Numerical study on two-degree-of-freedom vortex induced vibrations suppression of a circular cylinder via synthetic jets at different excitation frequencies

https://doi.org/10.1016/j.ijheatfluidflow.2020.108593Get rights and content

Highlights

  • In-phase synthetic jets have the best performance on 2DOF VIVs suppression.

  • Lock-in phenomena in low fsj* range may discount the 2DOF VIVs suppression.

  • When fsj* ≥ 3.2, δCd decreases with Δφ increasing, δCl shows reverse changing trend.

  • Vortex patterns are significantly different in two SJ phases when fsj* is very low.

Abstract

In this work, a pair of synthetic jets are investigated for control of vortex induced vibration (VIV) of a circular cylinder in uniform flow in the low Reynolds number regime. In particular, the study focuses on three representative phase differences (0, π/2, and π) between the pair of synthetic jets to study the influence of synthetic jet excitation frequency ratio fsj* (fsj* = fsj/fn,water) on 2DOF VIVs control by two-dimensional numerical simulation. The Reynolds number is fixed at 150, the mass ratio m* (m* = mosc/md) of the circular cylinder is 2.0, and the natural oscillation frequencies in the in-flow and cross-flow directions are equal. The amplitude response, frequency response, hydrodynamic forces, and wake patterns are analyzed. The results show that both in-flow and cross-flow oscillations of the circular cylinder can be significantly suppressed by synthetic jets with various phase differences, and the wake becomes symmetric when fsj* ≥ 4.0. When fsj* < 4.0, many fluctuations can be observed from the changing curves of in-flow and cross-flow oscillation amplitudes, and the oscillation may be enhanced by the occurrence of lock-in between the oscillation frequencies and the synthetic jet excitation frequencies. Besides, vortex shedding modes of the controlled cases are significantly different in blowing and suction phases of the synthetic jet, when the excitation frequency is very low, such as fsj* = 0.2.

Introduction

As a novel flow control method, synthetic jets (SJs) have gained a lot of attention over the last two decades. Synthetic jets are generated using an actuator that consists of a cavity with an orifice, backed with a diaphragm that is driven sinusoidally. This causes periodic expulsion and ingestion of fluid through the orifice (Jeyalingam and Jabbal, 2018), and a quasi-steady jet can be formed some distance from the orfice. This is called the syntheic jet as it is synthesised from the surrounding fluid. Compared with passive control technology (Ding et al., 2016; J. Wang et al., 2019; Zhu et al., 2019; Hu et al., 2019; Ding et al., 2020; L.J. Wang et al., 2019; Chen et al., 2017), synthetic jets can cause local and global modification by imparting momentum and vorticity to the external flow. Therefore, synthetic jets have been adopted in a variety of fields, such as delaying the flow separation (Monir et al., 2014; Choi et al., 2018), enhancing heat transfer (Paolillo et al., 2019), decreasing vibration and noise (Nelson et al., 2017), and so on.

In recent years, some scholars have tried to use this novel strategy to control the vortex formation and evolution in the wake of the circular cylinder (DeMauro et al., 2013; Feng and Wang, 2014; C.L. Wang et al., 2017). The alternating vortex shedding in the wake of the circular cylinder is responsible for the occurrence of vortex induced vibration (VIV) (Baek et al., 2001), especially when the phenomenon of “VIV lock-in” or “synchronization” occurs, causing strong oscillations to be excited (Yan et al., 2019; Feng et al., 2019). Feng and Wang (Feng and Wang, 2010) experimentally studied the flow around a circular cylinder controlled by a synthetic jet positioned at the rear stagnation point, at a Reynolds number of 950. They found that the synthetic jet vortex pair can induce a symmetric vortex shedding mode, and the synchronization between the wake vortex and the synthetic jet at a certain range of excitation frequency was also observed. Feng and Wang (Feng and Wang, 2012) further investigated the influence of the suction duty cycle factor of a synthetic jet generated by a non-sinusoidal waveform, on controlling the flow around a circular cylinder at Re = 950. The results showed that the flow separation around the circular cylinder can be well controlled by the synthetic jet during both suction and blowing cycles, and the blowing process had better control effect when the blowing and suction velocities were the same. In addition, the control efficiency on drag reduction was found to decrease with decreasing suction cycle factor. However, Wang et al. (Wang et al., 2016), using a pair of symmetric synthetic jets at Re = 100, found that the synthetic jets operational range for suppressing VIV of a circular cylinder was much narrower than that for the fixed circular cylinder in which the lift oscillation can be completely suppressed. This was attributed to the cylinder oscillation inducing large relative flow speeds around the cylinder, resulting in shear layers with larger vorticity.

