CAIE Further Paper 3 2023 November — Question 3 8 marks

Exam BoardCAIE
ModuleFurther Paper 3 (Further Paper 3)
Year2023
SessionNovember
Marks8
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments
TypeRing on wire with string
DifficultyChallenging +1.8 This is a challenging statics problem requiring careful setup of equilibrium equations (forces and moments), geometric reasoning to find perpendicular distances, and understanding of limiting friction. The 'about to slip up' condition determines friction direction and magnitude (F = μR). While the geometry is moderately complex and requires multiple steps, the problem follows standard mechanics methodology without requiring exceptional insight. The 8-mark allocation reflects substantial work, placing it well above average difficulty but not at the extreme end for Further Maths mechanics.
Spec3.03u Static equilibrium: on rough surfaces6.04e Rigid body equilibrium: coplanar forces

\includegraphics{figure_3} A uniform square lamina of side \(2a\) and weight \(W\) is suspended from a light inextensible string attached to the midpoint \(E\) of the side \(AB\). The other end of the string is attached to a fixed point \(P\) on a rough vertical wall. The vertex \(B\) of the lamina is in contact with the wall. The string \(EP\) is perpendicular to the side \(AB\) and makes an angle \(\theta\) with the wall (see diagram). The string and the lamina are in a vertical plane perpendicular to the wall. The coefficient of friction between the wall and the lamina is \(\frac{1}{2}\). Given that the vertex \(B\) is about to slip up the wall, find the value of \(\tan\theta\). [8]

Question 3:
AnswerMarks Guidance
3Let N be normal reaction at B and F the frictional force acting downwards
Tcos=F+WB1
→Tsin=NB1
Moments about B: Ta=Wsina+WcosaM1A1 A moments equation with all relevant forces.
1
F = N used
AnswerMarks
2M1
 1 
(cos+sin) cos− sin =1 oe
AnswerMarks Guidance
 2 M1 Combine to obtain equation in .
Equation in trigonometric functions only.
1 3
cossin= (sin)2
2 2
AnswerMarks Guidance
sin(cos−3sin)=0M1 Solve trigonometric equation.
1
tan=
AnswerMarks
3A1
8
AnswerMarks Guidance
QuestionAnswer Marks
Question 3:
3 | Let N be normal reaction at B and F the frictional force acting downwards
Tcos=F+W | B1
→Tsin=N | B1
Moments about B: Ta=Wsina+Wcosa | M1A1 | A moments equation with all relevant forces.
1
F = N used
2 | M1
 1 
(cos+sin) cos− sin =1 oe
 2  | M1 | Combine to obtain equation in .
Equation in trigonometric functions only.
1 3
cossin= (sin)2
2 2
sin(cos−3sin)=0 | M1 | Solve trigonometric equation.
1
tan=
3 | A1
8
Question | Answer | Marks | Guidance
\includegraphics{figure_3}

A uniform square lamina of side $2a$ and weight $W$ is suspended from a light inextensible string attached to the midpoint $E$ of the side $AB$. The other end of the string is attached to a fixed point $P$ on a rough vertical wall. The vertex $B$ of the lamina is in contact with the wall. The string $EP$ is perpendicular to the side $AB$ and makes an angle $\theta$ with the wall (see diagram). The string and the lamina are in a vertical plane perpendicular to the wall. The coefficient of friction between the wall and the lamina is $\frac{1}{2}$.

Given that the vertex $B$ is about to slip up the wall, find the value of $\tan\theta$. [8]

\hfill \mbox{\textit{CAIE Further Paper 3 2023 Q3 [8]}}