1.Institute of Urban Meteorology (IUM), China Meteorological Administration (CMA), Beijing 100089, China 2.State Key Laboratory of Numerical Modeling for Atmospheric Sciences and Geophysical Fluid Dynamics, Institute of Atmospheric Physics, Chinese Academy of Sciences, Beijing 100029, China Manuscript received: 2020-09-14 Manuscript revised: 2021-01-11 Manuscript accepted: 2021-02-19 Abstract:The partial cycle (PC) strategy has been used in many rapid refresh cycle systems (RRC) for regional short-range weather forecasting. Since the strategy periodically reinitializes the regional model (RM) from the global model (GM) forecasts to correct the large-scale drift, it has replaced the traditional full cycle (FC) strategy in many RRC systems. However, the extra spin-up in the PC strategy increases the computer burden on RRC and generates discontinuous small-scale systems among cycles. This study returns to the FC strategy but with initial fields generated by dynamic blending (DB) and data assimilation (DA). The DB ingests the time-varied large-scale information from the GM to the RM to generate less-biased background fields. Then the DA is performed. We applied the new FC strategy in a series of 7-day batch forecasts with the 3-hour cycle in July 2018, and February, April, and October 2019 over China using a Weather Research and Forecast (WRF) model-based RRC. A comparison shows that the new FC strategy results in less model bias than the PC strategy in most state variables and improves the forecast skills for moderate and light precipitation. The new FC strategy also allows the model to reach a balanced state earlier and gives favorable forecast continuity between adjacent cycles. Hence, this new FC strategy has potential to be applied in RRC forecast systems to replace the currently used PC strategy. Keywords: rapid refresh, weather forecast, full cycle, blending 摘要:当前的短期区域数值天气预报快速更新系统广泛使用了部分循环策略,而不是不间断的全循环策略。这是因为部分循环会周期性地从全球模式预报中重新初始化区域模式来修正大尺度漂移。然而,部分循环策略会增加额外的计算负担,并在相邻循环的预报结果之间制造小尺度系统的不连续性。本研究采用的快速更新系统将回归到全循环策略上来,但采用新发展的动态混合方法结合资料同化生成初始场。系统使用动态混合从全球模式预报中提取随时间变化的大尺度信息,并实时引入到区域模式中以产生较小误差的背景场。然后执行数据同化。在2018年7月和2019年2月、4月和10月期间,我们使用该方案对中国区域进行了3小时更新一次的7天批量预报。结果表明,在大多数状态变量上,新的全循环策略不但节省了计算资源,且比部分循环显示出更小的初始和预报偏差,更好的中、小量级降水的预测能力。该策略下模式初始化之后平衡速度较快,且相邻循环的预报之间连续性更好。因此,这种新的全循环策略有望应用于快速更新数值天气预报系统中,以取代当前大规模使用的部分循环策略。 关键词:快速更新, 天气预报, 全循环, 混合
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2.1. Model
RMAPS-ST is the RRC system that has operated at the Beijing Meteorological Service (BMS) since 2015. It uses the Weather Research and Forecast model (WRF version-3.8.1) and produces forecasts over a limited domain spanning China and adjacent areas (see Fig. 1). The horizontal resolution is 9 km, with 649 and 500 grid points in the x- and y-directions, respectively. There are 51 vertical terrain-following levels from the surface to the top level at 50 hPa. The time integration step is 45 s. The model physics schemes include the Thompson bulk microphysics scheme, the Rapid Radiative Transfer Model for Global Climate Models (RRTMG) for longwave and shortwave radiation, the Noah land surface model, the Monin–Obukhov surface layer scheme, the Yonsei University (YSU) planetary boundary layer scheme, and the New Tiedtke cumulus parameterization. In addition, RMAPS-ST employs 33 fine land-use categories based on United States Geological Survey (USGS) data (Xie et al., 2019; Zhong et al., 2020). More details on the WRF model and these scheme settings may be found in the WRF version 3 technical document (Skamarock et al., 2008). Figure1. Experimental domain and two typical examples of assimilated observations on (a) 1200 UTC July 11, 2018 and (b) 1800 UTC July 11, 2018.
