Experimental study on mitigating vortex-induced vibration of a bridge by using passive vortex generators
Introduction
As wind passes around the long span bridge deck, the spanwise vortices will shed in the near wake. If the vortex shedding frequency is close to the natural frequency of the bridge deck, it can cause vortex-induced resonance. A vortex-induced vibration (VIV) is one of the major issues in long-span bridge vibration. Although the VIV is a self-limited vibration, it can introduce large displacements and cause discomfort to the drivers (Battista and Pfeil, 2000, Frandsen, 2001, Fujino and Yoshitaka, 2002, Larsen et al., 2000). In addition, vortex-induced resonance always occurs at low wind speeds and can lead to long-term fatigue damage.
Many types of control methods for suppressing VIV have been proposed. However, passive flow control methods are usually selected because of their reliability and simplicity. Fujino and Siringoringo (2013) provided a review of these control methods in bridge engineering. Conventional passive flow control attachments, which are always attached to the leading and trailing edges, include guide vanes, fairing, flaps, wind spoiler and deflector (Fujino and Siringoringo, 2013). Among them, guide vanes are more popularly used in suppressing VIV since they provide better control effect. Larsen et al. (2000) installed guide vanes on the Greatbelt bridge deck, which was then subjected to severe VIV, and observed a reduction in the amplitude of the VIV from the wind tunnel test results. Later, Larsen et al. (2008) investigated the vortex response of a twin box bridge with and without the guide vanes at three different Reynolds numbers and observed that the guide vanes had no obvious control effects on the VIV at low Reynolds number as no sufficient flow rate passed it with high boundary layer. Therefore, it indicated that the control effects of the guide vanes were sensitive to the Reynolds numbers. Further, the aerodynamic countermeasures above always increase the maintenance efforts and construction costs since these attachments need be installed along with the bridge deck. In addition, Larsen and Wall (2012) explored the effect of the shape on the VIV of trapezoidal box girder bridge decks and found that it was possible to derive a virtually vibration-free deck. However, this approach could fail if the shape was restricted because of the other requirements. Additionally, the shape of a vibration-free deck might also not be considered esthetic.
As the regular vortex shedding is the main source of the VIV, suppressing spanwise vortex shedding is an efficient way to mitigate the VIV of a bridge deck. The three-dimensional spanwise-varying control, which directly or indirectly changes the spanwise aerodynamic shape of a bluff body, is more efficient than the spanwise homogeneous method (based on 2D framework) on attenuating vortex shedding. Kim and Choi (2005) compared the momentum required for drag reduction of a 3D spanwise-varying control method and a spanwise homogeneous method (base bleeding). The results indicated that the momentum required of the three-dimensional forcing was significantly less than that of a conventional two-dimensional forcing (base bleeding). The underlying mechanism of the three-dimensional spanwise-varying control can be ascribed to the action of the secondary wake instability, which is also called the 3D instability of spanwise vortices (Hwang et al., 2013). There are mainly two types of secondary instabilities existing in a bluff body wake, namely the Modes-A and Modes-B (Williamson, 1996a, Williamson, 1996b, Wu et al., 1996). Both instability modes act as waves in the spanwise wake vortices, which evolve into pairs of counter-rotating streamwise vortices connecting the Karman vortices. These secondary streamwise vortices cause the spanwise dislocation of the Karman vortices and the energy transfer from the spanwise vortices to the streamwise vortices (Doddipatla et al., 2008). Because of the highly efficient control effects of the 3D spanwise-varying control, its application for mitigating vortex shedding and/or achieving drag reduction has attracted much attention. The numerical simulation results of Darekar and Sherwin (2001) showed that for providing spanwise sinusoidal perturbations at the leading and trailing edges for a square cylinder, the spanwise vortex shedding was highly suppressed at 10 < Re(d) < 150 (d being the character length of the bluff body) when the perturbation wavelength was 5.6d. Kim and Choi (2005) investigated the control effects of spanwise-periodic blowing/suction on reducing mean drag of a circular cylinder at the Reynolds numbers between 40 and 3900. The numerical results showed that the spanwise-periodic blowing/suction attenuated or annihilated the Kármán vortex shedding and thus significantly reduced the mean drag and the drag and lift fluctuations. Dobre et al. (2006) significantly attenuated the spanwise vortex shedding around a square cylinder by using spanwise sinusoidal perturbations with wavelengths of 2.4 d at the trailing edge at Re(d) = 12 500. Park et al. (2006) achieved 33% base pressure recovery at the Reynolds numbers up to Re(d) = 60 000 using spanwise arrays of vertical rectangular tabs at the trailing edge. Deshpande and Sharma (2012) used segmented trailing edges to achieve up to 34% base pressure recovery and nearly completed the suppression of vortex shedding at Re(d) = 8750. More related studies can be found in a review by Choi et al. (2008).
