AIR-SEA
FLUXES FROM THE NCEP OPERATIONAL ANALYSIS/FORECAST SYSTEM
Glenn
H. White1, K. Campana1 and J. Janowiak2
1Environmental
Modelling 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 is often not evaluated as fully, 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 (NCEP-1; Kalnay et al., 1996; Kistler et al., 2001) and a second from 1979 to
the present (Kanamitsu et al.,
1999). The long, consistent data sets
from reanalyses provided a golden opportunity to evaluate surface fluxes
against independent estimates and many studies did so (Taylor, 2000, section
11.4). However, the operational NCEP
global system has evolved considerably from the versions used in the reanalyses
and it is not immediately obvious how applicable the lessons learned from
reanalysis are to the operational model.
This paper examines air-sea fluxes from the current NCEP operational system
and compares them to fluxes from NCEP’s Climate Data Assimilation System, the
continuation of the NCEP/NCAR (NCEP-1) reanalysis. It seeks to determine whether the system's physics has improved
over the last 6 years (the NCEP-1 reanalysis is based on the operational system
of 1995) and to gain insight into problems in the operational model physics.
Global Mean Balances
May 2000-April 2001
|
|
CDAS |
Operational |
Kiehl & Trenberth |
Range |
|
Precipitation |
2.85 mm/d |
3.00 |
2.69 |
2.69-3.1 (2.83,2.83) |
|
Evaporation |
2.90 |
3.02 |
|
|
|
Precipitation minus Evaporation |
-.05 |
-.02 |
|
|
|
Sensible heat |
16.53 W/m2 |
11.6 |
24 |
16-27(21,21) |
|
Latent heat |
84.06 |
87.46 |
78 |
78-90(82,82) |
|
Surface downward
short wave |
206.13 |
197.58 |
198 |
|
|
Upward short wave |
45.31 |
28.31 |
30 |
|
|
Net short wave |
160.82 |
169.27 |
168 |
142-174 (163, 168) |
|
Downward long wave |
334.66 |
336.7 |
324 |
|
|
Upward long wave |
395.89 |
397.5 |
390 |
|
|
Net long wave |
61.23 |
60.8 |
66 |
40-72(59, 63) |
|
Net radiation |
99.58 |
108.48 |
102 |
99-119 (104,103) |
|
Surface Net Heat
Flux |
-1 |
9.42 |
0 |
|
|
TOA downward short wave |
341.87 |
|
342 |
|
|
Upward short wave |
116.81 |
102.38 |
107 |
|
|
Outgoing long wave |
237.78 |
243.46 |
235 |
|
|
TOA net radiation |
-12.71 |
-3.97 |
|
|
|
Atmospheric heating |
-11.72 |
-13.39 |
|
|
Table
1 Global mean surface and top of the atmosphere fluxes averaged over May
2000-April 2001 from 0-6 hr forecasts from the NCEP-1 reanalysis or CDAS, and
the operational NCEP global analysis/forecast system compared to a
climatological estimate from Kiehl and Trenberth (1997). The last column gives the range of the
estimates reviewed by Kiehl and Trenberth and in parentheses the mean and
median value. Highlighted values
indicate substantial differences between CDAS and the operational analyses.
The
operational model considered here has higher resolution (T170, 42 levels) than
CDAS (T62, 28 levels) and uses satellite radiances in its assimilation rather
than NESDIS temperature soundings. It
has updated short wave radiation and boundary layer parameterisations and a
corrected surface albedo. It also has
changes to horizontal and vertical diffusion, gravity wave drag and a retuned
cloudiness parameterisation. To correct
a problem in the air-sea flux parameterisation (Zeng et al., 1998), a new thermal roughness based on TOGA COARE
observations is used in the operational model.
Since the period compared here, a new parameterisation of cloudiness
based on prognostic cloud liquid water and a parameterisation of cumulus
momentum mixing has been introduced in the operational system on May 15,
2001. The new cloudiness appears to
give more realistic surface net short wave near the equator and has more
low-level stratus clouds in the eastern sub-tropical oceans. Further tuning of the new cloudiness is
planned.
As shown in
Tables 1 and 2, the operational system has more realistic surface short wave
radiation than CDAS. However, the
surface energy balance is more out of balance in the operational system and
sensible heat flux in the operational system is lower than other
estimates. Oceanic evaporation in
NCEP-1 was higher than ship-based estimates and is higher still in the