The GM forecast data released by the European Centre for Medium-Range Weather Forecasts (ECMWF) (https://www.ecmwf.int/en/forecasts/datasets/catalogue-ecmwf-real-time-products) with a grid resolution of 0.25° × 0.25° provided the LBCs and ICs for the WRF spin-up in the RMAPS-ST system. The ECMWF forecasts provide the LBCs for the regional model, the re-initialization field for the partial cycle and the blended GM field for DB (see section 2.3). RMAPS-ST can receive rolling updated ECMWF forecast data every 12 hours (at 0000 and 1200 UTC), with 3-h forecast output, ranging up to 240 hours. RMAPS-ST uses the ECMWF forecasts starting from the previous 0000 or 1200 UTC due to reception latency of ECMWF data.
2 2.2. Data assimilation -->
2.2. Data assimilation
RMAPS-ST employs the 3DVAR algorithms from the WRF data assimilation (WRFDA, version-3.8.1) system (Barker et al., 2012). Following Sun and Wang (2013), five control variables are used for DA to reflect the convective systems development in the initial field: velocity components in the x- and y-directions, temperature, pseudo-relative humidity, and surface pressure. RMAPS-ST uses the National Meteorological Center (NMC) (Parrish and Derber, 1992) method to generate the background error covariance based on one-month forecasts in different seasons. RMAPS-ST assimilates various kinds of observations, including the upper-air wind, temperature, and specific humidity from radiosondes, aircraft reports and wind profilers. Surface wind, temperature, pressure, and specific humidity are obtained from land-based synoptic reports (SYNOP), aviation routine weather reports (METAR), and ship and buoy reports over the sea. Additionally, to improve the temporal and spatial distribution of the initial humidity in air columns, Global Positioning System Zenith Total Delay (GPSZTD) observations from over 500 sites in China are assimilated following quality control (Zhong et al., 2017). Note that not all of these assimilated observations are obtained regularly at every analysis time. For example, there are many more radiosonde observations at the conventional sounding time, i.e., 0000 and 1200 UTC, than at other times. There are also more aircraft reports during the daytime than at nighttime. Two typical distributions of the observations available for assimilation over China at 1200 UTC and 1800 UTC July 11, 2018, are shown in Fig. 1. The assimilation time-window for all observed data is ±1 h at each analysis time.
2 2.3. Dynamic blending -->
2.3. Dynamic blending
In the new FC strategy, DB blends the forecasts from ECMWF and WRF to form the first guess for DA. We use the blended field as the first guess for DA to provide a better background for DA than the WRF forecast itself from the previous cycle (?irokà et al. 2001; Gustafsson et al., 2018). Blending uses a Raymond sixth-order tangent low-pass filter to isolate the large-scale waveband from a limited area field x (labeled by $ F\left(x,{k}_{\rm{c}}\right) $); i.e., all perturbations with wavenumber smaller than the cutoff wavenumber, $ {k}_{\rm{c}} $ are retained. The remainder, $ x-F\left(x,{k}_{\rm{c}}\right) $, is the small-scale spectrum of x. $ F\left(x,{k}_{\rm{c}}\right) $ can be presented as the sum of the spectral components of x weighted by the response function of the Raymond filter $ f\left(k;{k}_{\rm{c}}\right) $, which is given by where $ N $ is the dimension size of $ x $ and k is the wavenumber of a specific component of x. Blending applies Eq. (1) to both WRF and ECMWF fields and combines the small-scale waveband from a WRF forecast field $ {x}_{\rm{r}} $ with the large-scale waveband from the corresponding ECMWF forecast field $ {x}_{\rm{g}} $, as follows: where $ {x}_{\rm{b}} $ is the blended field. $ F({x}_{\rm{g}},{k}_{\rm{c}}) $ and ${x}_{{\rm r}}-F\left({x}_{{\rm r}},{k}_{\rm{c}}\right)$ are the large-scale