CAIE FP2 2012 November — Question 10 EITHER

Exam BoardCAIE
ModuleFP2 (Further Pure Mathematics 2)
Year2012
SessionNovember
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments
TypeHemisphere or sphere resting on plane or wall
DifficultyChallenging +1.8 This is a challenging 3-sphere equilibrium problem requiring systematic force analysis at multiple contact points, friction inequalities, and geometric reasoning with angles. While the setup is complex with 6 unknowns (normal and friction forces at 4 contacts), the symmetry simplifies the algebra significantly. The problem demands careful free-body diagrams, resolution in two directions, and understanding limiting friction conditions, but follows a standard mechanics approach without requiring novel insight. It's harder than typical A-level mechanics due to the multi-body system and Further Maths context, but more straightforward than problems requiring geometric breakthroughs or extended proof chains.
Spec3.03r Friction: concept and vector form3.03t Coefficient of friction: F <= mu*R model3.03u Static equilibrium: on rough surfaces3.04a Calculate moments: about a point3.04b Equilibrium: zero resultant moment and force

\includegraphics[max width=\textwidth, alt={}]{d3e9a568-a9ea-483e-8e65-90fdc4a69781-5_389_702_484_719}
Two identical uniform rough spheres \(A\) and \(B\), each of weight \(W\) and radius \(a\), are at rest on a rough horizontal plane, and are not in contact with each other. A third identical sphere \(C\) rests on \(A\) and \(B\) with its centre in the same vertical plane as the centres of \(A\) and \(B\). The line joining the centres of \(A\) and \(C\) and the line joining the centres of \(B\) and \(C\) are each inclined at an angle \(\theta\) to the vertical (see diagram). The coefficient of friction between each sphere and the plane is \(\mu\). The coefficient of friction between \(C\) and \(A\), and between \(C\) and \(B\), is \(\mu ^ { \prime }\). The system remains in equilibrium. Show that $$\mu \geqslant \frac { \sin \theta } { 3 ( 1 + \cos \theta ) } \quad \text { and } \quad \mu ^ { \prime } \geqslant \frac { \sin \theta } { 1 + \cos \theta } .$$

Question 10:
Part (a)
AnswerMarks Guidance
Answer/WorkingMark Guidance
Stating or implying reactions \(R_P\), \(R_S\) same as for \(B\)B1
Stating or implying \(F_P = F_S\) by moments about \(O_A\)B1
Stating or implying 3 independent equations for \(F\), \(R_P\), \(R_S\)\(3 \times\) M1 A1
\(2R_P = 3W\) Up to 2 resolutions of forces
\(R_P = W + R_S \cos\theta + F_S \sin\theta\) \(\uparrow\) for \(A\)
\(2R_S \cos\theta + 2F_S \sin\theta = W\) \(\uparrow\) for \(C\)
\(R_P \cos\theta + F_P \sin\theta = R_S + W\cos\theta\) \(O_A \rightarrow O_C\) for \(A\)
Moments about \(S\) for \(A\): \(F_P(r + r\cos\theta) + Wr\sin\theta = R_P r\sin\theta\)
\(R_P = 3W/2\)A1
\(R_S = W/2\)A1
\(F = (W\sin\theta)/2(1+\cos\theta)\)A1 Find \(F\) at \(P\) and/or \(S\)
\(\mu \geq \sin\theta \ / \ 3(1+\cos\theta)\)A.G. M1 A1 Use \(F \leq \mu R_P\) to find bound for \(\mu\)
\(\mu' \geq \sin\theta \ / \ (1+\cos\theta)\)A.G. M1 Use \(F \leq \mu' R_S\) to find bound for \(\mu'\)
Total14
Part (b)
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(E(X) = \int_2^4 (5x^2 - x^3 - 4x)/10 \ dx\)M1 A1 Find \(E(X)\) using \(\int xf(x)dx\)
\(= \frac{1}{2}(4^3 - 2^3) - 3(4^4 - 2^4)/40 - 3(4^2 - 2^2)/5\)
\(= 28 - 18 - 7.2 = 2.8\)*A1
\((E(X) - 2.69)/2.69 = 0.041 < 0.1\)M1 A1 Verify \(E(X)\) within 10% of \(2.69\), A1 dep *A1
*or* \(1.1 \times 2.69 = 2.96 > E(X)\)
Subtotal5
\(60\int_{2.5}^{3.6}(5x - x^2 - 4)/10 \ dx\)M1 Show derivation of tabular entry
\(= 60[3(5x^2/2 - x^3/3 - 4x)/10]_{3.2}^{3.6}\)
*or* \([45x^2 - 6x^3 - 72x]_{3.2}^{3.6}\)
\(= 122.4 - 83.328 - 28.8\)
*or* \(60 \times 0.1712 = 10.272\)A.G. A1
Subtotal2
\(H_0\): \(f(x)\) fits data (A.E.F.)B1 State null hypothesis
\(O: \ldots 8\) ; \(E: \ldots 14.208\)B1 Combine last 2 cells since exp. value \(< 5\)
\(\chi^2 = 0.8126 + 0.0584 + 0.2011 + 2.7135 = 3.78[47]\)M1 *A1 Calculate \(\chi^2\) to 2 d.p.
\(\chi^2_{3,0.9} = 6.25[1]\)
\(\chi^2_{4,0.9} = 7.78\)*B1
Accept \(H_0\) if \(\chi^2 <\) tabular valueM1 Valid method for conclusion
\(3.78 < 6.25\) so \(f(x)\) does fitA1 Conclusion (A.E.F., dep *A1, *B1)
Subtotal7
# Question 10:

