A comparison of surface fluxes from the NCEP Global
Operational Analysis/Forecast System and the NCEP Reanalyses
Glenn H. White1, K. Campana1 and J.
Janowiak2
1Environmental Modeling Center/2Climate Prediction
Center
National Centers for Environmental Prediction/National
Weather Service
National Oceanic and Atmospheric Administration, U. S. Dept.
of Commerce
Washington, D.C., USA
Glenn.White@noaa.gov
Analysis/forecast systems used in
numerical weather prediction (NWP) have matured to the point that further
development requires the direct verification of model physics. Changes in
operational NWP systems are designed to improve their synoptic forecast
performance; their effect on surface fluxes are often not evaluated as fully as
their effect on synoptic performance, in part because reliable independent
estimates of surface fluxes are more difficult to obtain than measurements of
atmospheric fields.
NCEP conducted two major reanalyses,
one from 1948 to the present (Kalnay et
al., 1996; Kistler et al., 2000)
and a second from 1979 to the present (Kanamitsu et al., 1999). The long,
consistent data sets from reanalysis provided a golden opportunity to evaluate
surface fluxes against independent estimates over long periods, and many
studies did (Taylor, 2000, sect. 11.4).
However, the operational NCEP global system has developed considerably
from the versions used in the reanalyses and it is not clear how applicable the
lessons learned from reanalysis are to the operational model. Even relatively small changes can make large
differences in surface fluxes, as can be seen in the differences between the
first and second NCEP reanalyses (Taylor, 2000, sect. 11.4). This paper
examines the systematic performance of surface fluxes in the current NCEP
operational system and compares the fluxes to fluxes for the same period from
NCEP’s Climate Data Assimilation System (CDAS), the continuation of the first
NCEP/NCAR reanalysis.
|
|
CDAS |
Op |
K&T |
Range |
|
Precipitation |
2.829 mm/day |
3.035 |
2.69 |
2.69-3.1(2.83,2.83) |
|
Evaporation |
2.871 |
2.98 |
|
|
|
Precipitation-Evaporation |
-.042 |
.055 |
|
|
|
Sensible heat |
15.85 W/m2 |
12.5 |
24 |
16-27(21,21) |
|
Latent heat |
83.27 |
86.43 |
78 |
78-90(82,82) |
|
Sfc
downward short-wave |
206.34 |
198.59 |
198 |
|
|
Upward short-wave |
45.27 |
28.45 |
30 |
|
|
Net short-wave |
161.07 |
170.14 |
168 |
142-174(163, 168) |
|
Downward long-wave |
334.44 |
337.44 |
324 |
|
|
Upward long-wave |
395.79 |
397.47 |
390 |
|
|
Net long-wave |
61.36 |
60.03 |
66 |
40-72(59, 63) |
|
Net radiation |
99.72 |
110.11 |
102 |
99-119(104,103) |
|
Net heat flux |
0.59 |
11.18 |
0 |
|
|
TOA
downward short-wave |
341.83 |
|
342 |
|
|
Upward short-wave |
116.54 |
99.18 |
107 |
|
|
Outgoing long-wave |
237.9 |
242.73 |
235 |
|
|
TOA radiation balance |
-12.62 |
-0.09 |
|
|
|
Net
atmospheric heating |
-13.21 |
-11.27 |
|
|
Table 1. Global mean hydrological, surface energy and top of the atmosphere radiation budgets in 0-6 hour forecasts from CDAS and the NCEP operational global system during July 1999-June 2000 compared to Kiehl and Trenberth (1997) (K&T). The range is the range of global mean estimates examined in K&T, the two numbers in brackets are the mean and the mode of the estimates.
|
|
CDAS |
op |
COADS |
SRB |
|
Precipitation |
3.053
mm/day |
3.287 |
|
|
|
Evaporation |
3.322 |
3.473 |
|
|
|
Precipitation-Evaporation |
-.269 |
-.187 |
|
|
|
Sensible
heat |
12.49
W/m2 |
6.59 |
10.1 |
|
|
Latent
heat |
96.34 |
100.73 |
88 |
|
|
Sfc downward
short-wave |
199.97 |
195.29 |
|
|
|
Upward
short-wave |
35.58 |
18.36 |
|
|
|
Net
short-wave |
164.39 |
176.93 |
170.4 |
173.4 |
|
Downward
long-wave |
350.13 |
352.39 |
|
|
|
Upward
long-wave |
406.7 |
408.3 |
|
|
|
Net
long-wave |
56.57 |
55.91 |
49.2 |
41.9 |
|
Net
radiation |
107.82 |
121.02 |
|
|
|
Net
heat flux |
-1 |
13.7 |
23.3 |
|
|
TOA downward
short-wave |
347.38 |
|
|
|
|
Upward
short-wave |
116.58 |
95.68 |
|
|
|
Outgoing
long-wave |
239.56 |
245.88 |
|
|
|
TOA
radiation balance |
-8.76 |
5.83 |
|
|
|
Net atmospheric heating |
-7.75 |
-7.87 |
|
|
Land
|
|
CDAS |
Op |
|
Precipitation |
2.272 mm/day |
2.388 |
|
Evaporation |
1.75 |
1.792 |
|
Precipitation-Evaporation |
.521 |
.596 |
|
Sensible
heat |
24.23 W/m2 |
26.84 |
|
Latent
heat |
50.76 |
51.97 |
|
Sfc downward
short-wave |
222.18 |
207.6 |
|
Upward
short-wave |
69.37 |
53.24 |
|
Net
short-wave |
152.81 |
154.37 |
|
Downward
long-wave |
295.4 |
301.27 |
|
Upward
long-wave |
368.67 |
371.3 |
|
Net
long-wave |
73.27 |
70.03 |
|
Net
radiation |
79.54 |
84.34 |
|
Net
heat flux |
4.55 |
5.54 |
|
TOA downward
short-wave |
328.01 |
|
|
Upward
short-wave |
116.43 |
108.2 |
|
Outgoing
long-wave |
233.77 |
235.27 |
|
TOA
radiation balance |
-22.2 |
-15.46 |
|
Net atmospheric heating |
-26.74 |
-21 |
Table 2.
Global mean hydrological, surface energy, and TOA radiation budgets over
ocean and land during July 1999-June 2000.
COADS refers to estimates by da Silva et al. (1994) for 1981-92, SRB to satellite-based surface radiation
estimates by Darnell et al. (1992)
and Gupta et al. (1992).
The operational system
has more realistic downward and upward surface short wave radiation, due to
changes in the short wave radiation parameterization and new surface
albedo. The CDAS system had too high
surface albedo over the ocean. Both
systems, however, had more downward and net short wave surface radiation over
the Northern Hemisphere mid-latitude continents during March-May than SRB
climatological estimates. However, the
surface energy budget is more out of balance in the operational system than in
CDAS, especially over the ocean, and oceanic sensible heat flux in the
operational model is lower than other estimates. The radiation budget at the top of the atmosphere is much closer
to balance in the operational system, reflecting compensating errors in the
outgoing long wave and short wave radiation. Oceanic evaporation in the first
NCEP/NCAR reanalysis was higher than ship-based estimates (Smith et al., 1999) and evaporation in the
operational model is higher still; however, decreasing the evaporation would
increase the surface energy imbalance.
Fig.1 compares precipitation during
March-May 2000 from the NCEP operational
system and from CDAS
to OPI, an independent estimate based on rain gauges and infrared satellite
estimates. The NCEP1 reanalysis was
criticized for not concentrating tropical precipitation enough and that is
clearly evident. Precipitation from the
operational analysis/forecast system is clearly more like the OPI estimate in
the tropics than CDAS is.
Fig. 2 compares zonal mean top of
the atmosphere outgoing long wave radiation for March-May 2000 from the
operational model and CDAS to satellite measurements. Both have too much OLR in the subtropics, perhaps reflecting the
lack of aerosol in either system
and problems with
cloudiness in amount and properties.
Over the ocean the operational system is generally further from the
observations than CDAS, especially in the subtropics.
Fig. 3 displays differences in total cloudiness between the model estimates and Air Force operational nephanalyses for March-May 2000. Both CDAS and the operational analysis/forecast system show too much cloudiness in the tropics and at high northern latitudes. CDAS shows a dipole



