<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing with OASIS Tables v3.0 20080202//EN" "journalpub-oasis3.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" dtd-version="3.0">
  <front>
    <journal-meta>
<journal-id journal-id-type="publisher">GMD</journal-id>
<journal-title-group>
<journal-title>Geoscientific Model Development</journal-title>
<abbrev-journal-title abbrev-type="publisher">GMD</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Geosci. Model Dev.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1991-9603</issn>
<publisher><publisher-name>Copernicus Publications</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>

    <article-meta>
      <article-id pub-id-type="doi">10.5194/gmd-10-223-2017</article-id><title-group><article-title>Reinitialised versus continuous regional climate simulations
using ALARO-0 coupled to the land surface model SURFEXv5</article-title>
      </title-group><?xmltex \runningtitle{Reinitialised versus continuous regional climate simulations}?><?xmltex \runningauthor{J.~Berckmans et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Berckmans</surname><given-names>Julie</given-names></name>
          <email>julie.berckmans@meteo.be</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Giot</surname><given-names>Olivier</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff3">
          <name><surname>De Troch</surname><given-names>Rozemien</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff3">
          <name><surname>Hamdi</surname><given-names>Rafiq</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Ceulemans</surname><given-names>Reinhart</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff3">
          <name><surname>Termonia</surname><given-names>Piet</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Royal Meteorological Institute, Brussels, Belgium</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Centre of Excellence PLECO (Plant and Vegetation Ecology), Department of Biology, <?xmltex \hack{\break}?>University of Antwerp, Antwerp, Belgium</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Physics and Astronomy, Ghent University, Ghent, Belgium</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Julie Berckmans (julie.berckmans@meteo.be)</corresp></author-notes><pub-date><day>16</day><month>January</month><year>2017</year></pub-date>
      
      <volume>10</volume>
      <issue>1</issue>
      <fpage>223</fpage><lpage>238</lpage>
      <history>
        <date date-type="received"><day>17</day><month>June</month><year>2016</year></date>
           <date date-type="rev-request"><day>9</day><month>August</month><year>2016</year></date>
           <date date-type="rev-recd"><day>22</day><month>December</month><year>2016</year></date>
           <date date-type="accepted"><day>23</day><month>December</month><year>2016</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under a Creative Commons Attribution 3.0 Unported License. To view a copy of this license, visit <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by/3.0/">http://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://gmd.copernicus.org/articles/10/223/2017/gmd-10-223-2017.html">This article is available from https://gmd.copernicus.org/articles/10/223/2017/gmd-10-223-2017.html</self-uri>
<self-uri xlink:href="https://gmd.copernicus.org/articles/10/223/2017/gmd-10-223-2017.pdf">The full text article is available as a PDF file from https://gmd.copernicus.org/articles/10/223/2017/gmd-10-223-2017.pdf</self-uri>


