On the energetics of stratified turbulent mixing, irreversible thermodynamics, Boussinesq models, and the ocean heat engine controversy
Remi Tailleux

TL;DR
This paper revisits the energetics of stratified turbulence, clarifies the roles of different internal energy components, and discusses the implications for ocean circulation and the heat engine controversy.
Contribution
It introduces a new decomposition of internal energy and revises the understanding of energy conversion processes in stratified turbulence.
Findings
W_{r,turbulent} equals D(APE) in Boussinesq fluids, linking APE dissipation to GPE_r increase.
In non-Boussinesq fluids, the relation is approximate and W_{r,turbulent} can be negative.
Buoyancy forcing is as significant as mechanical forcing in driving ocean circulation.
Abstract
A key issue in stratified turbulence theory concerns the nature of the link between D(APE), the dissipation rate of available potential energy APE, and W_{r,turbulent}, the turbulent rate of change of background gravitational potential energy GPE_r, which are both controlled by molecular diffusion. For Boussinesq fluids with a linear equation of state, this link is simply W_{r,turbulent}=D(APE), widely interpreted as implying that GPE_r increases at the expense of APE, in contrast with the laminar case where GPE_r increases at the expense of internal energy (IE). This idea is revisited here by regarding IE as the sum of three distinct subcomponents: available internal energy (AIE), exergy (IE_{exergy}), and dead internal energy (IE_0). In this new view, D(APE) is the dissipation rate of APE into IE_0, while both W_{r,laminar} and W_{r,turbulent} convert IE_{exergy} into GPE_r. The…
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