the Creative Commons Attribution 4.0 License.
the Creative Commons Attribution 4.0 License.
Assessment of WRF (v 4.2.1) dynamically downscaled precipitation on subdaily and daily timescales over CONUS
Abhishekh Kumar Srivastava
Paul Aaron Ullrich
Deeksha Rastogi
Pouya Vahmani
Andrew Jones
Richard Grotjahn
This study analyzes the quality of simulated historical precipitation across the contiguous United States (CONUS) in a 12 km Weather Research and Forecasting model version 4.2.1 (WRF v 4.2.1)-based dynamical downscaling of the fifth-generation ECMWF atmospheric reanalysis (ERA5). This work addresses the following questions. First, how well are the 3 and 24 h precipitation characteristics (diurnal and annual cycles, precipitation frequency, annual and seasonal mean and maximum precipitation, and distribution of seasonal maximum precipitation) represented in the downscaled simulation, compared to ERA5? And second, how does the performance of the simulated WRF precipitation vary across seasons, regions, and timescales? Performance is measured against the National Centers for Environmental Prediction/Environmental Modeling Center (NCEP/EMC) 4 km Stage IV and Oregon State University Parameter-Elevation Regressions on Independent Slopes Model (PRISM) data on 3 and 24 h timescales, respectively. Our analysis suggests that the 12 km WRF exhibits biases typically found in other WRF simulations, including those at convection-permitting scales. In particular, WRF simulates both the timing and magnitude of the summer diurnal precipitation peak as well as ERA5 over most of the CONUS, except for a delayed diurnal peak over the Great Plains. As compared to ERA5, both the month and the magnitude of the precipitation peak annual cycle are remarkably improved in the downscaled WRF simulation. WRF slightly overestimates 3 and 24 h precipitation maximum over the CONUS, in contrast to ERA5, which generally underestimates these quantities mainly over the eastern half of the CONUS. Notably, WRF better captures the probability density distribution (PDF) of 3 and 24 h annual and seasonal maximum precipitation. WRF exhibits seasonally dependent precipitation biases across the CONUS, while ERA5's biases are relatively consistent year round over most of the CONUS. These results suggest that dynamical downscaling to a higher resolution improves upon some precipitation metrics but is susceptible to common regional climate model biases. Consequently, if used as input data for domain-specific models, we suggest moderate bias correction be applied to the dynamically downscaled product.
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Deeksha Rastogi is an employee of UT-Battelle, LLC, under contract DEAC05-00OR22725 with the US Department of Energy (DOE). Accordingly, the publisher, by accepting the article for publication, acknowledges that the US government retains a nonexclusive, paid-up, irrevocable, worldwide license to publish or reproduce the published form of this manuscript, or allow others to do so, for US government purposes. DOE will provide public access to these results of federally sponsored research in accordance with the DOE Public Access Plan (https://www.energy.gov/downloads/doe-public-access-plan, last access: 2 July 2023)
Dynamical downscaling refers to the use of regional climate models forced with initial and lateral boundary conditions derived from either a global climate model or reanalysis to generate high-resolution climate output (Giorgi and Mearns, 1991). These high-resolution simulations add value through better representation of regional weather and climate phenomena, especially over regions of complex and heterogeneous topography (Doblas-Reyes et al., 2021). For example, better representation of local topography, water bodies and land–sea contrast improves local-scale processes such as fine-scale convection, land–sea breeze, and nonlinear interactions between local, mesoscale, and large-scale processes (Caldwell et al., 2009; Di Luca et al., 2015; Ashfaq et al., 2016; Prein et al., 2016; Bozkurt et al., 2019; Rastogi et al., 2022). Both the higher resolution and improved representation of physical processes facilitate the study of future changes in the mean and variability of the weather and climate systems (Barsugli et al., 2013) and distill user-oriented regional climate information on local and regional scales (Rhoades et al., 2020; Doblas-Reyes et al., 2021; Ranasinghe et al., 2021).
Though increased resolution in downscaled climate models is fundamentally important for their utility at regional scales, it is not sufficient for ensuring reliable and accurate information. The biases in regional climate model output are well documented. These biases can originate from various sources, including the lateral boundary conditions (Christensen et al., 2008; Schoetter et al., 2012; Giorgi, 2019) and parameterization schemes (Iguchi et al., 2017; Kong et al., 2022). The biases may also vary with variable, region, and season of interest (Castro et al., 2005; Prein et al., 2015; Diaconescu et al., 2016; Srivastava et al., 2020, 2021, 2022). High-resolution and high-quality climate data have many uses for both advancing process understanding and for informing operations, particularly at local to regional scales. The ECMWF atmospheric reanalysis (ERA5; Hersbach et al., 2020) represents a great stride forward in the development of a complete historical meteorological dataset with sufficiently high temporal and spatial resolution to represent many forms of extreme weather and their impacts. However, for investigating water resource availability, mountain snowpack, and land–atmosphere fluxes, particularly in the context of multi-sectoral dynamics, even finer grid spacing is required. Given the broad interest among scientists and stakeholders in developing regional climate data products at ∘ grid spacing based on high-quality reanalysis, it is important to investigate to what degree (if any) the dynamically downscaled data improve upon the original ERA5 product. Such a study is further valuable for informing other dynamical downscaling efforts, such as the international Coordinated Regional Downscaling Experiment (CORDEX) program (Gutowski et al., 2016).
