A mass on a damped spring obeys

PHYSICS · Subjective · Fermi University Physics · Mathematical Methods for Physics · Oscillations, Waves & Acoustics · Simple, damped and driven oscillations

Mathematical Methods for Physics, Ch Fourier transforms, spectra and convolution

Problem

A mass on a damped spring obeys x¨+γx˙+ω02x=f(t)/m\ddot x + \gamma\dot x + \omega_0^2 x = f(t)/m, with m=0.20 kgm = 0.20\,\mathrm{kg}, ω0=50 rad s−1\omega_0 = 50\,\mathrm{rad\,s^{-1}} and γ=4.0 s−1\gamma = 4.0\,\mathrm{s^{-1}}. It is driven by f(t)=F0cos⁡(ωt)f(t) = F_0\cos(\omega t) with F0=3.0 NF_0 = 3.0\,\mathrm{N} and ω=48 rad s−1\omega = 48\,\mathrm{rad\,s^{-1}}. In the steady state the response is a single component, x(t)=Re(Xe−iωt)x(t) = \mathrm{Re}(Xe^{-i\omega t}), with complex amplitude XX, driven by F0e−iωtF_0e^{-i\omega t}. Using the rule d/dt→−iω\mathrm{d}/\mathrm{d}t \to -i\omega that the derivative theorem gives for a component varying as e−iωte^{-i\omega t}, obtain the peak displacement amplitude ∣X∣|X| without integrating the equation directly.

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