| Exam Board | OCR MEI |
|---|---|
| Module | M1 (Mechanics 1) |
| Marks | 18 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Forces, equilibrium and resultants |
| Type | Triangle of forces method |
| Difficulty | Standard +0.3 This is a standard M1 statics problem involving triangle of forces and resolving forces in equilibrium. Part (i) requires drawing a force triangle, part (ii) uses basic trigonometry with given values, part (iii) asks for standard equilibrium equations, and part (iv) involves straightforward substitution. All techniques are routine for M1 with no novel problem-solving required, making it slightly easier than average. |
| Spec | 3.03m Equilibrium: sum of resolved forces = 03.03n Equilibrium in 2D: particle under forces |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| Correct triangle of forces shape with \(F\) N, \(250\) N, \(25\) N, angle \(\theta\) | B1 | Shape of triangle; ignore position of \(\theta\) if marked in diagram |
| Correct arrows | B1 | 2 marks -1 per error but penalise no arrows only once and penalise no labels only once. Condone \(T\) written for \(F\). |
| Correct labels | B1 | In the case of a force diagram showing \(F\), \(25\) and \(250\) allow maximum of 2 marks with -1 per error |
| [3] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| \(\tan \alpha = \dfrac{25}{250}\) | M1 | M1 for recognising and using \(\alpha\) in the triangle |
| \(\Rightarrow \alpha = 5.7°\) | A1 | |
| \(F = \sqrt{25^2 + 250^2}\) | M1 | Use of Pythagoras |
| \(F = 251.2\) | A1 | At least 3 significant figures required |
| Distance \(= 30\tan\alpha = 30 \times 0.1 = 3\) m | B1 | CAO |
| [5] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| \(F\cos\theta = 250\), \(F\sin\theta = 25\), \(\tan\theta = \dfrac{25}{250}\) | M1 | |
| \(\Rightarrow \theta = 5.7°\) | A1 | |
| \(F\cos 5.7° = 250\) | M1 | |
| \(F = 251.2\) | A1 | At least 3 significant figures required |
| Distance \(= 30\tan\alpha = 30 \times 0.1 = 3\) m | B1 | CAO |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| Vertical equilibrium: \(S\cos\alpha = T\cos\beta + 250\) | M1, A1 | M1 for attempt at resolution in an equation involving both \(S\) and \(T\); condone sin-cos errors for the M mark only |
| Horizontal equilibrium: \(S\sin\alpha = T\sin\beta\) | A1 | |
| [3] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| \(S\sin 8.5° = T\sin 35° \Rightarrow S = 3.8805T\) | M1 | Using one equation to make \(S\) or \(T\) the subject in terms of the other |
| \((3.8805T)\cos 8.5° = T\cos 35° + 250\) | M1 | Substituting in the other equation |
| \(T = 82.8\) | A1 | CAO |
| \(S = 321.4\) | A1 | CAO |
| [4] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| \(S\sin 8.5° - T\sin 35° = 0\) and \(S\cos 8.5° - T\cos 35° = 250\), valid elimination of \(S\) or \(T\) | M1 | Valid method that has eliminated terms in either \(S\) or \(T\) (execution need not be perfect) |
| \(S = 321.4\) | A1 | CAO First answer |
| Substituting in either equation | M1 | Substituting to find the second answer |
| \(T = 82.8\) | A1 | CAO Second answer |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| Drawing and using a triangle of forces, or quoting and using Lami's Theorem | M1 | |
| \(\dfrac{S}{\sin 145°} = \dfrac{T}{\sin 8.5°} = \dfrac{250}{\sin 26.5°}\) | M1 | Correct form of these equations |
| \(S = 321.4\) | A1 | CAO |
| \(T = 82.8\) | A1 | CAO |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| Abi's weight is \(40g = 392\) N | M1 | Consideration of Abi's weight |
