CAIE FP2 2019 June — Question 4 10 marks

Exam BoardCAIE
ModuleFP2 (Further Pure Mathematics 2)
Year2019
SessionJune
Marks10
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments
TypeRod with end on ground or wall supported by string
DifficultyChallenging +1.2 This is a standard statics problem requiring resolution of forces, moments about a point, and friction at limiting equilibrium. While it involves multiple steps (geometry to find string angle, three equations from equilibrium conditions), the techniques are routine for Further Maths mechanics. The given tan θ = 2 simplifies calculations significantly, and the approach follows a standard template for rod-on-wall problems.
Spec3.03u Static equilibrium: on rough surfaces3.04a Calculate moments: about a point3.04b Equilibrium: zero resultant moment and force

4 \includegraphics[max width=\textwidth, alt={}, center]{2aaf3493-6509-4668-91a2-9f4708bbbb58-08_677_812_258_664} A uniform rod \(A B\) of length \(4 a\) and weight \(W\) rests with the end \(A\) in contact with a rough vertical wall. A light inextensible string of length \(\frac { 5 } { 2 } a\) has one end attached to the point \(C\) on the rod, where \(A C = \frac { 5 } { 2 } a\). The other end of the string is attached to a point \(D\) on the wall, vertically above \(A\). The vertical plane containing the \(\operatorname { rod } A B\) is perpendicular to the wall. The angle between the rod and the wall is \(\theta\), where \(\tan \theta = 2\) (see diagram). The end \(A\) of the rod is on the point of slipping down the wall and the coefficient of friction between the rod and the wall is \(\mu\). Find, in either order, the tension in the string and the value of \(\mu\).

Question 4:
AnswerMarks Guidance
AnswerMarks Guidance
\(A\): \(T \times \frac{5a}{2}\sin(\pi - 2\theta) - W \times 2a\sin\theta = 0\)M1 A1 Take moments for rod about one chosen point; \([\sin\theta = \frac{2}{\sqrt{5}}\), \(\cos\theta = \frac{1}{\sqrt{5}}\), \(\sin(\pi-2\theta) = \sin 2\theta = \frac{4}{5}]\)
\(C\): \(F_A \times \frac{5a}{2}\sin\theta - R_A \times \frac{5a}{2}\cos\theta - W \times \frac{1}{2}a\sin\theta = 0\)
\(B\): \(F_A \times 4a\sin\theta - R_A \times 4a\cos\theta - W \times 2a\sin\theta + T \times \frac{3a}{2}\sin(\pi-2\theta) = 0\)
\(G\): \(F_A \times 2a\sin\theta - R_A \times 2a\cos\theta - T \times \frac{1}{2}a\sin(\pi-2\theta) = 0\) (\(G\) is midpoint of \(AB\))
\(D\): \(R_A \times 5a\cos\theta - W \times 2a\sin\theta = 0\)
\(R_A = T\sin\theta\)B1 Find two more independent equations
\(F_A = W - T\cos\theta\)B1 e.g. resolution of forces on rod (a second moment equation may be used)
\(F_A = \mu R_A\)B1 Relate \(F_A\) and \(R_A\) (may be implied)
\(T = \frac{2W\sin\theta}{\frac{5}{2}\sin 2\theta} = \frac{2W}{5\cos\theta}\)M1 Find \(T\) by any method (e.g. from moments about \(A\))
\(= \frac{2W}{\sqrt{5}}\) or \(\frac{2\sqrt{5}}{5}W\) or \(0.894W\)A1
\(F_A = \frac{3}{5}W\) and \(R_A = \frac{4}{5}W\); \(\mu = \frac{3}{4}\) or \(0.75\)M1 A1 Find or imply \(F_A\) and \(R_A\) by any method (e.g. from resolutions) and hence \(\mu\)
A1
10
## Question 4:

| Answer | Marks | Guidance |
|--------|-------|----------|
| $A$: $T \times \frac{5a}{2}\sin(\pi - 2\theta) - W \times 2a\sin\theta = 0$ | M1 A1 | Take moments for rod about one chosen point; $[\sin\theta = \frac{2}{\sqrt{5}}$, $\cos\theta = \frac{1}{\sqrt{5}}$, $\sin(\pi-2\theta) = \sin 2\theta = \frac{4}{5}]$ |
| $C$: $F_A \times \frac{5a}{2}\sin\theta - R_A \times \frac{5a}{2}\cos\theta - W \times \frac{1}{2}a\sin\theta = 0$ | | |
| $B$: $F_A \times 4a\sin\theta - R_A \times 4a\cos\theta - W \times 2a\sin\theta + T \times \frac{3a}{2}\sin(\pi-2\theta) = 0$ | | |
| $G$: $F_A \times 2a\sin\theta - R_A \times 2a\cos\theta - T \times \frac{1}{2}a\sin(\pi-2\theta) = 0$ ($G$ is midpoint of $AB$) | | |
| $D$: $R_A \times 5a\cos\theta - W \times 2a\sin\theta = 0$ | | |
| $R_A = T\sin\theta$ | B1 | Find two more independent equations |
| $F_A = W - T\cos\theta$ | B1 | e.g. resolution of forces on rod (a second moment equation may be used) |
| $F_A = \mu R_A$ | B1 | Relate $F_A$ and $R_A$ (may be implied) |
| $T = \frac{2W\sin\theta}{\frac{5}{2}\sin 2\theta} = \frac{2W}{5\cos\theta}$ | M1 | Find $T$ by any method (e.g. from moments about $A$) |
| $= \frac{2W}{\sqrt{5}}$ or $\frac{2\sqrt{5}}{5}W$ or $0.894W$ | A1 | |
| $F_A = \frac{3}{5}W$ and $R_A = \frac{4}{5}W$; $\mu = \frac{3}{4}$ or $0.75$ | M1 A1 | Find or imply $F_A$ and $R_A$ by any method (e.g. from resolutions) and hence $\mu$ |
| | A1 | |
| | **10** | |

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\includegraphics[max width=\textwidth, alt={}, center]{2aaf3493-6509-4668-91a2-9f4708bbbb58-08_677_812_258_664}

A uniform rod $A B$ of length $4 a$ and weight $W$ rests with the end $A$ in contact with a rough vertical wall. A light inextensible string of length $\frac { 5 } { 2 } a$ has one end attached to the point $C$ on the rod, where $A C = \frac { 5 } { 2 } a$. The other end of the string is attached to a point $D$ on the wall, vertically above $A$. The vertical plane containing the $\operatorname { rod } A B$ is perpendicular to the wall. The angle between the rod and the wall is $\theta$, where $\tan \theta = 2$ (see diagram). The end $A$ of the rod is on the point of slipping down the wall and the coefficient of friction between the rod and the wall is $\mu$.

Find, in either order, the tension in the string and the value of $\mu$.\\

\hfill \mbox{\textit{CAIE FP2 2019 Q4 [10]}}