OCR MEI M1 — Question 5 18 marks

Exam BoardOCR MEI
ModuleM1 (Mechanics 1)
Marks18
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicNewton's laws and connected particles
TypeSingle particle, Newton's second law – scalar (1D, horizontal or inclined)
DifficultyModerate -0.3 This is a standard M1 mechanics question covering Newton's second law with constant acceleration in multiple scenarios. All parts use routine SUVAT equations and F=ma with straightforward arithmetic. Part (i) is a 'show that' requiring one calculation, parts (ii) and (iii) are direct applications of kinematic equations, and part (iv) requires finding deceleration then time. While multi-part, each step follows textbook methods with no novel problem-solving required, making it slightly easier than average.
Spec3.02d Constant acceleration: SUVAT formulae3.03d Newton's second law: 2D vectors3.03f Weight: W=mg3.03i Normal reaction force3.03v Motion on rough surface: including inclined planes

5 Fig. 8.1 shows a sledge of mass 40 kg . It is being pulled across a horizontal surface of deep snow by a light horizontal rope. There is a constant resistance to its motion. The tension in the rope is 120 N . \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{9bff41e0-7be0-4932-ae50-a612abb3fe19-5_125_852_391_638} \captionsetup{labelformat=empty} \caption{Fig. 8.1}
\end{figure} The sledge is initially at rest. After 10 seconds its speed is \(5 \mathrm {~ms} ^ { - 1 }\).
  1. Show that the resistance to motion is 100 N . When the speed of the sledge is \(5 \mathrm {~m} \mathrm {~s} ^ { - 1 }\), the rope breaks.
    The resistance to motion remains 100 N .
  2. Find the speed of the sledge
    (A) 1.6 seconds after the rope breaks,
    (B) 6 seconds after the rope breaks. The sledge is then pushed to the bottom of a ski slope. This is a plane at an angle of \(15 ^ { \circ }\) to the horizontal. \begin{figure}[h]
    \includegraphics[alt={},max width=\textwidth]{9bff41e0-7be0-4932-ae50-a612abb3fe19-5_263_854_1391_637} \captionsetup{labelformat=empty} \caption{Fig. 8.2}
    \end{figure} The sledge is attached by a light rope to a winch at the top of the slope. The rope is parallel to the slope and has a constant tension of 200 N . Fig. 8.2 shows the situation when the sledge is part of the way up the slope. The ski slope is smooth.
  3. Show that when the sledge has moved from being at rest at the bottom of the slope to the point when its speed is \(8 \mathrm {~m} \mathrm {~s} ^ { - 1 }\), it has travelled a distance of 13.0 m (to 3 significant figures). When the speed of the sledge is \(8 \mathrm {~ms} ^ { - 1 }\), this rope also breaks.
  4. Find the time between the rope breaking and the sledge reaching the bottom of the slope.