In this study, we evaluate historical precipitation over the contiguous United States (CONUS) in a 12 km Weather Research and Forecasting model version 4.2.1 (WRF v 4.2.1)-based dynamical downscaling of ERA5 over the period 1980–2020. This WRF-based historical simulation is part of an ensemble data product (Jones et al., 2022) that includes thermodynamic global warming (TGW) simulations under projected climate forcings (Jones et al., 2023). In this paper, we specifically ask the following two questions: (1) how well are the 3 and 24 h precipitation characteristics (diurnal and annual cycles, precipitation frequency, annual and seasonal mean and maximum precipitation, and distribution of seasonal maximum precipitation) represented in the downscaled WRF simulation, in comparison to ERA5? (2) How does the performance of the simulated WRF precipitation vary across seasons, regions, and timescales? The performance of 3 h ERA5 and WRF precipitation simulations are measured against the NCEP/EMC 4 km gridded Stage IV data (Stage IV). The performance of 24 h ERA5 and WRF precipitation simulations are measured against the Oregon State University Parameter-Elevation Regressions on Independent Slopes Model (PRISM) dataset.
The specific questions above are motivated by several important considerations. Most previous studies have focused on the accuracy of the simulated precipitation on daily or longer timescales (e.g., Bukovsky and Karoly, 2009; Caldwell et al., 2009; Rhoades et al., 2020; Srivastava et al., 2021, 2022; Gensini et al., 2023), likely because of availability of data on daily timescales. However, many of the high-impact precipitation-related physical processes (such as short-duration convective storms leading to extreme precipitation events or precipitation intermittency) occur at hourly timescales (Westra et al., 2013; Trenberth et al., 2017), and conclusions drawn from analyzing longer-timescale precipitation do not automatically translate to shorter timescales (Barbero et al., 2019). Further, regional climate models are known to be sensitive to both the resolved (e.g., horizontal resolution and simulation domain) and unresolved parameters (e.g., convection parameterization schemes), and so particular regional climate model configurations must be examined before they can be used for regional application (Giorgi and Mearns, 1999; Liang et al., 2004). The 12 km WRF simulation examined in this study uses a convective parameterization, which is considered to be a major source of model biases on both subdaily and daily timescales (Dirmeyer et al., 2012; Hanel and Buishand, 2010; Knist et al., 2020). Moreover, a seasonal analysis of precipitation is important as, generally, both the observation-based datasets (e.g., reanalyses) and models (e.g., WRF) better simulate precipitation in winter than in summer, mainly because winter precipitation is mostly dominated by predictable large-scale stratiform systems (Ebert et al., 2007) and summer precipitation is mainly influenced by unpredictable small-scale convective cells (Prein et al., 2015; Beck et al., 2019).
The rest of the paper is organized as follows: Sect. 2 describes the data and methodology used. Results are presented and discussed in Sect. 3, and also tabulated in Tables 2 and 3, then summarized in Sect. 4. Figures for percent biases are included in the Supplement.
2.1 Data
2.1.1 WRF downscaling of ERA5
The Weather Research and Forecasting model version 4.2.1 is a state of the art, fully compressible, non-hydrostatic, mesoscale numerical weather prediction system designed for both atmospheric research and operational forecasting applications (Skamarock et al., 2008). For this study, the WRF simulation is carried out at 12 km horizontal grid spacing and covers the 1980–2020 period (Fig. 1). The physical parameterizations chosen are Thomson microphysics (Thompson and Eidhammer, 2014), the Tiedke cumulus parameterization (Tiedtke, 1989; Zhang et al., 2011), the Mellor–Yamada–Janjic boundary layer scheme (Janjić, 1994), and the Eta similarity surface layer (Janjić, 1994). Noah is employed for modeling the land surface (Tewari et al., 2004). WRF is further coupled with an urban canopy model (UCM), which resolves urban surfaces, and its land use/land cover is based on National Land Cover Data (NLCD; Dewitz, 2021). Studies suggest that urbanization can enhance or suppress precipitation over different regions, situations, and urbanization phases. Some examples are as follows. Wang et al. (2015) show that urban warming during the early urbanization phase promotes increased sensible heat flux, enhanced convergence, and vertical motion, leading to urban modification of rainfall. Li et al. (2022) find that urbanization suppresses summer precipitation from mesoscale convective systems, isolated deep convection, and non-convective systems in the mid-Atlantic region east of the Rocky Mountains. Georgescu et al. (2021) report that physical growth of the built environment can either enhance or suppress extreme precipitation across CONUS metropolitan regions.