      <abstract>
    <p>Dynamical downscaling in a continuous approach using initial and boundary
conditions from a reanalysis or a global climate model is a common method for
simulating the regional climate. The simulation potential can be improved by
applying an alternative approach of reinitialising the atmosphere, combined
with either a daily reinitialised or a continuous land surface. We evaluated
the dependence of the simulation potential on the running mode of the
regional climate model ALARO coupled to the land surface model
Météo-France SURFace EXternalisée (SURFEX), and driven by the
ERA-Interim reanalysis. Three types of downscaling simulations were carried
out for a 10-year period from 1991 to 2000, over a western European domain at
20 km horizontal resolution: (1) a continuous simulation of both the
atmosphere and the land surface, (2) a simulation with daily
reinitialisations for both the atmosphere and the land surface and (3) a
simulation with daily reinitialisations of the atmosphere while the land
surface is kept continuous. The results showed that the daily
reinitialisation of the atmosphere improved the simulation of the 2 m
temperature for all seasons. It revealed a neutral impact on the daily
precipitation totals during winter, but the results were improved for the
summer when the land surface was kept continuous. The behaviour of the three
model configurations varied among different climatic regimes. Their seasonal
cycle for the 2 m temperature and daily precipitation totals was very
similar for a Mediterranean climate, but more variable for temperate and
continental climate regimes. Commonly, the summer climate is characterised by
strong interactions between the atmosphere and the land surface. The results
for summer demonstrated that the use of a daily reinitialised atmosphere
improved the representation of the partitioning of the surface energy fluxes.
Therefore, we recommend using the alternative approach of the daily
reinitialisation of the atmosphere for the simulation of the regional
climate.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>The first long-range simulation of the general circulation of the atmosphere
dates back to 1956 <xref ref-type="bibr" rid="bib1.bibx39" id="paren.1"/>. Today it is still the primary tool for
global climate projections. However, due to limited computer resources, the
current horizontal resolution of 100–200 km is still too coarse to resolve
sufficient detail for regional climate projections. Finer spatial resolution
that resolves the land surface heterogeneity can be obtained by nesting a
regional climate model (RCM), over a smaller domain, within a
coarse-resolution global climate model (GCM). This is also referred to as
dynamical downscaling. A GCM or global reanalysis data product provides the
large-scale meteorological and surface fields to the RCM as initial and
lateral boundary conditions. The global features are thus translated into
regional and local conditions over the region of interest <xref ref-type="bibr" rid="bib1.bibx18" id="paren.2"/>.
Hence, RCMs enable climate simulations over a smaller domain with finer-scale
horizontal resolution and with less expensive computational cost than running
a GCM at the same resolution.<?xmltex \hack{\newpage}?></p>
      <p>Since the late 1960s, the numerical weather prediction (NWP) community has
used high-resolution limited area models. The numerical approach was first
used for a regional climate simulation by <xref ref-type="bibr" rid="bib1.bibx13" id="text.3"/>. Their climate
simulation used the NWP model in forecasting mode with 3–5 daily
reinitialisations of the initial conditions. To be able to run them without
these short-term reinitialisations, the regional climate community applied
monthly to multidecadal simulations, with only a single
initialisation of the large-scale fields and
frequent updates of the lateral boundary conditions <xref ref-type="bibr" rid="bib1.bibx19" id="paren.4"/>. These
long-term continuous simulations required improvements in the representation
of physical processes in the RCMs. The continuous simulation is still the
most common in the RCM community <xref ref-type="bibr" rid="bib1.bibx29" id="paren.5"/>. However, by applying the
continuous approach, the simulated large-scale fields deviate from the
driving lateral boundary conditions <xref ref-type="bibr" rid="bib1.bibx46" id="paren.6"/>.</p>
      <p>The accuracy of the dynamical downscaling has improved by using short-term
reinitialisations to reduce systematic errors
<xref ref-type="bibr" rid="bib1.bibx27 bib1.bibx40 bib1.bibx31 bib1.bibx32" id="paren.7"/>. However, only few in the RCM
community adopted this method, mainly because of its higher computational
costs. Most studies <xref ref-type="bibr" rid="bib1.bibx27 bib1.bibx40 bib1.bibx31" id="paren.8"/> dealing with the
evaluation of reinitialised versus continuous climate simulations, examined
only short time periods of 1 month to 1 year. Using a daily
reinitialisation, <xref ref-type="bibr" rid="bib1.bibx27" id="text.9"/> showed improvements in the prediction
of precipitation for a case study of a large flooding event in the Elbe river
catchment in August 2002. Changing the period of reinitialisation, from
monthly to 10 daily, a reduction in systematic errors has been shown for
precipitation when using the 10-day reinitialisation <xref ref-type="bibr" rid="bib1.bibx40" id="paren.10"/>. Even in
a 20-year RCM simulation forced by reanalysis data, the sequence of events
was better preserved by using daily reinitialisations <xref ref-type="bibr" rid="bib1.bibx32" id="paren.11"/>.</p>
      <p>A model approach with short-term reinitialisations demands additional
simulation time at each reinitialisation start. This time is required to
reach dynamical equilibrium between the lateral boundary conditions and the
internal model physics and dynamics <xref ref-type="bibr" rid="bib1.bibx19" id="paren.12"/>. Beyond 24 h small
perturbations in the initial conditions of the atmosphere have only limited
impact on the simulation potential <xref ref-type="bibr" rid="bib1.bibx2" id="paren.13"/>. In contrast to the
atmosphere, the surface takes a longer time to reach dynamical equilibrium
with the overlaying atmosphere, from a few weeks to several seasons,
depending on the depth of the soil layer.</p>
      <p>The surface interacts with the climate through the soil moisture and soil
temperature, by influencing the surface energy budget <xref ref-type="bibr" rid="bib1.bibx19" id="paren.14"/>. The
soil moisture controls the partitioning of the incoming energy into latent
and sensible heat flux. The soil moisture limitation on the
evapotranspiration is largest during summer <xref ref-type="bibr" rid="bib1.bibx44" id="paren.15"/>. The
availability of soil moisture for evapotranspiration is determined by the 2 m
temperature <xref ref-type="bibr" rid="bib1.bibx25" id="paren.16"/>. As the land surface–atmosphere interactions
play a crucial role in the representation of the current and future climate
<xref ref-type="bibr" rid="bib1.bibx44" id="paren.17"/>, it is important to validate the model with
observations. In-site measurements can provide valuable estimates of the
surface energy fluxes. More specifically, FLUXNET establishes a global
network of eddy-covariance towers measuring these fluxes <xref ref-type="bibr" rid="bib1.bibx4" id="paren.18"/>.</p>
      <p>The objective of this study was to evaluate the simulation potential of three
regional climate downscaling approaches with different update frequencies of
the initial conditions: (1) a continuous simulation of both the atmosphere
and the land surface, (2) a simulation with daily reinitialisations for both
the atmosphere and the land surface and (3) a simulation with daily
reinitialisations of the atmosphere while the land surface is kept
continuous. We used the ALARO model to dynamically downscale the
European Centre for Medium-Range Weather Forecasts (ECMWF) Interim
Re-Analysis (ERA-Interim; <xref ref-type="bibr" rid="bib1.bibx12" id="altparen.19"/>). Within this study, ALARO was
coupled to the Météo-France SURFace
EXternalisée land surface model
(SURFEX; <xref ref-type="bibr" rid="bib1.bibx35" id="altparen.20"/>). We evaluated the mean 2 m temperature and mean
daily total precipitation by comparing with the 0.22<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> ECA&amp;D E-OBS
dataset <xref ref-type="bibr" rid="bib1.bibx23" id="paren.21"/>, and the surface energy fluxes by comparing with
the FLUXNET database <xref ref-type="bibr" rid="bib1.bibx4" id="paren.22"/>. The analysis covered a 10-year
period from 1991 to 2000, for a domain encompassing western Europe.</p>
      <p>The models, experimental design and observational datasets are described in
Sect. 2. The results for the mean surface parameters are covered in Sect. 3.
Section 4 demonstrates the results with respect to the surface energy
budget. Finally, conclusions are given in Sect. 5.</p>
</sec>
<sec id="Ch1.S2">
  <title>Model and experimental design</title>
<sec id="Ch1.S2.SS1">
  <title>Model definition</title>
      <p>The regional climate model used in this study is the ALARO model version 0
(ALARO-0), a configuration of the Aire Limitée Adaptation Dynamique
Développement International (ALADIN) model with improved physical
parameterisations <xref ref-type="bibr" rid="bib1.bibx17" id="paren.23"/>, combined with the Application de la
Recherche à l'Opérationnel à Meso-Echelle
(AROME), first baseline version
released in 1998. The ALADIN model is the limited area model version of the
global scale Action de Recherche Petite Echelle Grande Echelle Integrated
Forecast system (ARPEGE-IFS) <xref ref-type="bibr" rid="bib1.bibx8 bib1.bibx1" id="paren.24"/>. ARPEGE is a global
spectral model, with a Gaussian grid for the grid-point calculation. The
vertical discretisation uses hybrid terrain-following pressure coordinates.
The ALARO-0 model has been developed with the ARPEGE Calcul Radiatif Avec
Nebulosité (ACRANEB)
scheme for radiation based on <xref ref-type="bibr" rid="bib1.bibx42" id="text.25"/>. This ALARO-0 model
configuration has been operated at the Royal Meteorological Institute of
Belgium for
its operational numerical weather forecasts since 2010. The new physical
parameterisation within the ALARO-0 model was specifically designed to run at
convection-permitting scales, with a particular focus on an improved
convection and cloud scheme <xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx15 bib1.bibx17" id="paren.26"/>. The ALARO-0
model domain is centred over western Europe at 46.47<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and
2.58<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E with a dimension of <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>149</mml:mn><mml:mo>×</mml:mo><mml:mn>149</mml:mn></mml:mrow></mml:math></inline-formula> horizontal grid
points and spacing of 20 km in both horizontal axes, with a Lambert
conformal projection (Fig. <xref ref-type="fig" rid="Ch1.F1"/>). The model consists of 46 vertical
layers with the lowest model level at 17 km and the model top extending up
to 72 km.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p>The total domain on 20 km horizontal resolution and the subdomains
(BI, IP, FR, ME, AL, MD, EA) based on the subdomains selected in the
EURO-CORDEX framework. The colour represents the orography (m) in the
ALARO <inline-formula><mml:math display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SURFEX set-up. The two FLUXNET stations focused on in this study
are Vielsalm (maritime temperate climate) and Collelongo (humid subtropical
climate).</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/10/223/2017/gmd-10-223-2017-f01.pdf"/>

        </fig>

      <p>The parameterisation of the land surface in ALARO-0 was initially made with the
land surface scheme Interaction Soil–Biosphere–Atmosphere (ISBA;
<xref ref-type="bibr" rid="bib1.bibx38 bib1.bibx37" id="altparen.27"/>). This scheme was designed for NWP and climate
models, and describes the exchange of energy and water between the low-level
atmosphere, vegetation and the soil surface, by using either a diffusion
method <xref ref-type="bibr" rid="bib1.bibx6" id="paren.28"/>, or a force restore method based on two or three
layers <xref ref-type="bibr" rid="bib1.bibx38" id="paren.29"/>. Using the initial set-up with ISBA, ALARO-0 has
proven its skill for regional climate modelling with daily reinitialisations
<xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx11" id="paren.30"/>. In addition, this set-up has been validated for
continuous climate simulations and is now contributing to the EURO-CORDEX
project <xref ref-type="bibr" rid="bib1.bibx20 bib1.bibx24" id="paren.31"/>. Meanwhile the more recent land surface model
SURFEX, with additional parameterisations for urban surface types, has been
implemented in the ALARO-0 model <xref ref-type="bibr" rid="bib1.bibx22" id="paren.32"/>. A NWP application with
SURFEXv5 within ALARO-0 has shown neutral effects on the winter 2 m
temperature and on the vertical profile of the wind speed. However, it has
shown positive effects on the summer 2 m temperature, 2 m relative
humidity, and resulted in improved precipitation scores compared to the
previously used ISBA model <xref ref-type="bibr" rid="bib1.bibx22" id="paren.33"/>. Whereas the validation of the
implementation of SURFEXv5 within ALARO-0 has been done in a NWP context,
this validation is also required in the context of long-term climate
simulations. In this study, SURFEX uses the two-layer force restore method
for ISBA. The first layer is the surface superficial layer, that directly
interacts with the atmosphere, and the second layer is the combined bulk
surface and rooting layer, which is determined at the depth were soil
moisture flux becomes negligible for a period of ca. 1 week and is thus
more important as a reservoir for soil moisture during dry periods
<xref ref-type="bibr" rid="bib1.bibx38" id="paren.34"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p>The set-up of the three downscaling approaches CON, DRI and FS used
in this study. It represents the spin-up time for the different simulations,
the analysis period of the total experiment and the update frequency of the
lateral and initial boundary conditions.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/10/223/2017/gmd-10-223-2017-f02.pdf"/>

