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Geosci. Model Dev., 15, 413–428, 2022
https://doi.org/10.5194/gmd-15-413-2022
© Author(s) 2022. This work is distributed under
the Creative Commons Attribution 4.0 License.
WRF v.3.9 sensitivity to land surface model and horizontal
resolution changes over North America
Almudena García-García1,2, Francisco José Cuesta-Valero1,2, Hugo Beltrami1, J. Fidel González-Rouco3, and
Elena García-Bustamante4
1Climate & Atmospheric Sciences Institute, St. Francis Xavier University, Antigonish, Nova Scotia, Canada
2Department of Remote Sensing, Helmholtz Centre for Environmental Research – UFZ, Leipzig, Germany
3Physics of the Earth and Astrophysics Department, IGEO (UCM-CSIC), Universidad Complutense de Madrid,
Madrid, Spain
4Department of Energy, Research Center for Energy, Environment and Technology (CIEMAT), Madrid, Spain
Correspondence: Hugo Beltrami (hugo@stfx.ca)
Received: 19 July 2021 – Discussion started: 26 August 2021
Revised: 26 November 2021 – Accepted: 1 December 2021 – Published: 18 January 2022
Abstract. Understanding the differences between regional
simulations of land–atmosphere interactions and near-
surface conditions is crucial for a more reliable representa-
tion of past and future climate. Here, we explore the effect of
changes in the model’s horizontal resolution on the simulated
energy balance at the surface and near-surface conditions us-
ing the Weather Research and Forecasting (WRF) model. To
this aim, an ensemble of 12 simulations using three different
horizontal resolutions (25, 50 and 100 km) and four different
land surface model (LSM) configurations over North Amer-
ica from 1980 to 2013 is developed. Our results show that
finer resolutions lead to higher surface net shortwave radia-
tion and maximum temperatures at mid and high latitudes.
At low latitudes over coastal areas, an increase in resolution
leads to lower values of sensible heat flux and higher values
of latent heat flux, as well as lower values of surface temper-
atures and higher values of precipitation, and soil moisture in
summer. The use of finer resolutions leads then to an increase
in summer values of latent heat flux and convective and non-
convective precipitation and soil moisture at low latitudes.
The effect of the LSM choice is larger than the effect of hori-
zontal resolution on the near-surface temperature conditions.
By contrast, the effect of the LSM choice on the simulation
of precipitation is weaker than the effect of horizontal resolu-
tion, showing larger differences among LSM simulations in
summer and over regions with high latent heat flux. Compar-
ison between observations and the simulation of daily max-
imum and minimum temperatures and accumulated precip-
itation indicates that the CLM4 LSM yields the lowest bi-
ases in maximum and minimum mean temperatures but the
highest biases in extreme temperatures. Increasing horizon-
tal resolution leads to larger biases in accumulated precipi-
tation over all regions particularly in summer. The reasons
behind this are related to the partition between convective
and non-convective precipitation, specially noticeable over
western USA.
1 Introduction
Most assessments of climate change impacts on ecosys-
tems and societies are based on projections performed by
regional climate models (RCMs) and/or earth system mod-
els (ESMs; IPCC, 2013, 2019). Exploring inter-model dif-
ferences in present climate simulations is necessary to un-
derstand their contribution to the spread in future climate
projections and ultimately to better characterize or even re-
duce the uncertainty in the simulation of the response to a
given scenario (Cubasch et al., 2013). Understanding inter-
model differences is also important for paleoclimatic stud-
ies relying on regional climate model simulations to bridge
the gap between the local character of proxy reconstructions
and ESM global simulations (e.g., PALEOLINK; Gómez-
Navarro et al., 2018).
The representation of land–atmosphere interactions within
climate models has received considerable attention during
Published by Copernicus Publications on behalf of the European Geosciences Union.
414 A. García-García et al.: WRF sensitivity to horizontal resolution and LSM changes
the last decades due to their influence on surface climate,
vegetation and soil hydrology, and therefore, on climate vari-
ability (e.g., Lorenz et al., 2016; Vogel et al., 2017). For ex-
ample, energy and water exchanges between the lower atmo-
sphere and the ground surface have been shown to alter sur-
face conditions, particularly during extreme weather events
in summer (Seneviratne et al., 2006; Hirschi et al., 2011; Mi-
ralles et al., 2012; Hauser et al., 2016). Land–atmosphere
interactions have also been studied in the evaluation of cli-
mate model simulations, applying several metrics to char-
acterize surface energy fluxes and near-surface conditions
(Koven et al., 2013; Dirmeyer et al., 2013; Sippel et al., 2017;
García-García et al., 2019).
The representation of near-surface conditions (e.g., air and
soil temperatures, soil moisture, etc.) and energy and water
exchanges at the land surface in a climate model depends on
the processes simulated by the atmospheric and soil model
components, as well as on the degree of coupling imple-
mented between both model components (Koster et al., 2006;
Melo-Aguilar et al., 2018). Different land surface models
(LSMs) include varying levels of realism in the represen-
tation of soil physics, land cover type, soil water content,
snow cover, drip, runoff or infiltration. Thus, each LSM sim-
ulates somewhat different surface water and energy fluxes
(e.g., Lawrence et al., 2019). For example, the representa-
tion of surface albedo, evaporative resistance and aerody-
namic roughness by each LSM alters the simulation of the
surface energy balance and consequently affects the evolu-
tion of surface temperatures (Laguë et al., 2019; MacDougall
and Beltrami, 2017). The dependence of the simulated land–
atmosphere interactions on the LSM has been shown in pre-
vious studies using global (García-García et al., 2019) and
regional climate model simulations over North America (Pei
et al., 2014; García-García et al., 2020). There are examples
of these studies at local scales (Mooney et al., 2013; Whar-
ton et al., 2013; Chen et al., 2014; Van Den Broeke et al.,
2018; Liu et al., 2019; Zhuo et al., 2019) and at continen-
tal scales for Europe (Davin and Seneviratne, 2012; Mooney
et al., 2013).
