CAIE FP2 2011 June — Question 3 12 marks

Exam BoardCAIE
ModuleFP2 (Further Pure Mathematics 2)
Year2011
SessionJune
Marks12
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments
TypeTwo jointed rods in equilibrium
DifficultyChallenging +1.2 This is a standard two-rod statics problem requiring moments about two points, resolution of forces, and friction analysis. While it involves multiple steps and careful bookkeeping of forces at the hinge, the techniques are routine for Further Maths mechanics: take moments about A for each rod separately, resolve forces, then apply friction conditions. The geometry is straightforward (right angle at A), and the method is well-practiced in FM courses.
Spec3.03m Equilibrium: sum of resolved forces = 03.03t Coefficient of friction: F <= mu*R model6.04e Rigid body equilibrium: coplanar forces

3 \includegraphics[max width=\textwidth, alt={}, center]{3daca234-9b7f-41d4-bbaa-d35615a120fc-2_419_1102_1859_520} The diagram shows two uniform rods \(B A\) and \(A C\), smoothly hinged at \(A\). The rod \(B A\) has length \(8 a\) and weight \(W\); the rod \(A C\) has length \(6 a\) and weight \(2 W\). The rods are in equilibrium in a vertical plane with \(B\) and \(C\) resting on a rough horizontal floor and angle \(C A B\) equal to \(90 ^ { \circ }\). Show that the normal contact force at \(B\) is \(\frac { 26 } { 25 } W\). The coefficient of friction between each rod and the floor is \(\mu\). Find the least possible value of \(\mu\).

Question 3:
AnswerMarks Guidance
Working/AnswerMark Guidance
Moments for system about \(C\), denoting \(ACB\) by \(\theta\): \(N_B \times BC = 2W \times 3a\cos\theta + W(BC - 4a\sin\theta)\)M1 A1 (A.E.F.)
Substitute for \(BC\), \(\theta\): \(N_B \times 10a = 2W \times \frac{9a}{5} + W \times \frac{34a}{5}\)A1
Simplify to give \(N_B\): \(N_B = \frac{26}{25}W\)A1 A.G.
Find \(N_C\) by vertical resolution or moments: \(N_C = 3W - N_B = \frac{49}{25}W\)M1 A1
Find \(F_B\) (or \(F_C\)) by moments about \(A\): \(F_B \times \frac{24a}{5} = N_B \times \frac{32a}{5} - W \times \frac{16a}{5}\)M1
\(F_B = \frac{18}{25}W\ \text{or}\ 0{\cdot}72W\)A1
Find limiting value of \(\mu\) at \(B\) [or \(C\)] (A.E.F.): \(\frac{18}{26}\ [= 0{\cdot}692\ \text{or}\ \frac{18}{49} = 0{\cdot}367]\)M1 A1
Relate \(F_B\), \(F_C\) by e.g. horizontal resolution: \(F_C = F_B\ \left[= \frac{18}{25}W\right]\)B1
Deduce least possible value of \(\mu\) for system: \(\mu_{min} = \frac{9}{13}\ \text{or}\ 0{\cdot}692\)B1 [Subtotal: 8]
Total: 12
## Question 3:

| Working/Answer | Mark | Guidance |
|---|---|---|
| Moments for system about $C$, denoting $ACB$ by $\theta$: $N_B \times BC = 2W \times 3a\cos\theta + W(BC - 4a\sin\theta)$ | M1 A1 | (A.E.F.) |
| Substitute for $BC$, $\theta$: $N_B \times 10a = 2W \times \frac{9a}{5} + W \times \frac{34a}{5}$ | A1 | |
| Simplify to give $N_B$: $N_B = \frac{26}{25}W$ | A1 | **A.G.** | [Subtotal: 4] |
| Find $N_C$ by vertical resolution or moments: $N_C = 3W - N_B = \frac{49}{25}W$ | M1 A1 | |
| Find $F_B$ (or $F_C$) by moments about $A$: $F_B \times \frac{24a}{5} = N_B \times \frac{32a}{5} - W \times \frac{16a}{5}$ | M1 | |
| $F_B = \frac{18}{25}W\ \text{or}\ 0{\cdot}72W$ | A1 | |
| Find limiting value of $\mu$ at $B$ [or $C$] (A.E.F.): $\frac{18}{26}\ [= 0{\cdot}692\ \text{or}\ \frac{18}{49} = 0{\cdot}367]$ | M1 A1 | |
| Relate $F_B$, $F_C$ by e.g. horizontal resolution: $F_C = F_B\ \left[= \frac{18}{25}W\right]$ | B1 | |
| Deduce least possible value of $\mu$ for system: $\mu_{min} = \frac{9}{13}\ \text{or}\ 0{\cdot}692$ | B1 | [Subtotal: 8] |

**Total: 12**

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\includegraphics[max width=\textwidth, alt={}, center]{3daca234-9b7f-41d4-bbaa-d35615a120fc-2_419_1102_1859_520}

The diagram shows two uniform rods $B A$ and $A C$, smoothly hinged at $A$. The rod $B A$ has length $8 a$ and weight $W$; the rod $A C$ has length $6 a$ and weight $2 W$. The rods are in equilibrium in a vertical plane with $B$ and $C$ resting on a rough horizontal floor and angle $C A B$ equal to $90 ^ { \circ }$. Show that the normal contact force at $B$ is $\frac { 26 } { 25 } W$.

The coefficient of friction between each rod and the floor is $\mu$. Find the least possible value of $\mu$.

\hfill \mbox{\textit{CAIE FP2 2011 Q3 [12]}}