Edexcel M2 2018 January — Question 6 10 marks

Exam BoardEdexcel
ModuleM2 (Mechanics 2)
Year2018
SessionJanuary
Marks10
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicAdvanced work-energy problems
TypeEngine power on road constant/variable speed
DifficultyStandard +0.3 This is a standard M2 mechanics question involving power-force-velocity relationships and work-energy principle. Part (a) requires applying P=Fv with Newton's second law to find forces, while part (b) uses work-energy principle with given resistance and component of weight down the slope. Both parts follow routine M2 procedures with straightforward arithmetic, making it slightly easier than average A-level difficulty.
Spec6.02i Conservation of energy: mechanical energy principle6.02l Power and velocity: P = Fv

6. A car of mass 800 kg pulls a trailer of mass 300 kg up a straight road which is inclined to the horizontal at an angle \(\alpha\), where \(\sin \alpha = \frac { 1 } { 14 }\). The trailer is attached to the car by a light inextensible towbar which is parallel to the direction of motion of the car. The car's engine works at a constant rate of \(P \mathrm {~kW}\). The non-gravitational resistances to motion are constant and of magnitude 600 N on the car and 200 N on the trailer. At a given instant the car is moving at \(10 \mathrm {~m} \mathrm {~s} ^ { - 1 }\) and is accelerating at \(0.5 \mathrm {~m} \mathrm {~s} ^ { - 2 }\)
  1. Find the value of \(P\). When the car is moving up the road at \(12 \mathrm {~m} \mathrm {~s} ^ { - 1 }\), the towbar breaks. The trailer comes to instantaneous rest after moving a distance \(d\) metres up the road from the point where the towbar broke. The non-gravitational resistance to the motion of the trailer remains constant and of magnitude 200 N .
  2. Find, using the work-energy principle, the value of \(d\).

Question 6(a):
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(F = \frac{1000P}{10}\)M1 Use of \(P = Fv\)
Equation of motionM1 All terms required. Dimensionally correct. Accept separate equations for the car and trailer.
\(F - 300g\sin\alpha - 800g\sin\alpha - 200 - 600 = 1100 \times 0.5\)A1 Unsimplified equation(s) with at most one error
A1Correct unsimplified equation in \(F\) (or \(P\))
\(P = 21.2\)A1 Accept 21. Max. 3 sf
Question 6(b):
AnswerMarks Guidance
Answer/WorkingMark Guidance
Work-energy equation for the trailerM1 The Q requires work-energy. Equation for the trailer, with all terms dimensionally correct. Condone sign errors
\(200d = \frac{1}{2} \cdot 300 \cdot 12^2 - 300dg\sin\alpha\)A1 Unsimplified equation with at most one error
A1Correct unsimplified equation
Solve for \(d\)DM1 Dependent on the previous M1
\(d = 52.7\ \text{(m)}\) or \(53\ \text{(m)}\)A1 Max 3 sf
## Question 6(a):

| Answer/Working | Mark | Guidance |
|---|---|---|
| $F = \frac{1000P}{10}$ | M1 | Use of $P = Fv$ |
| Equation of motion | M1 | All terms required. Dimensionally correct. Accept separate equations for the car and trailer. |
| $F - 300g\sin\alpha - 800g\sin\alpha - 200 - 600 = 1100 \times 0.5$ | A1 | Unsimplified equation(s) with at most one error |
| | A1 | Correct unsimplified equation in $F$ (or $P$) |
| $P = 21.2$ | A1 | Accept 21. Max. 3 sf |

## Question 6(b):

| Answer/Working | Mark | Guidance |
|---|---|---|
| Work-energy equation for the trailer | M1 | The Q requires work-energy. Equation for the trailer, with all terms dimensionally correct. Condone sign errors |
| $200d = \frac{1}{2} \cdot 300 \cdot 12^2 - 300dg\sin\alpha$ | A1 | Unsimplified equation with at most one error |
| | A1 | Correct unsimplified equation |
| Solve for $d$ | DM1 | Dependent on the previous M1 |
| $d = 52.7\ \text{(m)}$ or $53\ \text{(m)}$ | A1 | Max 3 sf |
6. A car of mass 800 kg pulls a trailer of mass 300 kg up a straight road which is inclined to the horizontal at an angle $\alpha$, where $\sin \alpha = \frac { 1 } { 14 }$. The trailer is attached to the car by a light inextensible towbar which is parallel to the direction of motion of the car. The car's engine works at a constant rate of $P \mathrm {~kW}$. The non-gravitational resistances to motion are constant and of magnitude 600 N on the car and 200 N on the trailer.

At a given instant the car is moving at $10 \mathrm {~m} \mathrm {~s} ^ { - 1 }$ and is accelerating at $0.5 \mathrm {~m} \mathrm {~s} ^ { - 2 }$
\begin{enumerate}[label=(\alph*)]
\item Find the value of $P$.

When the car is moving up the road at $12 \mathrm {~m} \mathrm {~s} ^ { - 1 }$, the towbar breaks. The trailer comes to instantaneous rest after moving a distance $d$ metres up the road from the point where the towbar broke. The non-gravitational resistance to the motion of the trailer remains constant and of magnitude 200 N .
\item Find, using the work-energy principle, the value of $d$.\\

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\end{enumerate}

\hfill \mbox{\textit{Edexcel M2 2018 Q6 [10]}}