Challenging +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.
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]
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]}}