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    CONDITIONAL FLOW STATISTICS AND ALIGNMENT OF PRINCIPAL STRAIN RATES, VORTICITY, AND SCALAR GRADIENTS IN A TURBULENT NONPREMIXED JET FLAME

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    Type
    Conference Paper
    Authors
    Attili, Antonio
    Bisetti, Fabrizio cc
    KAUST Department
    Clean Combustion Research Center
    Date
    2015-06-30
    Permanent link to this record
    http://hdl.handle.net/10754/566966
    
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    Abstract
    The alignment of vorticity and gradients of conserved and reactive scalars with the eigenvectors of the strain rate tensor (i.e., the principal strains) is investigated in a direct numerical simulation of a turbulent nonpremixed flame achieving a Taylor’s scale Reynolds number in the range 100≤Reλ≤150 (Attili et al. Comb. Flame, 161, 2014). The vorticity vector displays a pronounced tendency to align with the direction of the intermediate strain. These alignment statistics are in almost perfect agreement with those in homogeneous isotropic turbulence (Ashurst et al. Physics of Fluids 30, 1987) and differ significantly from the results obtained in other nonpremixed flames in which vorticity alignment with the most extensive strain was observed (Boratavet al. Physics of Fluids 8, 1996). The gradients of conserved and reactive scalars align with the most compressive strain. It is worth noting that conditioning on the local values of the mixture fraction, or equivalently conditioning on the distance from the flame sheet, does not affect the statistics. Our results suggest that turbulence overshadows the effects of heat release and chemical reactions. This may be due to the larger Reynolds number achieved in the present study compared to that in previous works.
    Journal
    Proceedings of Ninth International Symposium on Turbulence and Shear Flow Phenomena (TSFP-9)
    Conference/Event name
    Ninth International Symposium on Turbulence and Shear Flow Phenomena (TSFP-9)
    Additional Links
    ftp://tepeu.sisal.unam.mx/TSFP9/full_paper/8C-4.pdf
    Collections
    Conference Papers; Clean Combustion Research Center

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