        </fig>

      <p>SURFEX uses a tiling approach with each tile providing information on the
surface fluxes according to the type of surface: nature, town, inland water
and sea. The initial parameterisation ISBA for the nature tile was conserved,
and the Town Energy Balance (TEB; <xref ref-type="bibr" rid="bib1.bibx33" id="altparen.35"/>) was added as a
parameterisation for the town tile. TEB uses a canopy approach with three
urban energy budgets for the layers roof, wall and road. The ISBA and TEB
schemes were combined, together with parameterisation schemes for inland
water and seas, and externalised, based on the algorithm of <xref ref-type="bibr" rid="bib1.bibx5" id="text.36"/>.
In other words, the code can be used inside a meteorological or climate
model, or in stand alone mode. Each tile is divided in different patches,
according to the tile type. These patches correspond to the plant functional
types described in ECOCLIMAP <xref ref-type="bibr" rid="bib1.bibx34" id="paren.37"/>. ECOCLIMAP is a 1 km
horizontal resolution global land cover database and assigns the tile
fraction and corresponding physical parameters (leaf area index: LAI, albedo, etc.) to
SURFEX.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>Experimental design</title>
      <p>The regional climate model was driven by initial and lateral boundary
conditions provided by the ERA-Interim reanalysis, available at a horizontal
resolution of ca. 79 km. A relaxation zone of eight grid points was used at
the lateral boundaries of the domain <xref ref-type="bibr" rid="bib1.bibx10" id="paren.38"/>. The zonal and
meridional wind components, atmospheric temperature, specific humidity,
surface pressure and soil moisture and soil temperature were updated every 6
model hours as lateral boundary conditions and interpolated to hourly
distributions. They were introduced as initial conditions across the domain.
A spin-up time was considered for the model to reach equilibrium between the
lateral boundary conditions and the internal model physics <xref ref-type="bibr" rid="bib1.bibx19" id="paren.39"/>.
Here we use an atmospheric spin-up, typically of a few days, and a land
surface spin-up, typically of a few months to 1 year. The analysis covered
a 10-year period from 00:00 UTC on 1 January 1991 to 00:00 UTC on
1 January 2001. Although the 10-year length is arbitrary, it is sufficiently
long to include some inter-annual variability and to generate a reasonable
sample of extreme events. The use of a NWP model in a long-term climate
setting for the performance of extreme precipitation events for a 10-year
period was recently demonstrated <xref ref-type="bibr" rid="bib1.bibx30" id="paren.40"/>. To evaluate the
sensitivity of the model to the update frequency of the initial conditions,
three types of downscaling approaches were conducted with ALARO-0 coupled to
SURFEXv5 and are detailed below.</p>
      <p>The first downscaling approach was done by simulating the model in a
continuous mode for both the atmosphere and the land surface (hereafter
called CON (“CONtinuous”); Fig. <xref ref-type="fig" rid="Ch1.F2"/>). The model was started at
00:00 UTC on 1 January 1990, and ran continuously until 00:00 UTC on
1 January 2001. The first year was treated as both atmospheric and land
surface spin-up, and was excluded from the analysis. The simulations were
interrupted and restarted monthly to allow for only sea surface temperatures (SSTs) to be updated. Other surface parameters that were updated monthly
using the climatological values from ECOCLIMAP were the vegetation fraction,
surface roughness length, surface emissivity, surface albedo, sand and clay
fractions.</p>
      <p>In the second downscaling approach, the model was reinitialised daily for
both the atmosphere and the land surface (hereafter called DRI (“Daily
ReInitialisation”); Fig. <xref ref-type="fig" rid="Ch1.F2"/>). The model started at 12:00 UTC on
1 January 1991, and each reinitialisation ran for 60 h. The first 36 h
were treated as atmospheric spin-up, and excluded from the analysis. By
applying this downscaling approach, the regional model stays close to the
ERA-Interim forcing <xref ref-type="bibr" rid="bib1.bibx46" id="paren.41"/>. However, the coarse representation
of the land surface by the reanalysis is not able to capture the fine-scale
heterogeneity, particularly the soil moisture and soil temperature.</p>
      <p>The third downscaling approach tries to find the best compromise between the
previous two approaches. The atmosphere was reinitialised daily and the land
surface was simulated continuously with a single
initialisation (hereafter called FS (“Free
Surface”); Fig. <xref ref-type="fig" rid="Ch1.F2"/>). This allowed the model to simulate the
atmospheric fields close to the reanalysis forcing, together with a surface
in equilibrium state. The model was run from 12:00 UTC on 1 March 1990 until
31 May 1991, and the atmosphere was reinitialised daily for a simulation time
of 60 h. The first 36 h were treated as atmospheric spin-up, and were
excluded from the analysis. The land surface conditions were kept continuous
by adding the land surface conditions for the 24 h period after the
atmospheric spin-up to the land surface conditions of the previous daily
simulation. In contrast to the atmospheric spin-up, the land surface spin-up
lasted from 1 March until 31 May 1990, and this 3-month period was excluded
from the analysis. Although CON required a 1-year spin-up, 3 months were
sufficient for the FS deep soil moisture to reach equilibrium state, when
starting in March (not shown). The simulations were done in parallel to each
year from 1990 to 2000, and the 3 monthly spin-up was replaced by the
analysis of the previous year.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p>Overview of the FLUXNET eddy-covariance sites used in this study.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="8">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="left"/>
     <oasis:colspec colnum="7" colname="col7" align="left"/>
     <oasis:colspec colnum="8" colname="col8" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">Site and reference</oasis:entry>  
         <oasis:entry colname="col2">Short</oasis:entry>  
         <oasis:entry colname="col3">Long. (<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E)</oasis:entry>  
         <oasis:entry colname="col4">Lat. (<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N)</oasis:entry>  
         <oasis:entry colname="col5">Alt. (m)</oasis:entry>  
         <oasis:entry colname="col6">Biome type</oasis:entry>  
         <oasis:entry colname="col7">Years</oasis:entry>  
         <oasis:entry colname="col8">Climate zone (Köppen)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Vielsalm</oasis:entry>  
         <oasis:entry colname="col2">BEVie</oasis:entry>  
         <oasis:entry colname="col3">6.00</oasis:entry>  
         <oasis:entry colname="col4">50.31</oasis:entry>  
         <oasis:entry colname="col5">491</oasis:entry>  
         <oasis:entry colname="col6">Mixed</oasis:entry>  
         <oasis:entry colname="col7">1996–2000</oasis:entry>  
         <oasis:entry colname="col8">Maritime temperate (Cfb)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Collelongo</oasis:entry>  
         <oasis:entry colname="col2">ITCol</oasis:entry>  
         <oasis:entry colname="col3">13.59</oasis:entry>  
         <oasis:entry colname="col4">41.85</oasis:entry>  
         <oasis:entry colname="col5">1645</oasis:entry>  
         <oasis:entry colname="col6">Deciduous</oasis:entry>  
         <oasis:entry colname="col7">1996–2000</oasis:entry>  
         <oasis:entry colname="col8">Humid subtropical (Cfa)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Brasschaat</oasis:entry>  
         <oasis:entry colname="col2">BEBra</oasis:entry>  
         <oasis:entry colname="col3">4.52</oasis:entry>  
         <oasis:entry colname="col4">51.31</oasis:entry>  
         <oasis:entry colname="col5">15</oasis:entry>  
         <oasis:entry colname="col6">Deciduous</oasis:entry>  
         <oasis:entry colname="col7">1997–2000</oasis:entry>  
         <oasis:entry colname="col8">Maritime temperate (Cfb)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Loobos</oasis:entry>  
         <oasis:entry colname="col2">NLLoo</oasis:entry>  
         <oasis:entry colname="col3">5.74</oasis:entry>  
         <oasis:entry colname="col4">52.17</oasis:entry>  
         <oasis:entry colname="col5">25</oasis:entry>  
         <oasis:entry colname="col6">Evergreen</oasis:entry>  
         <oasis:entry colname="col7">1996–2000</oasis:entry>  
         <oasis:entry colname="col8">Maritime temperate (Cfb)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Tharandt</oasis:entry>  
