CAIE Further Paper 3 2021 June — Question 4 8 marks

Exam BoardCAIE
ModuleFurther Paper 3 (Further Paper 3)
Year2021
SessionJune
Marks8
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 2
TypeVertical circle: tension at specific point
DifficultyChallenging +1.8 This is a challenging circular motion problem requiring energy conservation and circular motion dynamics at two positions, with the key insight that tension becomes zero at B. Students must set up equations at both A and B, use the perpendicular geometry, and solve simultaneously for the tension at A. The 8-mark allocation and the need to connect multiple concepts (energy, centripetal force, string becoming slack) place this well above average difficulty, though it follows a recognizable framework for Further Maths circular motion problems.
Spec6.02i Conservation of energy: mechanical energy principle6.05f Vertical circle: motion including free fall

\includegraphics{figure_4} 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 particle is initially held with the string taut at the point \(A\), where \(OA\) makes an angle \(\theta\) with the downward vertical through \(O\). The particle is then projected with speed \(u\) perpendicular to \(OA\) and begins to move upwards in part of a vertical circle. The string goes slack when the particle is at the point \(B\) where angle \(AOB\) is a right angle. The speed of the particle when it is at \(B\) is \(\frac{1}{2}u\) (see diagram). Find the tension in the string at \(A\), giving your answer in terms of \(m\) and \(g\). [8]

Question 4:
AnswerMarks
4Unless otherwise indicated, marks once gained cannot subsequently be lost, e.g. wrong working following a correct form of answer is ignored (isw).
42
1 mu2 − 1 m u  =mg ( acosθ+asinθ)
 
AnswerMarks Guidance
2 2 2*M1 Energy equation, with 2 KE terms and a two-part GPE term,
allow cos/sin mix.
3 ( )
u2 =2ag cosθ+sinθ
AnswerMarks
4A1
2
u
m
 
2
mgsinθ=
At B, tension in string is zero, so
a
(u2=4agsinθ
AnswerMarks Guidance
)B1 N2L
u2
AnswerMarks
EliminateDM1
tanθ=2
AnswerMarks
OEA1
mu2
At A, T −mgcosθ=
AnswerMarks Guidance
aB1 N2L
9 5
T = mg ( = 4.02mg)
AnswerMarks Guidance
5M1 A1 Substitute to find T.
Alternative method for question 4
2
1 mu2 − 1 m u  =mg ( acosθ+asinθ)
 
AnswerMarks Guidance
2 2 2*M1 Energy equation, with 2 KE terms and a two-part GPE term,
allow cos/sin mix.
3 u2 =2ag ( cosθ+sinθ)
AnswerMarks Guidance
4A1
QuestionAnswer Marks
42
u
m
 
2
mgsinθ=
At B, tension in string is zero, so
a
AnswerMarks Guidance
(u2=4agsinθ)B1 N2L
Eliminate θ : u2 = 8ag 5
AnswerMarks
5DM1 A1
mu2
At A, T −mgcosθ=
AnswerMarks Guidance
aB1 N2L
9 5
T = mg ( = 4.02mg)
AnswerMarks Guidance
5M1 A1 Substitute to find T.
8
AnswerMarks Guidance
QuestionAnswer Marks
Question 4:
4 | Unless otherwise indicated, marks once gained cannot subsequently be lost, e.g. wrong working following a correct form of answer is ignored (isw).
4 | 2
1 mu2 − 1 m u  =mg ( acosθ+asinθ)
 
2 2 2 | *M1 | Energy equation, with 2 KE terms and a two-part GPE term,
allow cos/sin mix.
3 ( )
u2 =2ag cosθ+sinθ
4 | A1
2
u
m
 
2
mgsinθ=
At B, tension in string is zero, so
a
(u2=4agsinθ
) | B1 | N2L
u2
Eliminate | DM1
tanθ=2
OE | A1
mu2
At A, T −mgcosθ=
a | B1 | N2L
9 5
T = mg ( = 4.02mg)
5 | M1 A1 | Substitute to find T.
Alternative method for question 4
2
1 mu2 − 1 m u  =mg ( acosθ+asinθ)
 
2 2 2 | *M1 | Energy equation, with 2 KE terms and a two-part GPE term,
allow cos/sin mix.
3 u2 =2ag ( cosθ+sinθ)
4 | A1
Question | Answer | Marks | Guidance
4 | 2
u
m
 
2
mgsinθ=
At B, tension in string is zero, so
a
(u2=4agsinθ) | B1 | N2L
Eliminate θ : u2 = 8ag 5
5 | DM1 A1
mu2
At A, T −mgcosθ=
a | B1 | N2L
9 5
T = mg ( = 4.02mg)
5 | M1 A1 | Substitute to find T.
8
Question | Answer | Marks | Guidance
\includegraphics{figure_4}

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 particle is initially held with the string taut at the point $A$, where $OA$ makes an angle $\theta$ with the downward vertical through $O$. The particle is then projected with speed $u$ perpendicular to $OA$ and begins to move upwards in part of a vertical circle. The string goes slack when the particle is at the point $B$ where angle $AOB$ is a right angle. The speed of the particle when it is at $B$ is $\frac{1}{2}u$ (see diagram).

Find the tension in the string at $A$, giving your answer in terms of $m$ and $g$. [8]

\hfill \mbox{\textit{CAIE Further Paper 3 2021 Q4 [8]}}