| Exam Board | OCR MEI |
|---|---|
| Module | M1 (Mechanics 1) |
| Marks | 16 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Newton's laws and connected particles |
| Type | Two connected particles, horizontal surface |
| Difficulty | Moderate -0.3 This is a multi-part mechanics question involving equilibrium and Newton's second law with connected particles. Parts (i)-(iii) are straightforward equilibrium problems requiring basic force resolution and Newton's first law. Part (iv) is a standard F=ma calculation. Part (v) appears incomplete but likely asks for acceleration or force in the rod. While it covers multiple scenarios, each individual part uses routine M1 techniques without requiring novel insight, making it slightly easier than average. |
| Spec | 3.03b Newton's first law: equilibrium3.03e Resolve forces: two dimensions3.03m Equilibrium: sum of resolved forces = 03.03r Friction: concept and vector form3.03v Motion on rough surface: including inclined planes |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| 25 N | B1 | Condone no units. Do not accept −25 N |
| [1] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| \(50\cos 25\) | M1 | Attempt to resolve 50 N. Accept \(s \leftrightarrow c\). No extra forces |
| \(= 45.31538\ldots\) so 45.3 N (3 s.f.) | A1 | cao but accept −45.3 |
| [2] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Resolving vertically: \(R + 50\sin 25 - 8 \times 9.8 = 0\) | M1 | All relevant forces with resolution of 50 N. No extras. Accept \(s \leftrightarrow c\) |
| \(R = 57.26908\ldots\) so 57.3 N (3 s.f.) | A1 | All correct |
| A1 | ||
| [3] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Newton's 2nd Law in direction DC: \(50\cos 25 - 20 = 18a\) | M1 | Newton's 2nd Law with \(m=18\). Accept \(F=mga\). Attempt at resolving 50 N. Allow 20 N omitted and \(s \leftrightarrow c\). No extra forces |
| \(a = 1.4064105\ldots\) so 1.41 m s\(^{-2}\) (3 s.f.) | A1 | Allow only sign error and \(s \leftrightarrow c\) |
| A1 | cao | |
| [3] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Resolution of weight down the slope | B1 | \(mg\sin 5°\) where \(m = 8\) or 10 or 18, wherever first seen |
| Either: Newton's 2nd Law down slope overall: \(18 \times 9.8 \times \sin 5° - 20 = 18a\) | 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 |
| \(a = -0.2569\ldots\) | A1 | cao |
| Newton's 2nd Law down slope, force in rod can be taken as tension or thrust. Taking it as tension \(T\) gives: | M1 | \(F=ma\). Must consider 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 |
| 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 |
| \(T = -3.888\ldots = -3.89\) N (3 s.f.) | A1 | If \(T\) taken as thrust, then \(T = +3.89\) |
| The force is a thrust | A1 | Dependent on \(T\) correct |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Newton's 2nd Law down slope, force in rod taken as tension \(T\): | M1 | \(F=ma\). Must consider 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 |
| M1 | \(F=ma\). Must consider motion of 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 | |
| For C: \(8 \times 9.8 \times \sin 5° - 5 + T = 8a\) | A1 | Award for either equation for C or equation for D correct. '\(-T\)' if \(T\) taken as thrust |
| For D: \(10 \times 9.8 \times \sin 5° - 15 - T = 10a\) | ||
| \(a = -0.2569\ldots\), \(T = -3.888\ldots = -3.89\) N (3 s.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 | |
| The force is a thrust | A1 | Dependent on \(T\) correct |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | 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 m s\(^{-1}\) (3 s.f.) | F1 | FT from magnitude of their \(a\) but must be consistent with its direction |
| [9] | ||
| Total [18] |
## Question 3:
### Part (i)
| Answer/Working | Mark | Guidance |
|---|---|---|
| 25 N | B1 | Condone no units. Do not accept −25 N |
| **[1]** | | |
### Part (ii)
| Answer/Working | Mark | Guidance |
|---|---|---|
| $50\cos 25$ | M1 | Attempt to resolve 50 N. Accept $s \leftrightarrow c$. No extra forces |
| $= 45.31538\ldots$ so 45.3 N (3 s.f.) | A1 | cao but accept −45.3 |
| **[2]** | | |
### Part (iii)
| Answer/Working | Mark | Guidance |
|---|---|---|
| Resolving vertically: $R + 50\sin 25 - 8 \times 9.8 = 0$ | M1 | All relevant forces with resolution of 50 N. No extras. Accept $s \leftrightarrow c$ |
| $R = 57.26908\ldots$ so 57.3 N (3 s.f.) | A1 | All correct |
| | A1 | |
| **[3]** | | |
### Part (iv)
| Answer/Working | Mark | Guidance |
|---|---|---|
| Newton's 2nd Law in direction DC: $50\cos 25 - 20 = 18a$ | M1 | Newton's 2nd Law with $m=18$. Accept $F=mga$. Attempt at resolving 50 N. Allow 20 N omitted and $s \leftrightarrow c$. No extra forces |
| $a = 1.4064105\ldots$ so 1.41 m s$^{-2}$ (3 s.f.) | A1 | Allow only sign error and $s \leftrightarrow c$ |
| | A1 | cao |
| **[3]** | | |
### Part (v)
| Answer/Working | Mark | Guidance |
|---|---|---|
| Resolution of weight down the slope | B1 | $mg\sin 5°$ where $m = 8$ or 10 or 18, wherever first seen |
| **Either:** Newton's 2nd Law down slope overall: $18 \times 9.8 \times \sin 5° - 20 = 18a$ | 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 |
| $a = -0.2569\ldots$ | A1 | cao |
| Newton's 2nd Law down slope, force in rod can be taken as tension or thrust. Taking it as tension $T$ gives: | M1 | $F=ma$. Must consider 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 |
| 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 |
| $T = -3.888\ldots = -3.89$ N (3 s.f.) | A1 | If $T$ taken as thrust, then $T = +3.89$ |
| The force is a thrust | A1 | Dependent on $T$ correct |
**Or:**
| Answer/Working | Mark | Guidance |
|---|---|---|
| Newton's 2nd Law down slope, force in rod taken as tension $T$: | M1 | $F=ma$. Must consider 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 |
| | M1 | $F=ma$. Must consider motion of 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 |
| For C: $8 \times 9.8 \times \sin 5° - 5 + T = 8a$ | A1 | Award for either equation for C or equation for D correct. '$-T$' if $T$ taken as thrust |
| For D: $10 \times 9.8 \times \sin 5° - 15 - T = 10a$ | | |
| $a = -0.2569\ldots$, $T = -3.888\ldots = -3.89$ N (3 s.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 |
| The force is a thrust | A1 | Dependent on $T$ correct |
**Then:**
| Answer/Working | Mark | 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 m s$^{-1}$ (3 s.f.) | F1 | FT from magnitude of **their** $a$ but must be consistent with its direction |
| **[9]** | | |
| **Total [18]** | | |
3 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]{f5f9b9b7-6766-4f8e-b011-506051104123-3_249_1096_314_558}
\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]{f5f9b9b7-6766-4f8e-b011-506051104123-3_297_1180_971_741}
\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]{f5f9b9b7-6766-4f8e-b011-506051104123-3_351_1285_2038_466}
\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 PhysicsAptMaths, statter \&REther this rod is in tension or thrust (compression).
\hfill \mbox{\textit{OCR MEI M1 Q3 [16]}}