| When \(\alpha = 60°\), \(S\cos 60° > 250 \Rightarrow S > 500\) | M1 | Consideration of vertical forces on the object. Condone no mention of Bob's rope |
| The tension in rope A would be greater than Abi's weight and so she would be lifted off the ground | A1 | The argument must be of high quality and must include consideration of the tension in Bob's rope |
| [3] |
| Answer | Marks | Guidance |
|---|---|---|
| Answer | Marks | Guidance |
| If Abi is on the ground, the maximum possible tension in rope A is Abi's weight of \(392\) N | M1 | Consideration of Abi's weight |
| So the maximum upward force on the object is \(392 \times \cos 60° = 192\) N. This is less than the weight of the object, and the tension in Bob's rope is pulling the box down. | M1 | Consideration of vertical forces on the object. Condone no mention of Bob's rope. Or: the box accelerated downwards |
| So Abi would be lifted off the ground | A1 | The argument must be of high quality and must include consideration of the tension in Bob's rope |
## Question 3(i):
| Answer | Marks | Guidance |
|--------|-------|----------|
| Correct triangle of forces shape with $F$ N, $250$ N, $25$ N, angle $\theta$ | B1 | Shape of triangle; ignore position of $\theta$ if marked in diagram |
| Correct arrows | B1 | 2 marks -1 per error but penalise no arrows only once and penalise no labels only once. Condone $T$ written for $F$. |
| Correct labels | B1 | In the case of a force diagram showing $F$, $25$ and $250$ allow maximum of 2 marks with -1 per error |
| [3] | | |
---
## Question 3(ii):
| Answer | Marks | Guidance |
|--------|-------|----------|
| $\tan \alpha = \dfrac{25}{250}$ | M1 | M1 for recognising and using $\alpha$ in the triangle |
| $\Rightarrow \alpha = 5.7°$ | A1 | |
| $F = \sqrt{25^2 + 250^2}$ | M1 | Use of Pythagoras |
| $F = 251.2$ | A1 | At least 3 significant figures required |
| Distance $= 30\tan\alpha = 30 \times 0.1 = 3$ m | B1 | CAO |
| [5] | | |
**Alternative:**
| Answer | Marks | Guidance |
|--------|-------|----------|
| $F\cos\theta = 250$, $F\sin\theta = 25$, $\tan\theta = \dfrac{25}{250}$ | M1 | |
| $\Rightarrow \theta = 5.7°$ | A1 | |
| $F\cos 5.7° = 250$ | M1 | |
| $F = 251.2$ | A1 | At least 3 significant figures required |
| Distance $= 30\tan\alpha = 30 \times 0.1 = 3$ m | B1 | CAO |
---
## Question 3(iii):
| Answer | Marks | Guidance |
|--------|-------|----------|
| Vertical equilibrium: $S\cos\alpha = T\cos\beta + 250$ | M1, A1 | M1 for attempt at resolution in an equation involving both $S$ and $T$; condone sin-cos errors for the M mark only |
| Horizontal equilibrium: $S\sin\alpha = T\sin\beta$ | A1 | |
| [3] | | |
---
## Question 3(iv):
| Answer | Marks | Guidance |
|--------|-------|----------|
| $S\sin 8.5° = T\sin 35° \Rightarrow S = 3.8805T$ | M1 | Using one equation to make $S$ or $T$ the subject in terms of the other |
| $(3.8805T)\cos 8.5° = T\cos 35° + 250$ | M1 | Substituting in the other equation |
| $T = 82.8$ | A1 | CAO |
| $S = 321.4$ | A1 | CAO |
| [4] | | |
**Alternative (linear simultaneous equations):**
| Answer | Marks | Guidance |
|--------|-------|----------|
| $S\sin 8.5° - T\sin 35° = 0$ and $S\cos 8.5° - T\cos 35° = 250$, valid elimination of $S$ or $T$ | M1 | Valid method that has eliminated terms in either $S$ or $T$ (execution need not be perfect) |
| $S = 321.4$ | A1 | CAO First answer |
| Substituting in either equation | M1 | Substituting to find the second answer |
| $T = 82.8$ | A1 | CAO Second answer |
**Alternative (Triangle of forces / Lami's Theorem):**
| Answer | Marks | Guidance |
|--------|-------|----------|