spectrum of ECMWF and small-scale spectrum of the WRF forecast, respectively. According to Eqs. (1) and (2), for perturbations with larger (smaller) scales than wavenumber $ {k}_{\rm{c}} $, $ {x}_{\rm{b}} $ gradually approaches the ECMWF (WRF) field (see Fig. 2 of Feng et al. 2020). Since $ {k}_{\rm{c}} $ determines the part of the spectrum that will be introduced into the RM, it is a key parameter in the blending process. Most previous studies commonly used an arbitrary fixed cutoff wavenumber $ {k}_{\rm{c}} $ (Yang, 2005a, b; Wang et al., 2014; Hsiao et al., 2015). However, DB computes the $ {k}_{\rm{c}} $ according to the real-time error distribution in the GM forecasts and the spectral characteristics of the RM forecasts, using the kinetic energy distribution as the criterion to find an acceptable GM waveband that should be blended with the RM (Feng et al., 2020). The blending is then conducted with the selected cutoff wavenumber. Two steps are implemented to determine the cutoff wavenumber in DB. The first is to select a large-scale waveband filtered by Eq. (1) from the ECMWF GM data. The waveband should be accurate enough as a candidate for blending. DB selects the GM large-scale waveband that has an acceptable bias tolerance at every level. The GM forecast biases are estimated (as a percentage) against the corresponding analysis by comparing their velocity difference in the form of kinetic energy $ D({k}_{\rm{g}}) $. With the propagation of error through all scales, the error in the longwave band $ D({k}_{\rm{g}}) $ will increase with $ {k}_{\rm{g}} $ (Durran and Gingrich, 2014; Durran and Weyn, 2016; Feng et al., 2020). The critical wavenumber $ {k}_{\rm{g}} $, which represents the upper bound of the GM wavenumber for blending, can be determined by a bias tolerance $ {\epsilon}_{\rm{g}} $ using the equation: Since the ECMWF analysis cannot be obtained in real-time, the $ {k}_{\rm{g}} $ is calculated using monthly historical ECMWF forecasts and analyses with $ {\epsilon}_{\rm{g}} $ taken as 5%. Because the model dissipation causes significant underestimation of kinetic energy in scales smaller than the scale corresponding to the effective resolution (Skamarock, 2004), only the scales larger than the effective resolution of ECMWF data are considered in blending. The effective resolution of ECMWF data in the experimental domain of RMAPS-ST is approximately 6 grid lengths of the original horizontal resolution of ECMWF data [see Fig. S1 in the Electronic Supplementary Material (ESM)], as derived from the model kinetic energy spectra (Skamarock, 2004; Warner, 2011). The second step of DB aims to maintain the growth of small-scale systems in the initial fields at every level, because introducing too many GM waves would dampen the growth of small-scale modes in the RM fields (an extreme case is the “cold restart” run, in which the small-scale modes are regenerated from scratch). DB calculates the residual small-scale waveband kinetic energy difference (labeled $ R\left({k}_{\rm{r}}\right) $) between the ECMWF forecast and WRF forecast and keeps $ R\left({k}_{\rm{r}}\right) $ at a prescribed level ${\epsilon}_{{\rm r}}$; i.e., The small-scale waveband is also obtained using the Raymond filter as Eq. (1) shows. This study determines $ {k}_{\rm{r}} $ with $ {\epsilon}_{\rm{r}} $ taken as 7%. The cutoff wavenumber $ {k}_{\rm{c}} $ is determined by choosing the smaller of the wavenumbers $ {k}_{\rm{g}} $ and $ {k}_{\rm{r}} $ from Eqs. (3) and (4), respectively. Finally, to avoid the dynamic imbalance of the WRF caused by using vertically inhomogeneous cutoff wavenumbers, the vertically averaged $ {k}_{\rm{c}} $ is used in RMAPS-ST. The cutoff wavenumbers in DB show the flow-dependent characteristic especially for diurnal oscillation (see Fig. S2). More details on the DB scheme can be found in Feng et al. (2020).
