paper

The rotation of a sedimenting anisotropic particle in a linearly stratified ambient

arXiv:2102.08580 · doi:10.1017/jfm.2021.1016

Abstract

We derive the torque on a spheroid of an arbitrary aspect ratio sedimenting in a linearly stratified ambient. The analysis demarcates regions in parameter space corresponding to broadside-on and edgewise (longside-on) settling in the limit , where and , the Reynolds and viscous Richardson numbers, respectively, are dimensionless measures of the importance of inertial and buoyancy forces relative to viscous ones. Here, is the spheroid semi-major axis, an appropriate settling velocity scale, the fluid viscosity, and the (constant)\,density gradient characterizing the stably stratified ambient, with being the fluid density taken to be a constant within the Boussinesq framework. A reciprocal theorem formulation identifies three contributions to the torque: (1) an inertial contribution that already exists in a homogeneous ambient, and orients the spheroid broadside-on; (2) an hydrostatic contribution due to the ambient linear stratification that also orients the spheroid broadside-on; and (3) a hydrodynamic contribution arising from the perturbation of the ambient stratification by the spheroid whose nature depends on ; being the Peclet number with the diffusivity of the stratifying agent. For , the hydrodynamic contribution is ) in the Stokes stratification regime characterized by , and orients the spheroid edgewise regardless of . The differing orientation dependencies of the inertial and large- hydrodynamic stratification torques imply that the broadside-on and edgewise settling regimes are separated by two distinct -dependent critical curves in the plane. The predictions are consistent with recent experimental observations.

34 pages, 15 figures

References in corpus (1)

Cited by in corpus (3)