OCR M4 2002 January — Question 4 8 marks

Exam BoardOCR
ModuleM4 (Mechanics 4)
Year2002
SessionJanuary
Marks8
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments of inertia
TypeEquation of motion angular acceleration
DifficultyChallenging +1.2 This is a Further Maths M4 question requiring the parallel axis theorem, rotational dynamics, and force analysis. Part (i) is standard application of parallel axis theorem (I = ½ma² + m(a/3)²). Parts (ii-iii) require torque equation and constraint forces, which are routine M4 techniques but involve multiple connected steps and careful vector consideration, making it moderately challenging even for Further Maths students.
Spec6.04d Integration: for centre of mass of laminas/solids6.05f Vertical circle: motion including free fall

4 A uniform circular disc has mass \(m\), radius \(a\) and centre \(C\). The disc is free to rotate in a vertical plane about a fixed horizontal axis passing through a point \(A\) on the disc, where \(C A = \frac { 1 } { 3 } a\).
  1. Find the moment of inertia of the disc about this axis. The disc is released from rest with \(C A\) horizontal.
  2. Find the initial angular acceleration of the disc.
  3. State the direction of the force acting on the disc at \(A\) immediately after release, and find its magnitude.

AnswerMarks Guidance
Parallel axes ruleM1, A1 \(I_A = I_c + m(\frac{a}{3})^2 = \frac{1}{3}ma^2 + \frac{1}{9}ma^2 = \frac{11}{9}ma^2\)
On release - Moment equationM1 \(M(A): C = I\ddot{\theta}\); \(mg(\frac{a}{4}) = (\frac{11}{9}ma^2)\ddot{\theta}\)
Angular accelerationA1 \(\ddot{\theta} = \frac{9g}{44a}\)
Force on disc at AM1 When released from rest, no 'central' force needed to maintain circular motion about A, so force on disc is purely vertical (upwards)
Vertical force equationM1 \(N2(1): mg - F = m(r\ddot{\theta})\)
Centripetal force calculationA1 \(F = mg - m(\frac{a}{3}a)(\frac{9g}{44a}) = \frac{8}{11}mg\)
**Parallel axes rule** | M1, A1 | $I_A = I_c + m(\frac{a}{3})^2 = \frac{1}{3}ma^2 + \frac{1}{9}ma^2 = \frac{11}{9}ma^2$

**On release - Moment equation** | M1 | $M(A): C = I\ddot{\theta}$; $mg(\frac{a}{4}) = (\frac{11}{9}ma^2)\ddot{\theta}$

**Angular acceleration** | A1 | $\ddot{\theta} = \frac{9g}{44a}$

**Force on disc at A** | M1 | When released from rest, no 'central' force needed to maintain circular motion about A, so force on disc is purely vertical (upwards)

**Vertical force equation** | M1 | $N2(1): mg - F = m(r\ddot{\theta})$

**Centripetal force calculation** | A1 | $F = mg - m(\frac{a}{3}a)(\frac{9g}{44a}) = \frac{8}{11}mg$

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4 A uniform circular disc has mass $m$, radius $a$ and centre $C$. The disc is free to rotate in a vertical plane about a fixed horizontal axis passing through a point $A$ on the disc, where $C A = \frac { 1 } { 3 } a$.\\
(i) Find the moment of inertia of the disc about this axis.

The disc is released from rest with $C A$ horizontal.\\
(ii) Find the initial angular acceleration of the disc.\\
(iii) State the direction of the force acting on the disc at $A$ immediately after release, and find its magnitude.

\hfill \mbox{\textit{OCR M4 2002 Q4 [8]}}