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A uniform solid sphere with centre C, radius 2a and mass 3M, is pivoted about a smooth horizontal axis and hangs at rest - CIE - A-Level Further Maths - Question 5 - 2011 - Paper 1

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A uniform solid sphere with centre C, radius 2a and mass 3M, is pivoted about a smooth horizontal axis and hangs at rest. The point O on the axis is vertically above... show full transcript

Worked Solution & Example Answer:A uniform solid sphere with centre C, radius 2a and mass 3M, is pivoted about a smooth horizontal axis and hangs at rest - CIE - A-Level Further Maths - Question 5 - 2011 - Paper 1

Step 1

i. the period of small oscillations.

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Answer

To find the period of small oscillations, we start with the principle of angular motion and use the equation of motion for the swinging system:

  1. The moment of inertia of the sphere about its diameter is given as: Ic=253M(2a)2=24Ma25I_c = \frac{2}{5} \cdot 3M (2a)^2 = \frac{24Ma^2}{5}

  2. Next, we find the moment of inertia about the axis through O, which is: IO=Ic+Mh2I_O = I_c + Mh^2 where h=2ah = 2a (the vertical distance from the center of the sphere to point O). Thus, IO=24Ma25+3M(2a)2=24Ma25+12Ma2=84Ma25I_O = \frac{24Ma^2}{5} + 3M(2a)^2 = \frac{24Ma^2}{5} + 12Ma^2 = \frac{84Ma^2}{5}

  3. The equation of motion for small oscillations based on SHM yields: Id2θdt2=MgsinθI \frac{d^2\theta}{dt^2} = -Mg \sin\theta For small angles, sinθ\sin\theta can be approximated with θ\theta: Id2θdt2=MgθI \frac{d^2\theta}{dt^2} = -Mg\theta

  4. Thus, we can express the angular frequency ω\omega as: ω2=MgI\omega^2 = \frac{Mg}{I} Substituting our expression for IOI_O into this, we get: ω2=Mg84Ma25=5g84a2\omega^2 = \frac{Mg}{\frac{84Ma^2}{5}} = \frac{5g}{84a^2}

  5. The period TT can then be calculated as: T=2πIMg=2π84Ma25Mg=2π84a25gT = 2\pi \sqrt{\frac{I}{Mg}} = 2\pi \sqrt{\frac{84Ma^2}{5Mg}} = 2\pi \sqrt{\frac{84a^2}{5g}}

Step 2

ii. the time from release until OP makes an angle $ rac{1}{2}\alpha$ with the downward vertical for the first time.

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Answer

To calculate the time from release until OP makes an angle rac{1}{2}\alpha with the downward vertical:

  1. From the earlier analysis, the angular position as a function of time can be written as: θ(t)=αcos(ωt)\theta(t) = \alpha \cos(\omega t)

  2. We need to find the time tt when: θ(t)=12α\theta(t) = \frac{1}{2}\alpha Setting the equations equal gives: 12α=αcos(ωt)\frac{1}{2}\alpha = \alpha \cos(\omega t) This simplifies to: 12=cos(ωt)\frac{1}{2} = \cos(\omega t)

  3. The solution to this is: ωt=π3t=1ωπ3\omega t = \frac{\pi}{3} \Rightarrow t = \frac{1}{\omega} \cdot \frac{\pi}{3}

  4. Recalling that: ω=5g84a2\omega = \sqrt{\frac{5g}{84a^2}} The time can then be expressed as: t=15g84a2π3=π84a235gt = \frac{1}{\sqrt{\frac{5g}{84a^2}}} \cdot \frac{\pi}{3} = \frac{\pi \sqrt{84a^2}}{3 \sqrt{5g}}. Thus, the final expression for the time is: t=πa8435gt = \frac{\pi a \sqrt{84}}{3 \sqrt{5g}}.

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