| Drawing and using a triangle of forces, or quoting and using Lami's Theorem | M1 | |
| $\dfrac{S}{\sin 145°} = \dfrac{T}{\sin 8.5°} = \dfrac{250}{\sin 26.5°}$ | M1 | Correct form of these equations |
| $S = 321.4$ | A1 | CAO |
| $T = 82.8$ | A1 | CAO |
---
## Question 3(v):
| Answer | Marks | Guidance |
|--------|-------|----------|
| Abi's weight is $40g = 392$ N | M1 | Consideration of Abi's weight |
| When $\alpha = 60°$, $S\cos 60° > 250 \Rightarrow S > 500$ | M1 | Consideration of vertical forces on the object. Condone no mention of Bob's rope |
| The tension in rope A would be greater than Abi's weight and so she would be lifted off the ground | A1 | The argument must be of high quality and must include consideration of the tension in Bob's rope |
| [3] | | |
**Alternative:**
| Answer | Marks | Guidance |
|--------|-------|----------|
| If Abi is on the ground, the maximum possible tension in rope A is Abi's weight of $392$ N | M1 | Consideration of Abi's weight |
| So the maximum upward force on the object is $392 \times \cos 60° = 192$ N. This is less than the weight of the object, and the tension in Bob's rope is pulling the box down. | M1 | Consideration of vertical forces on the object. Condone no mention of Bob's rope. Or: the box accelerated downwards |
| So Abi would be lifted off the ground | A1 | The argument must be of high quality and must include consideration of the tension in Bob's rope |
3 Abi and Bob are standing on the ground and are trying to raise a small object of weight 250 N to the top of a building. They are using long light ropes. Fig. 7.1 shows the initial situation.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{82f933a6-c17e-4b41-ae2b-3cc9d0ba975c-2_770_1068_368_530}
\captionsetup{labelformat=empty}
\caption{Fig. 7.1}
\end{center}
\end{figure}
Abi pulls vertically downwards on the rope A with a force $F$ N. This rope passes over a small smooth pulley and is then connected to the object. Bob pulls on another rope, B, in order to keep the object away from the side of the building.
In this situation, the object is stationary and in equilibrium. The tension in rope B, which is horizontal, is 25 N . The pulley is 30 m above the object. The part of rope A between the pulley and the object makes an angle $\theta$ with the vertical.\\
(i) Represent the forces acting on the object as a fully labelled triangle of forces.\\
(ii) Find $F$ and $\theta$.
Show that the distance between the object and the vertical section of rope A is 3 m .
Abi then pulls harder and the object moves upwards. Bob adjusts the tension in rope B so that the object moves along a vertical line.
Fig. 7.2 shows the situation when the object is part of the way up. The tension in rope A is $S \mathrm {~N}$ and the tension in rope B is $T \mathrm {~N}$. The ropes make angles $\alpha$ and $\beta$ with the vertical as shown in the diagram. Abi and Bob are taking a rest and holding the object stationary and in equilibrium.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{82f933a6-c17e-4b41-ae2b-3cc9d0ba975c-3_384_357_520_851}
\captionsetup{labelformat=empty}
\caption{Fig. 7.2}
\end{center}
\end{figure}
(iii) Give the equations, involving $S , T , \alpha$ and $\beta$, for equilibrium in the vertical and horizontal directions.\\
(iv) Find the values of $S$ and $T$ when $\alpha = 8.5 ^ { \circ }$ and $\beta = 35 ^ { \circ }$.\\
(v) Abi's mass is 40 kg .
Explain why it is not possible for her to raise the object to a position in which $\alpha = 60 ^ { \circ }$.
\hfill \mbox{\textit{OCR MEI M1 Q3 [18]}}