K. Akitomo et al., OPEN-OCEAN DEEP CONVECTION IN THE WEDDELL SEA - 2-DIMENSIONAL NUMERICAL EXPERIMENTS WITH A NONHYDROSTATIC MODEL, Deep-sea research. Part 1. Oceanographic research papers, 42(1), 1995, pp. 53-73
Numerical experiments with a two-dimensional nonhydrostatic model were
carried out to investigate the generation processes of open-ocean dee
p convection, deep water formation and ventilation around the Maud Ris
e in the Weddell Sea, Antarctica. The thermobaric effect, i.e. an incr
ease in the thermal expansion rate of sea water with pressure (water d
epth), is essential for the onset of deep convection in this region an
d for the overturning of the water column to occur abruptly. Thermal-l
ike plumes induced by the thermobaric instability destroy the thermocl
ine (halocline) and transport the cold and less-saline mixed layer wat
er into the warm and more-saline underlying layer. Then the underlying
water ascends to push the thermocline (halocline) up until it disappe
ars at the sea surface. It takes only a few days for the thermocline (
halocline) to disappear without sea-ice cover. On the other hand, it t
akes more than 30 days with a sea-ice cover because of the reduction o
f the cooling rate. The stability of the water column around the Maud
Rise in no-polynya winter 1986 was examined. The area over the rise is
likely to overturn before the end of the cooling season while the mar
ginal area is not. This suggests that the area over the rise may be on
e of the source regions for the convective features observed throughou
t the Weddell Sea. The rate of deep water formation due to this overtu
rning and the associated upward heat flux are estimated at 0.91 x 10(5
) m(3) s(-1) and 36 W m(-2) over one year, respectively, which are 2 s
imilar to 3 times of those caused by the entrainment of the Weddell De
ep Water into the mixed layer when no overturning occurs. No-overturni
ng stations on the margin of the rise are classified into two types. A
t one type of station, salinity in the relatively thick mixed layer is
too low for the water column to be destabilized before the end of the
cooling season; at the other type of station, the relatively thin mix
ed layer with a relatively high salinity and the warm Weddell Deep Wat
er inhibit an overturning through a previously described negative feed
back process. Sensitivity of the model result to several physical para
meters expressing turbulent mixing was also examined.