The initial and boundary conditions are obtained from the ERA5 dataset (Hersbach et al., 2020). ERA5 is a fifth-generation ECMWF reanalysis product that assimilates a suite of observations (e.g., aircraft, in situ, and satellite) into the Integrated Forecasting System (IFS) to produce hourly meteorological variables on a regular 0.25∘ latitude–longitude grid with 137 vertical levels.
2.1.2 Reference datasets
To evaluate the performance of 3 h WRF precipitation, NCEP/EMC 4 km Stage IV gridded data is used as reference (Lin and Mitchell, 2005). Stage IV is available at hourly temporal resolution and at 4 km horizontal grid spacing. Stage IV is generated at NCEP from the regional hourly and 6 h multi-sensor (radar and gauges) precipitation analyses produced by the 12 River Forecast Centers (RFCs) over the continental United States. Beck et al. (2019) report that, to minimize systematic biases in Stage IV data, the dataset is rescaled to match its long-term mean with that of the PRISM dataset (details given below) over the evaluation period (2008–2017).
The performance of 24 h WRF precipitation is evaluated against the Oregon State University Parameter-Elevation Regressions on Independent Slopes Model (PRISM) dataset at 4 km grid spacing (Daly et al., 2008). The daily PRISM data use in situ data with a digital elevation model to account for the complex meteorological response from orography, rain shadows, temperature inversions, slope aspect, coastal proximity, and other local features.
For comparison, ERA5, Stage IV, and PRISM precipitation datasets are interpolated to the 12 km WRF grid using first-order conservative remapping (Jones, 1999).
2.2 Method
In this study, we estimate precipitation metrics that characterize the frequency, total amount, intensity, and timing of the mean and extreme precipitation. The metrics are summarized in Table 1. We calculate the mean precipitation amount for 3 and 24 h durations using all precipitation values, including zeros. We use 0.25 and 1 mm thresholds for estimating the frequency and mean precipitation during wet 3 and 24 h periods, respectively. We use these thresholds to minimize the effect of excessive drizzle being present in regional climate models and reanalyses (e.g., Frei et al., 2006; Rajczak et al., 2013) and also to account for observational constraints (Schär et al., 2016). The differences between the mean precipitation amount and the mean wet-3 h and wet-24 h precipitation highlight the biases that result from excessive drizzle in the dataset. The precipitation thresholds in the study are consistent with those in previous studies (e.g., Rajczak et al., 2013; Rajczak and Schär, 2017; Xiao et al., 2018; Kooperman et al., 2022).
2.2.1 Diurnal and annual cycle of precipitation
The diurnal cycle of precipitation is estimated by fitting the first two harmonics to the monthly mean 3 h precipitation. Similarly, the annual cycle of precipitation is estimated by fitting the first two harmonics to the monthly mean 24 h precipitation. The timing of the diurnal peak of the 3 h precipitation is expressed in terms of local solar time (LST). Noon (12:00 LST) is the time when the Sun is highest in the sky at a location. LST hours are obtained from UTC hours as follows (Watters et al., 2021):
where tUTC and tLST are the coordinated universal time and local solar time, respectively. λ is the longitude, in degrees.
In this work, the subdaily precipitation is examined for the 2003–2019 period, and the daily precipitation is analyzed for the 2001–2020 period. These periods are chosen for two considerations. First, the hourly Stage IV data are available only after 2002. Second, any variability arising from the trend may be assumed to be insignificant in the 20-year record. The results are summarized for the seven National Climate Assessment (NCA) regions over the CONUS (https://www.globalchange.gov/content/nca5-regions, last access: 1 July 2023). The seven NCA regions are NW (northwest), SW (southwest), NGP (northern Great Plains), SGP (southern Great Plains), MW (midwest), SE (southeast), and NE (northeast).
3.1 Diurnal cycle of precipitation
Figure 2 shows the peak time of the JJA diurnal precipitation peak (TDPP) in ERA5, WRF, and Stage IV datasets (in hours at LST). We chose to analyze the JJA diurnal cycle because the diurnal variations are stronger in summer than in winter (Dai et al., 1999). Presumably, this is because winter variations of precipitation are dominated by frontal cyclones, and a frontal passage can occur at any time of day, thereby masking any diurnal cycle present. During summer, the frontal cyclone passages are much less frequent, allowing the diurnal cycle to be more visible (e.g., Kunkel et al., 2012). The observed (Stage IV) spatial pattern of TDPP shows that, mostly, precipitation peaks in the afternoon over most of the CONUS, except for regions to the east of the Rocky Mountains (the Great Plains and MW regions). The eastward propagating shift in nighttime diurnal peak east of the Rockies is consistent with mesoscale convective systems (MCSs) originating over the Rockies and moving eastward (Dai et al., 1999; Tan et al., 2019; Scaff et al., 2020; Watters et al., 2021). ERA5 generally reproduces the spatial pattern of the observed diurnal cycle, but the peak occurs earlier along the northern boundaries of the northern Great Plains (NGP) and west of the Great Lakes in the midwest (MW). The largest biases in ERA5 are found between 100–85∘ W, also noted in Watters et al. (2021) who compared biases in ERA5 against the multi-radar multi-sensor (MRMS) gauge-adjusted ground-based radar network product. Similar to ERA5, WRF simulates the observed timing of the diurnal precipitation peak everywhere except over the regions east of the Rockies. Over the regions falling east of 100∘ W, the observed late night to early morning peak in the diurnal cycle is delayed in the WRF simulation. Similar behavior was also noted in the convection-permitting WRF simulation of Scaff et al. (2020). The slow propagation eastward of convective systems is driven by cloud-scale phenomena that are not necessarily well captured by the models used to generate datasets.
