Penetrative turbulent convection from a localized circular
top source into a rotating,
linearly stratified ambient fluid of strength N has
been investigated in a laboratory
tank. Initially, the induced three-dimensional convective flow
penetrated rapidly into
the stratified water column until it reached an equilibrium depth
at which the
convective flow began to propagate radially outward. At this stage,
the usual cyclonic
vortices were generated around the convection source at the edge
of the radially propagating flow. Soon after, a thin ‘subsurface
anticyclone’ was formed at the level
of equilibrium depth beneath the convection source. Later, this
anticyclone dominated
the central part of the convective regime and did not allow
new cyclones to be injected
into the system. After reaching its maximum mean diameter
Da/R
≈10(R0;R)2/3 and
swirl velocity va
≈(B0R)1/3,
an anticyclone became unstable and split into two new
vortices that left the area beneath the source, allowing a new
anticyclone to form at its original place (here,
R0,R
=(B0/f3R2)
1/2 is the Rossby number based on R the
radius of the source, B0 is the surface
negative buoyancy flux, and f is the Coriolis
parameter). These observations provide crucial evidence that many
of the ‘subsurface
anticyclonic’ vortices detected in the stratified pycnocline
of the central Arctic Ocean
are indeed generated as a result of convective processes occurring
in this region.