Horizontal resolution is another factor to take into ac-
count in the study of land–atmosphere interactions in cli-
mate model simulations. ESMs are limited by computational
resources, using horizontal resolutions from approximately
250 to 100 km (e.g., CMIP5 models; Taylor et al., 2012),
while RCMs allow for using much finer resolutions. Anal-
ogously, the range of horizontal resolutions employed in
RCMs for climate studies is usually limited to approximately
50–25 km (e.g., CORDEX models; Giorgi and Gutowski,
2015). In spite of this enhanced resolution, an RCM’s abil-
ity to reproduce temporal variability like that of precipitation
at daily timescales is still limited, being greatly improved
by using resolutions of ∼4 km and convection-resolving
RCMs (Sun et al., 2016). Previous studies have shown some
resolution-induced improvements in the simulation of pre-
cipitation, wind and high-altitude temperatures at local and
regional scales with possible implications for the simula-
tion of climate dynamics (Ban et al., 2014; Gómez-Navarro
et al., 2015; Messmer et al., 2017; Hahmann et al., 2020;
Vegas-Cañas et al., 2020). Small-scale weather phenomena
such as sea breezes, snowstorms induced by the presence
of lakes, local winds, tropical cyclones and mesoscale con-
vective systems can be better represented with increased res-
olution (Wehner et al., 2010). Some studies have also sug-
gested a resolution-induced improvement in the representa-
tion of interactions between small- and large-scale dynami-
cal processes, ultimately leading to better large-scale atmo-
spheric flow (Lucas-Picher et al., 2017). Thus, the difference
in the resolution employed in RCMs and ESMs is expected to
improve the representation of land–atmosphere interactions
in RCMs through a more adequate discretization of equa-
tions, as well as through a more realistic representation of
small-scale processes and topographical features (Xue et al.,
2014; Rummukainen, 2016; Vegas-Cañas et al., 2020). The
improved representation of land–atmosphere interactions as-
sociated with finer resolutions is also expected to induce an
improvement in the simulation of near-surface conditions,
especially in the simulation of extreme events (Prein et al.,
2013; Di Luca et al., 2015; Rummukainen, 2016; Demory
et al., 2014).
Although the literature on the impact of the LSM choice
and changes in resolution on climate simulations is extensive,
most studies are focused on small domains and meteorolog-
ical events, providing little information about the impact of
the LSM choice and horizontal resolution changes on long-
term climatological variability. Here, we evaluate and com-
pare the influence of both factors, the LSM choice and hori-
zontal resolution, on the representation of energy and water
fluxes at the surface and consequently on the simulation of
near-surface conditions over North America for a climato-
logical period spanning the time interval 1980–2013. We use
the Weather Research and Forecasting (WRF) model (ver-
sion 3.9; Skamarock et al., 2008) that allows for testing a
number of LSM schemes, each varying in physical parame-
terization complexities. An ensemble of 12 simulations was
generated using three different horizontal resolutions (25, 50
and 100 km), four different LSM configurations and two veg-
etation options, i.e., prescribed or dynamical vegetation.
The WRF representation of climate at different resolutions
is expected to affect the simulation of atmospheric and sur-
face phenomena in several ways, through a different rep-
resentation of cloud formation or through a different level
of details in the description of orography and land cover.
Simulations with different LSMs provide information about
the advantages of using a comprehensive LSM, such as the
CLM4 LSM (Oleson et al., 2010), or a simpler LSM com-
ponent, such as the NOAH LSM (Tewari et al., 2004). Ad-
ditionally, the comparison of two identical model configura-
tions except for the prescribed or dynamical vegetation mode
provides information about the effect of a realistic evolution
of vegetation cover on the energy and water balance at the
Geosci. Model Dev., 15, 413–428, 2022 https://doi.org/10.5194/gmd-15-413-2022
A. García-García et al.: WRF sensitivity to horizontal resolution and LSM changes 415
surface. Thus, soil and near-surface variables from these 12
simulations are compared and also evaluated against temper-
ature and precipitation observations to explore two questions.
(1) How do changes in horizontal resolution within WRF af-
fect the simulation of land–atmosphere interactions and near-
surface conditions? (2) How do LSM differences in the simu-
lation of land–atmosphere interactions translate into different
near-surface conditions?
The descriptions of the WRF experiments and the method-
ology applied for the analysis are included in Sects. 2 and 3,
respectively. Section 4 presents the results of the analysis,
which are discussed using the available literature in Sect. 5.
The conclusions and importance of this work are summarized
in Sect. 6.
2 Description of the modelling experiment
We performed three sets of regional simulations (12 simula-
tions in total) over North America from 1980 to 2013 using
the Advanced Research WRF model (WRF v3.9; Skamarock
et al., 2008) with initial and boundary conditions from
the North American Regional Reanalysis product (NARR;
Mesinger et al., 2006). The NARR product was generated by
the National Centers for Environmental Prediction (NCEP)
Eta atmospheric model (Janjic, 1997), the NOAH LSM com-
ponent (Mitchell, 2005) and the Regional Data Assimilation
System (RDAS; Mesinger et al., 2006). The NARR data were
obtained from the National Center for Environmental Infor-
mation (NOAA) archive and provides data over a 32 km grid
with a 3-hourly temporal resolution. No nudging techniques
were applied within the domain of the simulation. The use
of nudging techniques imposes large-scale variability within
the inner scales of the domain of simulation, thus partially
muting the generation of local- and regional-scale dynami-
cal responses in favour of representing the large scale flow
of the driving conditions. Avoiding nudging, therefore, al-
lows for more clearly expressing the influences of increased
resolution and of changing the LSM component (von Storch
et al., 2000).
The three sets of simulations were performed using a
Lambert-type projection with resolutions of 25×25 km, 50×
50 km and 100 ×100 km. Each set includes four simulations
using three different LSM components: the NOAH LSM
(NOAH; Tewari et al., 2004), the NOAH LSM with multi-
parameterizations options (NOAH-MP; Niu et al., 2011) and
the Community Land Model version 4 LSM (CLM4; Oleson
et al., 2010). The fourth simulation included in each set was
performed using the NOAH-MP LSM with dynamic vegeta-
tion (NOAH-MP-DV), while vegetation was prescribed for
the other simulations. The rest of the WRF options remained
the same for all simulations, employing 27 atmospheric lev-
els, land cover categories from the Moderate Resolution
Imaging Spectroradiometer (MODIS; Barlage et al., 2005),
the WRF single moment (WSM) 6-class graupel scheme for
the microphysics (Hong and Lim, 2006), the Grell–Freitas
ensemble scheme (Grell and Freitas, 2014), the Yonsei Uni-
versity scheme for the description of the planetary bound-
ary layer scheme (YSU; Hong et al., 2006), the revised
MM5 Monin–Obukhov scheme (Jiménez et al., 2012) and
the Community Atmosphere Model (CAM) scheme (Collins
et al., 2004). The use of different horizontal resolutions re-
quires the use of different time steps for performing our
WRF simulations, as well as different time intervals for com-
puting radiation physics (radt option in WRF namelist). Ta-
ble 1 summarizes the differences between all simulations em-
ployed in this analysis.
