CAIE FP2 2011 June — Question 11 EITHER

Exam BoardCAIE
ModuleFP2 (Further Pure Mathematics 2)
Year2011
SessionJune
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments of inertia
TypeComposite body MI calculation
DifficultyChallenging +1.8 This is a multi-part Further Maths mechanics question requiring: (1) proving a given moment of inertia result using standard formulas and superposition, (2) applying the parallel axis theorem, and (3) using energy conservation with rotational dynamics. While it involves several steps and Further Maths content (moments of inertia), each part follows standard techniques without requiring novel geometric insight. The proof is guided by the given answer, and the energy method for the final part is a routine application once the moment of inertia is established.
Spec6.02i Conservation of energy: mechanical energy principle6.04c Composite bodies: centre of mass6.04d Integration: for centre of mass of laminas/solids6.04e Rigid body equilibrium: coplanar forces

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A rigid body is made from uniform wire of negligible thickness and is in the form of a square \(A B C D\) of mass \(M\) enclosed within a circular ring of radius \(a\) and mass \(2 M\). The centres of the square and the circle coincide at \(O\) and the corners of the square are joined to the circle (see diagram). Show that the moment of inertia of the body about an axis through \(O\), perpendicular to the plane of the body, is \(\frac { 8 } { 3 } M a ^ { 2 }\). Hence find the moment of inertia of the body about an axis \(l\), through \(A\), in the plane of the body and tangential to the circle. A particle \(P\) of mass \(M\) is now attached to the body at \(C\). The system is able to rotate freely about the fixed axis \(l\), which is horizontal. The system is released from rest with \(A C\) making an angle of \(60 ^ { \circ }\) with the upward vertical. Find, in terms of \(a\) and \(g\), the greatest speed of \(P\) in the subsequent motion.

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A rigid body is made from uniform wire of negligible thickness and is in the form of a square $A B C D$ of mass $M$ enclosed within a circular ring of radius $a$ and mass $2 M$. The centres of the square and the circle coincide at $O$ and the corners of the square are joined to the circle (see diagram). Show that the moment of inertia of the body about an axis through $O$, perpendicular to the plane of the body, is $\frac { 8 } { 3 } M a ^ { 2 }$.

Hence find the moment of inertia of the body about an axis $l$, through $A$, in the plane of the body and tangential to the circle.

A particle $P$ of mass $M$ is now attached to the body at $C$. The system is able to rotate freely about the fixed axis $l$, which is horizontal. The system is released from rest with $A C$ making an angle of $60 ^ { \circ }$ with the upward vertical. Find, in terms of $a$ and $g$, the greatest speed of $P$ in the subsequent motion.

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