AQA M2 2011 January — Question 7 15 marks

Exam BoardAQA
ModuleM2 (Mechanics 2)
Year2011
SessionJanuary
Marks15
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicHooke's law and elastic energy
TypeWork-energy with multiple stages
DifficultyStandard +0.3 This is a standard M2 elastic strings question with routine applications of Hooke's law and energy conservation. Part (a) is a bookwork proof, part (b)(i) is straightforward equilibrium, and parts (ii)-(iii) use standard energy methods with clear setups. The multi-part structure and energy conservation make it slightly above trivial, but all techniques are standard textbook exercises requiring no novel insight.
Spec6.02h Elastic PE: 1/2 k x^26.02i Conservation of energy: mechanical energy principle

7
  1. An elastic string has natural length \(l\) and modulus of elasticity \(\lambda\). The string is stretched from length \(l\) to length \(l + e\). Show, by integration, that the work done in stretching the string is \(\frac { \lambda e ^ { 2 } } { 2 l }\).
  2. A block, of mass 4 kg , is attached to one end of a light elastic string. The string has natural length 2 m and modulus of elasticity 196 N . The other end of the string is attached to a fixed point \(O\).
    1. A second block, of mass 3 kg , is attached to the 4 kg block and the system hangs in equilibrium, as shown in the diagram. \includegraphics[max width=\textwidth, alt={}, center]{9d039ec3-fd0a-40ae-9afe-7627439081df-16_374_291_890_877} Find the extension in the string.
    2. The block of mass 3 kg becomes detached from the 4 kg block and falls to the ground. The 4 kg block now begins to move vertically upwards. Find the extension of the string when the 4 kg block is next at rest.
    3. Find the extension of the string when the speed of the 4 kg block is a maximum.
      (3 marks)
      \includegraphics[max width=\textwidth, alt={}]{9d039ec3-fd0a-40ae-9afe-7627439081df-18_2486_1714_221_153}
      \includegraphics[max width=\textwidth, alt={}]{9d039ec3-fd0a-40ae-9afe-7627439081df-19_2486_1714_221_153}

Question 7(a):
AnswerMarks Guidance
Working/AnswerMark Guidance
Tension at extension \(x\): \(T = \frac{\lambda x}{l}\)B1
Work done \(= \int_0^e \frac{\lambda x}{l}\, dx\)M1 Integrating tension
\(= \left[\frac{\lambda x^2}{2l}\right]_0^e = \frac{\lambda e^2}{2l}\)A1 Completion, no errors
Question 7(b)(i):
AnswerMarks Guidance
Working/AnswerMark Guidance
At equilibrium: \(T = (4+3)g = 7g\)M1 Resolving for whole system
\(\frac{196 \times e}{2} = 7g\)A1 Correct equation
\(e = \frac{7g}{98} = 0.7\) mA1 cao
Question 7(b)(ii):
AnswerMarks Guidance
Working/AnswerMark Guidance
Using energy conservation from initial position (extension 0.7m) to restM1
Let new extension be \(x\). Change in EPE + change in GPE = 0M1 Setting up energy equation
\(\frac{196x^2}{4} - \frac{196(0.7)^2}{4} = 4g(x - 0.7)\)A1 A1
\(49x^2 - 24.01 = 39.2x - 27.44\)DM1 Solving
\(49x^2 - 39.2x + 3.43 = 0\)A1 \(x = 0.1\) m or \(x = 0.7\) m, so extension \(= 0.1\) m
Question 7(b)(iii):
AnswerMarks Guidance
Working/AnswerMark Guidance
Maximum speed when acceleration = 0, i.e. when \(T = 4g\)M1 A1
\(\frac{196e}{2} = 4g \Rightarrow e = \frac{4g}{98} = 0.4\) mA1 cao
# Question 7(a):

| Working/Answer | Mark | Guidance |
|---|---|---|
| Tension at extension $x$: $T = \frac{\lambda x}{l}$ | B1 | |
| Work done $= \int_0^e \frac{\lambda x}{l}\, dx$ | M1 | Integrating tension |
| $= \left[\frac{\lambda x^2}{2l}\right]_0^e = \frac{\lambda e^2}{2l}$ | A1 | Completion, no errors |

# Question 7(b)(i):

| Working/Answer | Mark | Guidance |
|---|---|---|
| At equilibrium: $T = (4+3)g = 7g$ | M1 | Resolving for whole system |
| $\frac{196 \times e}{2} = 7g$ | A1 | Correct equation |
| $e = \frac{7g}{98} = 0.7$ m | A1 | cao |

# Question 7(b)(ii):

| Working/Answer | Mark | Guidance |
|---|---|---|
| Using energy conservation from initial position (extension 0.7m) to rest | M1 | |
| Let new extension be $x$. Change in EPE + change in GPE = 0 | M1 | Setting up energy equation |
| $\frac{196x^2}{4} - \frac{196(0.7)^2}{4} = 4g(x - 0.7)$ | A1 A1 | |
| $49x^2 - 24.01 = 39.2x - 27.44$ | DM1 | Solving |
| $49x^2 - 39.2x + 3.43 = 0$ | A1 | $x = 0.1$ m or $x = 0.7$ m, so extension $= 0.1$ m |

# Question 7(b)(iii):

| Working/Answer | Mark | Guidance |
|---|---|---|
| Maximum speed when acceleration = 0, i.e. when $T = 4g$ | M1 A1 | |
| $\frac{196e}{2} = 4g \Rightarrow e = \frac{4g}{98} = 0.4$ m | A1 | cao |
7
\begin{enumerate}[label=(\alph*)]
\item An elastic string has natural length $l$ and modulus of elasticity $\lambda$. The string is stretched from length $l$ to length $l + e$.

Show, by integration, that the work done in stretching the string is $\frac { \lambda e ^ { 2 } } { 2 l }$.
\item A block, of mass 4 kg , is attached to one end of a light elastic string. The string has natural length 2 m and modulus of elasticity 196 N . The other end of the string is attached to a fixed point $O$.
\begin{enumerate}[label=(\roman*)]
\item A second block, of mass 3 kg , is attached to the 4 kg block and the system hangs in equilibrium, as shown in the diagram.\\
\includegraphics[max width=\textwidth, alt={}, center]{9d039ec3-fd0a-40ae-9afe-7627439081df-16_374_291_890_877}

Find the extension in the string.
\item The block of mass 3 kg becomes detached from the 4 kg block and falls to the ground. The 4 kg block now begins to move vertically upwards.

Find the extension of the string when the 4 kg block is next at rest.
\item Find the extension of the string when the speed of the 4 kg block is a maximum.\\
(3 marks)

\begin{center}
\includegraphics[max width=\textwidth, alt={}]{9d039ec3-fd0a-40ae-9afe-7627439081df-18_2486_1714_221_153}
\end{center}

\begin{center}
\includegraphics[max width=\textwidth, alt={}]{9d039ec3-fd0a-40ae-9afe-7627439081df-19_2486_1714_221_153}
\end{center}
\end{enumerate}\end{enumerate}

\hfill \mbox{\textit{AQA M2 2011 Q7 [15]}}