Edexcel M3 2009 January — Question 2 9 marks

Exam BoardEdexcel
ModuleM3 (Mechanics 3)
Year2009
SessionJanuary
Marks9
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicHooke's law and elastic energy
TypeElastic string equilibrium and statics
DifficultyStandard +0.3 This is a straightforward equilibrium problem requiring resolution of forces in two directions and application of Hooke's law. The setup is standard for M3 elastic strings, with clear given values and routine calculations for tension and elastic energy using familiar formulas.
Spec3.03m Equilibrium: sum of resolved forces = 06.02h Elastic PE: 1/2 k x^2

2. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{8374fa0f-cb28-497f-8696-877d7d0762f1-03_467_622_242_635} \captionsetup{labelformat=empty} \caption{Figure 1}
\end{figure} A particle \(P\) of mass \(m\) is attached to one end of a light elastic string, of natural length \(a\) and modulus of elasticity \(3 m g\). The other end of the string is attached to a fixed point \(O\). The particle \(P\) is held in equilibrium by a horizontal force of magnitude \(\frac { 4 } { 3 } m g\) applied to \(P\). This force acts in the vertical plane containing the string, as shown in Figure 1. Find (a) the tension in the string,
(b) the elastic energy stored in the string.

Question 2:
Part (a):
AnswerMarks Guidance
Working/AnswerMarks Guidance
\((\leftarrow)\quad T\sin\theta = \frac{4}{3}mg\)M1 A1
\((\uparrow)\quad T\cos\theta = mg\)A1
\(T^2 = \left(\frac{4}{3}mg\right)^2 + (mg)^2\)M1
\(T = \frac{5}{3}mg\)A1 (5)
Part (b):
AnswerMarks Guidance
Working/AnswerMarks Guidance
\(T = \frac{\lambda x}{a} \Rightarrow \frac{5}{3}mg = \frac{3mge}{a}\)M1 A1ft ft their \(T\)
\(e = \frac{5}{9}a\)
\(E = \frac{\lambda x^2}{2a} = \frac{3mg}{2a} \times \left(\frac{5}{9}a\right)^2 = \frac{25}{54}mga\)M1 A1 (4) [9]
## Question 2:

### Part (a):

| Working/Answer | Marks | Guidance |
|---|---|---|
| $(\leftarrow)\quad T\sin\theta = \frac{4}{3}mg$ | M1 A1 | |
| $(\uparrow)\quad T\cos\theta = mg$ | A1 | |
| $T^2 = \left(\frac{4}{3}mg\right)^2 + (mg)^2$ | M1 | |
| $T = \frac{5}{3}mg$ | A1 | **(5)** |

### Part (b):

| Working/Answer | Marks | Guidance |
|---|---|---|
| $T = \frac{\lambda x}{a} \Rightarrow \frac{5}{3}mg = \frac{3mge}{a}$ | M1 A1ft | ft their $T$ |
| $e = \frac{5}{9}a$ | | |
| $E = \frac{\lambda x^2}{2a} = \frac{3mg}{2a} \times \left(\frac{5}{9}a\right)^2 = \frac{25}{54}mga$ | M1 A1 | **(4) [9]** |

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2.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{8374fa0f-cb28-497f-8696-877d7d0762f1-03_467_622_242_635}
\captionsetup{labelformat=empty}
\caption{Figure 1}
\end{center}
\end{figure}

A particle $P$ of mass $m$ is attached to one end of a light elastic string, of natural length $a$ and modulus of elasticity $3 m g$. The other end of the string is attached to a fixed point $O$. The particle $P$ is held in equilibrium by a horizontal force of magnitude $\frac { 4 } { 3 } m g$ applied to $P$. This force acts in the vertical plane containing the string, as shown in Figure 1. Find (a) the tension in the string,\\
(b) the elastic energy stored in the string.\\

\hfill \mbox{\textit{Edexcel M3 2009 Q2 [9]}}