## Part (a)

| Answer/Working | Mark | Guidance |
|---|---|---|
| Stating or implying reactions $R_P$, $R_S$ same as for $B$ | B1 | |
| Stating or implying $F_P = F_S$ by moments about $O_A$ | B1 | |
| Stating or implying 3 independent equations for $F$, $R_P$, $R_S$ | $3 \times$ M1 A1 | |
| $2R_P = 3W$ | | Up to 2 resolutions of forces |
| $R_P = W + R_S \cos\theta + F_S \sin\theta$ | | $\uparrow$ for $A$ |
| $2R_S \cos\theta + 2F_S \sin\theta = W$ | | $\uparrow$ for $C$ |
| $R_P \cos\theta + F_P \sin\theta = R_S + W\cos\theta$ | | $O_A \rightarrow O_C$ for $A$ |
| Moments about $S$ for $A$: $F_P(r + r\cos\theta) + Wr\sin\theta = R_P r\sin\theta$ | | |
| $R_P = 3W/2$ | A1 | |
| $R_S = W/2$ | A1 | |
| $F = (W\sin\theta)/2(1+\cos\theta)$ | A1 | Find $F$ at $P$ and/or $S$ |
| $\mu \geq \sin\theta \ / \ 3(1+\cos\theta)$ | A.G. M1 A1 | Use $F \leq \mu R_P$ to find bound for $\mu$ |
| $\mu' \geq \sin\theta \ / \ (1+\cos\theta)$ | A.G. M1 | Use $F \leq \mu' R_S$ to find bound for $\mu'$ |
| **Total** | **14** | |

## Part (b)

| Answer/Working | Mark | Guidance |
|---|---|---|
| $E(X) = \int_2^4 (5x^2 - x^3 - 4x)/10 \ dx$ | M1 A1 | Find $E(X)$ using $\int xf(x)dx$ |
| $= \frac{1}{2}(4^3 - 2^3) - 3(4^4 - 2^4)/40 - 3(4^2 - 2^2)/5$ | | |
| $= 28 - 18 - 7.2 = 2.8$ | *A1 | |
| $(E(X) - 2.69)/2.69 = 0.041 < 0.1$ | M1 A1 | Verify $E(X)$ within 10% of $2.69$, A1 dep *A1 |
| *or* $1.1 \times 2.69 = 2.96 > E(X)$ | | |
| **Subtotal** | **5** | |
| $60\int_{2.5}^{3.6}(5x - x^2 - 4)/10 \ dx$ | M1 | Show derivation of tabular entry |
| $= 60[3(5x^2/2 - x^3/3 - 4x)/10]_{3.2}^{3.6}$ | | |
| *or* $[45x^2 - 6x^3 - 72x]_{3.2}^{3.6}$ | | |
| $= 122.4 - 83.328 - 28.8$ | | |
| *or* $60 \times 0.1712 = 10.272$ | A.G. A1 | |
| **Subtotal** | **2** | |
| $H_0$: $f(x)$ fits data (A.E.F.) | B1 | State null hypothesis |
| $O: \ldots 8$ ; $E: \ldots 14.208$ | B1 | Combine last 2 cells since exp. value $< 5$ |
| $\chi^2 = 0.8126 + 0.0584 + 0.2011 + 2.7135 = 3.78[47]$ | M1 *A1 | Calculate $\chi^2$ to 2 d.p. |
| $\chi^2_{3,0.9} = 6.25[1]$ | | |
| $\chi^2_{4,0.9} = 7.78$ | *B1 | |
| Accept $H_0$ if $\chi^2 <$ tabular value | M1 | Valid method for conclusion |
| $3.78 < 6.25$ so $f(x)$ does fit | A1 | Conclusion (A.E.F., dep *A1, *B1) |
| **Subtotal** | **7** | |
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\includegraphics[max width=\textwidth, alt={}]{d3e9a568-a9ea-483e-8e65-90fdc4a69781-5_389_702_484_719}
\end{center}

Two identical uniform rough spheres $A$ and $B$, each of weight $W$ and radius $a$, are at rest on a rough horizontal plane, and are not in contact with each other. A third identical sphere $C$ rests on $A$ and $B$ with its centre in the same vertical plane as the centres of $A$ and $B$. The line joining the centres of $A$ and $C$ and the line joining the centres of $B$ and $C$ are each inclined at an angle $\theta$ to the vertical (see diagram). The coefficient of friction between each sphere and the plane is $\mu$. The coefficient of friction between $C$ and $A$, and between $C$ and $B$, is $\mu ^ { \prime }$. The system remains in equilibrium. Show that

$$\mu \geqslant \frac { \sin \theta } { 3 ( 1 + \cos \theta ) } \quad \text { and } \quad \mu ^ { \prime } \geqslant \frac { \sin \theta } { 1 + \cos \theta } .$$

\hfill \mbox{\textit{CAIE FP2 2012 Q10 EITHER}}