Model reduction and mechanism for the vortex-induced vibrations of bluff bodies

We present an effective reduced-order model (ROM) technique to couple an incompressible flow with a transversely vibrating bluff body in a state-space format. The ROM of the unsteady wake flow is based on the Navier–Stokes equations and is constructed by means of an eigensystem realization algorithm (ERA). We investigate the underlying mechanism of vortex-induced vibration (VIV) of a circular cylinder at low Reynolds number via linear stability analysis. To understand the frequency lock-in mechanism and self-sustained VIV phenomenon, a systematic analysis is performed by examining the eigenvalue trajectories of the ERA-based ROM for a range of reduced oscillation frequency $(F_{s})$ , while maintaining fixed values of the Reynolds number ( $Re$ ) and mass ratio ( $m^{\ast }$ ). The effects of the Reynolds number $Re$ , the mass ratio $m^{\ast }$ and the rounding of a square cylinder are examined to generalize the proposed ERA-based ROM for the VIV lock-in analysis. The considered cylinder configurations are a basic square with sharp corners, a circle and three intermediate rounded squares, which are created by varying a single rounding parameter. The results show that the two frequency lock-in regimes, the so-called resonance and flutter, only exist when certain conditions are satisfied, and the regimes have a strong dependence on the shape of the bluff body, the Reynolds number and the mass ratio. In addition, the frequency lock-in during VIV of a square cylinder is found to be dominated by the resonance regime, without any coupled-mode flutter at low Reynolds number. To further discern the influence of geometry on the VIV lock-in mechanism, we consider the smooth curve geometry of an ellipse and two sharp corner geometries of forward triangle and diamond-shaped bluff bodies. While the ellipse and diamond geometries exhibit the flutter and mixed resonance–flutter regimes, the forward triangle undergoes only the flutter-induced lock-in for $30\leqslant Re\leqslant 100$ at $m^{\ast }=10$ . In the case of the forward triangle configuration, the ERA-based ROM accurately predicts the low-frequency galloping instability. We observe a kink in the amplitude response associated with 1:3 synchronization, whereby the forward triangular body oscillates at a single dominant frequency but the lift force has a frequency component at three times the body oscillation frequency. Finally, we present a stability phase diagram to summarize the VIV lock-in regimes of the five smooth-curve- and sharp-corner-based bluff bodies. These findings attempt to generalize our understanding of the VIV lock-in mechanism for bluff bodies at low Reynolds number. The proposed ERA-based ROM is found to be accurate, efficient and easy to use for the linear stability analysis of VIV, and it can have a profound impact on the development of control strategies for nonlinear vortex shedding and VIV.

[1]  C. Williamson Oblique and parallel modes of vortex shedding in the wake of a circular cylinder at low Reynolds numbers , 1989, Journal of Fluid Mechanics.

[2]  Rajeev K. Jaiman,et al.  Interaction dynamics of gap flow with vortex-induced vibration in side-by-side cylinder arrangement , 2016 .

[3]  P. S. Gurugubelli,et al.  Freely vibrating circular cylinder in the vicinity of a stationary wall , 2015 .

[4]  P. Schmid,et al.  Projection-free approximate balanced truncation of large unstable systems. , 2015, Physical review. E, Statistical, nonlinear, and soft matter physics.

[5]  Aimee S. Morgans,et al.  Feedback control of unstable flows: a direct modelling approach using the Eigensystem Realisation Algorithm , 2016, Journal of Fluid Mechanics.

[6]  Kyung-Soo Yang,et al.  Flow instabilities in the wake of a rounded square cylinder , 2016, Journal of Fluid Mechanics.

[7]  O. Marquet,et al.  Sensitivity analysis and passive control of cylinder flow , 2008, Journal of Fluid Mechanics.

[8]  C. Williamson Vortex Dynamics in the Cylinder Wake , 1996 .

[9]  Jean-Marc Chomaz,et al.  An asymptotic expansion for the vortex-induced vibrations of a circular cylinder , 2011, Journal of Fluid Mechanics.

[10]  Peter J. Schmid,et al.  Closed-loop control of an open cavity flow using reduced-order models , 2009, Journal of Fluid Mechanics.

[11]  A. K. Luo,et al.  In Transition , 2010, Annals of Internal Medicine.

[12]  Simao Marques,et al.  Prediction of Transonic Limit-Cycle Oscillations Using an Aeroelastic Harmonic Balance Method , 2015 .

[13]  C. Williamson,et al.  MOTIONS, FORCES AND MODE TRANSITIONS IN VORTEX-INDUCED VIBRATIONS AT LOW MASS-DAMPING , 1999 .

[14]  Yan Bao,et al.  Combined interface boundary condition method for fluid–rigid body interaction , 2012 .

[15]  P. Luchini,et al.  Structural sensitivity of the first instability of the cylinder wake , 2007, Journal of Fluid Mechanics.

[16]  R. Henderson,et al.  A study of two-dimensional flow past an oscillating cylinder , 1999, Journal of Fluid Mechanics.

[17]  W. Yao,et al.  A harmonic balance technique for the reduced-order computation of vortex-induced vibration , 2016 .

