AQA M2 2010 June — Question 4 12 marks

Exam BoardAQA
ModuleM2 (Mechanics 2)
Year2010
SessionJune
Marks12
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicVariable Force
TypeForce depends on time t
DifficultyStandard +0.3 This is a standard M2 variable force question requiring Newton's second law, integration of trigonometric and polynomial functions, and vector manipulation. While it has multiple parts, each step follows routine procedures: F=ma for acceleration, integration with boundary conditions for velocity, solving when j-component dominates for direction, and finding magnitude. The integration is straightforward (cos and t² terms) with no conceptual surprises, making it slightly easier than average.
Spec1.08d Evaluate definite integrals: between limits3.02f Non-uniform acceleration: using differentiation and integration3.03d Newton's second law: 2D vectors

4 A particle has mass 200 kg and moves on a smooth horizontal plane. A single horizontal force, \(\left( 400 \cos \left( \frac { \pi } { 2 } t \right) \mathbf { i } + 600 t ^ { 2 } \mathbf { j } \right)\) newtons, acts on the particle at time \(t\) seconds. The unit vectors \(\mathbf { i }\) and \(\mathbf { j }\) are directed east and north respectively.
  1. Find the acceleration of the particle at time \(t\).
  2. When \(t = 4\), the velocity of the particle is \(( - 3 \mathbf { i } + 56 \mathbf { j } ) \mathrm { m } \mathrm { s } ^ { - 1 }\). Find the velocity of the particle at time \(t\).
  3. Find \(t\) when the particle is moving due west.
  4. Find the speed of the particle when it is moving due west.
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Question 4:
Part (a)
AnswerMarks Guidance
\(\mathbf{a} = \frac{\mathbf{F}}{m} = \frac{1}{200}\left(400\cos\left(\frac{\pi}{2}t\right)\mathbf{i} + 600t^2\mathbf{j}\right)\)M1 Use of \(F = ma\)
\(\mathbf{a} = \left(2\cos\left(\frac{\pi}{2}t\right)\mathbf{i} + 3t^2\mathbf{j}\right) \text{ m s}^{-2}\)A1
Part (b)
AnswerMarks Guidance
\(\mathbf{v} = \int \mathbf{a} \, dt = \frac{2\sin\left(\frac{\pi}{2}t\right)}{\frac{\pi}{2}}\mathbf{i} + t^3\mathbf{j} + \mathbf{c}\)M1 Integrate acceleration
\(= \frac{4}{\pi}\sin\left(\frac{\pi}{2}t\right)\mathbf{i} + t^3\mathbf{j} + \mathbf{c}\)A1 Correct integration
When \(t=4\): \(-3\mathbf{i} + 56\mathbf{j} = \frac{4}{\pi}\sin(2\pi)\mathbf{i} + 64\mathbf{j} + \mathbf{c}\)M1 Substitute \(t=4\)
\(\mathbf{c} = -3\mathbf{i} - 8\mathbf{j}\)A1
\(\mathbf{v} = \left(\frac{4}{\pi}\sin\left(\frac{\pi}{2}t\right) - 3\right)\mathbf{i} + \left(t^3 - 8\right)\mathbf{j}\)A1
Part (c)
AnswerMarks Guidance
Moving due west: \(\mathbf{j}\) component \(= 0\) and \(\mathbf{i}\) component \(< 0\)M1
\(t^3 - 8 = 0 \Rightarrow t = 2\)A1
Check \(\mathbf{i}\) component: \(\frac{4}{\pi}\sin(\pi) - 3 = -3 < 0\) ✓A1 Confirm moving west
Part (d)
AnswerMarks Guidance
Speed \(= \left\frac{4}{\pi}\sin(\pi) - 3\right =
\(= 3 \text{ m s}^{-1}\)A1
# Question 4:

## Part (a)
| $\mathbf{a} = \frac{\mathbf{F}}{m} = \frac{1}{200}\left(400\cos\left(\frac{\pi}{2}t\right)\mathbf{i} + 600t^2\mathbf{j}\right)$ | M1 | Use of $F = ma$ |
|---|---|---|
| $\mathbf{a} = \left(2\cos\left(\frac{\pi}{2}t\right)\mathbf{i} + 3t^2\mathbf{j}\right) \text{ m s}^{-2}$ | A1 | |

## Part (b)
| $\mathbf{v} = \int \mathbf{a} \, dt = \frac{2\sin\left(\frac{\pi}{2}t\right)}{\frac{\pi}{2}}\mathbf{i} + t^3\mathbf{j} + \mathbf{c}$ | M1 | Integrate acceleration |
|---|---|---|
| $= \frac{4}{\pi}\sin\left(\frac{\pi}{2}t\right)\mathbf{i} + t^3\mathbf{j} + \mathbf{c}$ | A1 | Correct integration |
| When $t=4$: $-3\mathbf{i} + 56\mathbf{j} = \frac{4}{\pi}\sin(2\pi)\mathbf{i} + 64\mathbf{j} + \mathbf{c}$ | M1 | Substitute $t=4$ |
| $\mathbf{c} = -3\mathbf{i} - 8\mathbf{j}$ | A1 | |
| $\mathbf{v} = \left(\frac{4}{\pi}\sin\left(\frac{\pi}{2}t\right) - 3\right)\mathbf{i} + \left(t^3 - 8\right)\mathbf{j}$ | A1 | |

## Part (c)
| Moving due west: $\mathbf{j}$ component $= 0$ and $\mathbf{i}$ component $< 0$ | M1 | |
|---|---|---|
| $t^3 - 8 = 0 \Rightarrow t = 2$ | A1 | |
| Check $\mathbf{i}$ component: $\frac{4}{\pi}\sin(\pi) - 3 = -3 < 0$ ✓ | A1 | Confirm moving west |

## Part (d)
| Speed $= \left|\frac{4}{\pi}\sin(\pi) - 3\right| = |-3| = 3 \text{ m s}^{-1}$ | M1 | Substitute their $t$ |
|---|---|---|
| $= 3 \text{ m s}^{-1}$ | A1 | |

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4 A particle has mass 200 kg and moves on a smooth horizontal plane. A single horizontal force, $\left( 400 \cos \left( \frac { \pi } { 2 } t \right) \mathbf { i } + 600 t ^ { 2 } \mathbf { j } \right)$ newtons, acts on the particle at time $t$ seconds.

The unit vectors $\mathbf { i }$ and $\mathbf { j }$ are directed east and north respectively.
\begin{enumerate}[label=(\alph*)]
\item Find the acceleration of the particle at time $t$.
\item When $t = 4$, the velocity of the particle is $( - 3 \mathbf { i } + 56 \mathbf { j } ) \mathrm { m } \mathrm { s } ^ { - 1 }$.

Find the velocity of the particle at time $t$.
\item Find $t$ when the particle is moving due west.
\item Find the speed of the particle when it is moving due west.\\

\begin{center}
\includegraphics[max width=\textwidth, alt={}]{3ffa0a2b-aa7d-46eb-b92b-3e3ee59f235c-09_2484_1709_223_153}
\end{center}
\end{enumerate}

\hfill \mbox{\textit{AQA M2 2010 Q4 [12]}}