The cross-over from viscous to inertial lengthscales in rapidly-rotating convection

TL;DR

This study investigates the transition in rapidly-rotating convection from viscous to inertial dominance using numerical simulations, revealing that the inertial lengthscale surpasses the viscous scale in core convection.

Contribution

It identifies the crossover point where inertial effects dominate over viscous effects in rapidly-rotating convection through numerical analysis.

Findings

Inertial lengthscale approximately equals viscous lengthscale at crossover

Core convection is dominated by inertial scale, which is much larger than viscous scale

Transition occurs when inertial lengthscale matches viscous lengthscale

Abstract

Convection is the main heat transport mechanism in the Earth's liquid core and is thought to power the dynamo that generates the geomagnetic field. Core convection is strongly constrained by rotation while being turbulent. Given the difficulty in modelling these conditions, some key properties of core convection are still debated, including the dominant energy-carrying lengthscale. Different regimes of rapidly-rotating, unmagnetised, turbulent convection exist depending on the importance of viscous and inertial forces in the dynamics, and hence different theoretical predictions for the dominant flow lengthscale have been proposed. Here we study the transition from viscously-dominated to inertia-dominated regimes using numerical simulations in spherical and planar geometries. We find that the cross-over occurs when the inertial lengthscale approximately equals the viscous lengthscale. This suggests that core convection in the absence of magnetic fields is dominated by the inertial scale, which is hundred times larger than the viscous scale.