The convection of large and intermediate scale fluctuations in a turbulent mixing layer
The convection of large and intermediate scale fluctuations in a turbulent mixing layer
The convection velocity of large and intermediate scale velocity fluctuations in a nominally two-dimensional planar mixing layer, and its dependence upon the length scale, is explored by carrying out particle image velocimetry (PIV) experiments. A “global” convection velocity, containing the convection of all the length scales present in the flow, is produced by examining the autocorrelation functions between velocity fluctuations in successive PIV records across the mixing layer. This “global” convection velocity is found to be similar to the mean flow, although fluctuations on the low speed side of the mixing layer on average convect at speeds greater than the mean and fluctuations on the high speed side of the mixing layer are observed to convect at speeds less than the mean. Scale specific convection velocity profiles are then produced by examining the phase difference between the spectral content specific to one wavenumber in streamwise velocity fluctuation traces in successive PIV records, offset by time ?. Probability density functions (pdfs) are produced of this phase difference, which is subsequently converted into a convection displacement, and these show that the convection of single length scale fluctuations exhibits a significant variance, particularly so for larger scale fluctuations and in the high speed side of the mixing layer. Convection velocity profiles are produced from these pdfs using both the mean convection distance and the modal convection distance. It is observed that the convection velocity is relatively insensitive to the length scale of the fluctuations considered, particularly when the mean convection distance is used. A slight sensitivity to length scale is, however, observed for convection velocities based on the modal convection distance. This dependence is primarily observed in the high speed side of the mixing layer, in which smaller length-scale fluctuations convect more quickly than larger length-scale fluctuations. It is also observed that the magnitude of the fluctuation itself affects the convection velocity with larger magnitude fluctuations convecting less rapidly than lower magnitude ones at the largest length scales investigated with this behaviour being reversed at more intermediate length scales.
Buxton, O.H.R.
8f254efb-58aa-4d73-9b93-78ad2a5c0aad
de Kat, R.
d46a99a4-8653-4698-9ef4-46dd0c77ba5d
Ganapathisubramani, B.
5e69099f-2f39-4fdd-8a85-3ac906827052
10 December 2013
Buxton, O.H.R.
8f254efb-58aa-4d73-9b93-78ad2a5c0aad
de Kat, R.
d46a99a4-8653-4698-9ef4-46dd0c77ba5d
Ganapathisubramani, B.
5e69099f-2f39-4fdd-8a85-3ac906827052
Buxton, O.H.R., de Kat, R. and Ganapathisubramani, B.
(2013)
The convection of large and intermediate scale fluctuations in a turbulent mixing layer.
Physics of Fluids, 25.
(doi:10.1063/1.4837555).
Abstract
The convection velocity of large and intermediate scale velocity fluctuations in a nominally two-dimensional planar mixing layer, and its dependence upon the length scale, is explored by carrying out particle image velocimetry (PIV) experiments. A “global” convection velocity, containing the convection of all the length scales present in the flow, is produced by examining the autocorrelation functions between velocity fluctuations in successive PIV records across the mixing layer. This “global” convection velocity is found to be similar to the mean flow, although fluctuations on the low speed side of the mixing layer on average convect at speeds greater than the mean and fluctuations on the high speed side of the mixing layer are observed to convect at speeds less than the mean. Scale specific convection velocity profiles are then produced by examining the phase difference between the spectral content specific to one wavenumber in streamwise velocity fluctuation traces in successive PIV records, offset by time ?. Probability density functions (pdfs) are produced of this phase difference, which is subsequently converted into a convection displacement, and these show that the convection of single length scale fluctuations exhibits a significant variance, particularly so for larger scale fluctuations and in the high speed side of the mixing layer. Convection velocity profiles are produced from these pdfs using both the mean convection distance and the modal convection distance. It is observed that the convection velocity is relatively insensitive to the length scale of the fluctuations considered, particularly when the mean convection distance is used. A slight sensitivity to length scale is, however, observed for convection velocities based on the modal convection distance. This dependence is primarily observed in the high speed side of the mixing layer, in which smaller length-scale fluctuations convect more quickly than larger length-scale fluctuations. It is also observed that the magnitude of the fluctuation itself affects the convection velocity with larger magnitude fluctuations convecting less rapidly than lower magnitude ones at the largest length scales investigated with this behaviour being reversed at more intermediate length scales.
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Published date: 10 December 2013
Organisations:
Aerodynamics & Flight Mechanics Group
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Local EPrints ID: 367150
URI: http://eprints.soton.ac.uk/id/eprint/367150
ISSN: 1070-6631
PURE UUID: d2ccbf04-dde6-4d45-b9d4-1e126467dbcc
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Date deposited: 23 Jul 2014 16:32
Last modified: 15 Mar 2024 03:37
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Author:
O.H.R. Buxton
Author:
R. de Kat
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