         <oasis:entry colname="col2">DETha</oasis:entry>  
         <oasis:entry colname="col3">13.57</oasis:entry>  
         <oasis:entry colname="col4">50.96</oasis:entry>  
         <oasis:entry colname="col5">320</oasis:entry>  
         <oasis:entry colname="col6">Evergreen</oasis:entry>  
         <oasis:entry colname="col7">1996–2000</oasis:entry>  
         <oasis:entry colname="col8">Maritime temperate (Cfb)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Hesse</oasis:entry>  
         <oasis:entry colname="col2">FRHes</oasis:entry>  
         <oasis:entry colname="col3">7.07</oasis:entry>  
         <oasis:entry colname="col4">48.67</oasis:entry>  
         <oasis:entry colname="col5">293</oasis:entry>  
         <oasis:entry colname="col6">Deciduous</oasis:entry>  
         <oasis:entry colname="col7">1997–2000</oasis:entry>  
         <oasis:entry colname="col8">Maritime temperate (Cfb)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Le Bray</oasis:entry>  
         <oasis:entry colname="col2">FRLBr</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.77</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4">44.72</oasis:entry>  
         <oasis:entry colname="col5">62</oasis:entry>  
         <oasis:entry colname="col6">Evergreen</oasis:entry>  
         <oasis:entry colname="col7">1996–2000</oasis:entry>  
         <oasis:entry colname="col8">Maritime temperate (Cfb)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><caption><p>The daily mean 2 m temperature bias (<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C) and
root mean square error (RMSE) (in brackets)
between the downscaled simulations and E-OBS for the total domain and the
subdomains (BI, IP, FR, ME, AL, MD, EA) during DJF and JJA for the 10-year
period from 1991 to 2000.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="10">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:colspec colnum="10" colname="col10" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3">Total</oasis:entry>  
         <oasis:entry colname="col4">BI</oasis:entry>  
         <oasis:entry colname="col5">IP</oasis:entry>  
         <oasis:entry colname="col6">FR</oasis:entry>  
         <oasis:entry colname="col7">ME</oasis:entry>  
         <oasis:entry colname="col8">AL</oasis:entry>  
         <oasis:entry colname="col9">MD</oasis:entry>  
         <oasis:entry colname="col10">EA</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">DJF</oasis:entry>  
         <oasis:entry colname="col2">CON</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.8</mml:mn></mml:mrow></mml:math></inline-formula> (2.5)</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.1</mml:mn></mml:mrow></mml:math></inline-formula> (2.0)</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>2.2</mml:mn></mml:mrow></mml:math></inline-formula> (2.7)</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.5</mml:mn></mml:mrow></mml:math></inline-formula> (2.2)</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.3</mml:mn></mml:mrow></mml:math></inline-formula> (2.0)</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>3.0</mml:mn></mml:mrow></mml:math></inline-formula> (3.8)</oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>2.4</mml:mn></mml:mrow></mml:math></inline-formula> (3.1)</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.1</mml:mn></mml:mrow></mml:math></inline-formula> (2.0)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">DRI</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.2</mml:mn></mml:mrow></mml:math></inline-formula> (2.8)</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.0</mml:mn></mml:mrow></mml:math></inline-formula> (2.7)</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.6</mml:mn></mml:mrow></mml:math></inline-formula>     (2.7)</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.2</mml:mn></mml:mrow></mml:math></inline-formula> (2.9)</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.7</mml:mn></mml:mrow></mml:math></inline-formula> (2.6)</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.4</mml:mn></mml:mrow></mml:math></inline-formula> (3.4)</oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>2.1</mml:mn></mml:mrow></mml:math></inline-formula> (3.2)</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.3</mml:mn></mml:mrow></mml:math></inline-formula> (2.8)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">FS</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.0</mml:mn></mml:mrow></mml:math></inline-formula> (2.8)</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.3</mml:mn></mml:mrow></mml:math></inline-formula> (2.8)</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.3</mml:mn></mml:mrow></mml:math></inline-formula> (2.5)</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.7</mml:mn></mml:mrow></mml:math></inline-formula> (2.8)</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.4</mml:mn></mml:mrow></mml:math></inline-formula> (2.6)</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>2.1</mml:mn></mml:mrow></mml:math></inline-formula> (3.8)</oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.2</mml:mn></mml:mrow></mml:math></inline-formula> (2.7)</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.4</mml:mn></mml:mrow></mml:math></inline-formula> (2.8)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">JJA</oasis:entry>  
         <oasis:entry colname="col2">CON</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.6</mml:mn></mml:mrow></mml:math></inline-formula> (2.0)</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.7</mml:mn></mml:mrow></mml:math></inline-formula> (2.0)</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.5</mml:mn></mml:mrow></mml:math></inline-formula> (1.7)</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.2</mml:mn></mml:mrow></mml:math></inline-formula> (1.9)</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.3</mml:mn></mml:mrow></mml:math></inline-formula> (1.9)</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.8</mml:mn></mml:mrow></mml:math></inline-formula> (2.6)</oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.5</mml:mn></mml:mrow></mml:math></inline-formula> (2.0)</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.5</mml:mn></mml:mrow></mml:math></inline-formula> (1.8)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">DRI</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula> (2.3)</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.9</mml:mn></mml:mrow></mml:math></inline-formula> (2.0)</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.3</mml:mn></mml:mrow></mml:math></inline-formula> (2.2)</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.7</mml:mn></mml:mrow></mml:math></inline-formula> (2.4)</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.3</mml:mn></mml:mrow></mml:math></inline-formula> (2.1)</oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.8</mml:mn></mml:mrow></mml:math></inline-formula> (2.3)</oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.6</mml:mn></mml:mrow></mml:math></inline-formula> (2.3)</oasis:entry>  
         <oasis:entry colname="col10">0.0  (2.1)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">FS</oasis:entry>  
         <oasis:entry colname="col3">0.9 (2.7)</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.7</mml:mn></mml:mrow></mml:math></inline-formula> (2.2)</oasis:entry>  
         <oasis:entry colname="col5">0.5 (2.4)</oasis:entry>  
         <oasis:entry colname="col6">1.0 (3.1)</oasis:entry>  
         <oasis:entry colname="col7">1.3 (2.8)</oasis:entry>  
         <oasis:entry colname="col8">0.0 (2.5)</oasis:entry>  
         <oasis:entry colname="col9">0.7 (2.5)</oasis:entry>  
         <oasis:entry colname="col10">1.2 (2.8)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p>Daily mean 2 m temperature (<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C) for E-OBS DJF <bold>(a)</bold>
and JJA <bold>(b)</bold>, and absolute bias (<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C) of the model with E-OBS
for CON DJF <bold>(c)</bold> and JJA <bold>(d)</bold>, for DRI DJF <bold>(e)</bold> and
JJA <bold>(f)</bold> and for FS DJF <bold>(g)</bold> and JJA <bold>(h)</bold>, all at a
20 km horizontal resolution for the 10-year period from 1991 to 2000. Only the
significant biases are shown, using the Student's <inline-formula><mml:math display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> test at a 5 %
level, and non-significant biases are shown in white.</p></caption>
          <?xmltex \igopts{width=327.206693pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/10/223/2017/gmd-10-223-2017-f03.pdf"/>

