Taylor columns and inertial-like waves in a three-dimensional odd viscous liquid

TL;DR

This paper investigates how three-dimensional odd viscous liquids support inertial-like waves and Taylor columns, revealing novel wave phenomena and flow structures driven by non-dissipative odd viscosity effects.

Contribution

It demonstrates the existence of inertial-like waves and Taylor columns in 3D odd viscous liquids, extending classical fluid dynamics concepts to non-rotating, anisotropic fluids with odd viscosity.

Findings

Numerical simulations confirm inertial-like waves downstream of a moving body.

Wavelengths of oscillations match theoretical predictions.

Taylor columns form in steady flows due to odd viscosity effects.

Abstract

Odd viscous liquids are endowed with an intrinsic mechanism that tends to restore a displaced particle back to its original position. Since the odd viscous stress does not dissipate energy, inertial oscillations and inertial-like waves can become prominent in such a liquid. In this article we show that an odd viscous liquid in \emph{three} dimensions gives rise to such axially symmetric waves and also to plane-polarized waves. We tacitly assume that an anisotropy axis giving rise to odd viscous effects has already been established and proceed to investigate the effects of odd viscosity on fluid flow behavior. Numerical simulations of the full Navier-Stokes equations show the existence of inertial-like waves downstream a body that moves slowly along the axis of an odd viscous liquid-filled cylinder. The wavelength of the numerically-determined oscillations agrees well with the developed theoretical framework. When odd viscosity is the dominant effect in steady motions, a modified Taylor-Proudman theorem leads to the existence of Taylor columns inside such a liquid. Formation of the Taylor column can be understood as a consequence of helicity segregation and energy transfer along the cylinder axis at group velocity, by the accompanying inertial waves, whenever the reflection symmetry of the system is lost. A number of Taylor column characteristics known from rigidly-rotating liquids, are recovered here for a \emph{non-rotating} odd viscous liquid. These include counter-rotating swirling liquid flow above and below a body moving slowly along the anisotropy axis.