HTML
-
The WRF model (Skamarock et al. [15]; Wang et al. [16]) is a non-hydrostatic, fully compressible, primitive equation model. In this study, the WRF model was run with a 0.25° domain over the continental U. S. (Fig. 1). The physics schemes used in the model were as follows: the WRF Single-Moment 3-class scheme for microphysics; the RRTM scheme for longwave radiation and the Goddard shortwave scheme for shortwave radiation; the Noah Land Surface Model for the land surface; the Yonsei University scheme for the planetary boundary layer; and the Grell-Devenyi ensemble scheme for cumulus parameterization.
Figure 1. Study domain over the continental U.S. The shading indicates land (grey) and water (blue). The domain has a horizontal resolution of 0.25°.
The GFS whole atmospheric product set with a horizontal resolution of 0.5° × 0.5° and 47 unevenly distributed vertical levels with a top at 1 mb was used to provide the initial and boundary conditions for the WRF model. The GFS whole atmospheric data product has a vertical grid spacing of 25 mb below 100 mb, and another 10 levels between 100 mb and 1 mb (at 70, 50, 30, 20, 10, 7, 5, 3, 2 and 1 mb respectively).
The community gridpoint statistical interpolation (GSI) system was used as the data assimilation system in this study. The latest GSI version features the application of surface analysis, basic 3D-Var, an ensemble Kalman filter (EnKF), a Hybrid scheme, and 4D-Var if coupled with an adjoint GSI model-supported forecast system (Kleist [17]; Wang et al. [18]; Hu et al. [19]). With the help of the Community Radiative Transfer Model, GSI can assimilate both conventional and satellite radiance datasets. Detailed information can be found on the Developmental Testbed Center website (http://www.dtcenter.org/).
The GSI Hybrid scheme was used in this study. This scheme uses the background error covariance matrix, which is completely static or only slightly coupled to the dynamics of the forecast, and at the same time involves the fully flow-dependent background error covariance estimated from a set of ensembles of short-range forecasts with the WRF forecast model (Wang et al. [18]). The cost function for this hybrid data assimilation can be described as follows:
$$ J(\mathit{\boldsymbol{x}}) = \frac{1}{2}{\beta _1}{\left( {\mathit{\boldsymbol{x}} - {\mathit{\boldsymbol{x}}_b}} \right)^T}\mathit{\boldsymbol{B}}_f^{ - 1}\left( {\mathit{\boldsymbol{x}} - {\mathit{\boldsymbol{x}}_b}} \right) + \frac{1}{2}{\beta _2}{\left( {\mathit{\boldsymbol{x}} - {\mathit{\boldsymbol{x}}_b}} \right)^T}\mathit{\boldsymbol{B}}_{ens}^{ - 1}\left( {\mathit{\boldsymbol{x}} - {\mathit{\boldsymbol{x}}_b}} \right) + \frac{1}{2}{\left[ {{\mathit{\boldsymbol{y}}_o} - H(\mathit{\boldsymbol{x}})} \right]^T}{\mathit{\boldsymbol{R}}^{ - 1}}\left[ {{\mathit{\boldsymbol{y}}_o} - H(\mathit{\boldsymbol{x}})} \right], $$ (1) where x, xb and yo are vectors of the analysis, background fields and observations, respectively; Bf and Bens are the model static background error covariance and background error covariance estimated from a set of ensemble forecasts, respectively; R is the observational error covariance; H is the observation forward operator, which converts the model state to the observational state; and β1 and β2 are two factors whose inversions define the weights placed on the static covariance and the ensemble covariance, where these two factors satisfy the relation $\frac{1}{\beta_{1}}+\frac{1}{\beta_{2}}=1 $.
Two outer loops were used, and the maximum number of iteration steps for both loops was set to 50. Forty ensemble members were used in the Hybrid scheme, and a 20% weight was applied to the static covariance and an 80% weight to the ensemble covariance (Benjamin et al. [20]). The ensemble members were 6-hour WRF model forecasts of 40 initial conditions with random perturbations. The covariance localization scale (1000 km) was also applied to the ensemble covariance, to remove long-range spurious ensemble covariance through the removal of long-range spurious correlations and increase the effective ensemble size (Wang [21]).
The operationally available observations used in the GFS system, including conventional and satellite data, were used in the data assimilation system. The observations are constructed in BUFR format (binary universal form for the representation of meteorological data) and can be downloaded from the NCEP products website (http://www.nco.ncep.noaa.gov/pmb/products/gfs/). The conventional observations varied from in-situ observations covering both land and ocean, radiosondes, aircraft reports, to satellite retrievals, chemical compositions, etc. The satellite radiance/brightness temperature observations (level 1b) used in the data assimilation system included both infrared and microwave satellite instruments. The microwave instruments used here included: the AMSU-A (the Advanced Microwave Sounding Unit-A) onboard NOAA-15, NOAA-18, NOAA-19, MetOp-A, MetOp-B, and Aqua; the MHS (Microwave Humidity Sounder) onboard NOAA-18, NOAA-19, MetOp-A, and MetOp-B; the SSMI/S (Special Sensor Microwave Imager/Sounder) onboard the DMSP (Defense Meteorological Satellite Program)-f16, -f17, -f18, - f19 and - f20 satellites; and the ATMS (Advanced Technology Microwave Sounder) onboard the S-NPP (Suomi-NPOESS Preparatory Project) satellite. The infrared satellite instruments included: the HIRS/4 (High-resolution Infrared Radiation Sounder) onboard NOAA-19, MetOp-A, and MetOp-B (https://poes.gsfc.nasa.gov/hirs4.html); the AIRS (Atmospheric Infrared Sounder) launched in 2002 on Aqua (http://disc.sci.gsfc.nasa.gov/AIRS/documentation/airs_instrument_guide.shtml); the IASI (Infrared Atmospheric Sounding Interferometer) onboard MetOp-A and MetOp-B (https://wdc.dlr.de/sensors/iasi/); and the CrIS (Cross-track Infrared Sounder) launched along with the ATMS on S-NPP (https://jointmission.gsfc.nasa.gov/cris.html). A typical distribution of the conventional and satellite radiance observations at 1800 UTC 1 January 2015 is shown in Fig. 2.
