Characterization of velocity-gradient dynamics in incompressible turbulence using local streamline geometry
This study develops a comprehensive description of local streamline geometry and uses the resulting shape features to characterize velocity gradient ( $\unicode[STIX]{x1D608}_{ij}=\unicode[STIX]{x2202}u_{i}/\unicode[STIX]{x2202}x_{j}$ ) dynamics. The local streamline geometric shape parameters and s...
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Published in | Journal of fluid mechanics Vol. 895 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Cambridge
Cambridge University Press
25.07.2020
|
Subjects | |
Online Access | Get full text |
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Summary: | This study develops a comprehensive description of local streamline geometry and uses the resulting shape features to characterize velocity gradient (
$\unicode[STIX]{x1D608}_{ij}=\unicode[STIX]{x2202}u_{i}/\unicode[STIX]{x2202}x_{j}$
) dynamics. The local streamline geometric shape parameters and scale factor (size) are extracted from
$\unicode[STIX]{x1D608}_{ij}$
by extending the linearized critical point analysis. In the present analysis,
$\unicode[STIX]{x1D608}_{ij}$
is factorized into its magnitude (
$A\equiv \sqrt{\unicode[STIX]{x1D608}_{ij}\unicode[STIX]{x1D608}_{ij}}$
) and normalized tensor
$\unicode[STIX]{x1D623}_{ij}\equiv \unicode[STIX]{x1D608}_{ij}/A$
. The geometric shape is shown to be determined exclusively by four
$\unicode[STIX]{x1D623}_{ij}$
parameters: second invariant,
$q$
(
$=Q/A^{2}$
); third invariant,
$r$
(
$=R/A^{3}$
); intermediate strain rate eigenvalue,
$a_{2}$
; and vorticity component along intermediate strain rate eigenvector,
$\unicode[STIX]{x1D714}_{2}$
. Velocity gradient magnitude,
$A$
, plays a role only in determining the scale of the local streamline structure. Direct numerical simulation data of forced isotropic turbulence (
$Re_{\unicode[STIX]{x1D706}}\sim 200{-}600$
) is used to establish streamline shape and scale distribution, and then to characterize velocity-gradient dynamics. Conditional mean trajectories (CMTs) in
$q$
–
$r$
space reveal important non-local features of pressure and viscous dynamics which are not evident from the
$\unicode[STIX]{x1D608}_{ij}$
-invariants. Two distinct types of
$q$
–
$r$
CMTs demarcated by a separatrix are identified. The inner trajectories are dominated by inertia–pressure interactions and the viscous effects play a significant role only in the outer trajectories. Dynamical system characterization of inertial, pressure and viscous effects in the
$q$
–
$r$
phase space is developed. Additionally, it is shown that the residence time of
$q$
–
$r$
CMTs through different topologies correlate well with the corresponding population fractions. These findings not only lead to improved understanding of non-local dynamics, but also provide an important foundation for developing Lagrangian velocity-gradient models. |
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ISSN: | 0022-1120 1469-7645 |
DOI: | 10.1017/jfm.2020.286 |