Identification of coexisting dynamics in boundary layer flows through proper orthogonal decomposition with weighting matrices

A different version of the classic proper orthogonal decomposition (POD) procedure introducing spatial and temporal weighting matrices is proposed. Furthermore, a newly defined non-Euclidean (NE) inner product that retain similarities with the POD is introduced in the paper. The aim is to emphasize fluctuation events localized in spatio-temporal regions with low kinetic energy magnitude, which are not highlighted by the classic POD. The different variants proposed in this work are applied to numerical and experimental data, highlighting analogies and differences with respect to the classic and other normalized variants of POD available in the literature. The numerical test case provides a noise-free environment of the strongly organized vortex shedding behind a cylinder. Conversely, experimental data describing transitional boundary layers are used to test the capability of the procedures in strongly not uniform flows. By-pass and separated flow transition processes developing with high free-stream disturbances have been considered. In both cases streaky structures are expected to interact with other vortical structures (i.e. free-stream vortices in the by-pass case and Kelvin–Helmholtz rolls in the separated type) that carry a significant different amount of energy. Modes obtained by the non-Euclidean POD (NE-POD) procedure (where weighted projections are considered) are shown to better extract low energy events sparse in time and space with respect to modes extracted by other variants. Moreover, NE-POD modes are further decomposed as a combination of Fourier transforms of the related temporal coefficients and the normalized data ensemble to isolate the frequency content of each mode.

[1]  D. Simoni,et al.  Velocity and turbulence measurements in a separating boundary layer with and without passive flow control , 2007 .

[2]  A. Ianiro,et al.  Extended proper orthogonal decomposition of non-homogeneous thermal fields in a turbulent pipe flow , 2018 .

[3]  J. Borée,et al.  Spatio-temporal structure and cycle to cycle variations of an in-cylinder tumbling flow , 2011 .

[4]  L. Sirovich Turbulence and the dynamics of coherent structures. I. Coherent structures , 1987 .

[5]  Uri Shaham,et al.  Dynamic Mode Decomposition , 2013 .

[6]  O. Marxen,et al.  Vortex formation and vortex breakup in a laminar separation bubble , 2013, Journal of Fluid Mechanics.

[7]  Peter R. Voke,et al.  Large-eddy simulation of boundary-layer separation and transition at a change of surface curvature , 2001, Journal of Fluid Mechanics.

[8]  J. Borée,et al.  Extended proper orthogonal decomposition: a tool to analyse correlated events in turbulent flows , 2003 .

[9]  J.-M. Buchlin,et al.  Multi-scale proper orthogonal decomposition of complex fluid flows , 2018, Journal of Fluid Mechanics.

[10]  Robert J. Martinuzzi,et al.  Generalized phase average with applications to sensor-based flow estimation of the wall-mounted square cylinder wake , 2012, Journal of Fluid Mechanics.

[11]  William K. George,et al.  Reconstruction of the global velocity field in the axisymmetric mixing layer utilizing the proper orthogonal decomposition , 2000, Journal of Fluid Mechanics.

[12]  Christian Oliver Paschereit,et al.  Spectral proper orthogonal decomposition , 2015, Journal of Fluid Mechanics.

[13]  R. G. Jacobs,et al.  Simulations of bypass transition , 2001, Journal of Fluid Mechanics.

[14]  Pierre E. Sullivan,et al.  Separated-Shear-Layer Development on an Airfoil at Low Reynolds Numbers , 2008 .

[15]  M. Glauser,et al.  The proper orthogonal decomposition of pressure fluctuations surrounding a turbulent jet , 1997, Journal of Fluid Mechanics.

[16]  D. Lengani,et al.  Analysis of the Reynolds stress component production in a laminar separation bubble , 2017 .

[17]  Tamer A. Zaki,et al.  Conditional sampling of transitional boundary layers in pressure gradients , 2013, Journal of Fluid Mechanics.

[18]  Stefano Discetti,et al.  Estimation of time-resolved turbulent fields through correlation of non-time-resolved field measurements and time-resolved point measurements , 2018 .