The observed magnitude of the JJA precipitation diurnal cycle (using MDPP; precipitation magnitude during the peak of the diurnal cycle) is larger in the eastern CONUS compared to the western CONUS (Fig. 3). The largest MDPP magnitudes are observed along the Gulf coast and in Florida. ERA5 simulates the observed spatial pattern of the diurnal precipitation magnitude very well. Watters et al. (2021) found that ERA5 generally overestimates the magnitude over much of the CONUS in comparison to the Integrated Multi-satellitE Retrievals for GPM (IMERG) dataset, possibly due to reliance on the convection parameterization. The differing performance of ERA5 against the two different observational datasets (as noted in Watters et al., 2021 and our study) also points to uncertainties arising due to differences in reference datasets. WRF does capture the spatial pattern of the observed diurnal precipitation peak magnitude over most of the CONUS, except over the southeast where it overestimates the magnitude of the precipitation peak and over the central Great Plains region where it underestimates the magnitude more than ERA5. The dry biases over the midwest and parts of the central CONUS in WRF diurnal precipitation magnitude are consistent with those of Scaff et al. (2020), suggesting that current climate models, including WRF, underestimate MCS frequencies in summertime weak synoptic-scale forced conditions (Prein et al., 2020). The wet MDPP bias in WRF over the SE is also observed in previous WRF-based studies (e.g., Wang and Kotamarthi, 2014; Scaff et al., 2020). Sun and Bi (2019) showed that the WRF simulation with the Tiedke cumulus parameterization scheme exhibits an earlier and stronger diurnal cycle than that observed over land regions between 25∘ S and 25∘ N in boreal summer. As the convective scheme is the most crucial model component in capturing the diurnal cycle of precipitation (Shin et al., 2007), and precipitation from cumulus parameterization schemes dominates over the SE CONUS (Iguchi et al., 2017), we suspect that cumulus parameterization in the current WRF simulation may be responsible for the wet bias over the SE region.
3.2 Annual cycle of precipitation
Figure 4 shows the peak time (calendar month) of the monthly averaged precipitation (TMPP; the annual cycle of the monthly averaged precipitation). Using PRISM as a reference, maximum monthly precipitation occurs during winter season over the western CONUS and parts of Arkansas, Mississippi, Louisiana, and the NE CONUS. The majority of the Great Plains is dominated by the late spring and early summer precipitation, whereas the southeast region gets most of the rainfall in the summer season. This high-resolution spatial map of the annual cycle of monthly precipitation is consistent with previous studies (e.g., Bukovsky and Karoly, 2007). Stage IV also exhibits a similar annual precipitation cycle as PRISM; however, differences from PRISM emerge over multiple regions across the US such as SW (Utah), NE (Maine), and MW (northern and eastern boundaries of Lake Michigan). A few sources of biases in Stage IV may affect its results shown in Fig. 4 and subsequent figures. For example, a discontinuity in the mosaic-making process exists over a few regions such as over oceans and areas that cover the Great Lakes region. A few western RFCs, including Colorado Basin RFC (CBRFC), do not use radar estimates due to poor coverage over mountainous regions. Moreover, the inherent biases in radar rainfall estimation due to factors such as lack of radar coverage, brightband contamination, and biases existing in the algorithms are not completely avoidable (Nelson et al., 2016; Prat and Nelson, 2015). Both ERA5 and WRF are able to simulate the spatial pattern of peak time of the annual cycle. However, WRF outperforms ERA5 in simulating the spatial structure of the annual cycle, as it greatly improves ERA5 biases over the NE and parts of the SE and Great Plains regions.
The spatial pattern of the magnitude of the monthly averaged precipitation peak (MMPP) is shown in Fig. 5. The maximum monthly average precipitation occurs along the western coast, Sierra Nevada mountains, and in the southeastern region. Stage IV does capture the spatial pattern of the referenced precipitation magnitude; it exhibits underestimated precipitation (dry bias) of 20 % or more almost everywhere across the CONUS. The largest percent biases exist over the SE and SW regions (Figs. 5 and S2 in the Supplement). ERA5 underestimates the precipitation magnitude over the NE and SE regions and overestimates it over the southern Great Plains. On the other hand, WRF captures the spatial pattern of the magnitude very well across CONUS and exhibits much lower biases across the CONUS than ERA5.
In summary, both the timing and magnitude of the monthly averaged precipitation peak are improved in the downscaled WRF simulations compared to ERA5.