Data used for the verification included the conventional data used in the data assimilation system and the 3-hourly accumulated precipitation product from the Global Land Data Assimilation System (GLDAS) with a horizontal resolution of 0.125°. GLDAS is a global, high-resolution terrestrial modeling system that uses both ground and satellite-based observations to optimize the products at land surface states (Rodell et al. [22]; Gottschalck et al. [23]).
-
Three sets of WRF and data assimilation (hereafter referred to as Hybrid) experiments with different model tops and vertical resolutions were conducted during January and February in 2015. Each run of the WRF experiment made a 72-hour forecast, and the operationally available observations, including conventional and satellite data, were assimilated every 6 hours; thus, over 100 samples for each experiment. The model top was raised from 50 mb to 10 mb, and then to 1 mb to include more stratospheric information, step-by-step. Detailed information on the vertical resolution and domain configuration of all experiments is listed in Table 1. In the first set of experiments including both WRF and data assimilation runs, there were 30 atmospheric vertical levels, among which 10 were located in the stratosphere. To evaluate the sensitivity of stratospheric initial conditions and the assimilation of stratospheric observations, 51 and 63 levels were selected in the second and third sets of experiments, in which 20 and 40 levels were located in the stratosphere, respectively.
Central Point (37°N, 90°W) Projection Lat-Lon Domain Layer Resolution (°) Grid (Lon × Lat) 1 0.25 240 × 128 Experiment set 1
(WRF-50, Hybrid-50)
Vertical Layers
(Eta levels with model top at 50 mb)30 levels
1, 0.993, 0.983, 0.97, 0.954, 0.934, 0.909, 0.88, 0.8317505, 0.7835011, 0.7352517, 0.6870022,
0.6035514, 0.5279136, 0.4594781, 0.397675, 0.3419721, 0.2918729, 0.2469149, 0.2066672,
0.1707291, 0.1387277, 0.1103166, 0.08602321, 0.06535161, 0.04776186, 0.03279452,
0.02005862, 0.009221466, 0Experiment set 2
(WRF-10, Hybrid-10)
Vertical Layers
(Eta levels with model top at 10 mb)51 levels
1.000, 0.994, 0.986, 0.978, 0.968, 0.957, 0.945, 0.931, 0.915, 0.897, 0.876, 0.854, 0.829, 0.802,
0.772, 0.740, 0.705, 0.668, 0.629, 0.588, 0.550, 0.513, 0.478, 0.445, 0.413, 0.383, 0.355, 0.328,
0.303, 0.279, 0.256, 0.234, 0.214, 0.195, 0.177, 0.160, 0.144, 0.128, 0.114, 0.101, 0.088, 0.076,
0.065, 0.055, 0.045, 0.036, 0.028, 0.020, 0.012, 0.0056, 0.000Experiment set 3
(WRF-1, Hybrid-1)
Vertical Layers
(Eta levels with model top at 1 mb)63 levels
1, 0.993, 0.983, 0.97, 0.954, 0.934, 0.909, 0.88, 0.8413662, 0.8027326, 0.7640989, 0.7254651,
0.6569721, 0.5938299, 0.5356899, 0.4822229, 0.4331176, 0.3880801, 0.3468334, 0.309116,
0.2746814, 0.2432974, 0.2147456, 0.18882, 0.1653272, 0.1443878, 0.1260844, 0.1100854,
0.09610046, 0.08387615, 0.07319078, 0.06385061, 0.0556863, 0.04854981, 0.04231175,
0.03685901, 0.03209274, 0.02792649, 0.02428475, 0.02110147, 0.01831895, 0.01588672,
0.01376069, 0.01190231, 0.01027789, 0.008857966, 0.007616803, 0.006531891, 0.005583562,
0.004754621, 0.004030036, 0.003396671, 0.002843042, 0.002359111, 0.001936102,
0.001566348, 0.001243142, 0.0009606255, 0.0007136756, 0.0004978148, 0.0003091293,
0.0001441978, 0Table 1. Vertical resolutions for all experiments.
The performance from raising the model top and assimilating extra stratospheric observations was evaluated through comparison with conventional observations. First, statistical results of wind speed and temperature in the initial conditions and the predictions were produced using the averaged bias and root-mean-square deviation (RMSD) calculated against the conventional observations during the study period. The differences in initial temperature RMSDs indicated the differences in performance skill when the model top was raised or data assimilation was applied. The differences in predicted temperature RMSD profiles indicated the differences in forecast skill (Wang et al.[18]). Also, a snowstorm that occurred during 2 January to 4 January 2015 was used as a case study to demonstrate the importance of the inclusion of the entire stratosphere with data assimilation in severe weather predictions.