The LSM schemes used in this study differ in parameteri-
zation complexity, the NOAH being the most basic amongst
the three selected LSMs. The NOAH LSM describes soil and
vegetation processes for the closure of the water and energy
budgets, discretizing the soil into four soil layers that reach a
total of 2 m of depth (Tewari et al., 2004). Some limitations
have been associated in this soil model with the represented
bulk layer of canopy, snow and soil, its system to drain water
at the bottom of the soil column, and its simple snowmelt dy-
namics (Wharton et al., 2013). The NOAH-MP version of the
NOAH LSM improves soil hydrology and the representation
of terrestrial biophysical processes (Niu et al., 2011). This
scheme includes a separate vegetation canopy with a compre-
hensive description of vegetation properties. The NOAH-MP
also includes a multi-layer snow pack description with liquid
water storage and melting and refreezing capabilities. It in-
cludes the same soil structure as the NOAH LSM (four soil
layers, down to 2 m). The CLM4 LSM incorporates a com-
prehensive representation of biogeophysics and hydrology,
including a single-layer vegetation canopy, a five-layer snow-
pack and a 10-layer soil column down to a depth of 3.802m.
This scheme also characterizes each grid cell into five pri-
mary sub-grid land cover types (glacier, lake, wetland, urban
and vegetated), using up to four plant functional types (PFTs)
to describe vegetation physiology and structure.
3 Methodology
We study the impact of changing horizontal resolution on
surface energy fluxes and near-surface conditions as simu-
lated by the WRF model with different LSM components.
For this purpose, we estimated the temporal averages of sur-
face energy fluxes for the analysis period (1980–2013) fo-
cusing on the following energy components: net shortwave
radiation (SNET, Wm−2), net longwave radiation (LNET,
Wm−2), net radiation absorbed by the soil (RNET, Wm−2),
latent heat flux (LH, Wm−2), sensible heat flux (HFX,
Wm−2) and ground heat flux (GHF, Wm−2). The temporal
averages of near-surface conditions are estimated using out-
puts of 2 m air temperatures (SAT, ◦C), daily maximum SAT
(TASMAX, ◦C), daily minimum SAT (TASMIN, ◦C), soil
temperature at 1 m depth (GST 1 m, ◦C), accumulated con-
https://doi.org/10.5194/gmd-15-413-2022 Geosci. Model Dev., 15, 413–428, 2022
416 A. García-García et al.: WRF sensitivity to horizontal resolution and LSM changes
Table 1. Summary of the regional simulations performed in this analysis.
Name LSM Resolution Vegetation mode Simulation time step Radiation time step
NOAH 25 km 25 km Prescribed 2.5 min 6 min
NOAH 50 km NOAH 50 km Prescribed 5 min 20 min
NOAH 100 km 100 km Prescribed 10 min 20 min
NOAH-MP 25 km 25 km Prescribed 2.5 min 6 min
NOAH-MP 50 km NOAH-MP 50 km Prescribed 5 min 20 min
NOAH-MP 100 km 100 km Prescribed 10 min 20 min
NOAH-MP-DV 25 km 25 km Dynamic 2.5 min 6 min
NOAH-MP-DV 50 km NOAH-MP 50 km Dynamic 5 min 20 min
NOAH-MP-DV 100 km 100 km Dynamic 10 min 20 min
CLM4 25 km 25 km Prescribed 2.5 min 6 min
CLM4 50 km CLM4 50 km Prescribed 5 min 20 min
CLM4 100 km 100 km Prescribed 10 min 20 min
vective and non-convective precipitation at the surface (PRE-
CIP C and PRECIP NC, mmd−1), soil moisture contained in
the first soil metre (SM 1 m, m3m−3), and total cloud fraction
(TCLDFR, %). All values are computed using the annual and
seasonal (boreal winter, DJF; summer, JJA) averages over the
34-year period (1980–2013) after discarding the first year of
the simulation (1979) as spin-up, which is enough to avoid
the effect of initial conditions (García-García et al., 2020).
Thus, we estimated the anomalies of all outputs for each
LSM simulation relative to the multi-model mean (the mean
of CLM4, NOAH, NOAH-MP and NOAH-MP-DV outputs)
for each set of simulations with different resolution (25, 50
and 100 km). Similarly, we estimated the change in the sim-
ulation of all variables between the 100 and 50 km simula-
tions and between the 50 and 25 km simulations for all LSM
configurations. When required, outputs of all WRF experi-
ments were mapped to the grid of the observational refer-
ence employed in this study by selecting the nearest model
grid point. A Student’s ttest considering autocorrelation was
used to identify significant differences between simulations
with different LSMs and horizontal resolutions at the 95 %
confidence level.
Additionally, we evaluate the WRF performance in the
simulation of maximum and minimum air temperature and
accumulated precipitation against the Climatic Research
Unit Time-Series product version 4.03 (CRU; Harris et al.,
2014). The CRU database provides monthly data at a res-
olution of approximately 50 km. Previous studies have re-
ported inconsistencies between different observational prod-
ucts, particularly important for the evaluation of model sim-
ulations with different resolutions (e.g., Iles et al., 2020). To
avoid this issue, we included another observational database
in the analysis; the Daily Surface Weather Data version 3
(DAYMET; Thornton et al., 2016), with daily data at approx-
imately 1 km resolution over North America. This allows for
the comparison of uncertainties associated with the choice of
Figure 1. Subregions employed for the bias analysis, adapted from
Giorgi and Francisco (2000): Central America, CAM; western
North America, WNA; central North America, CNA; eastern North
America, ENA; Alaska, ALA; and Greenland, GRL.
the observational product and the uncertainties arising from
the model configuration. We calculated annual and seasonal
WRF and DAYMET biases in these variables relative to the
CRU data for the analysis period averaged over six subre-
gions due to the large climate differences over North Amer-
ica. These six subregions cover Central and North Amer-
ica (NA) and are adapted from Giorgi and Francisco (2000):
Central America, CAM; western North America, WNA; cen-
tral North America, CNA; eastern North America, ENA;
Alaska, ALA; and Greenland, GRL (Fig. 1). The impact of
horizontal resolution is expected to be larger on the simula-
tion of extreme events than on surface climatologies (Prein
et al., 2013; Di Luca et al., 2015; Rummukainen, 2016). We
examined this by calculating the bias in the 95th percentile of
maximum and minimum temperatures and accumulated pre-
cipitation within all experiments using the DAYMET product
as reference.
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A. García-García et al.: WRF sensitivity to horizontal resolution and LSM changes 417
4 Results
4.1 LSM influences on surface energy fluxes and
near-surface conditions
The net radiation absorbed by the ground surface enhances
turbulent (latent and sensible) fluxes at the surface and/or
warms the soil surface, which leads to an increase in the
emitted longwave radiation (Bonan, 2002). The relationship
between these variables is shown by their corresponding en-
semble mean of LSM simulations, indicating similar lati-
tudinal patterns in net radiation, turbulent fluxes and near-
surface temperatures with higher fluxes and temperatures at
lower latitudes (see for example Fig. 2 for the LSM ensem-
ble mean of the 50 km experiments). The net radiation results
from adding net shortwave and longwave radiations, whose
mean values have similar spatial distributions but with op-
posite sign (Fig. 2a). This indicates that more shortwave ra-
diation reaches the land surface than is reflected due to sur-
face albedo, while the radiation emitted from the soil due to
its surface temperature, is higher than the longwave radia-
tion reaching the soil surface (Fig. 2a). The energy propor-
tion of net radiation that is propagated through the soil is
much smaller than the rest of surface energy fluxes (Fig. 2b).
