A comparison of cloud and boundary layer variables in the ECMWF forecast model with observations at Surface Heat Budget of the Arctic Ocean (SHEBA) ice camp
Ja. Beesley et al., A comparison of cloud and boundary layer variables in the ECMWF forecast model with observations at Surface Heat Budget of the Arctic Ocean (SHEBA) ice camp, J GEO RES-A, 105(D10), 2000, pp. 12337-12349
Cloud and boundary layer variables from the European Centre for Medium-Rang
e Weather Forecasts (ECMWF) forecast model were compared with measurements
made from surface instruments and from upward looking 8 mm wavelength radar
and lidar at the Surface Heat Budget of the Arctic Ocean (SHEBA) ice camp
during November and December of 1997. The precipitation accumulation, near-
surface winds, and surface downward longwave irradiance predicted by the mo
del were in good agreement with SHEBA observations during this period. Howe
ver, surface downward longwave irradiance was underestimated by 10 W m(-2)
on average when low clouds were present in the model and observations. The
model demonstrated considerable skill in predicting the occurrence and vert
ical extent of cloudiness over SHEBA, with some tendency to overestimate th
e frequency of clouds below 1 km. A synthetic radar reflectivity estimated
from the ECMWF model variables was compared with 8 mm wavelength radar meas
urements. The two were broadly consistent only if the assumed snowflake siz
e distribution over SHEBA had a smaller proportion of large flakes than was
found in previous studies at lower latitudes. The ECMWF model assumes a te
mperature-dependent partitioning of cloud condensate between water and ice.
Lidar depolarization measurements at SHEBA indicate that both liquid and i
ce phase clouds occurred over a wide range of temperatures throughout the w
inter season, with liquid occurring at temperatures as low as 239 K. A much
larger fraction of liquid water clouds was observed than the ECMWF model p
redicted. The largest discrepancies between the ECMWF model and the observa
tions were in surface temperature (up to 15 K) and turbulent sensible heat
fluxes (up to 60 W m(-2)). These appear to be due at least partially to the
ECMWF sea ice model, which did not allow surface temperatures to respond n
early as rapidly to changing atmospheric conditions as was observed.