[19]  R. Guida,et al.  A wavelet-based intermittency detection technique from PIV investigations in transitional boundary layers , 2016 .

[20]  Robert J. Martinuzzi,et al.  Sensor-based estimation of the velocity in the wake of a low-aspect-ratio pyramid , 2015 .

[21]  D. Lengani,et al.  POD analysis of the unsteady behavior of a laminar separation bubble , 2014 .

[22]  Tamer A. Zaki,et al.  From Streaks to Spots and on to Turbulence: Exploring the Dynamics of Boundary Layer Transition , 2013, Flow, Turbulence and Combustion.

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

[24]  Laszlo Fuchs,et al.  Proper Orthogonal Decomposition for experimental investigation of swirling flame instabilities , 2010 .

[25]  O. N. Ramesh,et al.  On the origin of the inflectional instability of a laminar separation bubble , 2009, Journal of Fluid Mechanics.

[26]  D. Lengani,et al.  Identification and quantification of losses in a LPT cascade by POD applied to LES data , 2018 .

[27]  O. Marxen,et al.  The effect of small-amplitude convective disturbances on the size and bursting of a laminar separation bubble , 2011, Journal of Fluid Mechanics.

[28]  Ulrich Rist,et al.  Mean flow deformation in a laminar separation bubble: separation and stability characteristics , 2010, Journal of Fluid Mechanics.

[29]  J. Borée,et al.  Coupling time-resolved PIV flow-fields and phase-invariant proper orthogonal decomposition for the description of the parameters space in a transparent Diesel engine , 2007 .

[30]  L. Sirovich Turbulence and the dynamics of coherent structures. III. Dynamics and scaling , 1987 .

[31]  D. Lengani,et al.  Synchronization of multi-plane measurement data by means of POD: application to unsteady boundary layer transition , 2018, Experiments in Fluids.

[32]  Marianna Braza,et al.  Phase-averaged measurements of the turbulence properties in the near wake of a circular cylinder at high Reynolds number by 2C-PIV and 3C-PIV , 2006 .

[33]  T. J. Hanratty,et al.  Large-scale modes of turbulent channel flow: transport and structure , 2001, Journal of Fluid Mechanics.

[34]  Sandeep Saha,et al.  On shear sheltering and the structure of vortical modes in single- and two-fluid boundary layers , 2009, Journal of Fluid Mechanics.

[35]  M. Kotsonis,et al.  On the origin of spanwise vortex deformations in laminar separation bubbles , 2018, Journal of Fluid Mechanics.

[36]  J. Sørensen,et al.  Mutual inductance instability of the tip vortices behind a wind turbine , 2014, Journal of Fluid Mechanics.

[37]  Daniel C. Haworth,et al.  Application of the proper orthogonal decomposition to datasets of internal combustion engine flows , 2004 .

[38]  S. Yarusevych,et al.  Effects of free-stream turbulence intensity on transition in a laminar separation bubble formed over an airfoil , 2018, Experiments in Fluids.

[39]  Yingzheng Liu,et al.  Influence of wall proximity on characteristics of wake behind a square cylinder: PIV measurements and POD analysis , 2010 .

[40]  Charles E. Tinney,et al.  Low-dimensional characteristics of a transonic jet. Part 1. Proper orthogonal decomposition , 2008, Journal of Fluid Mechanics.

[41]  Mark N. Glauser,et al.  Orthogonal Decomposition of the Axisymmetric Jet Mixing Layer Including Azimuthal Dependence , 1987 .

[42]  Mark N. Glauser,et al.  Application of multipoint measurements for flow characterization , 1992 .

[43]  S. Brunton,et al.  Discovering governing equations from data by sparse identification of nonlinear dynamical systems , 2015, Proceedings of the National Academy of Sciences.

[44]  D. Lengani,et al.  Inspection of the dynamic properties of laminar separation bubbles: free-stream turbulence intensity effects for different Reynolds numbers , 2017 .

[45]  Steven L. Brunton,et al.  Dynamic mode decomposition - data-driven modeling of complex systems , 2016 .