Areas with high latent heat flux coincide with areas with
high convective precipitation rates at low and middle lati-
tudes (Fig. 2b and d). The soil moisture map shows high val-
ues southward in the Great Lakes region and low values in
dry areas such as Florida and the southwest USA, in agree-
ment with both convective and non-convective precipitation
(Fig. 2d and e).
The use of a different LSM component in WRF affects
the representation of soil and vegetation properties and pro-
cesses in the simulation, resulting in noticeable differences
in the simulated energy fluxes across the domain (Fig. 3).
For instance, the spatial pattern of the LSM anomalies rel-
ative to the multi-model mean in longwave net radiation is
similar to the minimum temperature anomalies (Figs. 3b and
4b), and the anomalies in latent heat flux show similar LSM
differences to the convective precipitation maps at low lati-
tudes (Figs. 3d and 5a). The spatial patter of the LSM anoma-
lies in sensible and latent heat fluxes shows opposite val-
ues around the mean. For example over the boreal forest,
the LSMs reaching the highest values of latent heat flux also
reach the lowest values of sensible heat flux at the same lo-
cations (Fig. 3d and f).
LSM differences in the simulation of surface fluxes and
near-surface conditions are similar among the experiments
with different resolutions (Figs. 3–5 and S2, S4 and S6 in the
Supplement). For example, based on the differences between
each LSM simulation with 50 km resolution and the 50 km
multi-model mean (Fig. 2), we can identify the CLM4 as the
LSM component simulating the highest net shortwave radia-
tion over most of North America for the annual, DJF and JJA
means (SNET in Figs. 3a and S1 in the Supplement). Mean-
Figure 2. Ensemble mean of the LSM simulations for the sur-
face energy fluxes and near-surface conditions: net shortwave radia-
tion (SNET), net longwave radiation (LNET), surface net radiation
(RNET) (a); latent heat flux (LH), sensible heat flux (HFX), ground
heat flux (GHF) (b); maximum temperature (TASMAX), minimum
temperature (TASMIN), surface air temperature (SAT), soil tem-
perature at 1 m depth (GST 1 m) (c); accumulated convective and
non-convective precipitation at the surface (PRECIP C and PRECIP
NC) (d); soil moisture contained in the first soil metre (SM 1 m) (e);
and total cloud cover fraction (TCLDFR) (f) for the WRF ensem-
ble mean. GHF results are also represented using its own colour
scale (g). Mean values are estimated as the temporal average for the
period 1980–2013 using simulations performed with 50 km resolu-
tion.
while, the NOAH-MP-DV simulation reaches the lowest net
shortwave radiation over the same areas (Fig. 3a). The WRF
simulation of net longwave radiation reaches negative values
(Fig. 2a) with the maximum values simulated by the NOAH
LSM and the minimum values simulated by the CLM4 LSM
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418 A. García-García et al.: WRF sensitivity to horizontal resolution and LSM changes
Figure 3. Anomalies of energy fluxes at the surface: (a) net short-
wave radiation (SNET), (b) net longwave radiation (LNET), (c) soil
net radiation (RNET), (d) latent heat flux (LH), (f) sensible heat flux
(HFX) and (g) ground heat flux (GHF) for each LSM simulation
relative to the LSM ensemble mean. Mean values are estimated as
the temporal average for the period 1980–2013 using simulations
performed with 50 km resolution. Grid cells with a non-significant
change at the 5 % significance level are masked in grey.
(Fig. 3b). The upward (negative) component of the net long-
wave radiation results from the Stefan–Boltzmann equation,
from which the outgoing longwave radiation LW ↑is propor-
tional to σ T 4
s, where Tsis surface temperature and σis the
Stefan–Boltzmann constant. Thus, the CLM4 simulation pro-
duces the largest outgoing longwave radiation (see Fig. S7
in the Supplement), shown in Fig. 3b by the largest nega-
tive anomalies and therefore the highest air and soil temper-
atures (Fig. 4). The opposite behaviour is performed by the
NOAH LSM, yielding the lowest upward longwave radia-
tion (Figs. 3b and S7), and one of the coldest temperature
climatologies relative to the multi-model mean (Fig. 4). The
relationship between the radiation and temperature anoma-
Figure 4. Anomalies of near-surface temperature conditions: (a)
daily maximum temperature (TASMAX), (b) daily minimum tem-
perature (TASMIN), (c) surface air temperature (SAT) and (d) soil
temperature at 1 m depth (GST 1 m) for each LSM simulation rel-
ative to the LSM ensemble mean. Mean values are estimated as
the temporal average for the period 1980–2013 using simulations
performed with 50 km resolution. Grid cells with a non-significant
change at the 5 % significance level are masked in grey.
lies is also supported by high spatial correlation coefficients
(Table S1 in the Supplement). These correlation coefficients
show the link of maximum temperatures to both shortwave
and longwave net radiation, particularly in summer, while
minimum temperatures show higher correlation with long-
wave net radiation than with shortwave net radiations in most
of the LSM simulations (Table S1).
The simulation of sensible heat flux reaches the highest
values using the CLM4 configuration over the boreal for-
est and the lowest values in western USA. Meanwhile, the
NOAH simulation reaches the lowest sensible heat fluxes
over the boreal forest and the highest values in western USA
(Fig. 3e). The spatial patterns of LSM anomalies in sensi-
ble heat flux are similar to the LSM anomalies in net short-
wave radiation and daily maximum temperatures (Figs. 3a
and 4a), which is also shown by high spatial correlation coef-
ficients, particularly in summer (Table S1). LSM differences
in ground heat flux are smaller than for the rest of the en-
ergy fluxes due to the small magnitude of the GHF in com-
parison with the rest of energy components (Fig. 2g). The
NOAH LSM reaches the lowest ground heat flux values for
the annual mean in most of the domain, showing nonethe-
less the highest ground heat flux values in summer at high
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A. García-García et al.: WRF sensitivity to horizontal resolution and LSM changes 419
Figure 5. Anomalies of near-surface humid conditions: (a) accumu-
lated convective and (b) non-convective precipitation at the surface
(PRECIP C and PRECIP NC), (c) soil moisture contained in the
first soil metre (SM 1 m), and (d) total cloud fraction (TCLDFR)
for each LSM simulation relative to the LSM ensemble mean. Mean
values are estimated as the temporal average for the period 1980–
2013 using simulations performed with 50 km resolution. Grid cells
with a non-significant change at the 5 % significance level are
masked in grey.
latitudes (Figs. 3f and S1). The spatial pattern of LSM dif-
ferences in ground heat flux differ from the soil temperature
results, whose spatial correlation coefficients are higher with
the longwave net radiation mainly in summer. LSM differ-
ences are larger for the simulation of soil temperatures than
for the simulation of air temperatures particularly at high lati-
tudes in summer where LSM differs largely in the simulation
of shortwave net radiation probably due to different estimates
of surface albedo under different land cover and soil moisture
values (Figs. 2a, 4c and d, 5c, and S3 in the Supplement).