While a number of studies have been carried out, on the influence of synthetic jets for VIV control of circular cylinders, only very limited number and range of parameters, of importance to the problem, have been investigated so far. When utilizing a pair of synthetic jets, their phase difference, location around the cylinder, orientation angle, actuation frequency relative to the natural frequencies, and momentum coefficient among others, could have a strong influence of on the flow around the cylinder, and therefore on VIV control. Therefore, in order to realize optimal synthetic jet based VIV flow control solutions for real world applications, it is necessary to fill the knowledge gaps though further studies on the influence of these crucial parameters. This is especially so, for two-degree-of-freedom (2DOF) vortex induced vibrations control. In our previous work (H.B. Wang et al., 2019), the effects of synthetic jet position angle α and momentum coefficient Cu on 2DOF VIVs have been revealed. Furthermore, we have shown that symmetric synthetic jets issued in the streamwise direction can effectively mitigate 2DOF VIVs of the circular cylinder when positioned at the leeward side of the cylinder, and when Cu ≥ 2.0. Synthetic jet (SJ) excitation frequency is another important parameter for SJ-based control. According to the work of Wang et al. (C.L. Wang et al., 2017), synthetic jets pairs with various phase differences, over a wide frequency range, can cause the appearance of various lock-in phenomena, which are not always helpful for one-degree-of-freedom VIV suppression.

In the present work, the study is extended to two-degree-of-freedom VIVs and the influence of synthetic excitation frequency and phase difference between the pair of synthetic jets, on VIV control, are systematically studied. The Reynolds number is fixed at 150 (Re = 150) in the present work, and the flow in the wake of the circular cylinder is two-dimensional (W.L. Chen et al., 2018; Shaaban and Mohany, 2018; Zou et al., 2019). Therefore, two-dimensional numerical simulations are conducted in the study.

The paper is arranged as follows. In Section 2, the physical model under study, the numerical method and details are described. In Section 3, the details of the findings obtained in this work are discussed. The conclusions are finally drawn in Section 4.

Section snippets

Physical model

The physical model studied in this work is shown in Fig. 1. The circular cylinder is elastically supported and allowed to oscillate in both in-flow (x) and cross-flow (y) directions. D denotes the diameter of the circular cylinder and equals 0.01 m in this work. K1 and C1 are the stiffness of the spring and the structural damping per unit length in the cross-flow direction, respectively. K2 and C2 are the stiffness of the spring and the structural damping per unit length in the in-flow

VIV response controlled by synthetic jets with phase difference

For the circular cylinder controlled by a pair of synthetic jets with phase difference, the cross-flow oscillation amplitudes and frequencies are shown in Fig. 4. The horizontal lines in Fig. 4 represent the oscillation amplitude and frequency of the uncontrolled case in the cross-flow direction. The amplitude ratios in this work are calculated by A/D =AmaxAmin2D where Amax and Amin are the maximum and minimum displacements relative to the time-averaged position, respectively. The oscillation

Conclusions

In this work, the influence of synthetic jet excitation frequencies on 2DOF VIVs response of a circular cylinder, at a Re = 150, is studied in detail by numerical simulations. Three representative phase differences of a pair of synthetic jets (0, π/2, and π) used for flow control, are selected. The oscillation characters, hydrodynamic forces, and vortex patterns are analyzed. According to the results and discussion above, the following conclusions can be drawn:

  • (1)

    The synthetic jet excitation

CRediT authorship contribution statement

Haibo Wang: Conceptualization, Methodology, Formal analysis, Investigation, Writing - original draft. Lin Ding: Conceptualization, Software, Resources, Data curation, Writing - original draft, Funding acquisition. Li Zhang: Writing - review & editing, Supervision, Project administration. Rajnish N. Sharma: Resources, Writing - review & editing. Lin Yang: Investigation, Visualization.

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgments

The authors gratefully acknowledge the support from the National Natural Science Foundation of China (Grant No.51776021). Mr. Haibo Wang sincerely acknowledges the sponsorship from China Scholarship Council (Grant No. 201806050171).

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