3.3 Evaluation of 3 h precipitation
Figure 6 shows the precipitation frequency of 3 h precipitation (PF3h). The precipitation frequency is computed as the counts of 3 h precipitation events with magnitude greater than 0.25 mm expressed as a percentage of the total number of 3 h time steps. Compared with Stage IV, ERA5 overestimates the precipitation frequency by 3 %–10 % in all seasons over most of the CONUS except over the NW and SW. It does underestimate the frequency over the hilly areas of the NW regions in JJA. WRF also exhibits more frequent precipitation mostly over NGP and MW regions in DJF and MAM. In contrast, WRF consistently underestimates precipitation frequency along the west coast. Also, notably, WRF overestimates the frequency over the SE in MAM and JJA and underestimates it in DJF. The spatial pattern of biases in the annual 3 h precipitation frequency in WRF is consistent with Kong et al. (2022), who found that precipitation frequency in WRF is more sensitive to the convective and radiation schemes than the precipitation amount.
Pmean3h (the mean of all 3 h precipitation values including zeros) is shown in Fig. 7. In Stage IV data, the 3 h mean precipitation is maximum over the coastal and mountainous regions of the western US (Washington, Oregon, and Sierra Mountains of California). The eastern half of the CONUS experiences more 3 h average precipitation than the western half (except in the coastal and mountainous regions). The maximum values of Stage IV 3 h precipitation observed along the northwestern US states are missing in the satellite-derived and bias-corrected gridded Climate Prediction Center Morphing technique (CMORPH) dataset, probably due to the insufficient representation of orography at grid spacing (Kong et al., 2022). ERA5 generally overestimates the 3 h mean precipitation over much of the CONUS throughout the year. On the other hand, while its performance is an improvement in many regions, WRF overestimates the precipitation over most of the CONUS (except SGP) annually or in winter and spring seasons. When compared across seasons, WRF underestimates the summer precipitation but overestimates the winter precipitation over the SGP region. Moreover, WRF simulates a much larger wet bias over the SE in summer than in any other season. The spatial pattern of the WRF simulated precipitation frequency is similar to the mean precipitation amount, suggesting that the subdaily precipitation frequency affects the corresponding subdaily mean precipitation in WRF. The spatial pattern of annual dry bias in the SGP and wet bias in the SE region is also found in the other WRF simulation employing the Tiedke cumulus parameterization scheme along with the rapid radiative transfer model for global models (RRTMG) radiation scheme (Kong et al., 2022).
Figure 8 shows the 3 h mean for precipitation greater than 0.25 mm 3 h−1 (S3hII). As shown for Stage IV, mean S3hII values are generally higher than Pmean3h across the CONUS. The highest S3hII values are observed over the SE and SGP regions, suggesting that 3 h precipitation in these regions is dominated by drizzling precipitation (<0.25 mm). Notably, except for parts of NGP, NW, and SW regions in DJF, ERA5 underestimates the mean S3hII over most of the CONUS in all seasons. This ERA5 bias, together with those shown in Figs. 6 and 7, suggest that ERA5 suffers from drizzling effect, causing it to precipitate more frequently but in lesser amounts when it rains. In contrast to ERA5, WRF simulates more S3hII values across the CONUS in DJF and less in JJA. Notably, the absolute S3hII biases in WRF are generally lower than those in ERA5 in most of the seasons and regions.
The spatial pattern of the 3 h annual maximum precipitation (Rx3h) is shown in Fig. 9. Rx3h in Stage IV exhibits higher values in the eastern half of the CONUS than in the western half. The spatial pattern and the magnitude in Stage IV is similar to that obtained from the Next-Generation Radar (NEXRAD) dataset in Wehner et al. (2021). ERA5 generally underestimates (mostly within ±5 mm) the maximum precipitation in all seasons and everywhere. On the other hand, WRF overestimates the 3 h annual maximum precipitation over the eastern half of the CONUS but shows clear seasonal variation in its biases over the western CONUS regions. For example, WRF slightly overestimates the precipitation maxima over parts of the NW, SW, and the GP regions in DJF but underestimates the maxima over those regions in JJA. A detailed investigation of biases in WRF is out of the scope of this paper, but we suspect that WRF biases in the Great Plains may be attributed to underestimated MCS frequencies (Prein et al., 2020), imperfect cumulus parameterization scheme, and biases in the representation of intensity, location, and diurnal cycle of the low-level jet in 12 km WRF simulation (Lee et al., 2017).
The above analysis of average 3 h annual maximum precipitation provides little information on whether the datasets reasonably simulate the distribution of the 3 h annual maximum precipitation. Figure 10 shows the probability density function (PDF) of the 3 h annual maximum precipitation. In each panel, the y axis uses a log scale to clearly show higher, less frequent precipitation values. It is apparent from the figures that ERA5 consistently underestimates extreme precipitation values over all NCA regions and across all seasons. WRF generally improves on the biases in ERA5 by producing higher extreme precipitation values and thereby bringing the PDF of extreme precipitation values close to the observed PDF.
