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Self-attenuation of extreme events in Navier–Stokes turbulence

Dhawal Buaria, Alain Pumir, Eberhard Bodenschatz

2020Nature Communications56 citationsDOIOpen Access PDF

Abstract

Turbulent fluid flows are ubiquitous in nature and technology, and are mathematically described by the incompressible Navier-Stokes equations. A hallmark of turbulence is spontaneous generation of intense whirls, resulting from amplification of the fluid rotation-rate (vorticity) by its deformation-rate (strain). This interaction, encoded in the non-linearity of Navier-Stokes equations, is non-local, i.e., depends on the entire state of the flow, constituting a serious hindrance in turbulence theory and even establishing regularity of the equations. Here, we unveil a novel aspect of this interaction, by separating strain into local and non-local contributions utilizing the Biot-Savart integral of vorticity in a sphere of radius R. Analyzing highly-resolved numerical turbulent solutions to Navier-Stokes equations, we find that when vorticity becomes very large, the local strain over small R surprisingly counteracts further amplification. This uncovered self-attenuation mechanism is further shown to be connected to local Beltramization of the flow, and could provide a direction in establishing the regularity of Navier-Stokes equations.

Topics & Concepts

TurbulenceVorticityPhysicsCompressibilityRADIUSClassical mechanicsMechanicsVortexStatistical physicsVorticity equationMechanism (biology)State (computer science)K-epsilon turbulence modelSPHERESDirect numerical simulationPotential vorticityStrain (injury)Deformation (meteorology)Incompressible flowK-omega turbulence modelFluid Dynamics and Turbulent FlowsFluid dynamics and aerodynamics studiesNavier-Stokes equation solutions
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