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3.1. Experimental design
Three batch experiments are performed for July 2018 (referred to as July cases) to compare the new FC strategy with both DA and DB (FC_DBDA), PC strategy with DA (PC_DA) and FC strategy with DA (FC_DA). The July cases cover seven-day 3-hour cycling runs for the period from 0000 UTC 11 July, 2018 to 2100 UTC 17 July, 2018 with a total of 56 forecast cycles. All experiments conduct a 6-hour WRF initialization to generate the initial fields in the first cycle and perform DA and a 24-hour WRF forecast in every cycle. FC_DA directly uses the 3-hour WRF forecast from the previous cycle as the first guess for DA (Fig. 2a). Experiment PC_DA is the same as FC_DA but reinitializes the forecast system from the ECMWF forecast once a day at 0000 UTC with a 6-hour spin-up process starting from the previous 1800 UTC (Fig. 2b, using the 1200 UTC+6 h EC forecast as the initial fields). FC_DBDA uses the blended fields of WRF and ECMWF forecasts as the first guess for DA at each cycle (Fig. 2c). In addition, since PC_DA does not assimilate observation during the spin-up process at 0000 UTC, we performed an additional experiment (FC_DBDA2, only performed for July cases) that is configured following FC_DBDA but generates the initial fields at 0000 UTC without DA at 1800 and 2100 UTC. The FC_DBDA shows similar performance to the FC_DBDA (Fig. S12?S16). Hence, we mainly compare the results of FC_DA, PC_DA and FC_DBDA. Figure2. Schematic of experiment FC_DA (a), PC_DA (b) and FC_DBDA (c) with a 3-hourly forecast cycle configuration. The WRF fields are the 3-hour forecasts from the previous cycle. The ECMWF fields are the forecasts at the same time starting from the previous 0000/1200 UTC.
FC_DBDA re-calculated the cutoff wavenumber $ {k}_{\rm{c}} $ at each cycle except at 0000 and 1200 UTC (referred to as 0000/1200 UTC). For the cycles starting from 0000/1200 UTC, we use the cutoff wavenumber determined in the previous cycle, since the re-initiated ECMWF forecasts would cause miscalculation of $ {k}_{\rm{c}} $ at these times. The altered GM initial fields would cause an overestimation of the residual small-scale kinetic energy difference. The blending processes are applied to the variables of velocity components in the x- and y-directions (u and v), vertical velocity (w), perturbation geopotential height (h), perturbation potential temperature ($ \theta $), water vapor mixing ratio ($ {q}_{v} $), and perturbation pressure ($ p $) at all model levels. To verify the effectiveness of the new FC strategy in other seasons, we also perform the PC_DA and FC_DBDA experiments for three other seven-day periods: from 0000 UTC 11 Feb to 2100 UTC 17 Feb 2019 (referred to as February cases), from 0000 UTC 11 Apr to 2100 UTC 17 Apr 2019 (referred to as April cases), and from 0000 UTC 11 Oct to 2100 UTC 17 Oct 2019 (referred to as October cases). In these periods, we use the same parameter settings and cycle strategy as in the July cases. The experiments in these three seasons aim to investigate the applicability of the FC_DBDA strategy in RMAPS-ST. FC_DA is not included in these three periods because (1) the PC_DA strategy is the operational cycle strategy in the current version of RMAPS-ST, (2) the FC_DA cycle strategy has shown poorer performance than PC_DA in previous studies (Benjamin et al., 2016) and in July cases (see section 5), and (3) computer resources are limited for this study.
