Scaling laws and flow structures of double diffusive convection in the finger regime

TL;DR

This study develops and validates scaling laws for double diffusive convection in the finger regime, revealing how salinity flux, flow velocity, and heat flux depend on key parameters and aligning with existing theories.

Contribution

The paper introduces new scaling laws for DDC in the finger regime, linking flow parameters to Rayleigh number and density ratio, and extends the theory to experimental data.

Findings

Salinity flux primarily depends on salinity Rayleigh number

Rescaled flow velocity and heat flux depend only on Rayleigh number

Salt-finger width and boundary layer thickness follow power-law scaling with Rayleigh number

Abstract

Direct numerical simulations are conducted for double diffusive convection (DDC) bounded by two parallel plates, with fluid properties similar to the values of seawater. The DDC flow is driven by an unstable salinity difference and stabilized at the same time by a temperature difference. For these conditions the flow can be in the finger regime. We develop scaling laws for three key response parameters of the system: The non-dimensional salinity flux $Nu_S$ mainly depends on the salinity Rayleigh number $Ra_S$, which measures the strength of the salinity difference, and exhibits a very weak dependence on the density ratio $\Lambda$, which is the ratio of the buoyancy forces induced by two scalar differences. The non-dimensional flow velocity $Re$ and the non-dimensional heat flux $Nu_T$ are dependent on both $Ra_S$ and $\Lambda$. However, the rescaled Reynolds number $Re\Lambda^{\alpha^{\rm eff}_u}$ and the rescaled convective heat flux $(Nu_T-1)\Lambda^{\alpha^{\rm eff}_T}$ depend only on $Ra_S$. The two exponents are dependent on the fluid properties and are determined from the numerical results. Moreover, the behaviors of $Nu_S$ and $Re\Lambda^{\alpha^{\rm eff}_u}$ agree with the predictions of the Grossmann-Lohse theory which was originally developed for the Rayleigh-B\'{e}nard flow. The non-dimensional salt-finger width and the thickness of the velocity boundary layers, after being rescaled by $\Lambda^{\alpha^{\rm eff}_u/2}$, collapse and obey a similar power-law scaling relation with $Ra_S$. When $Ra_S$ is large enough, salt fingers do not extend from one plate to the other and horizontal zonal flows emerge in the bulk region. We then show that the current scaling strategy can be successfully applied to the experimental results of a heat-copper-ion system~(Hage and Tilgner, Phys. Fluids, 22, 076603, 2010).