A pedestrian bridge deck is driven by footfall at a fixed angular frequency (a…

PHYSICS · Multi-part · Fermi University Physics · Oscillations, Waves & Acoustics · Simple, damped and driven oscillations · Simple, damped and driven oscillations

Mathematical Methods for Physics, Ch Second-order linear equations: damping, driving and resonance

Problem

A pedestrian bridge deck is driven by footfall at a fixed angular frequency ω=12.57 rad s−1\omega = 12.57\,\mathrm{rad\,s^{-1}} (a walking rate of 2.0 Hz2.0\,\mathrm{Hz}), with F0/m=3.0 m s−2F_0/m = 3.0\,\mathrm{m\,s^{-2}} and damping rate γ=1.0 s−1\gamma = 1.0\,\mathrm{s^{-1}} fixed by the deck's construction. Engineers consider three stiffening designs giving natural angular frequencies ω0=5.0 rad s−1\omega_0 = 5.0\,\mathrm{rad\,s^{-1}}, ω0=10 rad s−1\omega_0 = 10\,\mathrm{rad\,s^{-1}} and ω0=15 rad s−1\omega_0 = 15\,\mathrm{rad\,s^{-1}}. ((a)) Compute ∣A~∣|\tilde{A}| and the phase lag ϕ\phi for each of the three designs. ((b)) State which design gives the largest response to the walking drive and explain the trend in one sentence.

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