3.4 Evaluation of 24 h precipitation
For 24 h precipitation analysis, we use PRISM as reference data. We also evaluate 24 h precipitation in Stage IV against PRISM to quantify observational uncertainty.
Figure 11 shows the 24 h precipitation frequency (PF24h). The precipitation frequency is computed from the days when 24 h precipitation is more than 1 mm d−1. Stage IV consistently underestimates (in comparison to PRISM) the precipitation frequency over most of the CONUS. The largest biases in Stage IV precipitation frequency are observed over the NGP in winter and SW throughout the year (Fig. S7 in the Supplement). The underrepresented precipitation frequency in Stage IV may be related to its difficulty in detecting light and frozen precipitation across the CONUS and, most notably, in the western US because the precipitation processing system in Stage IV does not distinguish between liquid and frozen hydrometeor types (Smalley et al., 2014). ERA5 consistently overestimates PF24h by more than 5 % in all seasons over most of the CONUS except NW and SW regions. It also underestimates the precipitation frequency over the SW region in summer and fall. In contrast, WRF underestimates the frequency in the NW and SW regions and shows frequency biases in other regions that are seasonally dependent. For example, over the SE, WRF underestimates the frequency in DJF but overestimates it in JJA. Similarly, WRF overestimates the frequency over NGP and MW in DJF, but it underestimates the frequency over those regions in JJA. It is also notable that WRF underestimates the frequency over most of the CONUS in JJA (except SE) and SON. When compared with the biases in 3 h precipitation frequency (Fig. 6), the spatial pattern of the biases in ERA5 is similar for both 3 and 24 h precipitation. However, the 24 h precipitation frequency biases in WRF are larger than those for 3 h precipitation. This suggests that while ERA5 tends to exhibit more drizzle (i.e., low intensity precipitation), WRF generally concentrates precipitation into fewer days of the year than we see in observations.
Biases in 24 h precipitation mean (Pmean24h) are shown in Fig. 12. Stage IV shows dry bias as compared to PRISM over most of the CONUS in all seasons, except that it shows wet biases over sporadic locations in NW and SW regions. The corresponding percent bias in Pmean24h (Fig. S8) indicates large Stage IV relative dry biases in the western CONUS (NGP, NW, and SW) in DJF, possibly related to its inability to detect freezing and light precipitation events, as discussed in the previous subsection. ERA5 consistently exhibits a dry bias in 24 h mean precipitation over the southeast throughout the year. When compared with the frequency biases in Fig. 11, it appears that although ERA5 precipitates more frequently than PRISM, it precipitates less during wet days than PRISM. ERA5 generally exhibits wet biases over other regions. Over the NE, ERA5 shows dry biases over regions close to the coasts and wet biases over the inland areas – a pattern that may be associated with the insufficient ability of ERA5 parameterizations to produce sea breeze-induced precipitation (Crossett et al., 2020). WRF generally shows dry biases over the Great Plains, exhibiting typical model biases existing in the state-of-the-art climate models (Srivastava et al., 2020). The spatial patterns of 24 h frequency biases in WRF (Fig. 11) are similar to the 24 h mean precipitation. When compared with ERA5, WRF shows stronger dry biases over the Great Plains regions, particularly in JJA. It is interesting to note that the spatial pattern of the seasonal 24 h mean precipitation biases in WRF is quite similar to those simulated by another recent bias-corrected convection-permitting WRF simulation over the CONUS (Gensini et al., 2023) – for example, JJA dry biases in both the studies are spread over most the CONUS. Similarly dry biases over the SE region are quite similar. What is more striking is that the magnitude of the 24 h mean biases in our study are largely comparable to those in Gensini et al. (2023). The summer dry biases in the Great Plains have been reported in previous analyses of WRF simulations employing convection-permitting or convection-parameterizing configurations (Sun et al., 2016) and in other regional climate models, including WRF (Mearns et al., 2012; Gao et al., 2017). The summer dry biases in the Great Plains may be associated with the unrealistically strong coupling of convection with the surface heating over the Rocky Mountains and insufficiently resolved and slow propagating mesoscale systems (Mearns et al., 2012; Tripathi and Dominguez, 2013; Hu et al., 2018).
The 24 h mean wet-day precipitation (SDII) is shown in Fig. 13. As for the biases in Pmean24h (Fig. 12), Stage IV underestimates SDII almost everywhere but more prominently over the eastern half of the CONUS in all seasons. ERA5 underestimates SDII over the eastern half of the CONUS (parts of NGP, MW, SGP, and NE) across the year. The dry SDII biases, together with the overestimated frequency and mean precipitation in winter and spring over NGP, MW, and SGP, suggest that ERA5 has too little and too frequent precipitation bias. WRF exhibits wet SDII biases over most of the CONUS in DJF, except in a few places over the SGP and SE. On the other hand, it shows strong dry biases over the SGP and SE during spring and over the SGP, MW, and SE during summer.