2 3.2. Verification metrics -->
3.2. Verification metrics
We verify the performance of various forecast state variables, including u, v, $ \theta $, h, $ {q}_{v} $ and $ p $, using Root Mean Square Error (RMSE) and bias against the real observational data (see section 2.2) and GFS final reanalysis data (refer to as the GFS). The spatial 5-point smoothing operator is applied to verification variables to avoid the problems due to resolution difference between GFS (~30 km) and RMAPS-ST (9 km). We use GFS because it is a useful supplement for conventional observations, especially at these times with few radiosonde data such as 0600 and 1800 UTC. Quantitative precipitation forecasts are evaluated against observations from a national rain gauge network with more than 2600 sites over China (Fig. S3). We use two statistical indices to verify the precipitation forecasts - the Critical Success Index (CSI) and the Frequency BIAS (FBIAS) score. The rainfall events related to CSI and FBIAS are defined as precipitation amounts greater than or equal to a prescribed threshold such as 0.1, 1, 10, 25, and 50 mm. The spin-up speed of the model is represented by the mean surface pressure tendency (MSPT, see Eq. (7) of Benjamin et al., 2004a) over the experimental domain, following many previous studies (Benjamin et al., 2004a; Wang et al., 2014; Vendrasco et al., 2016; Feng et al., 2020). A favorable RRC system should have low and smooth MSPT in the first few integrating hours to maintain model balance.
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4.1. Verification of state variables
We first compare the multi-cycle averaged RMSE against upper-air observations for air temperature, specific humidity, u, and v. Figure 3 is the vertical profile of the RMSEs of initial fields ($ t=0\;{\rm{h}} $) from 900 to 100 hPa for the three experiments. The FC_DBDA has the smallest initial bias among the three experiments at almost all levels for wind and humidity fields. As for temperature, FC_DBDA has less RMSEs than FC_DA at 100?400 hPa and almost equal error at levels below 500 hPa. Compared with the PC_DA strategy used by the current version of RMASP-ST, the FC_DBDA strategy reduces the initial RMSE for air temperature and wind fields at most levels. For specific humidity, FC_DBDA has the smallest RMSEs at levels below 500 hPa. The forecast fields from FC_DBDA at t = 6 h and t = 24 h (Figs. S4 and S5) also show the smallest RMSEs of the three experiments for specific humidity, u, and v, indicating the initial bias reduction of FC_DBDA propagates to forecasts for at least several hours. Since the initial field of an RRC strongly depends on the forecast from the last cycle, this improvement in forecasts should be attributed to the cumulative effects of DB and DA in every cycle. In addition, we show the initial and forecast RMSEs of the near-surface diagnostic variables, including air temperature at 2 m, surface pressure, specific humidity at 2 m, and wind speed at 10 m (Fig. 4). The FC_DBDA has smaller RMSEs for temperature at 2 m and surface pressure than the other two strategies but has larger RMSEs for specific humidity at 2 m and wind speed at 10 m than PC_DA. It should be noted that we do not blend these diagnostic near-surface variables since they have little effect on model integration. These performance errors in near-surface variables are just the response of blended upper-air variables. Figure3. Multicycle-averaged vertical profiles of initial RMSE (t = 0 h) over the experimental domain in July cases against real observations for (a) air temperature (units: K), (b) specific humidity (units: 10–1 g kg–1), (c) velocity component in x-direction u (units: m s–1), and (d) velocity component in y-direction v (units: m s–1). The blue, black, and red curves denote the RMSEs of FC_DA, PC_DA, and FC_DBDA, respectively.
Figure4. Multicycle-averaged RMSE for 0–24 h forecasts over the experimental domain in July cases against real observations for (a) air temperature at 2 m (units: K), (b) surface pressure (units: hPa), (c) specific humidity at 2 m (units: g kg–1), and (d) wind speed at 10 m (units: m s–1). The blue, black, and red curves denote the RMSEs of FC_DA, PC_DA, and FC_DBDA, respectively.
