CAIE M2 2010 June — Question 6 10 marks

Exam BoardCAIE
ModuleM2 (Mechanics 2)
Year2010
SessionJune
Marks10
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicHooke's law and elastic energy
TypeParticle at midpoint of string between two horizontal fixed points: vertical motion
DifficultyStandard +0.3 This is a standard two-part Hooke's law problem requiring equilibrium analysis (resolving forces, using Hooke's law) and energy conservation. Part (i) involves routine resolution of forces and algebraic manipulation. Part (ii) applies conservation of energy with elastic potential energy, gravitational potential energy, and kinetic energy—a standard M2 technique. The geometry is straightforward and the multi-step nature is typical for this level, making it slightly easier than average.
Spec6.02h Elastic PE: 1/2 k x^26.02i Conservation of energy: mechanical energy principle6.04e Rigid body equilibrium: coplanar forces

\includegraphics{figure_6} A particle \(P\) of mass 0.35 kg is attached to the mid-point of a light elastic string of natural length 4 m. The ends of the string are attached to fixed points \(A\) and \(B\) which are 4.8 m apart at the same horizontal level. \(P\) hangs in equilibrium at a point 0.7 m vertically below the mid-point \(M\) of \(AB\) (see diagram).
  1. Find the tension in the string and hence show that the modulus of elasticity of the string is 25 N. [4]
\(P\) is now held at rest at a point 1.8 m vertically below \(M\), and is then released.
  1. Find the speed with which \(P\) passes through \(M\). [6]

(i)
AnswerMarks Guidance
\([0.35g = 2T/0.7 / (2(4^2 + 0.7^2)^{1/2})]\) Tension is 6.25N \([6.25 = 2 \times \frac{1}{4}]\) Modulus is 25NM1 A1 M1 A1 [4] For resolving forces on P vertically. For using \(T = 2v/L\) AG
(ii)
EE on release \(= 25 \times 2^2/(2 \times 4)\) EE when P is at M \(= 25 \times 0.8^2/(2 \times 4)\)
AnswerMarks Guidance
\(25 \times 2^2/(2 \times 4) = 0.35g \times 1.8 + 25 \times 0.8^2/(2 \times 4) + \frac{1}{2} 0.35v^2\) Speed is 4.90ms\(^{-1}\)M1 A1 A1 M1 A1 A1 [6] For using \(EE = 2x^2/2L\). For using \(EE\) on release \(= mgh + EE\) when P is at M \(+ \frac{1}{2}mv^2\)
## (i)

$[0.35g = 2T/0.7 / (2(4^2 + 0.7^2)^{1/2})]$ Tension is 6.25N $[6.25 = 2 \times \frac{1}{4}]$ Modulus is 25N | M1 A1 M1 A1 [4] | For resolving forces on P vertically. For using $T = 2v/L$ AG

## (ii)

EE on release $= 25 \times 2^2/(2 \times 4)$ EE when P is at M $= 25 \times 0.8^2/(2 \times 4)$

$25 \times 2^2/(2 \times 4) = 0.35g \times 1.8 + 25 \times 0.8^2/(2 \times 4) + \frac{1}{2} 0.35v^2$ Speed is 4.90ms$^{-1}$ | M1 A1 A1 M1 A1 A1 [6] | For using $EE = 2x^2/2L$. For using $EE$ on release $= mgh + EE$ when P is at M $+ \frac{1}{2}mv^2$

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\includegraphics{figure_6}

A particle $P$ of mass 0.35 kg is attached to the mid-point of a light elastic string of natural length 4 m. The ends of the string are attached to fixed points $A$ and $B$ which are 4.8 m apart at the same horizontal level. $P$ hangs in equilibrium at a point 0.7 m vertically below the mid-point $M$ of $AB$ (see diagram).

\begin{enumerate}[label=(\roman*)]
\item Find the tension in the string and hence show that the modulus of elasticity of the string is 25 N. [4]
\end{enumerate}

$P$ is now held at rest at a point 1.8 m vertically below $M$, and is then released.

\begin{enumerate}[label=(\roman*)]
\setcounter{enumi}{1}
\item Find the speed with which $P$ passes through $M$. [6]
\end{enumerate}

\hfill \mbox{\textit{CAIE M2 2010 Q6 [10]}}