AQA M2 2008 June — Question 5 12 marks

Exam BoardAQA
ModuleM2 (Mechanics 2)
Year2008
SessionJune
Marks12
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 1
TypePosition vector circular motion
DifficultyModerate -0.3 This is a structured multi-part question on circular motion that systematically guides students through standard differentiation and verification steps. While it requires multiple techniques (differentiation of trig functions, magnitude calculations, proving circular motion), each part is routine for M2 level with clear signposting, making it slightly easier than average overall.
Spec3.02a Kinematics language: position, displacement, velocity, acceleration6.05a Angular velocity: definitions6.05b Circular motion: v=r*omega and a=v^2/r

5 A particle moves on a horizontal plane in which the unit vectors \(\mathbf { i }\) and \(\mathbf { j }\) are directed east and north respectively. At time \(t\) seconds, the particle's position vector, \(\mathbf { r }\) metres, is given by $$\mathbf { r } = 8 \left( \cos \frac { 1 } { 4 } t \right) \mathbf { i } - 8 \left( \sin \frac { 1 } { 4 } t \right) \mathbf { j }$$
  1. Find an expression for the velocity of the particle at time \(t\).
  2. Show that the speed of the particle is a constant.
  3. Prove that the particle is moving in a circle.
  4. Find the angular speed of the particle.
  5. Find an expression for the acceleration of the particle at time \(t\).
  6. State the magnitude of the acceleration of the particle.

Part (a)
AnswerMarks Guidance
\(v = \frac{dr}{dt}\), \(v = -2\sin\frac{1}{4}ti - 2\cos\frac{1}{4}tj\)M1 A1 2 marks
Part (b)
AnswerMarks Guidance
Speed is \(\{(-2\sin\frac{1}{4}t)^2 + (-2\cos\frac{1}{4}t)^2\}^{\frac{1}{2}} = 2(\sin^2\frac{1}{4}t + \cos^2\frac{1}{4}t)^{\frac{1}{2}} = 2\) (constant)M1 m1 A1 3 marks
Part (c)
AnswerMarks Guidance
Magnitude of \(r\) is \(\{(8\cos\frac{1}{4}t)^2 + (8\sin\frac{1}{4}t)^2\}^{\frac{1}{2}} = 8\) (constant). Particle is moving in a circleM1 A1 2 marks
Part (d)
AnswerMarks Guidance
Using \(v = a\omega\), Angular speed is 0.25M1 A1 2 marks
Part (e)
AnswerMarks Guidance
\(a = -\frac{1}{2}\cos\frac{1}{4}ti + \frac{1}{2}\sin\frac{1}{4}tj\)M1 A1 2 marks
Part (f)
AnswerMarks Guidance
Magnitude of acceleration is \(\frac{1}{2}\)B1 1 mark
Total: 12 marks
**Part (a)**
$v = \frac{dr}{dt}$, $v = -2\sin\frac{1}{4}ti - 2\cos\frac{1}{4}tj$ | M1 A1 | 2 marks | No i, j: no marks

**Part (b)**
Speed is $\{(-2\sin\frac{1}{4}t)^2 + (-2\cos\frac{1}{4}t)^2\}^{\frac{1}{2}} = 2(\sin^2\frac{1}{4}t + \cos^2\frac{1}{4}t)^{\frac{1}{2}} = 2$ (constant) | M1 m1 A1 | 3 marks | Clear use of $\sin^2\theta + \cos^2\theta = 1$. Use of 2 values SC1

**Part (c)**
Magnitude of $r$ is $\{(8\cos\frac{1}{4}t)^2 + (8\sin\frac{1}{4}t)^2\}^{\frac{1}{2}} = 8$ (constant). Particle is moving in a circle | M1 A1 | 2 marks | $a = -kr \Rightarrow$ circle SC2

**Part (d)**
Using $v = a\omega$, Angular speed is 0.25 | M1 A1 | 2 marks | M1 for their $\frac{b}{c}$ if both found

**Part (e)**
$a = -\frac{1}{2}\cos\frac{1}{4}ti + \frac{1}{2}\sin\frac{1}{4}tj$ | M1 A1 | 2 marks

**Part (f)**
Magnitude of acceleration is $\frac{1}{2}$ | B1 | 1 mark

**Total: 12 marks**

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5 A particle moves on a horizontal plane in which the unit vectors $\mathbf { i }$ and $\mathbf { j }$ are directed east and north respectively.

At time $t$ seconds, the particle's position vector, $\mathbf { r }$ metres, is given by

$$\mathbf { r } = 8 \left( \cos \frac { 1 } { 4 } t \right) \mathbf { i } - 8 \left( \sin \frac { 1 } { 4 } t \right) \mathbf { j }$$
\begin{enumerate}[label=(\alph*)]
\item Find an expression for the velocity of the particle at time $t$.
\item Show that the speed of the particle is a constant.
\item Prove that the particle is moving in a circle.
\item Find the angular speed of the particle.
\item Find an expression for the acceleration of the particle at time $t$.
\item State the magnitude of the acceleration of the particle.
\end{enumerate}

\hfill \mbox{\textit{AQA M2 2008 Q5 [12]}}