        </fig>

      <p>We use 3-hourly output for the model evaluation
presented in the manuscript. The evaluation of atmospheric variables for
winter and summer was done for seven subdomains across Europe, to cover the
spatial variability of the domain (Fig. <xref ref-type="fig" rid="Ch1.F1"/>). This was in agreement
with the subdomains that were used in the EURO-CORDEX community
<xref ref-type="bibr" rid="bib1.bibx28" id="paren.42"/> and that were defined earlier in the framework of the
“Prediction of Regional scenarios and Uncertainties for Defining European
Climate change risks and Effects” (PRUDENCE) project <xref ref-type="bibr" rid="bib1.bibx9" id="paren.43"/>.
The subdomains used in this study were the British Isles (BI), the Iberian
Peninsula (IP), mid-Europe (ME), France (FR), the Alps (AL),
the Mediterranean (MD) and eastern Europe (EA). The subdomains IP, ME and EA
were chosen due to their diverse climate regimes to evaluate the yearly cycle
of the atmospheric and land surface variables. As land surface processes play
an important role primarily during summer, the model output was stored at
every hour for the summer period of June–July–August (JJA) during the
10-year period. We evaluated the partitioning of the sensible and latent heat
fluxes by the daily maximum Bowen ratio (BR; <xref ref-type="bibr" rid="bib1.bibx7" id="altparen.44"/>) for the
summer periods from 1996 to 2000 for the total study domain, and compared a
subset of FLUXNET stations using the corresponding model grid points. The
corresponding daily maximum BRs were analysed for the 10-year summer period
from 1991 to 2000. When the BR <inline-formula><mml:math display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 1, the latent heat flux (LE) is greater
than the sensible heat flux (H). Conversely when BR <inline-formula><mml:math display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 1, LE is less than
H. The diurnal cycles of all surface energy fluxes were also analysed and
validated against observations.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Observational reference data</title>
      <p>The results of the climate simulations were validated against E-OBS, a daily
high-resolution gridded observational dataset <xref ref-type="bibr" rid="bib1.bibx23" id="paren.45"/>. The dataset
consists of the daily mean temperature, the daily maximum and minimum
temperature, and the daily precipitation total. The most recent version v12.0
was selected on the 0.22<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> rotated pole grid, corresponding to a
25 km horizontal resolution in Europe. It covers the period 1 January 1950
to 30 June 2015. In order to validate the model data, the ALARO-0 data at
20 km horizontal resolution were bilinearly interpolated towards E-OBS at
25 km horizontal resolution and replotted to our study domain. A careful
interpretation of E-OBS is necessary, as this regridded non-homogeneously
distributed network applies a smoothing out of extreme precipitation and
consequently a large underestimation of the mean precipitation
<xref ref-type="bibr" rid="bib1.bibx23" id="paren.46"/>.</p>
      <p>For the validation of the surface fluxes in the model, we used measurements
from the FLUXNET level 3 flux tower database <xref ref-type="bibr" rid="bib1.bibx4" id="paren.47"/>. It provides
information on the energy exchange between the ecosystem and the atmosphere.
FLUXNET is a global network, and consists of flux towers using the
eddy-covariance method to monitor carbon dioxide and water vapour exchange
rates, and energy flux densities. No gap-filling has been done and the
comparison to the model output was only done at hours when observational data
were available. A number of sites were already part of a separate flux
measurement network <xref ref-type="bibr" rid="bib1.bibx3" id="paren.48"/>. The model validation was done using
grid cell averages compared to point observations, suggesting large
differences in the land cover representation. In total, a subset of seven
stations, which cover different biome types (Table <xref ref-type="table" rid="Ch1.T1"/>), were selected
to demonstrate the spatial variability of the domain by the model. However,
the main focus was on the Vielsalm and Collelongo sites (Fig. <xref ref-type="fig" rid="Ch1.F1"/>),
as their model grid cells represent more than 50 % of the corresponding
land cover, and cover different climate regimes.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Validation of the mean model state</title>
<sec id="Ch1.S3.SS1">
  <title>Spatial distribution</title>
<sec id="Ch1.S3.SS1.SSS1">
  <?xmltex \opttitle{Daily mean 2\,m temperature}?><title>Daily mean 2 m temperature</title>
      <p>The spatial distributions of the 10-year daily mean temperature bias
(absolute, (model <inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula> observed)) of CON, DRI and FS simulations were
compared to E-OBS (Fig. <xref ref-type="fig" rid="Ch1.F3"/>), for winter (DJF:
December–January–February) and summer (JJA). The
area-averaged bias during winter and summer for CON, DRI and FS for the
entire domain as well as for specific subdomains is presented in
Table <xref ref-type="table" rid="Ch1.T2"/>. CON simulated a cold bias in general, except for northern
Africa in summer, with a pronounced orographic effect, for both winter and
summer (Fig. <xref ref-type="fig" rid="Ch1.F3"/>c, d). The cold bias over the entire domain was
less pronounced in summer with a value of <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.6</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C compared to the
winter bias of <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.8</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C (Table <xref ref-type="table" rid="Ch1.T2"/>). Moreover, the Iberian
Peninsula, Mediterranean and eastern Europe resulted in a small bias of
<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C during summer as compared to E-OBS (Fig. <xref ref-type="fig" rid="Ch1.F3"/>d).
This is due to compensating effects, as the bias represents an average over
the subdomain and might be the result of large negative and large positive
biases over different parts of the particular subdomain compensating each
other. However, the area-averaged bias gives a good impression of the ranking
of the experiments <xref ref-type="bibr" rid="bib1.bibx28" id="paren.49"/>.</p>
      <p>With respect to CON, DRI demonstrated a reduction of the cold bias during
winter and summer, particularly for the eastern part of the domain
(Fig. <xref ref-type="fig" rid="Ch1.F3"/>e, f). The area-averaged bias for eastern Europe was close
to zero for DRI during winter and summer (Table <xref ref-type="table" rid="Ch1.T2"/>), in spite of
many significant non-zero bias points for the summer
(Fig. <xref ref-type="fig" rid="Ch1.F3"/>e, f). A large improvement of the 2 m temperature
simulation by DRI was also produced for mid-Europe and the Alps with a winter
bias of <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.7</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.4</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C respectively, which is about half of the
bias of CON. For summer, the bias decreases further to <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.3</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C (ME)
and <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.8</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C (AL); a 1 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C decrease relative to CON for
