Edexcel M3 — Question 6 12 marks

Exam BoardEdexcel
ModuleM3 (Mechanics 3)
Marks12
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicSimple Harmonic Motion
TypeMaximum acceleration in SHM
DifficultyStandard +0.3 This is a standard M3 SHM question with springs. Part (a) is routine equilibrium using Hooke's law. Parts (b-d) follow textbook procedures: showing F ∝ -x for SHM, finding period from ω = √(k/m), and calculating maximum acceleration from ω²a. The two-spring setup adds minor complexity but the method is entirely standard for M3, making it slightly easier than average overall.
Spec4.10f Simple harmonic motion: x'' = -omega^2 x6.02h Elastic PE: 1/2 k x^26.02i Conservation of energy: mechanical energy principle

The figure shows a swing consisting of two identical vertical light springs attached symmetrically to a light horizontal cross-bar and supported from a strong fixed horizontal beam. When a mass of 24 kg is placed at the mid-point of the cross-bar, both springs extend by 30 cm to the position \(A\), as shown. \includegraphics{figure_6} Each spring has natural length \(l\) m and modulus of elasticity \(\lambda\) N.
  1. Show that \(\lambda = 392l\). [2 marks]
The 24 kg mass is left on the bar and the bar is then displaced downwards by a further 20 cm.
  1. Prove that the system comprising the bar and the mass now performs simple harmonic motion with the centre of oscillation at the level \(A\). [5 marks]
  2. Calculate the number of oscillations made per second in this motion. [3 marks]
  3. Find the maximum acceleration which the mass experiences during the motion. [2 marks]

AnswerMarks Guidance
(a) \(24g = 2T = 2\frac{2}{3}(0.3)\)M1 A1
\(\frac{\lambda}{l} = \frac{24g \times 0.8}{2 \times 0.3} = 392\)
\(\lambda = 392l\)
(b) At dist. \(x\) from \(A\), \(mg - 2\lambda(0.3 + x) = mx\)M1 A1 A1
\(x = -\frac{2\lambda}{m} = -\frac{98}{3}x\)A1 A1
Hence S.H.M. with centre \(A\)
(c) \(\omega^2 = \frac{98}{3} = 32.7\)M1 A1 A1
Freq. \(= \frac{2\pi}{\omega} = \frac{\sqrt{32.7}}{2\pi} = 0.91 \text{ osc.s}^{-1}\)
(d) Max. acc. \(= \omega^2(0.2) = 6.54 \text{ ms}^{-2}\)M1 Total: 12 marks
**(a)** $24g = 2T = 2\frac{2}{3}(0.3)$ | M1 A1 |
$\frac{\lambda}{l} = \frac{24g \times 0.8}{2 \times 0.3} = 392$ | |
$\lambda = 392l$ | |

**(b)** At dist. $x$ from $A$, $mg - 2\lambda(0.3 + x) = mx$ | M1 A1 A1 |
$x = -\frac{2\lambda}{m} = -\frac{98}{3}x$ | A1 A1 |
Hence S.H.M. with centre $A$ | |

**(c)** $\omega^2 = \frac{98}{3} = 32.7$ | M1 A1 A1 |
Freq. $= \frac{2\pi}{\omega} = \frac{\sqrt{32.7}}{2\pi} = 0.91 \text{ osc.s}^{-1}$ | |

**(d)** Max. acc. $= \omega^2(0.2) = 6.54 \text{ ms}^{-2}$ | M1 | **Total: 12 marks**
The figure shows a swing consisting of two identical vertical light springs attached symmetrically to a light horizontal cross-bar and supported from a strong fixed horizontal beam. When a mass of 24 kg is placed at the mid-point of the cross-bar, both springs extend by 30 cm to the position $A$, as shown.

\includegraphics{figure_6}

Each spring has natural length $l$ m and modulus of elasticity $\lambda$ N.

\begin{enumerate}[label=(\alph*)]
\item Show that $\lambda = 392l$. [2 marks]
\end{enumerate}

The 24 kg mass is left on the bar and the bar is then displaced downwards by a further 20 cm.

\begin{enumerate}[label=(\alph*)]
\setcounter{enumi}{1}
\item Prove that the system comprising the bar and the mass now performs simple harmonic motion with the centre of oscillation at the level $A$. [5 marks]
\item Calculate the number of oscillations made per second in this motion. [3 marks]
\item Find the maximum acceleration which the mass experiences during the motion. [2 marks]
\end{enumerate}

\hfill \mbox{\textit{Edexcel M3  Q6 [12]}}