Preconditioned regions of the open ocean are usually characterised by local
ised cyclonic gyres that make these areas susceptible to deep convection. I
n this study the effect of the ambient circulation on the formation and sub
sequent lateral spreading of deep water formed during open ocean convection
was investigated in the laboratory. Oceanic convection was modelled using
a circular tank mounted on a rotating table. For experimental convenience t
he ambient circulation was produced by a differentially rotating false bott
om and convection was initiated by heating from below, rather than cooling
from above. The dominant mechanisms for lateral spreading of the warm conve
ctive fluid varied depending on the speed of the bottom rotation. Lateral t
ransport of heat was dominated by the propagation of baroclinic eddies from
the convective region into the ambient region for low bottom rotation rate
s and by Ekman transport for high bottom rotation rates. The cyclonic flow
field hindered lateral transport by baroclinic instabilities in the laborat
ory, thereby weakening the lateral transport of heat by this mechanism. At
the same time, the efficiency of Ekman transport as a means for lateral hea
t or buoyancy flux increased as bottom rotation rate increased. Together, t
hese two processes resulted in a slight increase in the lateral density ano
maly at steady state with increasing bottom rotation rate for anl Ohm < 0.4
and a rapid decrease in the lateral density anomaly for Delta Ohm/Ohm > 0.
4, where Delta Ohm is the rotation rate of the false bottom and Ohm is the
planetary rotation rate.