The Effects of Convection in Geostrophic Circulation
Abstract
Ocean circulation plays an important role in global climate
through the transport of heat and CO2. Surface fluxes of buoyancy
and momentum act as primary energy inputs to the circulation,
however the surface buoyancy contribution and the effects of
vertical convection are not well understood. We examine flow
driven by a buoyancy difference applied at a horizontal surface
in a closed rotating basin: this is rotating horizontal
convection. We use laboratory experiments, direct numerical
simulations and scaling analyses to examine the effect of
buoyancy and rotation on the mechanical energy budget and
dynamical regimes. In one of these regimes the large-scale
circulation is coupled to deep ‘chimney’ convection.
The direct numerical simulations solve for flow in a rectangular
box with a higher temperature applied over half of the base and a
lower temperature over the other half, and a uniform Coriolis
parameter. The emphasis is on circulation with a turbulent
thermal boundary layer and small-scale convection while having a
fully-resolved energy budget. The buoyancy forcing and Coriolis
parameter are varied to examine the two primary sinks of
mechanical energy: irreversible mixing (potential energy sink)
and viscous dissipation (kinetic energy sink). Turbulent mixing
and heat transport are reduced by rotation, while viscous
dissipation is independent of rotation rate. The reduction of
heat transport is consistent with existing geostrophic boundary
layer scaling, and is inherently linked to the total amount of
mixing. Even in the presence of strong rotation, energy from
surface buoyancy forcing mostly goes to mixing. For a
buoyancy-driven circulation in a basin comparable to the North
Atlantic we estimate that mixing is a sink for over 95% of the
mechanical energy supply, implying that buoyancy is an efficient
driver of ocean circulation.
The laboratory experiments closely resemble the simulations, but
have an imposed heat flux over the heated region. The experiments
further demonstrate the transition from non-rotating horizontal
convection to circulation governed by geostrophic boundary layer
flow. The flow is well described by a convective Rossby number,
which compares the strength of horizontal convective to Coriolis
accelerations in the boundary layer. For more rapid rotation the
momentum budget is dominated by fluctuating vertical
accelerations in a ‘chimney’ region of vertical plumes.
Chimney convection limits the geostrophic inhibition of
basin-scale circulation, halting the increase of temperature
difference across the basin (or decrease of Nusselt number) with
decreasing Rossby number. The North Atlantic Ocean is estimated
to lie in the regime controlled by chimney convection, which is
evidence for deep convection being an important limit on heat
transport.
The experiments and simulations show that buoyancy forcing
produces basin-scale gyres and boundary currents, features of
mid-latitude ocean circulation often attributed to wind stress.
The simulations are used to examine the contribution of boundary
currents and various other flow structures to the heat transport.
At the Rayleigh numbers achievable, the turbulent viscous
dissipation and irreversible mixing are primarily constrained to
the thermal boundary layer. These results can be extrapolated to
show the distribution of heat transport and energy dissipation in
a buoyancy-driven ocean.
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