2019
DOI: 10.1016/j.jweia.2019.03.010
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Energy budget analysis and engineering modeling of post-flutter limit cycle oscillation of a bridge deck

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Cited by 45 publications
(26 citation statements)
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“…Positive attack angle 3 • corresponded to more significant drift of heaving static equilibrium position than attack angle 0 • . This phenomenon was also reported by Zhang et al [14] in a numerical study on a flat box bridge deck (side ratio B/D = 12.3) but not mentioned by Amandolese et al [8] in studying the post-critical behavior of a thin plate. The heaving static deformation is probably because of the aerodynamic asymmetry induced by large-amplitude oscillations of instantaneous attack angle.…”
Section: Bifurcation Beyond Linear Flutter Boundarysupporting
confidence: 73%
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“…Positive attack angle 3 • corresponded to more significant drift of heaving static equilibrium position than attack angle 0 • . This phenomenon was also reported by Zhang et al [14] in a numerical study on a flat box bridge deck (side ratio B/D = 12.3) but not mentioned by Amandolese et al [8] in studying the post-critical behavior of a thin plate. The heaving static deformation is probably because of the aerodynamic asymmetry induced by large-amplitude oscillations of instantaneous attack angle.…”
Section: Bifurcation Beyond Linear Flutter Boundarysupporting
confidence: 73%
“…where t i is the time point where the torsional displacement α(t) crosses zero axis. The amplitude-dependent aerodynamic damping ratio ξ se can then be obtained by subtracting the structural damping ξ s from the total damping ratio calculated by Equation (14). Figure 13 shows the calculated time-varying damping ratios and frequency during the DTS and GTS processes in Figure 12.…”
Section: Amplitude-dependent Damping and Frequencymentioning
confidence: 99%
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