Bulletin of the American Physical Society
71st Annual Meeting of the APS Division of Fluid Dynamics
Volume 63, Number 13
Sunday–Tuesday, November 18–20, 2018; Atlanta, Georgia
Session Q30: Turbulent Jets and Shear Layers
12:50 PM–3:26 PM,
Tuesday, November 20, 2018
Georgia World Congress Center
Room: B402
Chair: Raul Cal, Portland State University
Abstract ID: BAPS.2018.DFD.Q30.12
Abstract: Q30.00012 : Vorticity vs TNTI - Entrainment Fundamentals
3:13 PM–3:26 PM
Presenter:
John F Foss
(Michigan State Univ)
Authors:
John F Foss
(Michigan State Univ)
Kyle M Bade
(Spraying Systems Co.)
Douglas Neal
(LaVision Inc.)
Richard Prevost
(LaVision Inc.)
Scott Morris
(Univ of Notre Dame)
A recent contribution by C. da Silva, et al. [1] presents results for the simulated flow: PJET, a temporally developing plane jet that could not be realized in a physical experiment. However, their results can be referenced to the PIV based vorticity observations of Foss, et al. [2]. Quantitatively similar results for the i) enstrophy distribution in [1] and ii) the mean square ωz distribution in [2] are found, relative to the border (IB) between the irrotational (entraining) and the vortical (interior) fluid domains. However, the physical features of interest: i) length of the IB with respect to its linear projection, ii) the intermittency distribution and iii) acceleration of the entraining fluid in its approach to the IB, are not available for the faux flow. The relatively high Reynolds number (Reλ) was 371 for [1], and higher: 590 for [2] using data from [3] for Reλ.
[1] Silva, et al. “The scaling of the TNTI at high Reynolds numbers” JFM (2018) vol. 843
[2] Foss, et al. (2017) “Single Stream Shear Layer and the Viscous Superlayer”, 10 C 4, Tenth International Symposium on Turbulence and Shear Flow Phenomena
[3] Morris, S.C. (2002) “The velocity and vorticity fields of a single stream shear layer” PhD Dissertation, Michigan State University
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DFD.Q30.12
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