Fig. 1 Precipitation during March-May 2000 from (top) OPI, based on satellite infrared measurements over the ocean and rain gauges over land, and from 0-6 hr forecasts by (middle) the NCEP operational analysis/forecast system and (bottom) CDAS. Contours 1, 3, 5, 7, 9, 13, 17, 21 mm/day, greater than 5 mm/day shaded.


Fig. 2 Zonal mean top of the atmosphere outgoing long wave radiation over (left) land and (right) ocean from satellite measurements and from 0-6 hr forecasts by the NCEP operational global analysis/forecast system and by CDAS in Watts/m2.
pattern in the west Pacific, with too little cloudiness over Indonesia and too much to the east, reflecting a failure to concentrate tropical convection enough. The operational system has too little cloudiness over the eastern subtropical oceans off Baja California and western South America, showing a deficiency in low-level stratus clouds. CDAS has more realistic low-level stratus clouds, but has too much off Baja California and off Africa and also misplaces them in some regions. The Global Modeling Branch recently adjusted its low-level clouds in response to complaints of too much low-level cloudiness over the Arabian Sea. The Global Modeling Branch is currently testing a prognostic cloud liquid water parameterization and is carefully evaluating the resulting cloudiness.
Conclusions
Surface fluxes in the NCEP operational global analysis/forecast system are distinctly different from CDAS. The precipitation pattern is substantially improved and short wave radiation is more realistic. However, sensible heat flux is now lower than other estimates and the ocean surface energy


Fig. 3 Differences in total cloud cover between 0-6 hr forecasts from (top) the NCEP operational analysis/forecast system and (bottom) CDAS and Air Force nephanalyses during March-May 2000. Contour interval 10%, zero omitted, values less than –10% shaded.
budget is more out of balance. Radiation and clouds still require substantial improvements. Knowledge of the surface fluxes also requires substantial improvement: for example, the magnitude of evaporation and the hydrological cycle is not well known. Estimates from ship-based observations imply that both CDAS and the operational model have too much evaporation; however, surface flux estimates from ship observations do not give a reasonable global surface energy balance. While uncertainties exist in independent estimates of surface fluxes and atmospheric physics in general, they are accurate enough (and errors in NWP systems’ physics are large enough) to point to ways to improve NWP systems substantially.
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