope. This situation is shown in Fig. 8.3.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{2efbb554-fe60-42ce-9213-8c66bfdb1d85-5_355_1294_2156_429}
\captionsetup{labelformat=empty}
\caption{Fig. 8.3}
\end{center}
\end{figure}
(v) Calculate the speed of the trolleys after 2 seconds and also the force in the rod connecting the trolleys, stating whether this rod is in tension or thrust (compression).
\hfill \mbox{\textit{OCR MEI M1 2011 Q8 [18]}}