Koopman-mode decomposition of the cylinder wake

Abstract The Koopman operator provides a powerful way of analysing nonlinear flow dynamics using linear techniques. The operator defines how observables evolve in time along a nonlinear flow trajectory. In this paper, we perform a Koopman analysis of the first Hopf bifurcation of the flow past a circular cylinder. First, we decompose the flow into a sequence of Koopman modes, where each mode evolves in time with one single frequency/growth rate and amplitude/phase, corresponding to the complex eigenvalues and eigenfunctions of the Koopman operator, respectively. The analytical construction of these modes shows how the amplitudes and phases of nonlinear global modes oscillating with the vortex shedding frequency or its harmonics evolve as the flow develops and later sustains self-excited oscillations. Second, we compute the dynamic modes using the dynamic mode decomposition (DMD) algorithm, which fits a linear combination of exponential terms to a sequence of snapshots spaced equally in time. It is shown that under certain conditions the DMD algorithm approximates Koopman modes, and hence provides a viable method to decompose the flow into saturated and transient oscillatory modes. Finally, the relevance of the analysis to frequency selection, global modes and shift modes is discussed.

[1]  J. B. Perot,et al.  An analysis of the fractional step method , 1993 .

[2]  B. R. Noack,et al.  A hierarchy of low-dimensional models for the transient and post-transient cylinder wake , 2003, Journal of Fluid Mechanics.

[3]  Damon Honnery,et al.  An error analysis of the dynamic mode decomposition , 2011, Experiments in Fluids.

[4]  H. Sung,et al.  Dynamic mode decomposition of turbulent cavity flows for self-sustained oscillations , 2011 .

[5]  Onofrio Semeraro,et al.  Analysis of time-resolved PIV measurements of a confined turbulent jet using POD and Koopman modes , 2012 .

[6]  J. Lumley Stochastic tools in turbulence , 1970 .

[7]  P. Schmid,et al.  Applications of the dynamic mode decomposition , 2011 .

[8]  I. Mezić,et al.  Analysis of Fluid Flows via Spectral Properties of the Koopman Operator , 2013 .

[9]  P. Holmes,et al.  Nonlinear Oscillations, Dynamical Systems, and Bifurcations of Vector Fields , 1983, Applied Mathematical Sciences.

[10]  Denis Sipp,et al.  Global stability of base and mean flows: a general approach and its applications to cylinder and open cavity flows , 2007, Journal of Fluid Mechanics.

[11]  Pierre Gaspard,et al.  Chaos, Scattering and Statistical Mechanics , 1998 .

[12]  Maurice Clerc,et al.  Why does it work , 2008 .

[13]  J. Chomaz,et al.  GLOBAL INSTABILITIES IN SPATIALLY DEVELOPING FLOWS: Non-Normality and Nonlinearity , 2005 .

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

[15]  Benoît Pier,et al.  On the frequency selection of finite-amplitude vortex shedding in the cylinder wake , 2002, Journal of Fluid Mechanics.

[16]  M. Provansal,et al.  Bénard-von Kármán instability: transient and forced regimes , 1987, Journal of Fluid Mechanics.

[17]  Gilead Tadmor,et al.  Mean field representation of the natural and actuated cylinder wake , 2010 .

[18]  P. Cvitanović,et al.  Periodic orbit expansions for classical smooth flows , 1991 .

[19]  B. O. Koopman,et al.  Hamiltonian Systems and Transformation in Hilbert Space. , 1931, Proceedings of the National Academy of Sciences of the United States of America.

[20]  J. Wesfreid,et al.  Stability properties of forced wakes , 2007, Journal of Fluid Mechanics.

[21]  Tim Colonius,et al.  The immersed boundary method: A projection approach , 2007, J. Comput. Phys..

[22]  M. Mackey,et al.  Chaos, Fractals, and Noise: Stochastic Aspects of Dynamics , 1998 .

[23]  I. Mezić Spectral Properties of Dynamical Systems, Model Reduction and Decompositions , 2005 .

[24]  Clarence W. Rowley,et al.  Variants of Dynamic Mode Decomposition: Boundary Condition, Koopman, and Fourier Analyses , 2012, J. Nonlinear Sci..

[25]  Peter J. Schmid,et al.  Application of the dynamic mode decomposition to experimental data , 2011 .

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

[27]  D. Barkley Linear analysis of the cylinder wake mean flow , 2006 .

[28]  P. Schmid Nonmodal Stability Theory , 2007 .

[29]  A. Hussain,et al.  The mechanics of an organized wave in turbulent shear flow. Part 3. Theoretical models and comparisons with experiments , 1972, Journal of Fluid Mechanics.

[30]  P. Gaspard,et al.  Liouvillian dynamics of the Hopf bifurcation. , 2001, Physical review. E, Statistical, nonlinear, and soft matter physics.

[31]  P. Monkewitz,et al.  LOCAL AND GLOBAL INSTABILITIES IN SPATIALLY DEVELOPING FLOWS , 1990 .

[32]  Denis Sipp,et al.  Direct and adjoint global modes of a recirculation bubble: lift-up and convective non-normalities , 2009, Journal of Fluid Mechanics.

[33]  G. Nicolis,et al.  Spectral signature of the pitchfork bifurcation: Liouville equation approach. , 1995, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[34]  Tomas W. Muld,et al.  Mode Decomposition on Surface-Mounted Cube , 2012 .