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 hinged to wall with rough contact at free end
DifficultyChallenging +1.8 This is a challenging statics problem requiring resolution of forces in two directions, taking moments about a strategic point, using the friction law at limiting equilibrium, and working with the geometry of the string constraint. It involves multiple simultaneous equations and careful geometric reasoning with the given tan θ = 2 condition. While the techniques are standard A-level mechanics (moments, resolution, friction), the multi-step coordination and geometric setup place it well above average difficulty for A-level, though not at the extreme end since the approach is systematic once the setup is understood.
Spec3.03u Static equilibrium: on rough surfaces6.04e Rigid body equilibrium: coplanar forces

\includegraphics{figure_4} A uniform rod \(AB\) of length \(4a\) 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 \(AC = \frac{3}{2}a\). The other end of the string is attached to a point \(D\) on the wall, vertically above \(A\). The vertical plane containing the rod \(AB\) 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 \(\mu\). [10]

Question 4:
AnswerMarks
4A: T × 5a/2 sin (π – 2θ) – W × 2a sin θ = 0
C: F × 5a/2 sin θ – R × 5a/2 cos θ – W × ½ a sin θ = 0
A A
B: F × 4a sin θ – R × 4a cos θ – W × 2a sin θ
A A
+ T × 3a/2 sin (π – 2θ) = 0
G: F × 2a sin θ – R × 2a cos θ – T × ½ a sin (π – 2θ) = 0
A A
(G is mid-point of AB)
D: R × 5a cos θ – W × 2a sin θ = 0
AnswerMarks Guidance
AM1 A1 Take moments for rod about one chosen point
[sin θ = 2/√5, cos θ = 1/√5, sin (π – 2θ) = sin 2θ = 4/5]
R = T sin θ
A
F = W – T cos θ
AnswerMarks Guidance
AB1 Find two more independent equations
B1e.g. resolution of forces on rod (a second moment equation may be
used)
F = µR
AnswerMarks Guidance
A AB1 Relate F and R (may be implied)
A A
AnswerMarks Guidance
T = (2W sin θ ) / (5/2 sin 2θ ) = 2W / (5 cos θ )M1 Find T by any method (e.g. from moments about A)
= 2W/√5 or (2√5/5) W or 0⋅894 WA1
F = (3/5) W and R = (4/5) W
A A
AnswerMarks Guidance
µ = ¾ or 0⋅75M1 A1 Find or imply F and R by any method (e.g. from resolutions)
A A
and hence µ
A1
10
AnswerMarks Guidance
QuestionAnswer Marks
Question 4:
4 | A: T × 5a/2 sin (π – 2θ) – W × 2a sin θ = 0
C: F × 5a/2 sin θ – R × 5a/2 cos θ – W × ½ a sin θ = 0
A A
B: F × 4a sin θ – R × 4a cos θ – W × 2a sin θ
A A
+ T × 3a/2 sin (π – 2θ) = 0
G: F × 2a sin θ – R × 2a cos θ – T × ½ a sin (π – 2θ) = 0
A A
(G is mid-point of AB)
D: R × 5a cos θ – W × 2a sin θ = 0
A | M1 A1 | Take moments for rod about one chosen point
[sin θ = 2/√5, cos θ = 1/√5, sin (π – 2θ) = sin 2θ = 4/5]
R = T sin θ
A
F = W – T cos θ
A | B1 | Find two more independent equations
B1 | e.g. resolution of forces on rod (a second moment equation may be
used)
F = µR
A A | B1 | Relate F and R (may be implied)
A A
T = (2W sin θ ) / (5/2 sin 2θ ) = 2W / (5 cos θ ) | M1 | Find T by any method (e.g. from moments about A)
= 2W/√5 or (2√5/5) W or 0⋅894 W | A1
F = (3/5) W and R = (4/5) W
A A
µ = ¾ or 0⋅75 | M1 A1 | Find or imply F and R by any method (e.g. from resolutions)
A A
and hence µ
A1
10
Question | Answer | Marks | Guidance
\includegraphics{figure_4}

A uniform rod $AB$ of length $4a$ 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 $AC = \frac{3}{2}a$. The other end of the string is attached to a point $D$ on the wall, vertically above $A$. The vertical plane containing the rod $AB$ 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 $\mu$. [10]

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