To the authors’ knowledge, very few studies have focused on the 3D spanwise-varying control effects on suppressing the VIV of bridges. El-Gammal et al. (2007) successfully suppressed the VIV of a girder by using spanwise periodic perturbation method (SPPM). In their study, the leading and the trailing edges of the deck were modified as a wave in the spanwise direction. However, the shape of the girder was changed dramatically, which could cause esthetic problems and affect other performance aspects. In this paper, the PVGs based on the 3D spanwise-varying control are proposed to attenuate the spanwise vortex shedding and mitigate the VIV of a bridge deck. The PVGs have been widely applied in airfoils to delay the boundary layer separation (Lin, 2002). The streamwise counter-rotating vortex structures (see Fig. 1, Von Stillfried et al., 2010) induced by vortex generators force the higher momentum fluid from the free stream towards the wall and increase the near-wall momentum. Consequently, the stabilised flow leads to the delay or prevention of separation of the boundary layers. As stated above, the streamwise vortices are able to cause the spanwise dislocation of the Karman vortices or even destroy the spanwise vortices. Therefore, the PVGs can be used to generate the streamwise counter-rotating vortex pairs directly and to activate the corresponding mode of secondary instability to suppress the spanwise vortex shedding and mitigate the VIV. Although the PVGs are widely used in boundary layer separation control, their application in controlling the VIV of bluff bodies is missing. Therefore, the main objectives of this study are to propose and design the spanwise-varying PVGs control method and then to investigate its control effects on suppressing the VIV of a bridge deck by wind tunnel tests.
Section snippets
Experiment setup
The present experiments were conducted in the wind tunnel at the Harbin Institute of Technology in China. The working section size of the wind tunnel was 4 m × 3 m × 25 m and its wind velocity range was from 2 m/s to 45 m/s. The maximum free stream turbulence intensity was 0.46% and the maximum free-stream non-uniformity was 1%. In this study, the oncoming flow in the tested cases was uniform and smooth. The wind induced motions of the deck model were measured by two laser reflexion sensors
Results and discussion
The results are presented as the plots of vertical or torsional response as function of the non-dimensional wind speed U/fvB or U/fαB, where U is the wind tunnel speed measured by a hot film anemometer set in the test section, fv and fα are the vertical bending frequency (5.25 Hz) and torsional frequency (9.61 Hz) respectively, B (775 mm) is the deck width. The vertical vibration displacement, y, is given as the root mean square (RMS) vertical response normalised by the section height H. The
Conclusions
Because of the high efficiency of 3D spanwise-varying method on suppressing vortex shedding behind the bluff body, the PVG, which can generate the streamwise vortices, was adopted to mitigate the VIV of a bridge. The wind tunnel tests were conducted to prove the control effects of the PVG on the VIV of both the naked bridge deck and the deck with railings. Major conclusions drawn are as follows:
- 1)
For the naked bridge deck, the spanwise-distributed PVGs with interval of 1–4H and 1–3H completely
Acknowledgement
The support for this work is provided in part by the National Natural Science Foundation of China (Grant No. 51378163) and is gratefully acknowledged. In addition, the work was performed in the Joint Laboratory of Wind Tunnel & Wave Flume at the School of Civil Engineering, Harbin Institute of Technology, in China.
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2022, Journal of Fluids and StructuresCitation Excerpt :When the HAMWTs were arranged at the TE, the vertical responses were close to zero, and the best control effect was produced. The results are similar to those obtained by Xin and Zhang (2018), who used passive vortex generators to create streamwise vortices to control VIV. Thus, the trailing edge is the critical position for controlling VIV.