Abstract

Wind-tunnel experiments are performed to investigate the effects of trailing-edge reattachment on the flutter behaviors of spring-suspended trailing-edge-changeable section models. Different Trailing edges (TE) were fixed at the back of a body to adjust reattachment of the vortex. A laser-displacement system was used to acquire the vibration signals. The relationship between flutter characteristics and TEs that affects the wake mode was analyzed. The results show that the motion of the wake vortex has a certain correlation with the flutter stability of the bridge deck. Limit cycle flutter (LCF) occurs to a section model with a 30° TE, whose amplitude gradually increases as the wind speed increases, and the vibration develops into a hard flutter when the wind speed is 12.43 m/s. A section model with 180 TE reaches a hard flutter when the wind speed is 15.31 m/s, without the stage of LCF. As the TE becomes more and more blunt, the critical wind speed, Us, gradually increases, meaning the flutter stability gradually increases. The results reveal that LCF may still occur to the bridge section with a streamlined front edge, and, in some cases, it also may have a range of wind speeds in which LCF occurs.

Highlights

  • Flutter is a phenomenon of aerodynamic instability caused by the interaction of fluid and the vibration of structure, which was first found on thin wings

  • The results show that only the first-order component of the self-excited force contributes significantly to the energy input of Limit cycle flutter (LCF) of the bridge deck, while the influence of the higher-order force component is negligible, which means considering only the first-order component of the self-excited nonlinear force can well predict the displacement response of LCF of the bridge deck

  • The results show that the width-to-depth ratio of the bridge deck plays an important role in the aerodynamic performance of the bridge

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Summary

Introduction

Flutter is a phenomenon of aerodynamic instability caused by the interaction of fluid and the vibration of structure, which was first found on thin wings. Based on Scanlan’s linear flutter theory, Bartoli et al [8] proposed an approximate method to calculate the critical wind speed and frequency of flutter by the analysis of a large number of dynamics and aerodynamics data, which only requires three flutter derivatives (H1∗ , A2∗ , and A3∗ ) or two flutter derivatives (H1∗ and A2∗ ) to perform the calculation, and greatly simplifies the approximate calculation of critical wind speed and frequency of flutter It is suitable for bridges with the section whose bending-torsion coupling is only affected by the shape of a structural mode or a higher mode, but it cannot completely replace more accurate analysis methods. Zhang et al in 2017 [15] researched the flutter characteristics of streamlined bridge decks by using a comprehensive wind tunnel test and introduced a nonlinear mathematical model to simulate the aeroelastic behavior of nonlinear torsional flutter. The blockage ratio is 4.25%.ratio is details of thedynamic model’scharacteristics dynamic characteristics are shown in Table

Measurement Details
Dynamic Response of Flutter with
Time history of displacement of the bridge deck in case
11. Time history of vibration divergence in 30c-90
Frequency Domain Analysis
Wavelet and Hilbert Analysis
16. Distribution of vibration casewhen
17. Phase trajectory case of
Phase Lag between Torsional and Vertcial Vibration
18. Phase trajectory of case
Discussion of Effect of TE
Conclusions
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