Edexcel M5 2010 June — Question 3 16 marks

Exam BoardEdexcel
ModuleM5 (Mechanics 5)
Year2010
SessionJune
Marks16
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments of inertia
TypeSmall oscillations period
DifficultyChallenging +1.8 This M5 compound pendulum question requires: (a) a non-trivial integration to find moment of inertia about a parallel axis through the apex of a triangle, (b) applying perpendicular axis theorem and parallel axis theorem to find MOI about D, then using rotational dynamics with torque = Iα, and (c) small angle approximation for SHM period. The integration setup requires careful coordinate geometry, and the multi-step application of MOI theorems with rotational SHM is beyond standard A-level core content, placing it well above average difficulty.
Spec6.04d Integration: for centre of mass of laminas/solids6.04e Rigid body equilibrium: coplanar forces6.05f Vertical circle: motion including free fall

  1. A uniform lamina \(A B C\) of mass \(m\) is in the shape of an isosceles triangle with \(A B = A C = 5 a\) and \(B C = 8 a\).
    1. Show, using integration, that the moment of inertia of the lamina about an axis through \(A\), parallel to \(B C\), is \(\frac { 9 } { 2 } m a ^ { 2 }\).
    The foot of the perpendicular from \(A\) to \(B C\) is \(D\). The lamina is free to rotate in a vertical plane about a fixed smooth horizontal axis which passes through \(D\) and is perpendicular to the plane of the lamina. The lamina is released from rest when \(D A\) makes an angle \(\alpha\) with the downward vertical. It is given that the moment of inertia of the lamina about an axis through \(A\), perpendicular to \(B C\) and in the plane of the lamina, is \(\frac { 8 } { 3 } m a ^ { 2 }\).
  2. Find the angular acceleration of the lamina when \(D A\) makes an angle \(\theta\) with the downward vertical. Given that \(\alpha\) is small,
  3. find an approximate value for the period of oscillation of the lamina about the vertical.

Question 3:
Part (a):
AnswerMarks Guidance
Working/AnswerMark Notes
\(\delta A = \frac{8x}{3}\delta x\)M1 A1
\(\delta m = \frac{8x}{3}\delta x \cdot \frac{m}{12a^2}\) or \(\delta m = \frac{8x}{3}\delta x \cdot \rho\)DM1
\(\delta I = \frac{8x}{3}\delta x \cdot \frac{m}{12a^2} \cdot x^2 \left(= \frac{2m}{9a^2}x^3\delta x\right)\)A1
\(I = \int_0^{3a} \frac{2m}{9a^2}x^3\,dx\)M1
\(= \frac{2m}{9a^2}\left[\frac{x^4}{4}\right]_0^{3a}\)
\(= \frac{9ma^2}{2}\) *A1 Total: (6)
Part (b):
AnswerMarks Guidance
Working/AnswerMark Notes
\(I_A = \frac{9ma^2}{2} + \frac{8ma^2}{3} = \frac{43ma^2}{6}\) (perp axes rule)M1 A1
\(I_A = I_G + m(2a)^2\) (parallel axes rule)DM1 A1
\(I_D = I_G + ma^2\) (parallel axes rule)A1
\(I_D = \frac{43ma^2}{6} - 3ma^2 = \frac{25ma^2}{6}\)A1
\(mga\sin\theta = -\frac{25ma^2}{6}\ddot{\theta}\)M1
\(\ddot{\theta} = -\frac{6g}{25a}\sin\theta\)A1 Total: (8)
Part (c):
AnswerMarks Guidance
Working/AnswerMark Notes
For small \(\theta\), \(\ddot{\theta} = -\frac{6g}{25a}\theta\) SHMM1
\(T = 2\pi\sqrt{\frac{25a}{6g}} = 5\pi\sqrt{\frac{2a}{3g}}\)A1 Total: (2), Q Total: 16
## Question 3:

### Part (a):

| Working/Answer | Mark | Notes |
|---|---|---|
| $\delta A = \frac{8x}{3}\delta x$ | M1 A1 | |
| $\delta m = \frac{8x}{3}\delta x \cdot \frac{m}{12a^2}$ or $\delta m = \frac{8x}{3}\delta x \cdot \rho$ | DM1 | |
| $\delta I = \frac{8x}{3}\delta x \cdot \frac{m}{12a^2} \cdot x^2 \left(= \frac{2m}{9a^2}x^3\delta x\right)$ | A1 | |
| $I = \int_0^{3a} \frac{2m}{9a^2}x^3\,dx$ | M1 | |
| $= \frac{2m}{9a^2}\left[\frac{x^4}{4}\right]_0^{3a}$ | | |
| $= \frac{9ma^2}{2}$ * | A1 | **Total: (6)** |

### Part (b):

| Working/Answer | Mark | Notes |
|---|---|---|
| $I_A = \frac{9ma^2}{2} + \frac{8ma^2}{3} = \frac{43ma^2}{6}$ (perp axes rule) | M1 A1 | |
| $I_A = I_G + m(2a)^2$ (parallel axes rule) | DM1 A1 | |
| $I_D = I_G + ma^2$ (parallel axes rule) | A1 | |
| $I_D = \frac{43ma^2}{6} - 3ma^2 = \frac{25ma^2}{6}$ | A1 | |
| $mga\sin\theta = -\frac{25ma^2}{6}\ddot{\theta}$ | M1 | |
| $\ddot{\theta} = -\frac{6g}{25a}\sin\theta$ | A1 | **Total: (8)** |

### Part (c):

| Working/Answer | Mark | Notes |
|---|---|---|
| For small $\theta$, $\ddot{\theta} = -\frac{6g}{25a}\theta$ SHM | M1 | |
| $T = 2\pi\sqrt{\frac{25a}{6g}} = 5\pi\sqrt{\frac{2a}{3g}}$ | A1 | **Total: (2), Q Total: 16** |

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\begin{enumerate}
  \item A uniform lamina $A B C$ of mass $m$ is in the shape of an isosceles triangle with $A B = A C = 5 a$ and $B C = 8 a$.\\
(a) Show, using integration, that the moment of inertia of the lamina about an axis through $A$, parallel to $B C$, is $\frac { 9 } { 2 } m a ^ { 2 }$.
\end{enumerate}

The foot of the perpendicular from $A$ to $B C$ is $D$. The lamina is free to rotate in a vertical plane about a fixed smooth horizontal axis which passes through $D$ and is perpendicular to the plane of the lamina. The lamina is released from rest when $D A$ makes an angle $\alpha$ with the downward vertical. It is given that the moment of inertia of the lamina about an axis through $A$, perpendicular to $B C$ and in the plane of the lamina, is $\frac { 8 } { 3 } m a ^ { 2 }$.\\
(b) Find the angular acceleration of the lamina when $D A$ makes an angle $\theta$ with the downward vertical.

Given that $\alpha$ is small,\\
(c) find an approximate value for the period of oscillation of the lamina about the vertical.

\hfill \mbox{\textit{Edexcel M5 2010 Q3 [16]}}