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Velocity gradient tensor, A₈₉ uᵢ/ xⱼ, in a turbulence flow field is modelled by separating the treatment of intermittent magnitude (A = A₈₉A₈₉) from that of the more universal normalised velocity gradient tensor, b₈₉ A₈₉/A. The boundedness and compactness of the b₈₉ -space along with its universal dynamics allow for the development of models that are reasonably insensitive to Reynolds number. The near-lognormality of the magnitude A is then exploited to derive a model based on a modified Ornstein–Uhlenbeck process. These models are developed using data-driven strategies employing high-fidelity forced isotropic turbulence data sets. A posteriori model results agree well with direct numerical simulation data over a wide range of velocity-gradient features and Reynolds numbers.
Das et al. (Wed,) studied this question.