Figure 14 shows biases in 24 h annual maximum precipitation (Rx1day). As for the other metrics, Stage IV underestimates Rx1day over the eastern half of the CONUS. The dry bias is most pronounced (∼20 %) over the Great Plains and MW during summer and over the NGP and northeastern parts of SW (>50 %) during winter (Fig. S10 in the Supplement). On the other hand, Rx1day values in Stage IV are very well represented over NW and SW in all seasons except winter. ERA5 shows strong and significant dry biases over the eastern CONUS throughout the year. The ERA5 wet biases over the western CONUS are smaller than over the eastern half. These patterns are roughly similar to the 3 h precipitation biases (Fig. 9). WRF generally shows seasonally dependent biases across CONUS. For example, it shows wet biases during winter and spring but a mix of wet and dry biases (SGP and MW) during summer and fall. When compared with ERA5, it is evident that though WRF reverses the sign of dry bias over most of the eastern CONUS (except parts of the Great Plains), WRF exhibits smaller magnitude of biases across the CONUS than ERA5.
Finally, the PDF of 24 h annual maximum precipitation (PDF24h) is shown in Fig. 15. Stage IV represents well the PDF24h over NW and SW. However, it does show problems in capturing the PDF24h over the NGP throughout the year. It is apparent that ERA5 severely underestimates the annual maximum precipitation across the CONUS and throughout the year. WRF does a much better job of simulating the observed distribution as it reduces the biases in ERA5 frequency distribution of 24 h annual maximum precipitation for most of the regions and seasons.
For the sake of convenience, the results discussed in this section are also tabulated in Tables 2 and 3.
This paper evaluates the performance of the 12 km Weather Research and Forecasting (WRF)-based dynamical downscaling of the fifth-generation ECMWF atmospheric reanalysis (ERA5) in simulating the subdaily and daily precipitation characteristics. In particular, we evaluate diurnal and annual cycles, frequency and mean precipitation, and annual maximum precipitation and its distribution. We addressed two questions specifically: (1) how well are the 3 and 24 h precipitation characteristics represented in the downscaled WRF simulation in comparison to those in ERA5; and (2) how does the performance of the simulated WRF precipitation vary across seasons, regions, and timescales? We measure the ERA5 and WRF precipitation simulation against the NCEP/EMC 4 km Stage IV and PRSIM data on 3 and 24 h timescales, respectively.
Our analysis suggests that WRF performs similarly to ERA5 in capturing the timing and magnitude of the JJA 3 h diurnal precipitation peak over most of the CONUS, except the Great Plains regions. Over the Great Plains, WRF exhibits a diurnal cycle delayed by a few hours, suggesting that the mesoscale convective systems, that originate in the Rockies and travel eastward, are slower in the WRF simulation – a typical model problem found in many previous studies. WRF simulates the timing (month) and magnitude of the monthly mean 24 h precipitation annual cycle much better than ERA5. Notably, WRF improves the timing of the annual cycle over the NE, SE, and areas surrounding the Gulf of Mexico.
One noticeable difference between ERA5 and WRF is that ERA5 generally displays similar signs of biases (positive or negative) in most of the precipitation characteristics examined throughout the year and across most of the CONUS. However, WRF exhibits seasonally dependent biases in the precipitation characteristics across the CONUS. For instance, ERA5 overestimates both the frequency and mean of the 3 h precipitation over most of the CONUS, except over parts of the western CONUS. On the other hand, WRF underestimates the frequency and mean of the 3 h precipitation over the SE in winter but overestimates these quantities in summer over that region. Similarly, WRF underestimates the mean 3 h precipitation over the central Great Plains region in summer but not in winter. Also, ERA5 generally underpredicts the 3 h annual and seasonal maximum precipitation throughout the year over the CONUS, but WRF overestimates it over the eastern CONUS in all seasons. What is interesting is that ERA5 performs poorly in simulating the observed probability distribution of the 3 h precipitation and thus severely underestimates the observed 3 h extreme precipitation, but WRF performs quite well in capturing the observed PDF, thereby reducing the biases in ERA5.
Similar to what was found for the 3 h precipitation, ERA5 does show similar biases in the 24 h precipitation, but WRF displays regionally and seasonally dependent biases. WRF overestimates the 24 h precipitation frequency over most of the CONUS (except NW and SW). The 12 km WRF generally exhibits seasonally dependent biases also found in the convection-permitting WRF simulation (Gensini et al., 2023). In this analysis, WRF underestimates the frequency throughout the CONUS in SON but overestimates the frequency over the eastern half of the CONUS in MAM. The underestimated frequency in WRF is more severe in JJA. Similarly, ERA5 underestimates the 24 h annual maximum precipitation over the eastern half of the CONUS, most notably in the Great Plains and SE regions; while these biases are generally reduced in magnitude in the WRF simulation, they also occur with a change in the sign. Notably, ERA5 underestimates the 24 h annual maximum precipitation over the SE, while WRF overestimates it (though by a smaller overall magnitude). As observed for 3 h precipitation, WRF shows remarkable improvements in the simulated probability distribution of the 24 h annual maximum precipitation; throughout the CONUS, ERA5 does have problems in capturing the extreme precipitation magnitudes, suggesting that its representation of the strongest precipitation extremes is overly conservative. These results are also summarized in Tables 2 and 3.
