CAIE M2 2018 June — Question 6 9 marks

Exam BoardCAIE
ModuleM2 (Mechanics 2)
Year2018
SessionJune
Marks9
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 1
TypeTwo strings, two fixed points
DifficultyStandard +0.8 This is a sophisticated 3D circular motion problem requiring geometric analysis to find string angles, consideration of limiting cases (one string going slack for minimum speed, strings breaking for maximum speed), and application of Newton's second law in both horizontal and vertical directions. The multi-constraint optimization and geometric setup elevate this above standard circular motion exercises.
Spec6.05c Horizontal circles: conical pendulum, banked tracks

\includegraphics{figure_6} A particle \(P\) of mass 0.2 kg is attached to one end of a light inextensible string of length 0.6 m. The other end of the string is attached to a fixed point \(A\). The particle \(P\) is also attached to one end of a second light inextensible string of length 0.6 m, the other end of which is attached to a fixed point \(B\) vertically below \(A\). The particle moves in a horizontal circle of radius 0.3 m, which has its centre at the mid-point of \(AB\), with both strings straight (see diagram).
  1. Calculate the least possible angular speed of \(P\). [4]
  2. Find the greatest possible speed of \(P\). [5]
The string \(AP\) will break if its tension exceeds 8 N. The string \(BP\) will break if its tension exceeds 5 N.

Question 6:

AnswerMarks Guidance
6(i)cosθ = 0.5 and sinθ = 3/2 B1
Tsinθ = 0.2 gM1 Resolve vertically for P. Note tension in BP is zero
Tcosθ = 0.2ω2 × 0.3M1 Use Newton's Second Law horizontally
ω = 4.39 rads−1A1
Total:4
QuestionAnswer Marks

AnswerMarks Guidance
6(ii)T sinθ = 0.2 g + T sinθ
A BM1 Resolve vertically for P
T sinθ = 0.2 g + 5sinθ
AnswerMarks Guidance
AM1 Use T = 5
B
T = 7.309
AnswerMarks Guidance
AA1
5cosθ + 7.309cosθ = 0.2v2/0.3M1 Use Newton's Second Law horizontally
v = 3.04 ms−1A1
Total:5
QuestionAnswer Marks
Question 6:
--- 6(i) ---
6(i) | cosθ = 0.5 and sinθ = 3/2 | B1 | θ is the angle that AP makes with the horizontal. Note tanθ = 3
Tsinθ = 0.2 g | M1 | Resolve vertically for P. Note tension in BP is zero
Tcosθ = 0.2ω2 × 0.3 | M1 | Use Newton's Second Law horizontally
ω = 4.39 rads−1 | A1
Total: | 4
Question | Answer | Marks | Guidance
--- 6(ii) ---
6(ii) | T sinθ = 0.2 g + T sinθ
A B | M1 | Resolve vertically for P
T sinθ = 0.2 g + 5sinθ
A | M1 | Use T = 5
B
T = 7.309
A | A1
5cosθ + 7.309cosθ = 0.2v2/0.3 | M1 | Use Newton's Second Law horizontally
v = 3.04 ms−1 | A1
Total: | 5
Question | Answer | Marks | Guidance
\includegraphics{figure_6}

A particle $P$ of mass 0.2 kg is attached to one end of a light inextensible string of length 0.6 m. The other end of the string is attached to a fixed point $A$. The particle $P$ is also attached to one end of a second light inextensible string of length 0.6 m, the other end of which is attached to a fixed point $B$ vertically below $A$. The particle moves in a horizontal circle of radius 0.3 m, which has its centre at the mid-point of $AB$, with both strings straight (see diagram).

\begin{enumerate}[label=(\roman*)]
\item Calculate the least possible angular speed of $P$. [4]

\item Find the greatest possible speed of $P$. [5]
\end{enumerate}

The string $AP$ will break if its tension exceeds 8 N. The string $BP$ will break if its tension exceeds 5 N.

\hfill \mbox{\textit{CAIE M2 2018 Q6 [9]}}