OCR M4 2004 January — Question 5 9 marks

Exam BoardOCR
ModuleM4 (Mechanics 4)
Year2004
SessionJanuary
Marks9
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments of inertia
TypeEnergy method angular speed
DifficultyChallenging +1.2 This is a standard M4 rotation problem requiring parallel axis theorem, torque equation, and energy methods. While it involves multiple steps and careful application of mechanics principles, the techniques are well-practiced at this level with no novel insights required. The presence of a constant frictional couple adds moderate complexity beyond basic textbook exercises.
Spec6.04d Integration: for centre of mass of laminas/solids

5 \includegraphics[max width=\textwidth, alt={}, center]{4cac1898-8251-4cda-bbbc-c2c30fde5a6e-2_618_627_1594_743} A uniform circular disc has mass 4 kg , radius 0.6 m and centre \(C\). The disc can rotate in a vertical plane about a fixed horizontal axis which is perpendicular to the disc and which passes through the point \(A\) on the disc, where \(A C = 0.4 \mathrm {~m}\). A frictional couple of constant moment 4.8 Nm opposes the motion. The disc is released from rest with \(A C\) horizontal (see diagram).
  1. Find the moment of inertia of the disc about the axis through \(A\).
  2. Find the angular acceleration of the disc immediately after it is released.
  3. Find the angular speed of the disc when \(C\) is first vertically below \(A\).

AnswerMarks Guidance
\(I_C = \frac{1}{2}mr^2 = \frac{1}{2} \times 4 \times 0.6^2 = 0.72\)B1 Moment of inertia of cylinder
\(I_A = I_C + m \times 0.4^2 = 1.36\) kg m²M1 A1 Parallel axes theorem applied correctly
\(C = I\alpha\)
\(39.2 \times 0.4 - 4.8 = 1.36 \times \alpha\)
AnswerMarks Guidance
\(\alpha = 8.00\) rad s⁻¹M1 A1 [3] Torque equation at release
Gain in K.E. = loss in G.P.E. - work done by friction
\(\frac{1}{2}I\omega^2 = 4 \times 9.8 \times 0.4 - 4.8 \times \frac{3}{4}\)
\(\omega^2 = 11.9708...\)
AnswerMarks Guidance
\(\omega = 3.46\) rad s⁻¹M1 M1 A1 [4] Energy equation with all three terms; solving for \(\omega\)
$I_C = \frac{1}{2}mr^2 = \frac{1}{2} \times 4 \times 0.6^2 = 0.72$ | B1 | Moment of inertia of cylinder

$I_A = I_C + m \times 0.4^2 = 1.36$ kg m² | M1 A1 | Parallel axes theorem applied correctly

$C = I\alpha$
$39.2 \times 0.4 - 4.8 = 1.36 \times \alpha$
$\alpha = 8.00$ rad s⁻¹ | M1 A1 | [3] Torque equation at release

Gain in K.E. = loss in G.P.E. - work done by friction
$\frac{1}{2}I\omega^2 = 4 \times 9.8 \times 0.4 - 4.8 \times \frac{3}{4}$
$\omega^2 = 11.9708...$
$\omega = 3.46$ rad s⁻¹ | M1 M1 A1 | [4] Energy equation with all three terms; solving for $\omega$

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5\\
\includegraphics[max width=\textwidth, alt={}, center]{4cac1898-8251-4cda-bbbc-c2c30fde5a6e-2_618_627_1594_743}

A uniform circular disc has mass 4 kg , radius 0.6 m and centre $C$. The disc can rotate in a vertical plane about a fixed horizontal axis which is perpendicular to the disc and which passes through the point $A$ on the disc, where $A C = 0.4 \mathrm {~m}$. A frictional couple of constant moment 4.8 Nm opposes the motion. The disc is released from rest with $A C$ horizontal (see diagram).\\
(i) Find the moment of inertia of the disc about the axis through $A$.\\
(ii) Find the angular acceleration of the disc immediately after it is released.\\
(iii) Find the angular speed of the disc when $C$ is first vertically below $A$.

\hfill \mbox{\textit{OCR M4 2004 Q5 [9]}}