The CLM4 simulation produces the highest latent heat
flux values and convective precipitation rates, particularly
over southwestern NA, while the NOAH simulation provides
the lowest latent heat flux and convective precipitation val-
ues over the same areas (Figs. 3d and 5a). LSM differences
in latent heat flux, convective and non-convective precipita-
tion are larger in summer (Figs. S1 and S5 in the Supple-
ment). LSM differences in JJA convective precipitation rates
are particularly large at low latitudes, where the CLM4 LSM
produces high latent heat flux over the western part of the
domain and low latent heat flux over the eastern NA rela-
tive to the multi-model mean (Figs. S1 and S5). These differ-
ences between the east and west in the CLM4 simulation of
latent heat flux are not reflected in the values of convective
precipitation rates, hence the low spatial correlation coeffi-
cients between both variables (Table S2 in the Supplement).
There are also LSM differences in the non-convective term
of precipitation, with larger anomalies in summer than in
winter (Figs. 5b and S5). Thus, the NOAH LSM produces
the highest precipitation anomaly at mid-latitudes, where the
same LSM produces high values of total cloud fraction rela-
tive to the multi-model mean (Fig. 5b and d). This relation-
ship between non-convective precipitation and cloud cover
is also shown by high spatial correlation coefficients (Ta-
ble S2). There are large LSM differences in the simulation
of soil moisture, with the CLM4 LSM generating the driest
conditions and the NOAH-MP experiments the wettest soils
(Figs. 5c and S5). Although the LSM differences are large in
the representation of humid conditions, the relationship be-
tween precipitation, latent heat flux, soil moisture and cloud
fraction is weaker than the relationship between radiation and
temperatures in the WRF experiments.
Larger LSM differences in the simulation of shortwave
and longwave radiations and temperatures are found over
very vegetated areas such as the boreal forest and eastern
USA (Figs. 3 and 4). The comparison of the NOAH-MP
experiments with prescribed and dynamic vegetation also
shows larger differences in air temperatures over these areas.
This suggests that the different representation of vegetation
in each LSM yields to different estimates of soil properties,
such as surface albedo, evaporative resistance and aerody-
namic roughness, affecting the simulation of radiation and
temperatures. The LSM differences in latent heat flux and
convective precipitation are larger at low latitudes, with the
NOAH LSM yielding the most different values relative to the
rest of LSMs. This can be associated with the issues identi-
fied in the NOAH LSM to simulate soil hydrology (Wharton
et al., 2013).
4.2 Resolution impact on surface energy fluxes and
near-surface conditions
The response of surface energy fluxes and near-surface con-
ditions to changes in spatial resolution varies considerably
with the season, while they behave similarly using different
LSM components (Figs. 6 and S8–S13 in the Supplement).
We consider the results of the NOAH-MP-DV experiments
as an example to minimize the number of figures in the pa-
per. Changes in resolution alter the surface energy fluxes in
DJF mainly over regions of complex topography and coastal
areas, while in JJA the simulation of energy fluxes is affected
by resolution over the whole domain except over a region in
the central USA and northern areas of Hudson Bay (Fig. 6).
In JJA, the use of coarser horizontal resolutions induces a
decrease in the net radiation absorbed by soil at high lati-
https://doi.org/10.5194/gmd-15-413-2022 Geosci. Model Dev., 15, 413–428, 2022
420 A. García-García et al.: WRF sensitivity to horizontal resolution and LSM changes
Figure 6. Seasonal mean difference in surface energy fluxes be-
tween the 100 and 50 km simulations (left) and between the 50
and 25 km simulations (right). All outputs are from the NOAH-MP-
DV simulations for the period 1980–2013. Grid cells with a non-
significant change at the 5 % significance level are masked in grey.
All outputs from the 25, 50 and 100 km simulations were mapped
to a common grid (CRU grid) using the nearest model grid point.
tudes, mainly caused by a decrease in net shortwave radia-
tion (Fig. 6a and c). The decrease in net radiation induced by
coarser resolutions limits the energy available for turbulent
energy fluxes at high latitudes. Thus, values of latent and sen-
sible heat fluxes also decrease at coarser resolutions at high
latitudes (Fig. 6d and e). The use of coarser resolutions also
induces higher sensible heat fluxes at low latitudes, which is
balanced by lower latent heat flux (Fig. 6d and e).
Changes in downward shortwave radiation at the surface
are mainly driven by changes in cloud cover, but changes in
atmospheric water vapour and aerosols may also affect the
shortwave radiation reaching the ground surface (Hatzianas-
tassiou et al., 2005). Changes in surface albedo also lead to
Figure 7. Seasonal mean difference in near-surface temperature
conditions between the 100 and 50 km simulations (left) and be-
tween the 50 and 25 km simulations (right). All outputs are from
the NOAH-MP-DV simulations for the period 1980–2013. Grid
cells with a non-significant change at the 5 % significance level are
masked in grey. All outputs from the 25, 50 and 100 km simulations
were mapped to a common grid (CRU grid) using the nearest model
grid point.
changes in the upward component of shortwave radiation,
thus affecting SNET. The resolution differences in estimat-
ing albedo and land cover in our results are smaller than those
associated with the cloud cover and the microphysics of the
model, particularly in JJA. Thus, the effect of resolution on
the downward component of shortwave radiation, which is
dependent on cloud formation and atmospheric composition,
is larger than the resolution effect on the upward component
of shortwave radiation, which is dependent on albedo val-
ues (Fig. S14 in the Supplement). The resolution changes in
winter SNET at southern latitudes of the Rocky Mountains
that are not related to cloud cover seem to be associated with
the upward component of shortwave radiation and therefore
with the resolution effect on surface albedo values (Figs. 6a,
8d and S14).
Consistent with the effect of LSM differences on near-
surface conditions (Sect. 4.1), the spatial pattern of the res-
olution impact on net shortwave radiation is similar to the
resolution-induced changes in daily maximum temperatures
(Figs. 6a and 7a). The response of minimum temperature to
changing resolution is, however, smaller than for maximum
temperatures at middle–high latitudes (Fig. 7b). Over eastern
Geosci. Model Dev., 15, 413–428, 2022 https://doi.org/10.5194/gmd-15-413-2022
A. García-García et al.: WRF sensitivity to horizontal resolution and LSM changes 421
Figure 8. Seasonal mean difference in near-surface humid condi-
tions between the 100 and 50 km simulations (left) and between the
50 and 25 km simulations (right). All outputs are from the NOAH-
MP-DV simulations for the period 1980–2013. Grid cells with a
non-significant change at the 5 % significance level are masked in
grey. All outputs from the 25, 50 and 100km simulations were
mapped to a common grid (CRU grid) using the nearest model grid
point.