operational model; decreasing the evaporation would increase the surface energy
imbalance.
Global Mean Balances
May
2000-Apr. 2001
Ocean
|
|
CDAS |
Operational |
COADS |
SRB |
|
Precipitation |
3.1 mm/day |
3.29 |
|
|
|
Evaporation |
3.4 |
3.52 |
|
|
|
Precipitation minus Evaporation |
-.29 |
-.23 |
|
|
|
Sensible heat |
12.71 W/m2 |
6.27 |
10.1 |
|
|
Latent heat |
98.47 |
101.97 |
88 |
|
|
Surface downward short wave |
199.85 |
195.04 |
|
|
|
Upward
short wave |
35.15 |
18.25 |
|
|
|
Net
short wave |
164.7 |
176.79 |
170.4 |
173.4 |
|
Downward long wave |
352.06 |
350.89 |
|
|
|
Upward long wave |
408.11 |
408.19 |
|
|
|
Net long wave |
56.04 |
57.29 |
49.2 |
41.9 |
|
Net radiation |
108.66 |
119.50 |
|
|
|
Surface Net heat
Flux |
-2.52 |
11.25 |
23.3 |
|
|
TOA downward short wave |
349.53 |
|
|
|
|
Upward short wave |
117.95 |
98.71 |
|
|
|
Outgoing long wave |
239.46 |
246.60 |
|
|
|
TOA net radiation |
-7.87 |
4.22 |
|
|
|
Net atmospheric heating |
-5.35 |
-7.03 |
|
|
Table
2 Global mean fluxes over the ocean for May 2000-April 2001. COADS refers to climatological estimates by
da Silva et al. (1994) for 1981-92,
SRB to satellite based radiation estimates by Darnell et al. (1992) and Gupta et
al. (1992).
Figure 1 compares precipitation
during June-August 2000 from 0-6 hr forecasts from the NCEP operational system
and from CDAS to OPI, an independent estimate based on rain gauges and infrared
satellite estimates. The NCEP1
reanalysis did not concentrate 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.
Figure 2 displays total cloudiness
for March-May 2000 from U.S. Air Force nephanalyses, CDAS and the NCEP
operational system. The operational
system clearly resembles the nephanalyses more in the tropics, except in the
eastern subtropical oceans. The
operational system clearly has too few low-level stratus clouds in these
regions, a common problem in NWP data assimilation systems (Taylor, 2001).
Differences in surface fluxes for
March-May 2000 between CDAS and the NCEP operational system are shown in Fig.
3. Large differences in surface net
heat flux can be seen and are clearly dominated by differences in surface net
short wave flux. Large differences in
net short wave can be seen over the Indonesian region, where CDAS has too
little cloudiness, and in the eastern subtropical oceans where the operational
system has too little.
Air-sea
fluxes from the currently operational NCEP global analysis/forecast system are
distinctly different from CDAS. The
precipitation pattern is substantially improved and short wave radiation is
more realistic. Surface winds and stress in the Pacific are stronger and in
better agreement with other estimates.
However, oceanic sensible heat flux is now lower than other estimates
and the ocean surface energy balance is more out of balance. Radiation and clouds still require
substantial improvement. Low-level stratus clouds in particular are a problem;
the lack of them in the operational system distorts the surface radiation
budget. Our knowledge of the surface fluxes also requires substantial
improvement for model development: 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, it is not clear that
surface flux estimates from such observations and parameterisation schemes
yield reasonable global surface energy balance.



Figure
1 Precipitation during June-July 2001 from (top) OPI based on raingauges and
satellite estimates and from 0-6 h forecasts from (middle) the operational
system and (bottom) CDAS. Contours in
mm/day.



Figure
2 Total cloud cover in per cent for March-May 2000 from (top) U.S. Air Force
nephanalyses and from 0-6 h forecasts from (middle) CDAS and (bottom) the
operational analysis/forecast system.




Figure
3 Differences in (top left) sensible heat, (bottom left) latent heat, (top
right) surface net short wave and (bottom right) surface net heat flux during
March-May 2000, CDAS minus operational system, in Watts/m2. Positive
values denote more upward flux in CDAS on the left, more downward flux in CDAS
on the right. Contour and shading are
the same in each figure.
REFERENCES
da
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