Bulletin of the American Physical Society
75th Annual Meeting of the Division of Fluid Dynamics
Volume 67, Number 19
Sunday–Tuesday, November 20–22, 2022; Indiana Convention Center, Indianapolis, Indiana.
Session A36: Turbulence: Flow Generation and Flow Measurements Developments
8:00 AM–9:57 AM,
Sunday, November 20, 2022
Room: 245
Chair: Nimish Pujara, University of Wisconsin-Madison
Abstract: A36.00001 : Turbulence decay in a von Kármán swirling flow
8:00 AM–8:13 AM
Presenter:
Farid Aligolzadeh
(Norwegian University of Science and Technology (NTNU))
Authors:
Farid Aligolzadeh
(Norwegian University of Science and Technology (NTNU))
Paweł Baj
(Warsaw University of Technology)
James R Dawson
(Norwegian University of Science and Technology (NTNU))
In this study, we investigate the decay of high Reynolds number turbulence at the center of a large von Kármán swirling flow facility (2m height and 2m across). The facility consists of a dodecagonal with two counter-rotating impellers that produces stationary homogenous turbulence near the center of the tank with low mean velocity and intense fluctuations. To measure the decay rate, we run the impellers until the flow reaches a stationary state and then stop them and immediately start measuring the velocity field in a plane at the center of the tank using Stereoscopic Particle Image Velocimetry (S-PIV). We run the experiment for 3 different Reynolds numbers ReR=R2ω/ν=2.54×105,1.91×105,1.27×105 where R is the impeller radius, ω is the angular velocity of the impeller and ν is the kinematic viscosity of the flow. Over 30 runs for each ReR were obtained to ensure reasonable convergence of the turbulent statistics. We calculate the spatially averaged kinetic energy over the field of view (FoV) from the PIV measurements and show that, after a proper normalization, the kinetic energy remains approximately constant for a short period after the impellers are stopped before transitioning to the expected power law decay. Our results consistently follow the power law k∼tn with a decay exponent n≅-1.6 .
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