these subdomains. The frequent reinitialisations keep the large scales closer
to the ERA-Interim forcing, whereas ALARO and ARPEGE are bound to a cold bias
<xref ref-type="bibr" rid="bib1.bibx45 bib1.bibx20" id="paren.50"/>.</p>
      <p>The performance of the FS simulation was different for winter and summer
(Fig. <xref ref-type="fig" rid="Ch1.F3"/>g, h). The simulation of the 2 m temperature during
winter was the best of all three approaches when using FS. Large parts of the
domain resulted in biases close to zero for the British Isles, France,
mid-Europe and eastern Europe (Fig. <xref ref-type="fig" rid="Ch1.F3"/>g). The bias decreased by
ca. 1 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C in FS compared to CON for these subdomains
(Table <xref ref-type="table" rid="Ch1.T2"/>). During summer, the sign of the bias reversed from
negative to positive, except for some isolated areas (Fig. <xref ref-type="fig" rid="Ch1.F3"/>h).
The Alps were characterised by a zero bias on the northern flank and mixed
cold and warm bias on the southern flank compensating each other
(Table <xref ref-type="table" rid="Ch1.T2"/>). Large parts of the Iberian Peninsula and the
Mediterranean exhibited a warm bias (Fig. <xref ref-type="fig" rid="Ch1.F3"/>h), resulting in
positive values close to zero (Table <xref ref-type="table" rid="Ch1.T2"/>). Mid-Europe, France and
eastern Europe were mainly characterised by a positive bias of around
1 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C (Table <xref ref-type="table" rid="Ch1.T2"/>). These positive biases for FS might be
related to rapidly decreasing soil moisture values in spring and summer (not
shown). The temperature–soil moisture relation is strongest for FS, as this
simulation benefits from soil moisture memory by allowing the land surface to
be fully interactive with the atmosphere <xref ref-type="bibr" rid="bib1.bibx26" id="paren.51"/>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><caption><p>The daily accumulated precipitation bias (%) and
root mean square error (RMSE) (in brackets)
between the downscaled simulations and E-OBS for the total domain and the
subdomains (BI, IP, FR, ME, AL, MD, EA) during DJF and JJA for the 10-year
period from 1991 to 2000. </p></caption><oasis:table frame="topbot"><oasis:tgroup cols="10">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:colspec colnum="10" colname="col10" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3">Total</oasis:entry>  
         <oasis:entry colname="col4">BI</oasis:entry>  
         <oasis:entry colname="col5">IP</oasis:entry>  
         <oasis:entry colname="col6">FR</oasis:entry>  
         <oasis:entry colname="col7">ME</oasis:entry>  
         <oasis:entry colname="col8">AL</oasis:entry>  
         <oasis:entry colname="col9">MD</oasis:entry>  
         <oasis:entry colname="col10">EA</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">DJF</oasis:entry>  
         <oasis:entry colname="col2">CON</oasis:entry>  
         <oasis:entry colname="col3">16.6 (3.8)</oasis:entry>  
         <oasis:entry colname="col4">4.5 (4.5)</oasis:entry>  
         <oasis:entry colname="col5">16.1 (4.6)</oasis:entry>  
         <oasis:entry colname="col6">29.0 (3.6)</oasis:entry>  
         <oasis:entry colname="col7">25.4 (2.7)</oasis:entry>  
         <oasis:entry colname="col8">11.2 (4.7)</oasis:entry>  
         <oasis:entry colname="col9">46.0 (6.2)</oasis:entry>  
         <oasis:entry colname="col10">35.3 (2.3)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">DRI</oasis:entry>  
         <oasis:entry colname="col3">20.9 (4.8)</oasis:entry>  
         <oasis:entry colname="col4">6.6 (5.2)</oasis:entry>  
         <oasis:entry colname="col5">21.2 (5.6)</oasis:entry>  
         <oasis:entry colname="col6">26.8 (4.8)</oasis:entry>  
         <oasis:entry colname="col7">27.9 (3.8)</oasis:entry>  
         <oasis:entry colname="col8">24.1 (6.3)</oasis:entry>  
         <oasis:entry colname="col9">41.6 (7.1)</oasis:entry>  
         <oasis:entry colname="col10">45.7 (3.1)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">FS</oasis:entry>  
         <oasis:entry colname="col3">36.3 (5.4)</oasis:entry>  
         <oasis:entry colname="col4">16.9 (5.5)</oasis:entry>  
         <oasis:entry colname="col5">31.3 (6.2)</oasis:entry>  
         <oasis:entry colname="col6">38.2 (5.2)</oasis:entry>  
         <oasis:entry colname="col7">35.7 (4.0)</oasis:entry>  
         <oasis:entry colname="col8">26.7 (6.7)</oasis:entry>  
         <oasis:entry colname="col9">108.5 (9.9)</oasis:entry>  
         <oasis:entry colname="col10">64.1 (3.5)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">JJA</oasis:entry>  
         <oasis:entry colname="col2">CON</oasis:entry>  
         <oasis:entry colname="col3">12.1 (4.2)</oasis:entry>  
         <oasis:entry colname="col4">24.7 (4.4)</oasis:entry>  
         <oasis:entry colname="col5">11.5 (2.9)</oasis:entry>  
         <oasis:entry colname="col6">12.0 (4.4)</oasis:entry>  
         <oasis:entry colname="col7">11.9 (5.0)</oasis:entry>  
         <oasis:entry colname="col8">32.6 (7.3)</oasis:entry>  
         <oasis:entry colname="col9">60.7 (3.5)</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>2.6</mml:mn></mml:mrow></mml:math></inline-formula> (5.4)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">DRI</oasis:entry>  
         <oasis:entry colname="col3">22.5 (4.7)</oasis:entry>  
         <oasis:entry colname="col4">27.0 (4.7)</oasis:entry>  
         <oasis:entry colname="col5">30.0 (3.4)</oasis:entry>  
         <oasis:entry colname="col6">18.3 (5.1)</oasis:entry>  
         <oasis:entry colname="col7">8.8  (5.5)</oasis:entry>  
         <oasis:entry colname="col8">48.2 (8.9)</oasis:entry>  
         <oasis:entry colname="col9">84.8 (3.8)</oasis:entry>  
         <oasis:entry colname="col10">6.8  (5.9)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">FS</oasis:entry>  
         <oasis:entry colname="col3">3.6  (4.5)</oasis:entry>  
         <oasis:entry colname="col4">17.4 (4.6)</oasis:entry>  
         <oasis:entry colname="col5">13.0 (3.2)</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>7.0</mml:mn></mml:mrow></mml:math></inline-formula> (4.6)</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>13.4</mml:mn></mml:mrow></mml:math></inline-formula> (5.1)</oasis:entry>  
         <oasis:entry colname="col8">23.5 (8.3)</oasis:entry>  
         <oasis:entry colname="col9">52.4 (3.6)</oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>8.2</mml:mn></mml:mrow></mml:math></inline-formula> (5.7)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p>Daily accumulated precipitation (mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) for E-OBS DJF
<bold>(a)</bold> and JJA <bold>(b)</bold>, and relative bias (%) of the model with
E-OBS for CON DJF <bold>(c)</bold> and JJA <bold>(d)</bold>, for DRI DJF <bold>(e)</bold>
and JJA <bold>(f)</bold> and for FS DJF <bold>(g)</bold> and JJA <bold>(h)</bold>, all at
a 20 km horizontal resolution for a 10-year period from 1991 to 2000. Only the
significant biases are shown, using the <inline-formula><mml:math display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> test at a 5 % level, and
non-significant biases are shown in white.</p></caption>
            <?xmltex \igopts{width=327.206693pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/10/223/2017/gmd-10-223-2017-f04.pdf"/>

