Measurement of unsteady flow structures in a low-speed wind tunnel using continuous wave laser-based TR-PIV: near wake behind a circular cylinder

The unsteady measurement of spatiotemporally varying flow structures in a low-speed wind tunnel using a continuous wave (CW) laser-based time-resolved particle image velocimetry (TR-PIV) setup was extensively evaluated in the near wake behind a circular cylinder. A CW laser with a maximum power of 25 W in combination with a high-speed camera operating at 7 kHz was used to determine the wake flows at two different free-stream flow speeds: U0 = 5 and 10 m/s. Three different camera exposure times were selected for comparison: τ = 20, 50, and 80 μs. In the experiments, the low-repetition conventional PIV setup using the high-power pulsed laser (τ = 8 ns, 135 mJ/pulse) was used to determine the time-mean and statistical flow quantities, which served as the reference for determining the deviation in the TR-PIV measurements. At the lower flow speed of U0 = 5 m/s, the time-mean-separated flow patterns and the streamwise velocity profiles in all of the TR-PIV systems showed satisfactory agreement with the conventional PIV measurements, along with accurate capture of the large-scale Karman vortex and its harmonic behaviors. At the higher flow speed of U0 = 10 m/s, the measurement at τ = 50 μs gave a relatively accurate representation of the statistical flow quantities. At the longest exposure time of τ = 80 μs, considerable deviations in the time-mean streamwise fluctuation intensity and the TKE (turbulence kinetic energy) were observed due to the streaky particle image. The strong swirling motion of the large-scale vortical structures increased the deviation in the TR-PIV measurements, which increased with the increasing camera exposure time. Further POD analysis demonstrated that the leading energetic modes in the system with τ = 50 μs accurately determined the spatial features of the Karman-like vortex and its harmonic events. However, inaccurate vector representation of the second harmonic events was observed in the system with τ = 80 μs. Finally, for both flow speeds, the lower-order reconstructed phase-dependent representations of the Karman-like vortex and its harmonic behaviors were composed of the time-series velocity vector fields determined using the system with τ = 50 μs, thus providing a straightforward quantitative view of the coupled unsteady events.Graphical Abstract

[1]  Mark M. Weislogel,et al.  More investigations in capillary fluidics using a drop tower , 2013 .

[2]  M. Tokeshi,et al.  High-speed micro-PIV measurements of transient flow in microfluidic devices , 2004 .

[3]  Younjong Kim,et al.  Vortex Buffeting of Aircraft Tail: Interpretation via Proper Orthogonal Decomposition , 2005 .

[4]  Haiyan Hu,et al.  Efficient reduced-order modeling of unsteady aerodynamics robust to flight parameter variations , 2014 .

[5]  Yingzheng Liu,et al.  Proper orthogonal decomposition of wall-pressure fluctuations under the constrained wake of a square cylinder , 2011 .

[6]  Satyanarayanan R. Chakravarthy,et al.  Proper orthogonal and dynamic mode decompositions of time-resolved PIV of confined backward-facing step flow , 2014, Experiments in Fluids.

[7]  Amir Elzawawy,et al.  Time Resolved Particle Image Velocimetry Techniques with Continuous Wave Laser and their Application to Transient Flows , 2012 .

[8]  K. Thole,et al.  Effects of non-axisymmetric endwall contouring and film cooling on the passage flowfield in a linear turbine cascade , 2015 .

[9]  Liu Liu Shi,et al.  PIV measurement of separated flow over a blunt plate with different chord-to-thickness ratios , 2010 .

[10]  C. Willert,et al.  High-speed particle image velocimetry for the efficient measurement of turbulence statistics , 2015 .

[11]  Yingzheng Liu,et al.  The identification of coherent structures using proper orthogonal decomposition and dynamic mode decomposition , 2014 .

[12]  Sean P. Kearney,et al.  Pulse-burst PIV in a high-speed wind tunnel , 2015 .

[13]  R. Hout Time-resolved PIV measurements of the interaction of polystyrene beads with near-wall-coherent structures in a turbulent channel flow , 2011 .

[14]  Roi Gurka,et al.  POD of vorticity fields: A method for spatial characterization of coherent structures , 2006 .

[15]  F. Scarano,et al.  Phase-resolved characterization of vortex shedding in the near wake of a square-section cylinder at incidence , 2005 .

[16]  T. Arts,et al.  Spatio-temporal analysis of the turbulent flow in a ribbed channel , 2013 .

[17]  Yingzheng Liu,et al.  Wall-pressure fluctuations of separated and reattaching flow over blunt plate with chord-to-thickness ratio c/d = 9.0 , 2012 .

[18]  Fabien Anselmet,et al.  Use of PIV to highlight possible errors in hot-wire Reynolds stress data over a 2D rough wall , 2014 .

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

[20]  F. Scarano,et al.  On the use of helium-filled soap bubbles for large-scale tomographic PIV in wind tunnel experiments , 2015 .

[21]  Yingzheng Liu,et al.  Measurement of flow around a cactus-analogue grooved cylinder at ReD=5.4×104: Wall-pressure fluctuations and flow pattern , 2014 .

[22]  Yingzheng Liu,et al.  Wake dynamics behind a seal-vibrissa-shaped cylinder: a comparative study by time-resolved particle velocimetry measurements , 2016 .