Higher Order Turbulence Around Different Circular Cylinders Using Particle Image Velocimetry

Author(s):  
Gaurav Misuriya ◽  
T I Eldho ◽  
B S Mazumder

Abstract Wakes and higher-order turbulence around circular cylinder of different diameters are investigated using particle image velocimetry measurements. The cylinder Reynolds number (Red) is defined by the depth averaged velocity, cylinder diameter and kinematic viscosity. The influence of Red on third-order moment of velocity fluctuations, turbulent kinetic energy (TKE) flux, TKE budget and turbulent length scales are presented. The intermittency factor and quadrant analysis around the cylinders are discussed for Red values ranging from 12,600 to 21,000. Intermittency factor increased with Red. Red effect modulated the energy budget mainly near free surface upstream and near bed downstream. Stream-wise and transverse TKE fluxes decreased significantly with Red, but not the vertical flux. Stream wise skewness changed sign from positive to negative with a certain critical distance on downstream, while vertical skewness showed reversed with Red. Negative stream-wise skewness and positive vertical skewness indicate the occurrence of ejection events. Production and dissipation rates increased with Red on the downstream, whereas opposite trend was observed for dissipation on the upstream. Increase of Red led to increase in Kolmogorov length-scale much higher on the upstream than downstream, whereas it showed depleting effect on Taylor's length-scale on upstream and increasing effect on the downstream. Ejection and sweep events were more prominent in the downstream near the cylinder than upstream with higher values of shear stress on the downstream. The sum of shear stress contributions of all quadrant events increased consistently with increase in Red near the cylinder.

2016 ◽  
Vol 804 ◽  
pp. 278-297 ◽  
Author(s):  
J. P. J. Stevenson ◽  
K. P. Nolan ◽  
E. J. Walsh

The free shear layer that separates from the leading edge of a round-nosed plate has been studied under conditions of low (background) and elevated (grid-generated) free stream turbulence (FST) using high-fidelity particle image velocimetry. Transition occurs after separation in each case, followed by reattachment to the flat surface of the plate downstream. A bubble of reverse flow is thereby formed. First, we find that, under elevated (7 %) FST, the time-mean bubble is almost threefold shorter due to an accelerated transition of the shear layer. Quadrant analysis of the Reynolds stresses reveals the presence of slender, highly coherent fluctuations amid the laminar part of the shear layer that are reminiscent of the boundary-layer streaks seen in bypass transition. Instability and the roll-up of vortices then follow near the crest of the shear layer. These vortices are also present under low FST and in both cases are found to make significant contributions to the production of Reynolds stress over the rear of the bubble. But their role in reattachment, whilst important, is not yet fully clear. Instantaneous flow fields from the low-FST case reveal that the bubble of reverse flow often breaks up into two or more parts, thereby complicating the overall reattachment process. We therefore suggest that the downstream end of the ‘separation isoline’ (the locus of zero absolute streamwise velocity that extends unbroken from the leading edge) be used to define the instantaneous reattachment point. A histogram of this point is found to be bimodal: the upstream peak coincides with the location of roll-up, whereas the downstream mode may suggest a ‘flapping’ motion.


Author(s):  
Andrew M. Walker ◽  
Clifton R. Johnston ◽  
Gary M. Dobson

Currently, an echo particle image velocimetry (ePIV) system for the investigation of in vivo blood flow and shear stress is under development at the University of Calgary. To date, encouraging preliminary results have been obtained when comparing ePIV derived velocities to analytical solutions. However, large discrepancies were noted between our steady state ePIV derived velocities and velocities measured using pulse wave Doppler (PWD). Ultrasound beam thickness, off axis centerline measurements and PWD angle of interrogation likely account for the differences observed.


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