| Exam Board | CAIE |
|---|---|
| Module | Further Paper 3 (Further Paper 3) |
| Year | 2020 |
| Session | Specimen |
| Marks | 10 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Circular Motion 1 |
| Difficulty | Standard +0.8 Part (a) is a standard conical pendulum problem requiring resolution of forces and circular motion equations (routine for Further Maths). Part (b) is more demanding, requiring energy conservation combined with the condition for string going slack (tension = 0) in vertical circular motion, then solving the resulting equation—this involves multiple concepts and careful algebraic manipulation, placing it moderately above average difficulty. |
| Spec | 6.05c Horizontal circles: conical pendulum, banked tracks6.05d Variable speed circles: energy methods |
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 $O$.
\begin{enumerate}[label=(\alph*)]
\item
\includegraphics{figure_5a}
The particle $P$ moves in a horizontal circle with a constant angular speed $\omega$ with the string inclined at $60°$ to the downward vertical through $O$ (see diagram).
Show that $\omega^2 = \frac{2g}{a}$. [4]
\item The particle now hangs at rest and is then projected horizontally so that it begins to move in a vertical circle with centre $O$. When the string makes an angle $\theta$ with the downward vertical through $O$, the angular speed of $P$ is $\sqrt{\frac{2g}{a}}$. The string first goes slack when $OP$ makes an angle $\theta$ with the upward vertical through $O$.
Find the value of $\cos \theta$. [6]
\end{enumerate}
\hfill \mbox{\textit{CAIE Further Paper 3 2020 Q5 [10]}}