TY - JOUR
T1 - A study of properties of vortex stretching and enstrophy generation in numerical and laboratory turbulence
AU - Tsinober, A.
AU - Shtilman, L.
AU - Vaisburd, H.
PY - 1997/12
Y1 - 1997/12
N2 - Dynamically relevant alignments are used in order to show that regions with weak vorticity are not structureless, non-Gaussian and dynamically not passive. For example, the structure of vorticity in quasi-homogeneous/isotropic turbulent flows is associated with strong alignment between vorticity ω and the eigenvectors of the rate of strain tensor λi, (especially - but not only - between ω and λ2) rather than with intense vorticity only. Consequently, much larger regions of turbulent flow than just those with intense vorticity are spatially structured. The whole flow field - even with the weakest measurable enstrophy - is strongly non-Gaussian, which among other things is manifested in strong alignment between vorticity and the vortex stretching vector Wi = ωjSij. It is shown that the quasi-two-dimensional regions corresponding to large cos(ω,λ2) are qualitatively different from purely two-dimensional ones, e.g. in that they possess essentially nonvanishing enstrophy generation, which is larger than its mean for the whole field.
AB - Dynamically relevant alignments are used in order to show that regions with weak vorticity are not structureless, non-Gaussian and dynamically not passive. For example, the structure of vorticity in quasi-homogeneous/isotropic turbulent flows is associated with strong alignment between vorticity ω and the eigenvectors of the rate of strain tensor λi, (especially - but not only - between ω and λ2) rather than with intense vorticity only. Consequently, much larger regions of turbulent flow than just those with intense vorticity are spatially structured. The whole flow field - even with the weakest measurable enstrophy - is strongly non-Gaussian, which among other things is manifested in strong alignment between vorticity and the vortex stretching vector Wi = ωjSij. It is shown that the quasi-two-dimensional regions corresponding to large cos(ω,λ2) are qualitatively different from purely two-dimensional ones, e.g. in that they possess essentially nonvanishing enstrophy generation, which is larger than its mean for the whole field.
UR - http://www.scopus.com/inward/record.url?scp=0031420459&partnerID=8YFLogxK
U2 - 10.1016/S0169-5983(97)00022-1
DO - 10.1016/S0169-5983(97)00022-1
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AN - SCOPUS:0031420459
SN - 0169-5983
VL - 21
SP - 477
EP - 494
JO - Fluid Dynamics Research
JF - Fluid Dynamics Research
IS - 6
ER -