CAIE Further Paper 3 2022 June — Question 2 5 marks

Exam BoardCAIE
ModuleFurther Paper 3 (Further Paper 3)
Year2022
SessionJune
Marks5
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 2
TypeVertical circle: string becomes slack
DifficultyChallenging +1.2 This is a standard circular motion problem requiring energy conservation and the slack-string condition (tension = 0). While it involves multiple steps (energy equation, centripetal force equation, solving simultaneously), the approach is methodical and well-practiced in Further Maths. The algebraic manipulation is moderate, making it above average but not exceptionally challenging for Further Maths students.
Spec6.02i Conservation of energy: mechanical energy principle6.05f Vertical circle: motion including free fall

One end of a light inextensible string of length \(a\) is attached to a fixed point \(O\). A particle of mass \(m\) is attached to the other end of the string. The particle is held at the point \(A\) with the string taut. The angle between \(OA\) and the downward vertical is equal to \(\alpha\), where \(\cos \alpha = \frac{4}{5}\). The particle is projected from \(A\), perpendicular to the string in an upwards direction, with a speed \(\sqrt{3ga}\). It then moves along a circular path in a vertical plane. The string first goes slack when it makes an angle \(\theta\) with the upward vertical through \(O\). Find the value of \(\cos \theta\). [5]

Question 2:
AnswerMarks
21 1
 mv2  m3gamgacoscos
AnswerMarks Guidance
2 2M1 A1 Energy equation.
m
T mgcos v2
AnswerMarks Guidance
aB1 N2L
4
agcos3ga2gacos2ga
AnswerMarks Guidance
5M1 Combine to find cos.
7
cos
AnswerMarks
15A1
5
AnswerMarks Guidance
QuestionAnswer Marks
Question 2:
2 | 1 1
 mv2  m3gamgacoscos
2 2 | M1 A1 | Energy equation.
m
T mgcos v2
a | B1 | N2L
4
agcos3ga2gacos2ga
5 | M1 | Combine to find cos.
7
cos
15 | A1
5
Question | Answer | Marks | Guidance
One end of a light inextensible string of length $a$ is attached to a fixed point $O$. A particle of mass $m$ is attached to the other end of the string. The particle is held at the point $A$ with the string taut. The angle between $OA$ and the downward vertical is equal to $\alpha$, where $\cos \alpha = \frac{4}{5}$. The particle is projected from $A$, perpendicular to the string in an upwards direction, with a speed $\sqrt{3ga}$. It then moves along a circular path in a vertical plane. The string first goes slack when it makes an angle $\theta$ with the upward vertical through $O$.

Find the value of $\cos \theta$. [5]

\hfill \mbox{\textit{CAIE Further Paper 3 2022 Q2 [5]}}