          </fig>

      <p>In summary, CON underestimated winter and summer 2 m temperature by
1–2 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C on average. With respect to CON, DRI showed a general
positive effect during winter and summer. Consequently, the use of a daily
reinitialised atmosphere improved the representation of the 2 m temperature
for both winter and summer compared to a continuous simulation of the
atmosphere. The winter bias was further improved for most subdomains for FS
compared to CON. For summer, most subdomains experienced a warm bias, in the
same order of magnitude as CON. The difference might point at the interaction
of the land surface and the atmosphere being stronger with FS, because of the
soil moisture memory.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS2">
  <title>Daily accumulated precipitation</title>
      <p>The spatial distributions of the 10-year daily accumulated precipitation bias
(relative, (model <inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula> observed) <inline-formula><mml:math display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> observed) of CON, DRI and FS were
compared to E-OBS, for the winter and the summer seasons (Fig. <xref ref-type="fig" rid="Ch1.F4"/>).
The relative biases during winter and summer for CON, DRI and FS are
presented for the entire domain as well as for the specific subdomains in
Table <xref ref-type="table" rid="Ch1.T3"/>. The precipitation pattern of E-OBS during winter
displayed the highest values of <inline-formula><mml:math display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 3 mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> over Portugal,
north-western Spain, western England, Scotland and Ireland, the Adriatic Coast
and the northern flanks of the Alps (Fig. <xref ref-type="fig" rid="Ch1.F4"/>a, b). During summer,
similar amounts of rainfall were concentrated over the Alps and the
Carpathians, whereas the lowest values of <inline-formula><mml:math display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 1 mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> were concentrated over the Iberian
Peninsula, the Mediterranean and northern Africa.</p>
      <p>During winter, all simulations demonstrated a similar spatial variability of
the wet bias, except for a dry bias in northern Africa
(Fig. <xref ref-type="fig" rid="Ch1.F4"/>c, e, g). In general, ALARO was forced towards the too wet
driving fields of ERA-Interim <xref ref-type="bibr" rid="bib1.bibx32" id="paren.52"/>, which can explain part
of the overestimated precipitation. More specifically, the overestimation of
winter precipitation was strongest in the Mediterranean and eastern Europe
with values from 35.3 to 108.5 % for all simulation modes
(Table <xref ref-type="table" rid="Ch1.T3"/>). The large values in the Mediterranean agreed with the
large underestimation of 2 m temperature, as this region is characterised by
a strong dependence of temperature and precipitation <xref ref-type="bibr" rid="bib1.bibx14" id="paren.53"/>. The
area-averaged bias for the entire domain was larger for FS in winter with ca.
36.3 % compared to 16.6 and 20.9 % for CON and DRI. The too wet driving
field of ERA-Interim was superimposed on the smaller cold bias of FS,
suggesting a higher precipitation bias than CON and DRI.</p>
      <p>During summer, the simulations showed different spatial variability
(Fig. <xref ref-type="fig" rid="Ch1.F4"/>d, f, h). In comparison to the winter bias, the summer
precipitation bias for CON was reduced over the continental part with
positive and negative biases over the southern part of the domain
(Fig. <xref ref-type="fig" rid="Ch1.F4"/>d). The Mediterranean expressed a high wet bias of
60.7 % for CON, but the absolute values in summer were close to zero, as
it is characterised by a climate with dry summers (Fig. <xref ref-type="fig" rid="Ch1.F4"/>b). The
bias pattern over the continental part was very similar for DRI compared to
CON during summer, whereas southern Europe showed increased wet biases for
DRI (Fig. <xref ref-type="fig" rid="Ch1.F4"/>f). The Iberian Peninsula, France and the Mediterranean
demonstrated a bias of 30.0, 18.3 and 84.8 % respectively, compared to
11.5, 12.0 and 60.7 % with CON (Table <xref ref-type="table" rid="Ch1.T3"/>). The performance of
FS was similar to CON for southern and eastern Europe (Fig. <xref ref-type="fig" rid="Ch1.F4"/>h).
This is in contrast to the continental part of the domain, where the
precipitation signal reversed relative to CON and DRI and a small dry bias
persisted (<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>7.0</mml:mn></mml:mrow></mml:math></inline-formula> % for France, <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>13.4</mml:mn></mml:mrow></mml:math></inline-formula> % for mid-Europe and
<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>8.2</mml:mn></mml:mrow></mml:math></inline-formula> % for eastern Europe respectively). Consequently, the summer
precipitation was simulated better by FS than by CON and DRI. During summer,
the influence of the soil moisture memory on the atmosphere is more
important, resulting in an improved representation of the precipitation with
FS.</p>
      <p>In summary, the model was characterised by a wet bias in winter and summer.
The spatial variability during winter was very similar for all simulations;
therefore, the use of a daily reinitialised atmosphere had a neutral impact on the
winter precipitation. During summer, the precipitation showed a different
behaviour with the different simulation modes. In summer for the southern
part of the domain, precipitation bias experienced a neutral effect with DRI,
whereas the precipitation bias increased for the continental part. Frequent
reinitialisations did not allow the land surface to build up a soil moisture
memory, resulting in less skill for the representation of the precipitation.
However, the precipitation bias improved with FS for the continental part.
Therefore, the combination of the daily reinitialised atmosphere together
with a continuous surface is crucial in summer to get the best results.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p>Mean annual cycle of the daily 2 m temperature (<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C) with
E-OBS, CON, DRI and FS for <bold>(a)</bold> the Iberian Peninsula,
<bold>(b)</bold> mid-Europe, and <bold>(c)</bold> eastern Europe and daily
accumulated precipitation (mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) for <bold>(d)</bold> the Iberian
Peninsula, <bold>(e)</bold> mid-Europe and <bold>(f)</bold> eastern Europe, averaged
over the 10-year period from 1991 to 2000. Both the mean and standard
deviation (SD) are displayed as text.</p></caption>
            <?xmltex \igopts{width=327.206693pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/10/223/2017/gmd-10-223-2017-f05.pdf"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Mean annual cycle</title>
<sec id="Ch1.S3.SS2.SSS1">
  <?xmltex \opttitle{Daily mean 2\,m temperature}?><title>Daily mean 2 m temperature</title>
      <p>To validate specific subdomains within the larger domain on a monthly scale,
the mean annual cycles of the downscaled simulations were compared to the
observations (Fig. <xref ref-type="fig" rid="Ch1.F5"/>). We focused on the following subdomains
(Fig. <xref ref-type="fig" rid="Ch1.F1"/>): (1) the Iberian Peninsula at the western boundary of
the domain with its warm and dry summer climate, (2) mid-Europe with its
temperate climate and (3) eastern Europe at the eastern boundary of the
domain with its continental climate.</p>
      <p>The daily mean 2 m temperature reached 23 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C for the Iberian
Peninsula, and 20 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C for both mid-Europe and eastern Europe
(Fig. <xref ref-type="fig" rid="Ch1.F5"/>a–c). For these selected subdomains, all downscaled
simulations presented very similar autumn (SON: September–October–November)
temperatures, but underestimated them with respect to E-OBS. Therefore, the
autumn temperature is not sensitive to the updated frequency of the initial
conditions. Regarding the other seasons, the simulations revealed a different
behaviour in the representation of the 2 m temperature with respect to the
observations.</p>
      <p>For the Iberian Peninsula, the 2 m temperature was generally underestimated
for all seasons (Fig. <xref ref-type="fig" rid="Ch1.F5"/>a). Except for autumn, FS was closer to
the observations as compared to CON and DRI, resulting in a yearly mean
temperature of 12.5 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, which was closer to the observed yearly mean
temperature of 13.7 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C as compared to 11.6 and 11.9 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C by
CON and DRI respectively. Therefore, summer 2 m temperature was well
simulated by FS for this subdomain. For mid-Europe, CON and DRI
underestimated the 2 m temperature for all seasons, and FS was very close to
the observations from February to May (Fig. <xref ref-type="fig" rid="Ch1.F5"/>b). However, FS
overestimated the summer 2 m temperature and CON and DRI underestimated the
summer 2 m temperature. Still, the yearly mean value of 9.0 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C by
FS was very close to the observational mean of 9.3 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. For eastern
Europe, DRI and FS demonstrated almost identical behaviour for the simulation
of the 2 m temperature during winter and spring (MAM: March–April–May)
with small biases (Fig. <xref ref-type="fig" rid="Ch1.F5"/>c), whereas CON underestimated the 2 m
temperature. Similar to mid-Europe, FS overestimated the summer 2 m
temperature with ca. 1 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C and CON underestimated the summer 2 m
temperature with ca. 1 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C in eastern Europe. Yet again, the yearly
mean value of 8.5 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C by FS was very similar as compared to the
observations with a value of 8.6 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, while largest differences
occurred using CON with a value of 7.5 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C.</p>
      <p>In summary, the yearly mean temperature was underestimated by CON for all
subdomains. In general, ALARO is bound to a cold bias <xref ref-type="bibr" rid="bib1.bibx20" id="paren.54"/>. Along
the selected subdomains, there were larger differences between the
simulations in mid-Europe and eastern Europe compared to the Iberian
Peninsula. The dry climate of the Iberian Peninsula is less dominated by land
surface–atmosphere interactions, as soil moisture does not impact the
evapotranspiration availability <xref ref-type="bibr" rid="bib1.bibx44" id="paren.55"/>. DRI was able to
simulate the 2 m temperature better for mid-Europe and eastern Europe as
compared to CON for winter, spring and summer. FS had the best yearly mean
2 m temperature, but the summer 2 m temperature was overestimated by FS for
mid-Europe and eastern Europe.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p>Daily maximum Bowen ratio averaged over the 5-year JJA period from
1996 to 2000 for <bold>(a)</bold> CON, <bold>(b)</bold> DRI and <bold>(c)</bold> FS and
averaged over the 10-year JJA period 1991–2000 for <bold>(d)</bold> CON,
<bold>(e)</bold> DRI and <bold>(f)</bold> FS. The dots represent the values for the
FLUXNET stations Vielsalm, Collelongo, Brasschaat, Loobos, Tharandt, Hesse
and Le Bray.</p></caption>
            <?xmltex \igopts{width=327.206693pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/10/223/2017/gmd-10-223-2017-f06.pdf"/>