[18]  Anthony Leonard,et al.  Flow-induced vibration of a circular cylinder at limiting structural parameters , 2001 .

[19]  Sanjay Mittal,et al.  Lock-in in vortex-induced vibration , 2016, Journal of Fluid Mechanics.

[20]  L. Morino,et al.  ON THE INSTABILITY OF A SPRING-MOUNTED CIRCULAR CYLINDER IN A VISCOUS FLOW AT LOW REYNOLDS NUMBERS , 2000 .

[21]  G. Karniadakis,et al.  Suppression of vortex-induced vibrations by fairings: A numerical study , 2015 .

[22]  Rajeev K. Jaiman,et al.  A fully implicit combined field scheme for freely vibrating square cylinders with sharp and rounded corners , 2015 .

[23]  Denis Sipp,et al.  Model reduction for fluids using frequential snapshots , 2011 .

[24]  S. Mittal,et al.  Vortex-induced oscillations at low Reynolds numbers: Hysteresis and vortex-shedding modes , 2005 .

[25]  Jer-Nan Juang,et al.  An eigensystem realization algorithm for modal parameter identification and model reduction. [control systems design for large space structures] , 1985 .

[26]  K. C.H.,et al.  Oblique and parallel modes of vortex shedding in the wake of a circular cylinder at low Reynolds numbers , 2005 .

[27]  Lukas Novotny,et al.  Strong coupling, energy splitting, and level crossings: A classical perspective , 2010 .

[28]  T. P. Miyanawala,et al.  Partitioned iterative and dynamic subgrid-scale methods for freely vibrating square-section structures at subcritical Reynolds number , 2016 .

[29]  Mark C. Thompson,et al.  The beginning of branching behaviour of vortex-induced vibration during two-dimensional flow , 2006 .

[30]  The structure of primary instability modes in the steady wake and separation bubble of a square cylinder , 2014 .

[31]  Turgut Sarpkaya,et al.  A critical review of the intrinsic nature of vortex-induced vibrations , 2004 .

[32]  Peter W. Bearman,et al.  Circular cylinder wakes and vortex-induced vibrations , 2011 .

[33]  P. Schmid,et al.  Dynamic mode decomposition of numerical and experimental data , 2008, Journal of Fluid Mechanics.

[34]  Weiwei Zhang,et al.  Mechanism of frequency lock-in in vortex-induced vibrations at low Reynolds numbers , 2015, Journal of Fluid Mechanics.

[35]  Clarence W. Rowley,et al.  Model Reduction for fluids, Using Balanced Proper Orthogonal Decomposition , 2005, Int. J. Bifurc. Chaos.

[36]  Rajeev K. Jaiman,et al.  A stable second-order partitioned iterative scheme for freely vibrating low-mass bluff bodies in a uniform flow , 2016 .

[37]  Clarence W. Rowley,et al.  Reduced-order models for control of fluids using the eigensystem realization algorithm , 2008, 0907.1907.

[38]  C. Rowley,et al.  Feedback control of unstable steady states of flow past a flat plate using reduced-order estimators , 2009, Journal of Fluid Mechanics.

[39]  Rajeev K. Jaiman,et al.  Transient fluid–structure interaction with non-matching spatial and temporal discretizations , 2011 .

[40]  E. de Langre,et al.  Frequency lock-in is caused by coupled-mode flutter , 2006 .

[41]  Florent Renac,et al.  Computation of eigenvalue sensitivity to base flow modifications in a discrete framework: Application to open-loop control , 2014, J. Comput. Phys..

[42]  Ming Zhao,et al.  Numerical simulation of vortex-induced vibration of a square cylinder at a low Reynolds number , 2013 .

[43]  I. Mezić,et al.  Spectral analysis of nonlinear flows , 2009, Journal of Fluid Mechanics.

[44]  Rajeev K. Jaiman,et al.  A stable second-order scheme for fluid-structure interaction with strong added-mass effects , 2014, J. Comput. Phys..

[45]  H. M. B L A C K B U R N,et al.  A study of two-dimensional flow past an oscillating cylinder , 2022 .

[46]  Rajeev K. Jaiman,et al.  Wake stabilization mechanism of low-drag suppression devices for vortex-induced vibration , 2017 .

[47]  C. Williamson,et al.  Vortex-Induced Vibrations , 2004, Wind Effects on Structures.

[48]  A. Roshko,et al.  Vortex formation in the wake of an oscillating cylinder , 1988 .

[49]  B. Moore Principal component analysis in linear systems: Controllability, observability, and model reduction , 1981 .

[50]  J. Peraire,et al.  Balanced Model Reduction via the Proper Orthogonal Decomposition , 2002 .

[51]  B. R. Noack,et al.  On the transition of the cylinder wake , 1995 .

[52]  A. Kaboudian,et al.  On the origin of wake-induced vibration in two tandem circular cylinders at low Reynolds number , 2016 .

[53]  M. Thompson,et al.  Low-Reynolds-number wakes of elliptical cylinders: from the circular cylinder to the normal flat plate , 2014, Journal of Fluid Mechanics.

[54]  Β. L. HO,et al.  Editorial: Effective construction of linear state-variable models from input/output functions , 1966 .