Question
Question: A thin ring of volume mass density $\rho$, cross-sectional area A, radius R and young's modulus of e...
A thin ring of volume mass density ρ, cross-sectional area A, radius R and young's modulus of elasticity E, is rotated about an axis passing through its centre with angular velocity ω. If increases in cirumference (assumed small) is aE18πR3ρω2. Find a.

9
Solution
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Tension in the rotating ring: Consider a small element of the ring of mass dm at radius R. The centrifugal force acting on this element is dF=dm⋅Rω2. If the volume mass density is ρ and the cross-sectional area is A, the mass of an infinitesimal arc element ds=Rdθ is dm=ρ⋅A⋅ds=ρARdθ. The centrifugal force on this element is dF=(ρARdθ)Rω2=ρAR2ω2dθ. This outward force is balanced by the inward radial component of the tension T in the ring. For a small angle dθ, the inward radial component of tension is Tdθ. Equating these, Tdθ=ρAR2ω2dθ, which gives the tension T=ρAR2ω2.
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Strain and increase in circumference: Young's modulus E is defined as stress/strain. The stress in the ring material is σ=T/A. The strain is ϵ=σ/E=(T/A)/E=T/(AE). The increase in the circumference ΔC is given by ΔC=ϵ⋅C, where C=2πR is the original circumference. Substituting the expression for strain: ΔC=AET⋅(2πR) Substituting the expression for tension T=ρAR2ω2: ΔC=AEρAR2ω2⋅(2πR)=E2πR3ρω2
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Finding 'a': The problem states that the increase in circumference is aE18πR3ρω2. Equating our derived expression for ΔC with the given expression: E2πR3ρω2=aE18πR3ρω2 Cancelling the common terms (π, R3, ρ, ω2, E) from both sides, we get: 2=a18 Solving for a: a=218=9