North America, JJA minimum temperature increases with the
use of coarser resolutions, while it decreases over western
North America (Fig. 7b). The response of mean temperature
to resolution is mainly driven by the resolution impact on
maximum temperatures since both show similar spatial pat-
terns (Fig. 7c). Although the impact of resolution on air and
soil temperatures shows similar spatial patterns, in winter air
temperatures are more affected by changes in resolution than
soil temperatures, particularly at high latitudes and elevation
where snow may be present (Fig. 7c and d). Thus, soil tem-
peratures are more sensible to JJA changes in the energy bud-
get induced by reducing resolution, while in DJF soil temper-
ature remains insulated from resolution-induced changes in
surface conditions probably because of the insulating effect
of snow cover (García-García et al., 2019).
Non-convective precipitation increases with the use of
coarser horizontal resolutions over the Rocky Mountains,
particularly in winter, where the model also represents a
higher percentage of cloud cover with coarser resolutions
(Fig. 8b and d). Over the east coast of the USA, the use of
coarser resolutions leads to lower non-convective precipita-
tion rates (Fig. 8b). This behaviour is also present in JJA
over the arctic areas of our domain (Fig. 8b). Although the
response of convective precipitation to resolution in winter
is not significant, in JJA the use of coarser horizontal res-
olutions yields a decrease in convective precipitation over
coastal areas and the Rocky Mountains, where the simulation
also reaches lower latent heat flux values (Figs. 6d and 8a).
Although the spatial pattern of soil moisture is very patchy in
DJF and JJA, soil moisture tends to decrease at low latitudes
in JJA with the use of coarser resolutions (Fig. 8c). At mid-
latitudes, however, the use of coarser resolutions leads to an
increase in soil moisture during the year at most locations
(Fig. 8c).
In summary, at low NA latitudes the JJA values of the
three variables associated with the surface water balance
(LH, PRECIP and SM 1 m) decrease with the use of coarser
horizontal resolutions, although showing large spatial vari-
ability (Figs. 6d and 8a and c). At middle and high NA lati-
tudes, there are differences in the response of the water bal-
ance variables to the use of coarser resolutions. For exam-
ple, soil moisture increases with coarser resolutions over a
large area at mid-latitudes, while convective precipitation in-
creases just over a few grid cells in central NA, decreasing
over most coastal areas (Fig. 8a and c). Latent heat flux de-
creases with the use of coarser resolutions over most regions
at high and middle latitudes, particularly over coastal areas
(Fig. 6d).
4.3 Comparison of temperature and precipitation
against observations
For the comparison of the effect of LSM and horizontal reso-
lution changes on climate simulations, we estimate the bias in
all WRF simulations relative to the CRU observational prod-
uct (Harris et al., 2014). As a measure of the possible uncer-
tainties in observational databases, we also estimate the bias
in the DAYMET product relative to the CRU data. The in-
consistencies between both observational data are noticeably
smaller than the biases in the WRF experiments for all vari-
ables in all regions, except for minimum temperatures in the
CAM region and for precipitation in the ALA region (Fig. 9,
see a representation of the regions in Fig. 1).
The WRF model underestimates annual and seasonal
means of daily maximum temperatures over most of North
America at all resolutions, compared grid cell by grid cell
(Fig. S15 in the Supplement) and on average over subdo-
mains (Fig. 9a). These biases are generally less pronounced
for the experiments using the CLM4 LSM at most loca-
tions and in all seasons. The impact of horizontal resolution
on these values is weaker than the LSM dependence over
each domain, showing a greater effect of resolution on max-
imum temperatures in summer than in winter over western
North America and at high latitudes (WNA, ALA and GRL
in Fig. 9a). Over these areas, finer horizontal resolutions are
https://doi.org/10.5194/gmd-15-413-2022 Geosci. Model Dev., 15, 413–428, 2022
422 A. García-García et al.: WRF sensitivity to horizontal resolution and LSM changes
Figure 9. Regional mean annual and seasonal biases in maximum and minimum temperatures (◦C) and in accumulated precipitation
(mmd−1) for all experiments and the DAYMET data product relative to the CRU database from 1980 to 2013. Biases are estimated av-
eraging over six subregions (Fig. 1) adapted from Giorgi and Francisco (2000): Central America, CAM; western North America, WNA;
central North America, CNA; eastern North America, ENA; Alaska, ALA; and Greenland, GRL.
associated with warmer JJA maximum temperatures, reduc-
ing the bias relative to the CRU dataset at middle latitudes
(Figs. 7a and 9a). In the ALA and GRL regions, the WRF
model with the CLM4 and the NOAH-MP LSM compo-
nents overestimates JJA maximum temperatures, increasing
the bias in these simulations with the use of finer resolutions
(Fig. 9a). The WRF bias in maximum temperatures in win-
ter is greatly improved over the boreal forest and the Rocky
Mountains areas by using the CLM4 as LSM (Fig. S15).
Over the same areas the CLM4 simulated very high values
of shortwave net radiation and sensible heat flux in compar-
ison with the rest of the land surface models (Fig. 3a and
e), which may be related to the CLM4 albedo estimate. De-
spite the WRF underestimation of mean maximum temper-
ature, extreme maximum temperatures are overestimated by
the WRF model, particularly at high latitudes and using the
CLM4 LSM (Fig. 10a). As expected based on the litera-
ture, the resolution effect on the bias in extreme maximum
temperatures is larger than on the bias in mean maximum
temperatures; however LSM differences are still larger than
resolution-induced changes.
The performance of the WRF model in reproducing
daily minimum temperatures from the CRU observations is
slightly better than reproducing maximum temperatures at
middle and low latitudes, but it is worse at high latitudes par-
ticularly in DJF (Fig. 9b). Experiments using the CLM4 LSM
yield a warmer climatology over most areas and for all sea-
sons than the experiments with the other LSM components,
implying smaller biases in the CLM4 simulations for most of
the regions (Fig. 9b). The WRF bias in minimum temperature
is large in winter over the central and eastern areas of North
America and at middle and high latitudes (subdomains ALA,
GRL, CNA and ENA in Fig. 9b). The resolution impact on
these results is again weaker than the effect of the LSM com-
ponent. In summer, the WRF-NOAH experiments show a
large negative bias in minimum temperatures over the NA
southeastern coast (Fig. S16 in the Supplement), areas where
the same experiments also shown high values of longwave
net radiation and low values of sensible heat flux (Fig. 3b and
e). The simulation of extreme minimum temperatures is also
overestimated for all experiments and regions except for the
CAM region in summer, showing particularly large biases in
winter (Fig. 10b). Thus, although the WRF model underes-
timates mean maximum and minimum temperatures, it over-
estimates the intensity of hot extremes associated with min-
imum and maximum temperatures. The effect of dynamic
vegetation (NOAH-MP vs. NOAH-MP-DV) on the biases in
extreme and mean maximum and minimum temperatures re-
mains constant using different resolutions, reaching larger bi-
ases and colder maximum and minimum temperatures with
dynamic vegetation than with prescribed vegetation for most
of the regions (Fig. 9a and b).
