AQA M2 2015 June — Question 4 10 marks

Exam BoardAQA
ModuleM2 (Mechanics 2)
Year2015
SessionJune
Marks10
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 1
TypeTwo strings, two fixed points
DifficultyStandard +0.3 This is a standard M2 circular motion problem with two strings. Part (a) requires resolving vertically (straightforward equilibrium), part (b) involves resolving horizontally and algebraic manipulation to reach a given answer, and part (c) solves simultaneous equations. While it requires careful resolution of forces and understanding of circular motion, it follows a well-established method with no novel insight needed. Slightly easier than average due to the structured parts and 'show that' guidance.
Spec3.03n Equilibrium in 2D: particle under forces6.05b Circular motion: v=r*omega and a=v^2/r6.05c Horizontal circles: conical pendulum, banked tracks

4 A particle, \(P\), of mass 5 kg is attached to two light inextensible strings, \(A P\) and \(B P\). The other ends of the strings are attached to the fixed points \(A\) and \(B\). The point \(A\) is vertically above the point \(B\). The particle moves at a constant speed, \(v \mathrm {~m} \mathrm {~s} ^ { - 1 }\), in a horizontal circle of radius 0.6 metres with centre \(B\). The string \(A P\) is inclined at \(20 ^ { \circ }\) to the vertical, as shown in the diagram. Both strings are taut when the particle is moving. \includegraphics[max width=\textwidth, alt={}, center]{691c50b4-50b2-4e3a-a7e0-60f8ec35ee3c-08_835_568_568_719}
  1. Find the tension in the string \(A P\).
  2. The speed of the particle is \(v \mathrm {~m} \mathrm {~s} ^ { - 1 }\). Show that the tension, \(T _ { B P }\), in the string \(B P\) is given by $$T _ { B P } = \frac { 25 } { 3 } v ^ { 2 } - 5 g \tan 20 ^ { \circ }$$
  3. Find \(v\) when the tensions in the two strings are equal.

Question 4:
Part (a)
AnswerMarks Guidance
Answer/WorkingMarks Guidance
Resolving vertically: \(T_{AP}\cos 20° = 5g\)M1 Resolving vertically with \(T_{AP}\)
\(T_{AP} = \frac{5g}{\cos 20°}\)A1 Correct equation
\(T_{AP} = 52.3\) NA1 cao
Part (b)
AnswerMarks Guidance
Answer/WorkingMarks Guidance
Horizontal equation: \(T_{AP}\sin 20° - T_{BP} = \frac{mv^2}{r} = \frac{5v^2}{0.6}\)M1 Applying Newton's second law horizontally
\(T_{BP} = T_{AP}\sin 20° - \frac{5v^2}{0.6}\)A1 Correct equation
\(T_{BP} = \frac{5g}{\cos 20°}\sin 20° - \frac{25v^2}{3} = 5g\tan 20° - \frac{25}{3}v^2\)A1 Correctly shown (given result)
Part (c)
AnswerMarks Guidance
Answer/WorkingMarks Guidance
Setting \(T_{AP} = T_{BP}\): \(\frac{5g}{\cos 20°} = \frac{25}{3}v^2 - 5g\tan 20°\)M1 Equating the two tensions
\(\frac{5g}{\cos 20°} + 5g\tan 20° = \frac{25}{3}v^2\)M1 Rearranging
\(v^2 = \frac{3}{25}\left(\frac{5g}{\cos 20°} + 5g\tan 20°\right)\)A1 Correct expression
\(v = 2.74\) m s\(^{-1}\)A1 cao
# Question 4:

## Part (a)

| Answer/Working | Marks | Guidance |
|---|---|---|
| Resolving vertically: $T_{AP}\cos 20° = 5g$ | M1 | Resolving vertically with $T_{AP}$ |
| $T_{AP} = \frac{5g}{\cos 20°}$ | A1 | Correct equation |
| $T_{AP} = 52.3$ N | A1 | cao |

## Part (b)

| Answer/Working | Marks | Guidance |
|---|---|---|
| Horizontal equation: $T_{AP}\sin 20° - T_{BP} = \frac{mv^2}{r} = \frac{5v^2}{0.6}$ | M1 | Applying Newton's second law horizontally |
| $T_{BP} = T_{AP}\sin 20° - \frac{5v^2}{0.6}$ | A1 | Correct equation |
| $T_{BP} = \frac{5g}{\cos 20°}\sin 20° - \frac{25v^2}{3} = 5g\tan 20° - \frac{25}{3}v^2$ | A1 | Correctly shown (given result) |

## Part (c)

| Answer/Working | Marks | Guidance |
|---|---|---|
| Setting $T_{AP} = T_{BP}$: $\frac{5g}{\cos 20°} = \frac{25}{3}v^2 - 5g\tan 20°$ | M1 | Equating the two tensions |
| $\frac{5g}{\cos 20°} + 5g\tan 20° = \frac{25}{3}v^2$ | M1 | Rearranging |
| $v^2 = \frac{3}{25}\left(\frac{5g}{\cos 20°} + 5g\tan 20°\right)$ | A1 | Correct expression |
| $v = 2.74$ m s$^{-1}$ | A1 | cao |

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4 A particle, $P$, of mass 5 kg is attached to two light inextensible strings, $A P$ and $B P$. The other ends of the strings are attached to the fixed points $A$ and $B$. The point $A$ is vertically above the point $B$. The particle moves at a constant speed, $v \mathrm {~m} \mathrm {~s} ^ { - 1 }$, in a horizontal circle of radius 0.6 metres with centre $B$. The string $A P$ is inclined at $20 ^ { \circ }$ to the vertical, as shown in the diagram. Both strings are taut when the particle is moving.\\
\includegraphics[max width=\textwidth, alt={}, center]{691c50b4-50b2-4e3a-a7e0-60f8ec35ee3c-08_835_568_568_719}
\begin{enumerate}[label=(\alph*)]
\item Find the tension in the string $A P$.
\item The speed of the particle is $v \mathrm {~m} \mathrm {~s} ^ { - 1 }$.

Show that the tension, $T _ { B P }$, in the string $B P$ is given by

$$T _ { B P } = \frac { 25 } { 3 } v ^ { 2 } - 5 g \tan 20 ^ { \circ }$$
\item Find $v$ when the tensions in the two strings are equal.
\end{enumerate}

\hfill \mbox{\textit{AQA M2 2015 Q4 [10]}}