2019
DOI: 10.1016/j.jfluidstructs.2019.05.010
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Experimental investigation of flutter characteristics of shallowΠsection at post-critical regime

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Cited by 44 publications
(14 citation statements)
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“…The solving of Equation (29) was performed by an explicit Newmark-β method through an iteration procedure. During the calculation, the amplitude-dependent effect of structural damping ratios ( α0 ξ , h0 ξ ) and frequencies ( t0 ω , h0 ω ) were also considered, for which one can refer to the previous studies by Gao and Zhu [6]. Figure 22 shows the calculated post-critical LCOs for Case B1 when U* = 7.785.…”
Section: Aerodynamic Nonlinearitymentioning
confidence: 99%
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“…The solving of Equation (29) was performed by an explicit Newmark-β method through an iteration procedure. During the calculation, the amplitude-dependent effect of structural damping ratios ( α0 ξ , h0 ξ ) and frequencies ( t0 ω , h0 ω ) were also considered, for which one can refer to the previous studies by Gao and Zhu [6]. Figure 22 shows the calculated post-critical LCOs for Case B1 when U* = 7.785.…”
Section: Aerodynamic Nonlinearitymentioning
confidence: 99%
“…Experimental and numerical evidences suggest that the aerodynamic nonlinearity under large amplitude will introduce a secondary stabilizing effect and the flutter performance manifests as a soft-type nonlinear flutter instability [2][3][4][5][6][7][8][9][10][11][12][13][14]. When wind velocity exceeds beyond linear flutter boundary, there is a possible existence of nonlinear post-critical limit cycle oscillation (LCOs) due to the aerodynamic nonlinearity.…”
Section: Introductionmentioning
confidence: 99%
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