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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\rho, 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\omega. If increases in cirumference (assumed small) is 18πR3ρω2aE\frac{18\pi R^{3}\rho\omega^{2}}{aE}. Find a.

Answer

9

Explanation

Solution

  1. Tension in the rotating ring: Consider a small element of the ring of mass dmdm at radius RR. The centrifugal force acting on this element is dF=dmRω2dF = dm \cdot R\omega^2. If the volume mass density is ρ\rho and the cross-sectional area is AA, the mass of an infinitesimal arc element ds=Rdθds = R d\theta is dm=ρAds=ρARdθdm = \rho \cdot A \cdot ds = \rho A R d\theta. The centrifugal force on this element is dF=(ρARdθ)Rω2=ρAR2ω2dθdF = (\rho A R d\theta) R\omega^2 = \rho A R^2 \omega^2 d\theta. This outward force is balanced by the inward radial component of the tension TT in the ring. For a small angle dθd\theta, the inward radial component of tension is TdθT d\theta. Equating these, Tdθ=ρAR2ω2dθT d\theta = \rho A R^2 \omega^2 d\theta, which gives the tension T=ρAR2ω2T = \rho A R^2 \omega^2.

  2. Strain and increase in circumference: Young's modulus EE is defined as stress/strain. The stress in the ring material is σ=T/A\sigma = T/A. The strain is ϵ=σ/E=(T/A)/E=T/(AE)\epsilon = \sigma/E = (T/A)/E = T/(AE). The increase in the circumference ΔC\Delta C is given by ΔC=ϵC\Delta C = \epsilon \cdot C, where C=2πRC = 2\pi R is the original circumference. Substituting the expression for strain: ΔC=TAE(2πR)\Delta C = \frac{T}{AE} \cdot (2\pi R) Substituting the expression for tension T=ρAR2ω2T = \rho A R^2 \omega^2: ΔC=ρAR2ω2AE(2πR)=2πR3ρω2E\Delta C = \frac{\rho A R^2 \omega^2}{AE} \cdot (2\pi R) = \frac{2\pi R^3 \rho \omega^2}{E}

  3. Finding 'a': The problem states that the increase in circumference is 18πR3ρω2aE\frac{18\pi R^{3}\rho\omega^{2}}{aE}. Equating our derived expression for ΔC\Delta C with the given expression: 2πR3ρω2E=18πR3ρω2aE\frac{2\pi R^3 \rho \omega^2}{E} = \frac{18\pi R^{3}\rho\omega^{2}}{aE} Cancelling the common terms (π\pi, R3R^3, ρ\rho, ω2\omega^2, EE) from both sides, we get: 2=18a2 = \frac{18}{a} Solving for aa: a=182=9a = \frac{18}{2} = 9