The small-scale structure of passive scalar mixing in turbulent boundary layers

The objective is to contribute to several issues regarding the traditional view of the local structure of passive scalar fields: (1) probability density function (PDF) of the scalar concentration and scalar gradient, (2) the scalar power spectrum, (3) the structure functions, and (4) correlation fun...

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Main Author: Dasi, Lakshmi P.
Format: Others
Language:en_US
Published: Georgia Institute of Technology 2006
Subjects:
Online Access:http://hdl.handle.net/1853/7599
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spelling ndltd-GATECH-oai-smartech.gatech.edu-1853-75992013-01-07T20:12:43ZThe small-scale structure of passive scalar mixing in turbulent boundary layersDasi, Lakshmi P.Correlation functionFractal dimensionMixingPassive scalarScalar field theorySpectrum analysisStructure functionTurbulent boundary layerThe objective is to contribute to several issues regarding the traditional view of the local structure of passive scalar fields: (1) probability density function (PDF) of the scalar concentration and scalar gradient, (2) the scalar power spectrum, (3) the structure functions, and (4) correlation functions and multi-point correlators. In addition, the research provides a geometric description of two-dimensional transects of the passive scalar iso-surfaces using the tools of fractal geometry. The local structure is analyzed as a function of large-scale anisotropy, intermittency factor, Reynolds number, and initial condition of the scalar injection. Experiments were performed in the bed boundary layer produced by a uniform depth open channel flow of water in a tilting flume for Re_lamda = 63, 94, and 120. A small nozzle iso-kinetically delivers a passive scalar of high Schmidt number ( Sc = 1000) at mid-depth to generate the turbulent scalar field. Three nozzle diameters are used to study the effects of the injection length scale. High-resolution planar laser induced fluorescence (PLIF) technique is used to measure the scalar field. The local structure far from isotropic and is influenced even at the smallest scales by large-scale anisotropy, initial injection length scale and the Reynolds number of the flow. The PDF of the scalar fluctuations is non-Gaussian and dependent on large-scale anisotropy. The PDF of scalar gradients show the influence of large-scale anisotropy on the structure at the smallest scales. The spectrum of the scalar field deviates from the in the inertial convection regime and is dependent on large-scale anisotropy, external intermittency, and low Reynolds number. There is no evidence of Batchelors k^-1 scaling law. The scaling exponents of the even-ordered structure functions appear to be inversely correlated with the kurtosis of the scalar fluctuations. The fractal geometry of the two dimensional transects of passive scalar iso-surfaces is scale dependent. The fractal dimension is 1.0 at the smallest length scale and increases in a universal manner in the viscous-convective regime. The coverage length underestimate reflects this universal behavior with practical significance. The lacunarity function shows that the instantaneous scalar field is most in-homogenous around the Kolmogorov scale.Georgia Institute of Technology2006-01-18T22:27:46Z2006-01-18T22:27:46Z2004-08-17Dissertation18136102 bytesapplication/pdfhttp://hdl.handle.net/1853/7599en_US
collection NDLTD
language en_US
format Others
sources NDLTD
topic Correlation function
Fractal dimension
Mixing
Passive scalar
Scalar field theory
Spectrum analysis
Structure function
Turbulent boundary layer
spellingShingle Correlation function
Fractal dimension
Mixing
Passive scalar
Scalar field theory
Spectrum analysis
Structure function
Turbulent boundary layer
Dasi, Lakshmi P.
The small-scale structure of passive scalar mixing in turbulent boundary layers
description The objective is to contribute to several issues regarding the traditional view of the local structure of passive scalar fields: (1) probability density function (PDF) of the scalar concentration and scalar gradient, (2) the scalar power spectrum, (3) the structure functions, and (4) correlation functions and multi-point correlators. In addition, the research provides a geometric description of two-dimensional transects of the passive scalar iso-surfaces using the tools of fractal geometry. The local structure is analyzed as a function of large-scale anisotropy, intermittency factor, Reynolds number, and initial condition of the scalar injection. Experiments were performed in the bed boundary layer produced by a uniform depth open channel flow of water in a tilting flume for Re_lamda = 63, 94, and 120. A small nozzle iso-kinetically delivers a passive scalar of high Schmidt number ( Sc = 1000) at mid-depth to generate the turbulent scalar field. Three nozzle diameters are used to study the effects of the injection length scale. High-resolution planar laser induced fluorescence (PLIF) technique is used to measure the scalar field. The local structure far from isotropic and is influenced even at the smallest scales by large-scale anisotropy, initial injection length scale and the Reynolds number of the flow. The PDF of the scalar fluctuations is non-Gaussian and dependent on large-scale anisotropy. The PDF of scalar gradients show the influence of large-scale anisotropy on the structure at the smallest scales. The spectrum of the scalar field deviates from the in the inertial convection regime and is dependent on large-scale anisotropy, external intermittency, and low Reynolds number. There is no evidence of Batchelors k^-1 scaling law. The scaling exponents of the even-ordered structure functions appear to be inversely correlated with the kurtosis of the scalar fluctuations. The fractal geometry of the two dimensional transects of passive scalar iso-surfaces is scale dependent. The fractal dimension is 1.0 at the smallest length scale and increases in a universal manner in the viscous-convective regime. The coverage length underestimate reflects this universal behavior with practical significance. The lacunarity function shows that the instantaneous scalar field is most in-homogenous around the Kolmogorov scale.
author Dasi, Lakshmi P.
author_facet Dasi, Lakshmi P.
author_sort Dasi, Lakshmi P.
title The small-scale structure of passive scalar mixing in turbulent boundary layers
title_short The small-scale structure of passive scalar mixing in turbulent boundary layers
title_full The small-scale structure of passive scalar mixing in turbulent boundary layers
title_fullStr The small-scale structure of passive scalar mixing in turbulent boundary layers
title_full_unstemmed The small-scale structure of passive scalar mixing in turbulent boundary layers
title_sort small-scale structure of passive scalar mixing in turbulent boundary layers
publisher Georgia Institute of Technology
publishDate 2006
url http://hdl.handle.net/1853/7599
work_keys_str_mv AT dasilakshmip thesmallscalestructureofpassivescalarmixinginturbulentboundarylayers
AT dasilakshmip smallscalestructureofpassivescalarmixinginturbulentboundarylayers
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