CAIE M2 2017 June — Question 6 9 marks

Exam BoardCAIE
ModuleM2 (Mechanics 2)
Year2017
SessionJune
Marks9
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 1
TypeElastic string – conical pendulum (string inclined to vertical)
DifficultyStandard +0.3 This is a standard circular motion problem with elastic strings requiring resolution of forces, Hooke's law, and energy calculations. While it involves multiple steps (tension from extension, vertical/horizontal force resolution, angular speed calculation, then energy comparison), these are routine M2 techniques with no novel insight required. The multi-part structure and 9 total marks indicate moderate length, but the methods are textbook-standard, placing it slightly above average difficulty.
Spec6.02h Elastic PE: 1/2 k x^26.02i Conservation of energy: mechanical energy principle6.05c Horizontal circles: conical pendulum, banked tracks

A particle \(P\) of mass \(0.15\) kg is attached to one end of a light elastic string of natural length \(0.4\) m and modulus of elasticity \(12\) N. The other end of the string is attached to a fixed point \(A\). The particle \(P\) moves in a horizontal circle which has its centre vertically below \(A\), with the string inclined at \(\theta°\) to the vertical and \(AP = 0.5\) m.
  1. Find the angular speed of \(P\) and the value of \(\theta\). [5]
  2. Calculate the difference between the elastic potential energy stored in the string and the kinetic energy of \(P\). [4]

Question 6:

AnswerMarks Guidance
6(i)T = 12 × 0.1 / 0.4 ( = 3 N) B1
3sinθ = 0.15ω2(0.5sinθ)M1 Uses Newton's Second Law horizontally
ω = 6.32 rads−1A1
Tcosθ = 0.15g (cosθ = 0.5)M1 Resolves vertically
θ = 60A1
Total:5

AnswerMarks Guidance
6(ii)v = 6.32 × 0.5sin60 B1 FT
KE = 0.15(6.32 × 0.5sin60)2 / 2 (=0.5625J)B1
Difference = 0.5625 – 12 × 0.12 / (2 × 0.4)M1 Uses EE = λx2 / (2L)
Difference = 0.4125 JA1
Total:4
Question 6:
--- 6(i) ---
6(i) | T = 12 × 0.1 / 0.4 ( = 3 N) | B1 | Uses T = λx / L
3sinθ = 0.15ω2(0.5sinθ) | M1 | Uses Newton's Second Law horizontally
ω = 6.32 rads−1 | A1
Tcosθ = 0.15g (cosθ = 0.5) | M1 | Resolves vertically
θ = 60 | A1
Total: | 5
--- 6(ii) ---
6(ii) | v = 6.32 × 0.5sin60 | B1 FT | Uses v = rω and r = 0.5sin60
KE = 0.15(6.32 × 0.5sin60)2 / 2 (=0.5625J) | B1
Difference = 0.5625 – 12 × 0.12 / (2 × 0.4) | M1 | Uses EE = λx2 / (2L)
Difference = 0.4125 J | A1
Total: | 4
A particle $P$ of mass $0.15$ kg is attached to one end of a light elastic string of natural length $0.4$ m and modulus of elasticity $12$ N. The other end of the string is attached to a fixed point $A$. The particle $P$ moves in a horizontal circle which has its centre vertically below $A$, with the string inclined at $\theta°$ to the vertical and $AP = 0.5$ m.

\begin{enumerate}[label=(\roman*)]
\item Find the angular speed of $P$ and the value of $\theta$. [5]

\item Calculate the difference between the elastic potential energy stored in the string and the kinetic energy of $P$. [4]
\end{enumerate}

\hfill \mbox{\textit{CAIE M2 2017 Q6 [9]}}