Classical Mechanics (Kibble & Berkshire) · Problem 5.5

Energy conservation — T.W.B. Kibble, F.H. Berkshire

Physics — Mechanics · free-linear-oscillations

Problem

A damped oscillator satisfies the equation x¨+2Kx˙+Ω2x=0\ddot{x} + 2K\dot{x} + \Omega^2 x = 0 where KK and Ω\Omega are positive constants with K<ΩK < \Omega (under-damping). At time t=0t = 0 the particle is released from rest at the point x=ax = a. Show that the subsequent motion is given by x=ae−Kt(cos⁡ΩDt+KΩDsin⁡ΩDt),x = ae^{-Kt}\left(\cos\Omega_D t + \frac{K}{\Omega_D}\sin\Omega_D t\right), where ΩD=(Ω2−K2)1/2\Omega_D = (\Omega^2 - K^2)^{1/2}. Find all the turning points of the function x(t)x(t) and show that the ratio of successive maximum values of xx is e−2πK/ΩDe^{-2\pi K/\Omega_D}. A certain damped oscillator has mass 10 kg, period 5 s and successive maximum values of its displacement are in the ratio 3:13:1. Find the values of the spring and damping constants α\alpha and β\beta.

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