This work adds to the literature addressing the value of dynamical downscaling to higher resolution. Our results echo similar past studies, which generally show a mixture of improvement and deterioration in the quality of simulated fields. Although we find that dynamical downscaling with WRF simulates observed precipitation characteristics reasonably well on both the daily and subdaily timescales, improvements do not emerge everywhere. Particularly, WRF exhibits several common biases found in many other models, which are likely suppressed in ERA5 through data assimilation. As hypothesized in this study, WRF does show seasonally and regionally dependent biases in precipitation, while ERA5's biases are less seasonal. Nonetheless, WRF greatly improves upon the PDFs of annual maximum precipitation at both 3 and 24 h timescales and improves on the month and magnitude of the seasonal precipitation cycle. This suggests the WRF product is generally more useful when it comes to its representation of precipitation extremes – which seems to be a consequence of the fact WRF tends to produce generally flashier precipitation. These results suggest care should be taken in using the WRF simulations for further applications such as future regional climate projections or regional hydrologic modeling.
A related question is how much bias is acceptable in a climate model. The acceptable level of biases really depends on the application of the climate data. Although the data could be used directly in analysis, we expect a large portion of users will use the data to force other models. In that case, tolerance for biases depends on the type, scope, and scale of the downstream modeling frameworks. Nonetheless, the question is hard to answer quantitatively given that a large uncertainty exists even among observational datasets (e.g., Srivastava et al., 2020, 2022). Still, one can qualitatively assess the model's performance by comparing it with other models or observational datasets. We assessed the observational uncertainty in 24 h precipitation representation by comparing precipitation characteristics between PRISM and Stage IV in 24 h precipitation analysis. We found that biases in WRF are generally smaller in magnitude than in Stage IV. For example, annual 24 h precipitation frequency (PF24h) is better simulated in WRF than in Stage IV, and biases in the magnitude of monthly average precipitation peak (MMPP) are much smaller in WRF than in Stage IV. Similarly, WRF shows comparable (e.g., DJF PDF24h in NW and SW) or even better (e.g., NGP in all seasons) simulation of Rx1day PDF (PDF24h) than Stage IV. These analyses suggest that WRF reasonably simulates the observed precipitation characteristics across the CONUS.
While the 12 km grid spacing of these simulations is a clear refinement on the native resolution of ERA5, ultimately, it would be far more desirable to run the downscaled simulation in the convection-resolving regime (i.e., 3 km or finer). We expect the match between the precipitation frequency distribution in the tail will improve monotonically with resolution. Until convection-resolving scales are reached, important processes such as horizontal propagation of mesoscale convective systems will not be properly represented. Consequently, when it becomes possible to reach these spatial scales at climatological timescales with available computing power, we would advocate for the metrics explored in this study to be revisited.
The WRF source code is available on https://www2.mmm.ucar.edu/wrf/users/download/get_source.html (last access: 5 July 2023) and https://doi.org/10.5065/D68S4MVH (Skamarock et al., 2008). ERA5 is publicly accessible from https://doi.org/10.5065/BH6N-5N20 (European Centre for Medium-Range Weather Forecasts, 2019). PRISM precipitation data can be downloaded from https://prism.oregonstate.edu/ (Daly et al., 2008), and Stage IV data are available on https://doi.org/10.5065/D6PG1QDD (Du, 2011). The 40-year historical WRF dataset can be downloaded from https://doi.org/10.57931/1885756 (Jones et al., 2022).
The supplement related to this article is available online at: https://doi.org/10.5194/gmd-16-3699-2023-supplement.
AKS: conceptualization, methodology, software, validation, formal analysis, investigation, and writing (original draft – review and editing). PAU: conceptualization, validation, resources, writing (original draft – review and editing), supervision, project administration, and funding acquisition. DR, PV, and AJ: model simulation and writing (review and editing). RG: writing (original draft – review and editing) and supervision.
The contact author has declared that none of the authors has any competing interests.
Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
This work is supported by the Department of Energy Office of Science award number DE-SC0016605, “A Framework for Improving Analysis and Modeling of Earth System and Intersectoral Dynamics at Regional Scales.” The climate forcing for this paper was developed collaboratively between the IM3 and HyperFACETS projects, both of which are supported by the US Department of Energy, Office of Science, as part of research in MultiSector Dynamics, and Regional and Global Model Analysis, Earth and Environmental System Modeling Program. A portion of this research used the computing resources of the National Energy Research Scientific Computing Center (NERSC), a US Department of Energy Office of Science User Facility located at Lawrence Berkeley National Laboratory, operated under contract no. DE-AC02-05CH11231.
This research has been supported by the US Department of Energy (grant nos. DE-SC0016605, DE-AC02-05CH11231, and DEAC05-00OR22725).
This paper was edited by Axel Lauer and reviewed by two anonymous referees.
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