Edexcel M4 2005 June — Question 5 12 marks

Exam BoardEdexcel
ModuleM4 (Mechanics 4)
Year2005
SessionJune
Marks12
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments
TypePotential energy with elastic strings/springs
DifficultyChallenging +1.8 This M4 question requires setting up potential energy for a compound system (gravitational + elastic) with non-uniform rod rotating about a fixed point, then finding equilibrium via calculus. The geometry is non-trivial (relating rod angle to string extension through the constraint), and part (b) requires solving a transcendental equation. While systematic, it demands careful coordinate work, energy formulation for rotation, and multi-step algebraic manipulation beyond standard textbook exercises.
Spec1.07n Stationary points: find maxima, minima using derivatives6.02h Elastic PE: 1/2 k x^26.02i Conservation of energy: mechanical energy principle6.04e Rigid body equilibrium: coplanar forces

A non-uniform rod \(BC\) has mass \(m\) and length \(3l\). The centre of mass of the rod is at distance \(l\) from \(B\). The rod can turn freely about a fixed smooth horizontal axis through \(B\). One end of a light elastic string, of natural length \(l\) and modulus of elasticity \(\frac{mg}{6}\), is attached to \(C\). The other end of the string is attached to a point \(P\) which is at a height \(3l\) vertically above \(B\).
  1. Show that, while the string is stretched, the potential energy of the system is $$mgl(\cos^2 \theta - \cos \theta) + \text{constant},$$ where \(\theta\) is the angle between the string and the downward vertical and \(-\frac{\pi}{2} < \theta < \frac{\pi}{2}\). [6]
  2. Find the values of \(\theta\) for which the system is in equilibrium with the string stretched. [6]

Part (c)
AnswerMarks
\(GPE = -mg L \cos 2\theta\)B1
\(EPE = \frac{m_g(6\sin\theta - L)^2}{6}\)M1
\(= \frac{m_g}{12}(36\cos^2\theta - 12\cos\theta + L^2)\)
AnswerMarks
\(= mg(3\cos^2\theta - \cos\theta) + C\)M1
\(V = -mgL(2\cos^2\theta - 1) + mg L(3\cos^2\theta - \cos\theta) + c\)
AnswerMarks
\(= mgL(\cos^2\theta - \cos\theta) + c\)M1, M1 (guidance: "unclear2DF..."), A1 (6)
Part (d)
\(\frac{dV}{d\theta} = mgL(-2\cos\theta \sin\theta - \sin\theta) = 0\)
\(\sin\theta(-2\cos\theta + 1) = 0\)
AnswerMarks
\(\sin\theta = 0\) or \(\cos\theta = \frac{1}{2}\)M1 A1, M1
\(\theta = 0\) or \(\theta = \pm \frac{\pi}{3}\)A1, A1 (6), (12)
## Part (c)
$GPE = -mg L \cos 2\theta$ | B1 |

$EPE = \frac{m_g(6\sin\theta - L)^2}{6}$ | M1 |

$= \frac{m_g}{12}(36\cos^2\theta - 12\cos\theta + L^2)$

$= mg(3\cos^2\theta - \cos\theta) + C$ | M1 |

$V = -mgL(2\cos^2\theta - 1) + mg L(3\cos^2\theta - \cos\theta) + c$

$= mgL(\cos^2\theta - \cos\theta) + c$ | M1, M1 (guidance: "unclear2DF..."), A1 (6) |

## Part (d)
$\frac{dV}{d\theta} = mgL(-2\cos\theta \sin\theta - \sin\theta) = 0$

$\sin\theta(-2\cos\theta + 1) = 0$

$\sin\theta = 0$ or $\cos\theta = \frac{1}{2}$ | M1 A1, M1 |

$\theta = 0$ or $\theta = \pm \frac{\pi}{3}$ | A1, A1 (6), (12) |

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A non-uniform rod $BC$ has mass $m$ and length $3l$. The centre of mass of the rod is at distance $l$ from $B$. The rod can turn freely about a fixed smooth horizontal axis through $B$. One end of a light elastic string, of natural length $l$ and modulus of elasticity $\frac{mg}{6}$, is attached to $C$. The other end of the string is attached to a point $P$ which is at a height $3l$ vertically above $B$.

\begin{enumerate}[label=(\alph*)]
\item Show that, while the string is stretched, the potential energy of the system is
$$mgl(\cos^2 \theta - \cos \theta) + \text{constant},$$
where $\theta$ is the angle between the string and the downward vertical and $-\frac{\pi}{2} < \theta < \frac{\pi}{2}$. [6]
\item Find the values of $\theta$ for which the system is in equilibrium with the string stretched. [6]
\end{enumerate}

\hfill \mbox{\textit{Edexcel M4 2005 Q5 [12]}}