| Exam Board | CAIE |
|---|---|
| Module | Further Paper 3 (Further Paper 3) |
| Year | 2023 |
| Session | November |
| Marks | 11 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Circular Motion 2 |
| Type | Maximum/minimum tension or reaction |
| Difficulty | Challenging +1.8 This is a challenging Further Mechanics problem requiring multiple concepts: conservation of angular momentum about the pivot, energy conservation, circular motion with tension analysis, and the key insight that equal tensions at 60° provides a constraint relating x to a. While systematic, it demands careful coordinate geometry, simultaneous equations, and extended multi-step reasoning across three interconnected parts—significantly harder than standard A-level but not requiring exceptional creativity. |
| Spec | 6.02i Conservation of energy: mechanical energy principle6.05e Radial/tangential acceleration |
| Answer | Marks |
|---|---|
| 6(a) | Angular speeds of P and Q are equal, |
| Answer | Marks |
|---|---|
| x 3a−x | M1 |
| Answer | Marks | Guidance |
|---|---|---|
| Q 3a−x | A1 | Shown convincingly: angular speeds equal stated. |
| Answer | Marks |
|---|---|
| 6(b) | m4ag |
| Answer | Marks |
|---|---|
| 3a−x | B1 |
| Answer | Marks |
|---|---|
| x | B1 |
| Answer | Marks |
|---|---|
| 3a−x x | M1 |
| Answer | Marks | Guidance |
|---|---|---|
| 4a(3a−x)=(3a−x)2+4ax, x2 +2ax−3a2 =0 | M1 | Solve to find x. |
| Answer | Marks |
|---|---|
| (x−a)(x+3a)=0, x=a | A1 |
| Answer | Marks | Guidance |
|---|---|---|
| Question | Answer | Marks |
| Answer | Marks |
|---|---|
| 6(c) | Energy changes from initial position: |
| Answer | Marks | Guidance |
|---|---|---|
| 2 | B1 | KEs correct. |
| B1FT | GPEs correct. |
| Answer | Marks | Guidance |
|---|---|---|
| | M1 | Energy equation. |
| Answer | Marks | Guidance |
|---|---|---|
| 5 5 | A1 | AEF |
Question 6:
--- 6(a) ---
6(a) | Angular speeds of P and Q are equal,
v v
so Q = P
x 3a−x | M1
2x ag
v =
Q 3a−x | A1 | Shown convincingly: angular speeds equal stated.
AG
2
--- 6(b) ---
6(b) | m4ag
For P: T +mgcos60=
3a−x | B1
mv2
For Q: T −mgcos60= Q
x | B1
m.4ag mv2
Eliminate T: −mgcos60+ =mgcos60+ Q
3a−x x | M1
m4ag mx4ag
=1+
3a−x (3a−x)2
4a(3a−x)=(3a−x)2+4ax, x2 +2ax−3a2 =0 | M1 | Solve to find x.
Obtain 3-term quadratic equation.
(x−a)(x+3a)=0, x=a | A1
5
Question | Answer | Marks | Guidance
--- 6(c) ---
6(c) | Energy changes from initial position:
1 ( 4ag−u2)
Gain in KE of P: m
2
1 u 2
Loss in KE of Q: m −v Q 2
2 2
Loss in GPE of P = mg(3a−x)(1−cos60) (=mga)
1
Gain in GPE of Q = mgx(1−cos60) = mga
2 | B1 | KEs correct.
B1FT | GPEs correct.
1 m ( 4ag−u2) − 1 m u 2 −v Q 2 =−mgx(1−cos60)+mg(3a−x)(1−cos60)
2 2 2
| M1 | Energy equation.
5
Simplify: 4ag− u2 +ag =ag
4
16 4
u2 = ag, u= 5ag
5 5 | A1 | AEF
4
A particle $P$ of mass $m$ is attached to one end of a light inextensible rod of length $3a$. An identical particle $Q$ is attached to the other end of the rod. The rod is smoothly pivoted at a point $O$ on the rod, where $OQ = x$. The system, of rod and particles, rotates about $O$ in a vertical plane.
At an instant when the rod is vertical, with $P$ above $Q$, the particle $P$ is moving horizontally with speed $u$. When the rod has turned through an angle of $60°$ from the vertical, the speed of $P$ is $2\sqrt{ag}$, and the tensions in the two parts of the rod, $OP$ and $OQ$, have equal magnitudes.
\begin{enumerate}[label=(\alph*)]
\item Show that the speed of $Q$ when the rod has turned through an angle of $60°$ from the vertical is $\frac{2x}{3a-x}\sqrt{ag}$. [2]
\item Find $x$ in terms of $a$. [5]
\item Find $u$ in terms of $a$ and $g$. [4]
\end{enumerate}
\hfill \mbox{\textit{CAIE Further Paper 3 2023 Q6 [11]}}