CAIE Further Paper 3 2023 June — Question 1 4 marks

Exam BoardCAIE
ModuleFurther Paper 3 (Further Paper 3)
Year2023
SessionJune
Marks4
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 2
TypeVertical circle: string becomes slack
DifficultyChallenging +1.2 This is a standard vertical circular motion problem requiring energy conservation and the condition for string going slack (tension = 0). While it involves multiple steps (energy equation, centripetal force equation, eliminating velocity, solving for cos θ), the approach is methodical and well-practiced in Further Maths. The given cos α = 3/5 simplifies calculations. Slightly above average difficulty due to the algebraic manipulation required and being a Further Maths topic.
Spec6.02i Conservation of energy: mechanical energy principle6.05e Radial/tangential acceleration

A particle \(P\) of mass \(m\) is attached to one end of a light inextensible string of length \(a\). The other end of the string is attached to a fixed point \(O\). The particle \(P\) is held at the point \(A\), where \(OA\) makes an angle \(\alpha\) with the downward vertical through \(O\), and with the string taut. The particle \(P\) is projected perpendicular to \(OA\) in an upwards direction with speed \(\sqrt{3ag}\). It then starts to move along a circular path in a vertical plane. The string goes slack when \(P\) is at \(B\), where \(OB\) makes an angle \(\theta\) with the upward vertical. Given that \(\cos \alpha = \frac{3}{5}\), find the value of \(\cos \theta\). [4]

Question 1:
AnswerMarks
11 1
m.3ag mv2 mgacoscos
AnswerMarks Guidance
2 2M1 Energy equation, 4 terms, dimensionally correct,
mass must be present, allow sign errors, allow sin in
both terms on RHS
mv2
mgcos
AnswerMarks Guidance
aB1 N2L, may include tension initially but not awarded
until tension = 0 used
3 1 4 
mag m.agcosmga cos
 
2 2 5 
3 7
cos
AnswerMarks Guidance
2 10M1 Dependent on tension = 0 and on an energy
equation, eliminate v2.
7
cos
AnswerMarks Guidance
15A1 If no m in energy equation and no further errors,
award SCB2 for correct final answer
4
AnswerMarks Guidance
QuestionAnswer Marks
Question 1:
1 | 1 1
m.3ag mv2 mgacoscos
2 2 | M1 | Energy equation, 4 terms, dimensionally correct,
mass must be present, allow sign errors, allow sin in
both terms on RHS
mv2
mgcos
a | B1 | N2L, may include tension initially but not awarded
until tension = 0 used
3 1 4 
mag m.agcosmga cos
 
2 2 5 
3 7
cos
2 10 | M1 | Dependent on tension = 0 and on an energy
equation, eliminate v2.
7
cos
15 | A1 | If no m in energy equation and no further errors,
award SCB2 for correct final answer
4
Question | Answer | Marks | Guidance
A particle $P$ of mass $m$ is attached to one end of a light inextensible string of length $a$. The other end of the string is attached to a fixed point $O$. The particle $P$ is held at the point $A$, where $OA$ makes an angle $\alpha$ with the downward vertical through $O$, and with the string taut. The particle $P$ is projected perpendicular to $OA$ in an upwards direction with speed $\sqrt{3ag}$. It then starts to move along a circular path in a vertical plane. The string goes slack when $P$ is at $B$, where $OB$ makes an angle $\theta$ with the upward vertical.

Given that $\cos \alpha = \frac{3}{5}$, find the value of $\cos \theta$. [4]

\hfill \mbox{\textit{CAIE Further Paper 3 2023 Q1 [4]}}