Question 5:
Part (i)
AnswerMarks Guidance
AnswerMarks Guidance
\(v = u + at\)M1 Use of a suitable constant acceleration formula
\(5 = 0 + a \times 10 \Rightarrow a = 0.5\)A1 Note: The value of \(a\) is not required by the question so may be implied by subsequent working
\(F = ma \Rightarrow 120 - R = 40 \times 0.5\)M1 Use of Newton's 2nd Law with correct elements
\(R = 100\text{ N}\)E1
[4]
Part (ii)(A)
AnswerMarks Guidance
AnswerMarks Guidance
\(F = ma \Rightarrow -100 = 40a\)M1 Equation to find \(a\) using Newton's 2nd Law
\(\Rightarrow a = -2.5\)A1
When \(t = 1.6\): \(v = 5 + (-2.5) \times 1.6 = 1\text{ ms}^{-1}\)A1 CAO
[3]
Part (ii)(B)
AnswerMarks Guidance
AnswerMarks Guidance
When \(t = 6\), it is stationary. \(v = 0\text{ ms}^{-1}\)B1
[1]
Part (iii)
AnswerMarks Guidance
AnswerMarks Guidance
Motion parallel to the slope: Component of weight down slope \(= 40g\sin 15°\ (= 101.457...)\)B1
\(200 - 40g\sin 15° = 40a\)M1 Equation of motion with correct elements present. No extra forces.
\(a = 2.463...\) This result is not asked for in the question
\(v^2 - u^2 = 2as \Rightarrow 8^2 = 2 \times 2.46... \times s\)M1 Use of a suitable constant acceleration formula, or combination of formulae. Dependent on previous M1.
\(\Rightarrow s = 12.989...\) rounding to \(13.0\text{ m}\)E1 Note: If rounding is not shown for \(s\), the acceleration must satisfy \(2.452... < a < 2.471...\)
[4]
Part (iv)
AnswerMarks Guidance
AnswerMarks Guidance
Let \(a\) be acceleration up the slope
\(-40 \times 9.8 \times \sin 15° = 40a\)M1 Use of Newton's 2nd Law parallel to the slope
\(a = -2.536...\), i.e. \(2.536\text{ ms}^{-2}\) down the slopeA1 Condone sign error
\(s = ut + \frac{1}{2}at^2\)
\(-12.989... = 8t + \frac{1}{2} \times (-2.536...)t^2\)M1 Dependent on previous M1. Use of a suitable constant acceleration formula (or combination) in a relevant manner.
\(1.268...t^2 - 8t - 12.989... = 0\)A1 Signs must be correct
\(t = \dfrac{8 \pm \sqrt{64 - 4 \times 1.268... \times (-12.989...)}}{2 \times 1.268...}\)M1 Attempt to solve a relevant three-term quadratic equation
\(t = -1.339...\) or \(7.647...\), so \(t = 7.65\) secondsA1
[6]
Alternative 2-stage method for Part (iv):
AnswerMarks Guidance
AnswerMarks Guidance
\(-40 \times 9.8 \times \sin 15° = 40a \Rightarrow a = -2.536...\)M1, A1 Use of Newton's 2nd Law parallel to slope; condone sign error
\(v = u + at \Rightarrow 0 = 8 - 2.536...t \Rightarrow t = 3.154...\)M1, A1 Use of suitable constant acceleration formula for either \(t\) or \(s\)
\(s = 8 \times 3.154... - \frac{1}{2} \times 2.536... \times 3.154...^2 \Rightarrow s = 12.616...\)
Distance to bottom \(= 12.989... + 12.616... = 25.605...\)
\(s = ut + \frac{1}{2}at^2 \Rightarrow 25.605... = \frac{1}{2} \times 2.536... \times t^2\)M1 Use of a suitable constant acceleration formula
\(t = 4.493...\)
Total time \(= 3.154... + 4.493... = 7.647...\text{ s}\)A1
## Question 5:

### Part (i)

| Answer | Marks | Guidance |
|--------|-------|----------|
| $v = u + at$ | M1 | Use of a suitable constant acceleration formula |
| $5 = 0 + a \times 10 \Rightarrow a = 0.5$ | A1 | Note: The value of $a$ is not required by the question so may be implied by subsequent working |
| $F = ma \Rightarrow 120 - R = 40 \times 0.5$ | M1 | Use of Newton's 2nd Law with correct elements |
| $R = 100\text{ N}$ | E1 | |
| **[4]** | | |

### Part (ii)(A)

| Answer | Marks | Guidance |
|--------|-------|----------|
| $F = ma \Rightarrow -100 = 40a$ | M1 | Equation to find $a$ using Newton's 2nd Law |
| $\Rightarrow a = -2.5$ | A1 | |
| When $t = 1.6$: $v = 5 + (-2.5) \times 1.6 = 1\text{ ms}^{-1}$ | A1 | CAO |
| **[3]** | | |

### Part (ii)(B)

| Answer | Marks | Guidance |
|--------|-------|----------|
| When $t = 6$, it is stationary. $v = 0\text{ ms}^{-1}$ | B1 | |
| **[1]** | | |

### Part (iii)

| Answer | Marks | Guidance |
|--------|-------|----------|
| Motion parallel to the slope: Component of weight down slope $= 40g\sin 15°\ (= 101.457...)$ | B1 | |
| $200 - 40g\sin 15° = 40a$ | M1 | Equation of motion with correct elements present. No extra forces. |
| $a = 2.463...$ | | This result is not asked for in the question |
| $v^2 - u^2 = 2as \Rightarrow 8^2 = 2 \times 2.46... \times s$ | M1 | Use of a suitable constant acceleration formula, or combination of formulae. Dependent on previous M1. |
| $\Rightarrow s = 12.989...$ rounding to $13.0\text{ m}$ | E1 | Note: If rounding is not shown for $s$, the acceleration must satisfy $2.452... < a < 2.471...$ |
| **[4]** | | |