We also verify the initial fields and 6 h and 24 h forecasts for the state variables using GFS final reanalysis data (Fig. S6–S8). Like the verification results against real observations, FC_DBDA shows the smallest initial and forecast RMSEs at almost all levels among the three experiments. The FC_DBDA mainly improves the temperature and wind at most levels and the humidity fields at mid-levels. To examine the effects of different cycle strategies on WRF initial fields in detail, we also investigate the spatial patterns of initial bias for geopotential height at the 18th model level (~500 hPa) and specific humidity at the 12th model level (~700 hPa) (Fig. 5) over the experimental domain. The FC_DA shows the strong positive initial bias in geopotential height over central and eastern China and the negative bias over the south Tibetan Plateau and South Asia. The distribution of bias indicates an underestimation of the East Asian Trough (EAT) intensity, which is often located over eastern China and the western Pacific (e.g., Wang et al., 2009). Also, there is an overestimation of specific humidity over a belt from the Indochina Peninsula to northeast China, which is the main Moisture Transport Pathway (MTP) for summer precipitation in China (e.g., Zhao et al., 2016). Over the subtropical high region, i.e., the western Pacific, FC_DA underestimates the humidity. These results indicate that an RRC cannot rectify the large-scale errors only using DA. By contrast, PC_DA can rectify such bias to some degree due to the periodic restarting process from ECMWF forecasts, but the FC_DBDA improves the initial fields with better performance: most of the positive RMSEs of geopotential height over eastern China and specific humidity over the MTP are corrected. Consequently, the different effects of initial bias correction of the three strategies propagate to the forecast and generate similar bias patterns of state variables (Figs. S9 and S10), which would cause different performances in precipitation forecasts. Figure5. Geographical distribution of multicycle-averaged initial field (contour lines) and initial bias (shaded) of geopotential height (units: m) (a, b, and c) at the 18th model level (~500 hPa) and of specific humidity (units: g kg–1) (d, e and f) at the 12th model level (~700 hPa) in July cases against GFS final reanalysis data for (a) and (d) FC_DA, (b) and (e) PC_DA, and (c) and (f) FC_DBDA respectively. All fields are preprocessed using 5-points smoothing to avoid the impact of horizontal resolution difference between WRF and GFS final reanalysis data.
2 4.2. Verification of precipitation forecasts -->
4.2. Verification of precipitation forecasts
We use multi-cycle averaged CSI and FBIAS scores of 3-hour accumulated precipitation with the precipitation amount thresholds of 0.1, 1, 5, 10, 25, and 50 mm to evaluate the forecast skill of the three experiments (Fig. 6). For events with the 3-hour accumulated precipitation less than 0.1, 1, and 5 mm, the FC_DBDA has higher CSI and less FBIAS than the other two strategies. For the uncommon heavy rain events with 3-hour accumulated precipitation larger than 10, 25, and 50 mm, FC_DBDA has the highest CSI score in more than half the forecasts. Without large-scale constraints, modeled small-scale systems would develop much easier in FC_DA. As a result, FC_DA has better FBIAS scores for heavy rain events but worse CSI scores than the other two experiments. In contrast, FC_DBDA tends to depress the development of heavy precipitation events, which provide smoother control variables than FC_DA. To summarize, the FC_DBDA strategy has better precipitation forecast skills than FC_DA and PC_DA, especially for light to moderate precipitation events. Figure6. Multicycle-averaged CSI (a–f) and FBIAS (g–l) scores of 3-h accumulated precipitation over the experimental domain in July cases for precipitation amount greater than or equal to 0.1, 1, 10, 25, and 50 mm. The blue, black, and red bars denote the scores of FC_DA, PC_DA, and FC_DBDA, respectively.
Figure 7 shows forecasts of time-averaged 24-hour accumulated precipitation, obtained by summing precipitation forecasts for the 5th–7th hour from all cycles. We compare the precipitation forecasts with the rain gauge data, which is interpolated to model grid cells using nearest neighbor interpolation. We only use the site observations within 9 km of every grid cell (i.e., length of 1 grid cell) to minimize the interpolation error. The FC_DBDA strategy results in precipitation patterns in closest agreement with the rain gauge observations. PC_DA experiments performed slightly better than FC_DA in the North China Plain (NCP) and South China (SC). Comparing with FC_DA and PC_DA, the FC_DBDA mitigates the over-predicted precipitation over the long rainfall belt from Northeast to Southwest China and the light rain areas in SC. In particular, FC_DBDA predicts the three small rainfall belts located in the NCP, which are not correctly reproduced by FC_DA and PC_DA experiments. Besides, FC_DBDA also favorably predicts the heavy rainfall over Hainan Island. These improvements in the FC_DBDA experiments are possibly related to the forecast reduction in humidity bias (Fig. 5 and Fig. S10). FC_DA and PC_DA overestimate the low-level humidity on the MTP from Northeast to Southwest China and trigger more spurious precipitation in these regions. In contrast, the accuracy of the humidity fields in FC_DBDA favors a better precipitation pattern. Figure7. Time-averaged accumulated 24-hour precipitation forecasts in July cases for observations from (a) rain gauges and (b–d) forecasts from (b) FC_DA, (c) PC_DA, (d) FC_DBDA experiments. The accumulated precipitation in these experiments is calculated from the sum of the 5th–7th hour precipitation forecasts in every cycle.
