@article{
 title = {The anisotropic structure of turbulence and its energy spectrum},
 type = {article},
 year = {2016},
 pages = {11701},
 volume = {28},
 websites = {http://aip.scitation.org/doi/10.1063/1.4939471},
 month = {4},
 id = {15cb2dab-6eab-3807-90eb-f579a18bc5c5},
 created = {2021-04-09T15:23:13.967Z},
 file_attached = {false},
 profile_id = {75799766-8e2d-3c98-81f9-e3efa41233d0},
 group_id = {c9329632-2a50-3043-b803-cadc8dbdfc3f},
 last_modified = {2021-04-09T15:23:13.967Z},
 read = {false},
 starred = {false},
 authored = {false},
 confirmed = {false},
 hidden = {false},
 source_type = {article},
 private_publication = {false},
 abstract = {The spectral energy distribution in turbulent flows is observed to follow a k−5/3 power scaling, as originally predicted by Kolmogorov’s theory. However, the underlying assumptions in Kolmogorov’s theory appear not to hold with most experimental and numerical data showing evidence of small-scale anisotropy and significant direct energy transfer between the large- and the small-scales. Here, we present a flow structure that reconciles the k−5/3 spectrum with small-scale universality, small-scale anisotropy, and direct scale interactions. The flow structure is a shear layer, which contains the small-scales of motion and is bounded by the large-scales. The anisotropic shear layer reveals the expected scaling of the energy spectrum in nearly all directions.},
 bibtype = {article},
 author = {Elsinga, G E and Marusic, I},
 doi = {10.1063/1.4939471},
 journal = {Physics of Fluids},
 number = {1}
}

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