CAIE FP2 2018 November — Question 3 9 marks

Exam BoardCAIE
ModuleFP2 (Further Pure Mathematics 2)
Year2018
SessionNovember
Marks9
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 2
TypeVertical circle: string becomes slack
DifficultyChallenging +1.8 This is a challenging Further Maths mechanics problem requiring energy conservation, circular motion dynamics, and the condition for slack string (tension = 0). Part (i) involves setting up energy and centripetal force equations at the slack point, requiring careful angle work with the given tan α = 15/8. Part (ii) requires finding where maximum tension occurs (lowest point) and applying T = mg + mv²/r. The multi-step reasoning, coordinate geometry with the specific angle, and integration of multiple mechanics principles place this well above average difficulty, though it follows a recognizable framework for conical pendulum problems.
Spec6.05d Variable speed circles: energy methods6.05f Vertical circle: motion including free fall

\includegraphics{figure_3} A particle of mass \(m\) is attached to one end of a light inextensible string of length \(a\). The other end of the string is attached to a fixed point \(O\). The point \(A\) is such that \(OA = a\) and \(OA\) makes an angle \(\alpha\) with the upward vertical, where \(\tan \alpha = \frac{15}{8}\). The particle is projected downwards from \(A\) with speed \(u\) perpendicular to the string and moves in a vertical plane (see diagram). The string becomes slack after the string has rotated through \(270°\) from its initial position, with the particle now at the point \(B\). \begin{enumerate}[label=(\roman*)] \item Show that \(u^2 = 2ag\). [5] \item Find the maximum tension in the string as the particle moves from \(A\) to \(B\). [4] \end{enumerate]

Question 3:

AnswerMarks
3(i)½mv 2 = ½mu2 – mga (sin α – cos α)
B
[v 2 = u2 – (14/13) ag]
AnswerMarks Guidance
BM1A1 Find speed v at B by conservation of energy (A0 if no m)
B
[sin α = 12/13, cos α = 5/13]
[T =] mv 2/a – mg sin α = 0 [v 2 = (12/13) ag]
AnswerMarks Guidance
B B BB1 Equate tension T at B to zero by using F = ma radially
B
AnswerMarks Guidance
u2 = (3 sin α – 2 cos α) agM1 Combine to verify u2
= (36/13 – 10/13) ag = 2 ag AGA1
5
AnswerMarks Guidance
QuestionAnswer Marks

AnswerMarks
3(ii)EITHER: ½mv 2 = ½mu2 + mga (1 + cos α)
C
or ½mv 2 + mga (1 + sin α) [v 2 = 62ag/13]
AnswerMarks Guidance
B CM1 Find v 2 at lowest point C by conservation of energy
C
T = mv 2/a + mg
AnswerMarks Guidance
max CB1 Find tension T at lowest point from F = ma radially
max
AnswerMarks Guidance
= 62mg/13 + mgM1 Combine to find T
max
AnswerMarks
= 75mg/13 or 5.77 mg or 57.7 mA1
OR: ½mV2 = ½mu2 + mga (cos α + cos θ )
AnswerMarks Guidance
[V2 = 2ag (18/13 + cos θ )](M1 Find V2 at general point by conservation of energy
(where OP is e.g. at θ to downward vertical)
AnswerMarks Guidance
T = mV2/a + mg cos θ = (36/13 + 3 cos θ ) mgB1 Find tension T at general point from F = ma radially
T = (36/13 + 3) mg
AnswerMarks Guidance
maxM1 Combine to find T at lowest point where θ = 0
max
AnswerMarks
= 75mg/13 or 5.77 mg or 57.7 mA1)
4
AnswerMarks Guidance
QuestionAnswer Marks
Question 3:
--- 3(i) ---
3(i) | ½mv 2 = ½mu2 – mga (sin α – cos α)
B
[v 2 = u2 – (14/13) ag]
B | M1A1 | Find speed v at B by conservation of energy (A0 if no m)
B
[sin α = 12/13, cos α = 5/13]
[T =] mv 2/a – mg sin α = 0 [v 2 = (12/13) ag]
B B B | B1 | Equate tension T at B to zero by using F = ma radially
B
u2 = (3 sin α – 2 cos α) ag | M1 | Combine to verify u2
= (36/13 – 10/13) ag = 2 ag AG | A1
5
Question | Answer | Marks | Guidance
--- 3(ii) ---
3(ii) | EITHER: ½mv 2 = ½mu2 + mga (1 + cos α)
C
or ½mv 2 + mga (1 + sin α) [v 2 = 62ag/13]
B C | M1 | Find v 2 at lowest point C by conservation of energy
C
T = mv 2/a + mg
max C | B1 | Find tension T at lowest point from F = ma radially
max
= 62mg/13 + mg | M1 | Combine to find T
max
= 75mg/13 or 5.77 mg or 57.7 m | A1
OR: ½mV2 = ½mu2 + mga (cos α + cos θ )
[V2 = 2ag (18/13 + cos θ )] | (M1 | Find V2 at general point by conservation of energy
(where OP is e.g. at θ to downward vertical)
T = mV2/a + mg cos θ = (36/13 + 3 cos θ ) mg | B1 | Find tension T at general point from F = ma radially
T = (36/13 + 3) mg
max | M1 | Combine to find T at lowest point where θ = 0
max
= 75mg/13 or 5.77 mg or 57.7 m | A1)
4
Question | Answer | Marks | Guidance
\includegraphics{figure_3}

A particle of mass $m$ is attached to one end of a light inextensible string of length $a$. The other end of the string is attached to a fixed point $O$. The point $A$ is such that $OA = a$ and $OA$ makes an angle $\alpha$ with the upward vertical, where $\tan \alpha = \frac{15}{8}$. The particle is projected downwards from $A$ with speed $u$ perpendicular to the string and moves in a vertical plane (see diagram). The string becomes slack after the string has rotated through $270°$ from its initial position, with the particle now at the point $B$.

\begin{enumerate}[label=(\roman*)]
\item Show that $u^2 = 2ag$.
[5]

\item Find the maximum tension in the string as the particle moves from $A$ to $B$.
[4]
\end{enumerate]

\hfill \mbox{\textit{CAIE FP2 2018 Q3 [9]}}