Geosci. Model Dev., 15, 413–428, 2022 https://doi.org/10.5194/gmd-15-413-2022
A. García-García et al.: WRF sensitivity to horizontal resolution and LSM changes 423
Figure 10. Regional mean annual and seasonal biases in extreme maximum and minimum temperatures (◦C) and in extreme precipitation
(mmd−1) for all experiments and the DAYMET data product relative to the CRU database from 1980 to 2013. Extremes are calculated as
the 95th percentile of the annual and seasonal temporal series at each grid cell. Biases are estimated averaging over six subregions (Fig. 1)
adapted from Giorgi and Francisco (2000): Central America, CAM; western North America, WNA; central North America, CNA; eastern
North America, ENA; Alaska, ALA; and Greenland, GRL.
The WRF model simulates large positive biases in daily
accumulated precipitation at the surface over most of North
America during all seasons, with larger biases in summer
(Figs. 9c and S17 in the Supplement). A negative bias is
also present in all experiments over the southeastern USA
and the eastern coast of North America in summer and win-
ter (Fig. S17). Dry biases are reduced when using finer hor-
izontal resolutions, while wet biases are larger when using
smaller scales (Fig. 9c). This is due to the intensification of
the water cycle with the use of finer horizontal resolutions
discussed in Sect. 4.2 and presented in Figs. 6d and 8. For ex-
ample in winter, the dry bias shown in all experiments over
the southeastern NA is associated with an increase in non-
convective precipitation using finer resolutions (Figs. S17
and 8b). In summer, the bias in precipitation is larger us-
ing finer resolutions over most of coastal areas where an in-
crease in convective precipitation and latent heat flux was
shown with the use of finer resolutions (Figs. 6d, 8a and
S17). The impact of resolution on the accumulated precip-
itation is stronger than the effect of the LSM component,
which affects precipitation mainly in summer (Fig. 9). The
results show a larger bias in extreme precipitation than for
the mean accumulated precipitation but yielding similar con-
clusions (Fig. 10).
In summary, the LSM impact on temperatures is larger
than the resolution effect, while the opposite is true for pre-
cipitation climatologies; i.e., differences in precipitation aris-
ing from changes in resolution are larger than LSM differ-
ences (Fig. 9). The influence of both the LSM choice and
resolution intensifies in summer compared with the rest of
seasons probably because of the larger energy exchanges and
the consequent intensification of land–atmosphere coupling
in summer (Zhang et al., 2008; Mei and Wang, 2012). The
CLM4 LSM generates the smallest biases relative to the CRU
database in the WRF simulation of mean maximum and min-
imum temperatures; however it also yields the larger biases
in extreme maximum and minimum temperatures. The use
of finer resolutions leads to slightly larger or smaller biases
in the simulation of maximum and minimum temperatures
depending on the LSM component and the region, while the
use of finer resolutions implies larger biases in mean and ex-
treme precipitation at low and middle latitudes for all LSM
components, particularly in summer.
5 Discussion
The dependence of climate simulations on the LSM com-
ponent shown in this study agrees with conclusions drawn
from previous analyses at different temporal and spatial
https://doi.org/10.5194/gmd-15-413-2022 Geosci. Model Dev., 15, 413–428, 2022
424 A. García-García et al.: WRF sensitivity to horizontal resolution and LSM changes
scales (Chen et al., 2014; Van Den Broeke et al., 2018; Liu
et al., 2019; Zhuo et al., 2019; Davin and Seneviratne, 2012;
Mooney et al., 2013; Laguë et al., 2019; García-García et al.,
2020). For example, using the Consortium for Small-scale
Modeling (COSMO) and WRF RCMs, Davin and Senevi-
ratne (2012) and Mooney et al. (2013) identified an LSM
sensitivity of temperature and precipitation conditions over
Europe which intensifies in summer. Additionally, our anal-
ysis has shown that the impact of the LSM choice on the
WRF simulation of precipitation is weaker than its impact
on temperature, in agreement with studies over a small re-
gion in Italy (Zhuo et al., 2019), over Europe (Mooney et al.,
2013), and over the western and central USA at seasonal
scales (Jin et al., 2010; Chen et al., 2014; Van Den Broeke
et al., 2018). The implementation and calculation of surface
properties (albedo, surface roughness and evaporative resis-
tances) by each LSM can be the cause of the LSM differences
in the simulation of energy fluxes (Laguë et al., 2019). Thus,
LSM differences in SNET are probably related to albedo val-
ues within each LSM. The large LSM differences in sensible
heat flux over the boreal forest are likely related to the LSM
estimates of surface roughness, while the large latent heat
flux differences at low latitudes are probably associated with
different estimates of evaporative resistances and the treat-
ment of soil water in each LSM.
The great WRF sensibility to precipitation rates to resolu-
tion is also supported by the literature (e.g., Pieri et al., 2015).
Our results also show large seasonal differences, mainly
caused by the different contribution of convective precipi-
tation in summer and winter. In summer at middle and low
latitudes, the use of finer grid cells leads to a change in the en-
ergy partition into sensible and latent heat flux, increasing la-
tent heat, and decreasing sensible heat (Fig. 6). This increase
in latent heat flux over these areas is probably the cause of
the higher values of convective precipitation (Fig. 8a). This
resolution-induced increase in precipitation through changes
in convective processes has also been suggested in the litera-
ture (Prein et al., 2016). At high latitudes both turbulent heat
fluxes increase in summer with the use of finer resolutions
mainly due to the increase in shortwave net radiation proba-
bly related to the decrease in cloud cover shown in Fig. 8d.
These changes in cloud cover with resolution may be caused
by the performance of the microphysical parameterizations
at different resolutions and the improvement in the represen-
tation of orography (Pieri et al., 2015; Prein et al., 2016).