### Part (iv)

| Answer | Marks | Guidance |
|--------|-------|----------|
| Let $a$ be acceleration up the slope | | |
| $-40 \times 9.8 \times \sin 15° = 40a$ | M1 | Use of Newton's 2nd Law parallel to the slope |
| $a = -2.536...$, i.e. $2.536\text{ ms}^{-2}$ down the slope | A1 | Condone sign error |
| $s = ut + \frac{1}{2}at^2$ | | |
| $-12.989... = 8t + \frac{1}{2} \times (-2.536...)t^2$ | M1 | Dependent on previous M1. Use of a suitable constant acceleration formula (or combination) in a relevant manner. |
| $1.268...t^2 - 8t - 12.989... = 0$ | A1 | Signs must be correct |
| $t = \dfrac{8 \pm \sqrt{64 - 4 \times 1.268... \times (-12.989...)}}{2 \times 1.268...}$ | M1 | Attempt to solve a relevant three-term quadratic equation |
| $t = -1.339...$ or $7.647...$, so $t = 7.65$ seconds | A1 | |
| **[6]** | | |

**Alternative 2-stage method for Part (iv):**

| Answer | Marks | Guidance |
|--------|-------|----------|
| $-40 \times 9.8 \times \sin 15° = 40a \Rightarrow a = -2.536...$ | M1, A1 | Use of Newton's 2nd Law parallel to slope; condone sign error |
| $v = u + at \Rightarrow 0 = 8 - 2.536...t \Rightarrow t = 3.154...$ | M1, A1 | Use of suitable constant acceleration formula for either $t$ or $s$ |
| $s = 8 \times 3.154... - \frac{1}{2} \times 2.536... \times 3.154...^2 \Rightarrow s = 12.616...$ | | |
| Distance to bottom $= 12.989... + 12.616... = 25.605...$ | | |
| $s = ut + \frac{1}{2}at^2 \Rightarrow 25.605... = \frac{1}{2} \times 2.536... \times t^2$ | M1 | Use of a suitable constant acceleration formula |
| $t = 4.493...$ | | |
| Total time $= 3.154... + 4.493... = 7.647...\text{ s}$ | A1 | |
5 Fig. 8.1 shows a sledge of mass 40 kg . It is being pulled across a horizontal surface of deep snow by a light horizontal rope. There is a constant resistance to its motion.

The tension in the rope is 120 N .

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{9bff41e0-7be0-4932-ae50-a612abb3fe19-5_125_852_391_638}
\captionsetup{labelformat=empty}
\caption{Fig. 8.1}
\end{center}
\end{figure}

The sledge is initially at rest. After 10 seconds its speed is $5 \mathrm {~ms} ^ { - 1 }$.
\begin{enumerate}[label=(\roman*)]
\item Show that the resistance to motion is 100 N .

When the speed of the sledge is $5 \mathrm {~m} \mathrm {~s} ^ { - 1 }$, the rope breaks.\\
The resistance to motion remains 100 N .
\item Find the speed of the sledge\\
(A) 1.6 seconds after the rope breaks,\\
(B) 6 seconds after the rope breaks.

The sledge is then pushed to the bottom of a ski slope. This is a plane at an angle of $15 ^ { \circ }$ to the horizontal.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{9bff41e0-7be0-4932-ae50-a612abb3fe19-5_263_854_1391_637}
\captionsetup{labelformat=empty}
\caption{Fig. 8.2}
\end{center}
\end{figure}

The sledge is attached by a light rope to a winch at the top of the slope. The rope is parallel to the slope and has a constant tension of 200 N . Fig. 8.2 shows the situation when the sledge is part of the way up the slope.

The ski slope is smooth.
\item Show that when the sledge has moved from being at rest at the bottom of the slope to the point when its speed is $8 \mathrm {~m} \mathrm {~s} ^ { - 1 }$, it has travelled a distance of 13.0 m (to 3 significant figures).

When the speed of the sledge is $8 \mathrm {~ms} ^ { - 1 }$, this rope also breaks.
\item Find the time between the rope breaking and the sledge reaching the bottom of the slope.
\end{enumerate}

\hfill \mbox{\textit{OCR MEI M1  Q5 [18]}}