2 4.3. Model balance issues -->
4.3. Model balance issues
We use the multicycle-averaged MSPT in the first six forecast hours to show the degree of model balance for FC_DA, FC_DBDA, and the spin-up process of PC_DA (Fig. 8). The results of cycles that start from non-0000/1200 UTC and those that start from 0000/1200 UTC cycles are presented separately because the ECMWF forecast used in RMAPS-ST restarts at 00/12 UTC (see section 2.1). Since the ECMWF forecast provides the LBCs and blended fields, such a change will slow down the model spin-up speed at 0000/1200 UTC relative to non-0000/1200 UTC (Fig. 8a). Figure8. Multicycle-averaged MSPT during the first 6 forecast hours for the July cases. The black, red, and yellow lines denote the results of the FC_DA, the spin-up process of PC_DA, and the FC_DBDA, respectively. The solid (dashed) lines denote the results of cycles that start from non-0000/1200 UTC (0000/1200 UTC) cycles for the two continuous cycle strategies.
The FC_DBDA strategy reaches model balance much faster than the spin-up process from the ECMWF forecasts used by PC_DA, since the FC_DBDA strategy includes the small-scale information from the WRF forecast in the previous cycle. The PC_DA strategy requires almost 2 hours of spin-up to achieve balance (Fig. 8b). Moreover, due to the DA adjustment, MSPT in FC_DA and FC_DBDA fluctuate sharply at the beginning of initialization but quickly become smooth after 20 minutes. Considering that the FC_DA only adjusts the initial fields using DA and the FC_DBDA strategy directly blends the longwave band of ECMWF forecasts into WRF without a cold-start process, FC_DBDA does add some noise to the initialization fields and has a slightly larger MSPT at the initial time than FC_DA. However, the MSPT curves of FC_DBDA are smooth, suggesting that the model balance is less affected by the FC_DBDA strategy and can be quickly re-adjusted within a short period. In addition to the MSPT, we found that the RMSE of surface pressure in FC_DBDA at the initial time and the first 3 hours is stable and smaller than in the other two experiments (Fig. 4b). The results also suggest that the model balance of the FC_DBDA strategy is acceptable in the RRC system.
2 4.4. Forecast continuity issue -->
4.4. Forecast continuity issue
To provide stable predictions for operational weather centers, the forecast precipitation pattern for a specific time should change little between two adjacent cycles. Here we explore the difference between the 3 h precipitation from the current cycle and the 6 h precipitation from the previous cycle in the three experiments (Fig. 9). The precipitation differences between adjacent cycles in FC_DBDA are smaller than in the FC_DA and PC_DA experiments in North China, Northeastern China and Central China. Considering that the RMAPS-ST focuses on the precipitation forecast in China, the results are acceptable. For precipitation over parts of southwest China and most marine areas, PC_DA and FC_DA are slightly better than FC_DBDA, which suggested that the dynamic blending process has few adverse effects on the forecast continuity of the precipitation pattern in other areas of the experimental domain. Figure9. Multicycle-averaged precipitation differences between the 3-h precipitation (mm) from the current cycle and the 6-h precipitation from the previous cycle in (b) FC_DA, (c) PC_DA, (d) FC_DBDA experiments.