CAIE FP2 2015 November — Question 1 9 marks

Exam BoardCAIE
ModuleFP2 (Further Pure Mathematics 2)
Year2015
SessionNovember
Marks9
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments
TypeRod with end on ground or wall supported by string
DifficultyStandard +0.8 This is a multi-step statics problem requiring resolution of forces in two directions, taking moments about a strategic point, and using the geometric constraint tan θ = 2 tan α. While the techniques are standard for Further Mechanics (resolving forces, moments, smooth contacts), the problem requires careful geometric reasoning to relate the angles and systematic algebraic manipulation across multiple equations. It's more demanding than typical A-level mechanics but not exceptionally difficult for Further Maths students.
Spec6.04e Rigid body equilibrium: coplanar forces

1 \includegraphics[max width=\textwidth, alt={}, center]{27d3ee31-7c6e-4451-9c3d-aa4cfc0fdb22-2_744_504_255_824} A uniform ladder \(A B\), of length \(3 a\) and weight \(W\), rests with the end \(A\) in contact with smooth horizontal ground and the end \(B\) against a smooth vertical wall. One end of a light inextensible rope is attached to the ladder at the point \(C\), where \(A C = a\). The other end of the rope is fixed to the point \(D\) at the base of the wall and the rope \(D C\) is in the same vertical plane as the ladder \(A B\). The ladder rests in equilibrium in a vertical plane perpendicular to the wall, with the ladder making an angle \(\theta\) with the horizontal and the rope making an angle \(\alpha\) with the horizontal (see diagram). It is given that \(\tan \theta = 2 \tan \alpha\). Find, in terms of \(W\) and \(\alpha\), the tension in the rope and the magnitudes of the forces acting on the ladder at \(A\) and at \(B\).

Question 1:
AnswerMarks Guidance
Answer/WorkingMarks Guidance
\(R_B = T\cos\alpha\)M1 A1 Resolve horizontally
\(R_A = W + T\sin\alpha\)M1 A1 Resolve vertically
\(R_B 3a\sin\theta = W(3a/2)\cos\theta + Ta(\sin\alpha\cos\theta + \cos\alpha\sin\theta)\) *or* \(+Ta\sin(\alpha+\theta)\) *or* \(+T3a\cos\theta\sin\alpha\)M1 A1 Moments about \(A\) (\(a\) may be omitted)
\(R_A 3a\cos\theta = W(3a/2)\cos\theta + T2a(\sin\alpha\cos\theta + \cos\alpha\sin\theta)\) *or* \(+T2a\sin(\alpha+\theta)\) *or* \(+T3a\sin\theta\cos\alpha\)(M1 A1) Moments about \(B\)
\(R_A a\cos\theta + W(a/2)\cos\theta = R_B 2a\sin\theta\)(M1 A1) Moments about \(C\)
\(R_A 3a\cos\theta - W(3a/2)\cos\theta = R_B 3a\sin\theta\)(M1 A1) Moments about \(D\)
\(T = W/2\sin\alpha\) *or* \(\frac{1}{2}W\operatorname{cosec}\alpha\)B1 Solve for \(T\), \(R_A\), \(R_B\) (AEF in \(W\) and \(\alpha\))
\(R_A = 3W/2\)B1
\(R_B = W/2\tan\alpha\) *or* \(\frac{1}{2}W\cot\alpha\)B1 Total: 9 marks
## Question 1:

| Answer/Working | Marks | Guidance |
|---|---|---|
| $R_B = T\cos\alpha$ | M1 A1 | Resolve horizontally |
| $R_A = W + T\sin\alpha$ | M1 A1 | Resolve vertically |
| $R_B 3a\sin\theta = W(3a/2)\cos\theta + Ta(\sin\alpha\cos\theta + \cos\alpha\sin\theta)$ *or* $+Ta\sin(\alpha+\theta)$ *or* $+T3a\cos\theta\sin\alpha$ | M1 A1 | Moments about $A$ ($a$ may be omitted) |
| $R_A 3a\cos\theta = W(3a/2)\cos\theta + T2a(\sin\alpha\cos\theta + \cos\alpha\sin\theta)$ *or* $+T2a\sin(\alpha+\theta)$ *or* $+T3a\sin\theta\cos\alpha$ | (M1 A1) | Moments about $B$ |
| $R_A a\cos\theta + W(a/2)\cos\theta = R_B 2a\sin\theta$ | (M1 A1) | Moments about $C$ |
| $R_A 3a\cos\theta - W(3a/2)\cos\theta = R_B 3a\sin\theta$ | (M1 A1) | Moments about $D$ |
| $T = W/2\sin\alpha$ *or* $\frac{1}{2}W\operatorname{cosec}\alpha$ | B1 | Solve for $T$, $R_A$, $R_B$ (AEF in $W$ and $\alpha$) |
| $R_A = 3W/2$ | B1 | |
| $R_B = W/2\tan\alpha$ *or* $\frac{1}{2}W\cot\alpha$ | B1 | Total: 9 marks |

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\includegraphics[max width=\textwidth, alt={}, center]{27d3ee31-7c6e-4451-9c3d-aa4cfc0fdb22-2_744_504_255_824}

A uniform ladder $A B$, of length $3 a$ and weight $W$, rests with the end $A$ in contact with smooth horizontal ground and the end $B$ against a smooth vertical wall. One end of a light inextensible rope is attached to the ladder at the point $C$, where $A C = a$. The other end of the rope is fixed to the point $D$ at the base of the wall and the rope $D C$ is in the same vertical plane as the ladder $A B$. The ladder rests in equilibrium in a vertical plane perpendicular to the wall, with the ladder making an angle $\theta$ with the horizontal and the rope making an angle $\alpha$ with the horizontal (see diagram). It is given that $\tan \theta = 2 \tan \alpha$. Find, in terms of $W$ and $\alpha$, the tension in the rope and the magnitudes of the forces acting on the ladder at $A$ and at $B$.

\hfill \mbox{\textit{CAIE FP2 2015 Q1 [9]}}