B. Dong et Pj. Valdes, SIMULATIONS OF THE LAST GLACIAL MAXIMUM CLIMATES USING A GENERAL-CIRCULATION MODEL - PRESCRIBED VERSUS COMPUTED SEA-SURFACE TEMPERATURES, Climate dynamics, 14(7-8), 1998, pp. 571-591
The climate during the Last Glacial Maximum (LGM) has been simulated u
sing the UK Universities Global Atmospheric Modelling Programme (UGAMP
) general circulation model (GCM) with both prescribed sea surface tem
peratures (SSTs) based on the CLIMAP reconstruction and computed SSTs
with a simple thermodynamic slab ocean. Consistent with the Paleoclima
te Modelling Intercomparison Project (PMIP), the other boundary condit
ions include the large changes in ice-sheet topography and geography,
a lower sea level, a lower concentration of CO, in the atmosphere, and
a slightly different insolation pattern at the top of the atmosphere.
The results are analysed in terms of changes in atmospheric circulati
on. Emphasis is given to the changes in surface temperatures, planetar
y waves, storm tracks and the associated changes in distribution of pr
ecipitation. The model responds in a similar manner to the changes in
boundary conditions to previous studies in global mean statistics, but
differs in its treatment of regional climates. Results also suggest t
hat both the land ice sheets and sea ice introduce significant changes
in planetary waves and transient eddy activity, which in turn affect
regional climates. The computed SST simulations predict less sea ice a
nd cooler tropical temperatures than those based on CLIMAP SSTs. It is
unclear as to whether this is a model and/or a data problem, but the
resulting changes in land temperatures and precipitation can be large.
Snow mass budget analysis suggests that there is net ice loss along t
he southern edges of the Laurentide and Fennoscandian ice sheets and n
et ice gain over other parts of the two ice sheets. The net accumulati
on is mainly due to the decrease in ablation in the cold climate rathe
r than to the changes in snowfall. The characteristics of the Greenlan
d ice-sheet mass balance in the LGM simulations is also quite differen
t from those in the present-day (PD) simulations. The ablation in the
LGM simulations is negligible while it is a very important process in
the ice mass budget in the PD simulations.