Previous evaluations of RCMs using several soil models
over different domains reached the conclusion that the most
complex LSM components – that is, the LSM components
representing more physical phenomena – outperform others
(Chen et al., 2014; Van Den Broeke et al., 2018; Liu et al.,
2019). Over North America, our results indicate that the
WRF simulation of temperature conditions using the CLM4
LSM outperforms the simulation of mean maximum and
minimum temperatures generated by the NOAH and NOAH-
MP LSMs, but it yields larger biases in extreme maximum
and minimum temperatures (Figs. 9 and 10). The simulation
of precipitation in summer is, however, slightly better repre-
sented by the NOAH LSM than by the other LSM compo-
nents (Fig. 9). Nonetheless, the comparison of all WRF ex-
periments with observations shows overestimated values of
precipitation over most of North America, which is in agree-
ment with other studies using WRF over the western USA
(Jin et al., 2010; Chen et al., 2014) and over Europe (Pieri
et al., 2015). Atmospheric parameterizations were not tested
in our study; however, other WRF sensitivity experiments us-
ing several microphysics schemes over Europe found a posi-
tive bias in precipitation for all simulations, which was con-
siderably reduced in summer within a convective-permitting
simulation (Pieri et al., 2015); that is, the positive bias in pre-
cipitation has been reported in WRF simulations over dif-
ferent domains using several LSM components, horizontal
resolutions, microphysics parameterizations and reanalysis
products as initial and boundary conditions (Figs. 9 in this
paper, Pieri et al., 2015; Chen et al., 2014; Jin et al., 2010).
Therefore, the results included here, together with the results
reported in the literature, suggest that the use of finer res-
olutions may raise precipitation biases in WRF simulations
over North America, but the implementation of convective-
permitting processes and other atmospheric parameteriza-
tions could reduce this bias.
6 Conclusions
This study has shown the effect of changes in horizontal res-
olution and LSM choice on the simulation of energy fluxes
at the surface and temperature and water conditions near the
surface. The effect of both model choices intensifies in sum-
mer due to the increase in energy and water exchanges be-
tween the lower atmosphere and the land surface. Enhancing
horizontal resolution leads to higher precipitation climatolo-
gies for all LSMs over coastal areas at low latitudes mainly
due to an increase in convective precipitation also associated
with an increase in latent heat flux. Our results highlight the
important role of the LSM choice in the WRF representa-
tion of the energy partition at the surface, which mainly af-
fects the simulation of near-surface temperatures over North
America. Additionally, these results demonstrate the impact
of the LSM choice on simulated atmospheric conditions,
showing LSM-dependent differences in the simulated cloud
fraction and non-convective precipitation rates. This is prob-
ably associated with the land–atmospheric coupled character
of our simulations and the interactions between small- and
large-scale dynamical processes.
The evaluation of the WRF simulations against observa-
tions supports the use of the CLM4 LSM as the best choice
within the evaluated options for WRF simulations over North
America, although it may overestimate temperature extreme
events. The use of finer resolutions yields a small improve-
ment in the representation of minimum temperatures within
Geosci. Model Dev., 15, 413–428, 2022 https://doi.org/10.5194/gmd-15-413-2022
A. García-García et al.: WRF sensitivity to horizontal resolution and LSM changes 425
WRF at middle and high latitudes. Nonetheless, the use of
finer resolutions should be implemented with caution since
it may increase the WRF bias in mean and extreme pre-
cipitation. Further sensitivity experiments using other atmo-
spheric parameterizations and other resolutions fine enough
for convective-permitting processes (<5 km) or for altering
the hydrostatic balance of the model (≈10 km) are necessary
to determine the best WRF configuration for downscaling cli-
mate simulations over North America for paleoclimate and
climate change studies. However, the large computational re-
sources required to perform a sensitivity analysis including
convective-permitting processes would require a reduction in
the area of interest or in the length of the simulation.
Information provided by downscaling studies is used for
building climate change policies through the information col-
lected in assessment reports (IPCC, 2013; Mbow et al., 2017;
USGCRP, 2018). Thus, sensitivity studies like the one pre-
sented here are crucial to understand and ultimately restrict
uncertainties in climate simulations with direct benefits to
society and environment. Particularly, these results should
be considered for downscaling studies over North America
aimed at projecting future or past conditions and informing
policymakers.
Code and data availability. As described in Sect. 2, here we
used the Research and Forecasting model (WRF, version 3.9,
http://www.wrf-model.org, last access: 12 January 2022, Ska-
marock et al., 2008). The outputs of all simulations to-
gether with the code used to estimate the presented re-
sults are available at https://doi.org/10.5281/zenodo.5106087
(García-García et al., 2021). The NARR product (Mesinger
et al., 2006) was obtained from https://www.ncei.noaa.gov/data/
north-american-regional-reanalysis/access/3-hourly/ (last access:
12 January 2022). The CRU TS4.03 database can be downloaded
from the University of East Anglia web page (https://doi.org/
10.5285/10d3e3640f004c578403419aac167d82, University of East
Anglia Climatic Research Unit et al., 2020). The DAYMET V3
database (Thornton et al., 2016) is available at https://doi.org/10.
3334/ORNLDAAC/1328.
Supplement. The supplement related to this article is available on-
line at: https://doi.org/10.5194/gmd-15-413-2022-supplement.
Author contributions. AGG designed the modelling experiment,
performed the simulations and analyzed model outputs. All authors
(AGG, FJCV, HB, JFGR and EGB) contributed to the interpretation
and discussion of results. AGG wrote the manuscript with continu-
ous feedback from FJCV, HB, JFGR and EGB.
Competing interests. The contact author has declared that neither
they nor their co-authors have any competing interests.
Disclaimer. Publisher’s note: Copernicus Publications remains
neutral with regard to jurisdictional claims in published maps and
institutional affiliations.
Acknowledgements. We thank the Mesoscale and Microscale Me-
teorology (MMM), the National Center for Atmospheric Re-
search (NCAR), the National Oceanic and Atmospheric Admin-
istration (NOAA), the Climatic Research Unit (CRU) at the
University of East Anglia and the Oak Ridge National Lab-
oratory Distributed Active Archive Center (ORNL DAAC) for
making the WRF code and the NARR, CRU and DAYMET
datasets available. This analysis contributes to the PALEOLINK
project (http://www.pastglobalchanges.org/science/wg/2k-network/
projects/paleolink/intro, last access: 4 May 2021), part of the
PAGES 2k network. All WRF simulations were performed in the
computational facilities provided by the Atlantic Computational Ex-
cellence Network (ACENET-Compute Canada). During the elabo-
ration of this analysis, Almudena García-García and Francisco José
Cuesta-Valero were partially funded by Hugo Beltrami’s Canada
Research Chair program, the School of Graduate Students at Memo-
rial University of Newfoundland and the Research Office at St.
Francis Xavier University. Francisco José Cuesta-Valero is also
funded by the Alexander von Humboldt Foundation.
Financial support. This research has been supported by the Cana-
dian Network for Research and Innovation in Machining Technol-
ogy, Natural Sciences and Engineering Research Council of Canada
(grant no. DG 140576948), the Canada Excellence Research Chairs,
Government of Canada (grant no. 230687), and the Canada Foun-
dation for Innovation (CFI).
Review statement. This paper was edited by David Lawrence and
reviewed by two anonymous referees.
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