          </fig>

</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <title>Daily accumulated precipitation</title>
      <p>Similar to temperature, the monthly means of the daily accumulated
precipitation, averaged over the 10-year period, are shown in
Fig. <xref ref-type="fig" rid="Ch1.F5"/> for the Iberian Peninsula, mid-Europe and eastern Europe.
When comparing the observations, the seasonal variability was most pronounced
for the Iberian Peninsula, with minimum precipitation values of ca.
0.5 mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> during summer, and maximum precipitation values of ca.
3 mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> during spring, autumn and beginning of the winter
(Fig. <xref ref-type="fig" rid="Ch1.F5"/>d). The precipitation in mid-Europe reached highest values
of ca. 3 mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> during summer (Fig. <xref ref-type="fig" rid="Ch1.F5"/>e). The continental
climate of eastern Europe presented average values of 1 mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for
winter and spring, while most rainfall occurred in the summer of ca.
2.5 mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (Fig. <xref ref-type="fig" rid="Ch1.F5"/>f).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><caption><p>Daily cycle of the energy fluxes (W m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) in JJA 1996–2000 for
Vielsalm in the top row and Collelongo in bottom row for <bold>(a, c)</bold> H,
and <bold>(b, d)</bold> LE, for the FLUXNET observations and their corresponding
model grid points by CON, DRI and FS. The error bars represent the estimated
uncertainties of the observed turbulent fluxes.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/10/223/2017/gmd-10-223-2017-f07.pdf"/>

          </fig>

      <p>In general, the agreement of the simulations was the largest during autumn. For
the Iberian Peninsula, the seasonal pattern of the downscaled simulations
followed the seasonal pattern of E-OBS, despite a general overestimation of
the precipitation (Fig. <xref ref-type="fig" rid="Ch1.F5"/>d). This overestimation was stronger in
winter and in spring for the Iberian Peninsula, and is in agreement with
<xref ref-type="bibr" rid="bib1.bibx32" id="text.56"/>. For these two seasons, E-OBS showed an undercatch of
the precipitation, which might have amplified the model biases
<xref ref-type="bibr" rid="bib1.bibx41" id="paren.57"/>. CON and DRI were closer to the observations than FS in
winter and spring, resulting in yearly mean values of 1.9, 2.0 and
2.1 mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> respectively for CON, DRI and FS, as compared to the
observational mean value of 1.7 mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. In mid-Europe, the model
overestimated the precipitation for most of the year, except for summer
(Fig. <xref ref-type="fig" rid="Ch1.F5"/>e). During summer, FS showed a large underestimation,
whereas CON and DRI showed similar overestimates of precipitation. The
precipitation in eastern Europe (Fig. <xref ref-type="fig" rid="Ch1.F5"/>f) was overestimated by
the model during most of the year, except for summer <xref ref-type="bibr" rid="bib1.bibx32" id="paren.58"/>,
where there is considerable agreement on the estimation of the summer
precipitation. The yearly mean precipitation by CON was lowest with
2.0 mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and highest when using FS with 2.1 mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, as
compared to 1.6 mm day<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> by the observations (Fig. <xref ref-type="fig" rid="Ch1.F5"/>f).</p>
      <p>In summary, the three downscaling approaches generally overestimated the
precipitation over these three regions in all seasons except during JJA. On a
yearly basis, the differences between CON, DRI and FS were small; on the other hand, on a
monthly basis the magnitude of differences were regionally dependent with
larger differences between the model simulations for mid-Europe and eastern
Europe compared to the Iberian Peninsula.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S4">
  <title>Validation of surface fluxes</title>
      <p>The spatial distributions of the 5-year daily maximum BR, at
the time of maximum H and LE, of CON, DRI and FS were compared to FLUXNET
observations, for the summer period only (Fig. <xref ref-type="fig" rid="Ch1.F6"/>a–c). The
corresponding spatial distributions of the 10-year daily maximum BR of CON,
DRI and FS were evaluated with respect to the results for the 5-year period
(Fig. <xref ref-type="fig" rid="Ch1.F6"/>d–f). The mean diurnal cycles of the surface energy fluxes
are illustrated over the 5-year summer period from 1996 to 2000 for the FLUXNET
stations of Vielsalm and Collelongo and their corresponding model grid points
(Fig. <xref ref-type="fig" rid="Ch1.F7"/>, Table <xref ref-type="table" rid="Ch1.T4"/>).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4" specific-use="star"><caption><p>The daily maximum surface energy fluxes (W m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) averaged over
the 5-year JJA period from 1996 to 2000 and the 10-year period from 1991 to 2000 (in
brackets).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3">RN</oasis:entry>  
         <oasis:entry colname="col4">H</oasis:entry>  
         <oasis:entry colname="col5">LE</oasis:entry>  
         <oasis:entry colname="col6">G</oasis:entry>  
         <oasis:entry colname="col7">BR</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Vielsalm</oasis:entry>  
         <oasis:entry colname="col2">OBS</oasis:entry>  
         <oasis:entry colname="col3">417</oasis:entry>  
         <oasis:entry colname="col4">151</oasis:entry>  
         <oasis:entry colname="col5">134</oasis:entry>  
         <oasis:entry colname="col6">11</oasis:entry>  
         <oasis:entry colname="col7">1.12</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">CON</oasis:entry>  
         <oasis:entry colname="col3">395 (404)</oasis:entry>  
         <oasis:entry colname="col4">118 (113)</oasis:entry>  
         <oasis:entry colname="col5">250 (261)</oasis:entry>  
         <oasis:entry colname="col6">47 (47)</oasis:entry>  
         <oasis:entry colname="col7">0.47 (0.43)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">DRI</oasis:entry>  
         <oasis:entry colname="col3">388 (398)</oasis:entry>  
         <oasis:entry colname="col4">151 (159)</oasis:entry>  
         <oasis:entry colname="col5">195 (193)</oasis:entry>  
         <oasis:entry colname="col6">57 (58)</oasis:entry>  
         <oasis:entry colname="col7">0.78 (0.82)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">FS</oasis:entry>  
         <oasis:entry colname="col3">405 (411)</oasis:entry>  
         <oasis:entry colname="col4">139 (152)</oasis:entry>  
         <oasis:entry colname="col5">229 (221)</oasis:entry>  
         <oasis:entry colname="col6">46 (49)</oasis:entry>  
         <oasis:entry colname="col7">0.61 (0.69)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Collelongo</oasis:entry>  
         <oasis:entry colname="col2">OBS</oasis:entry>  
         <oasis:entry colname="col3">538</oasis:entry>  
         <oasis:entry colname="col4">253</oasis:entry>  
         <oasis:entry colname="col5">192</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>1.39</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7">1.32</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">CON</oasis:entry>  
         <oasis:entry colname="col3">480 (481)</oasis:entry>  
         <oasis:entry colname="col4">159 (147)</oasis:entry>  
         <oasis:entry colname="col5">270 (289)</oasis:entry>  
         <oasis:entry colname="col6">111 (108)</oasis:entry>  
         <oasis:entry colname="col7">0.59 (0.51)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">DRI</oasis:entry>  
         <oasis:entry colname="col3">496 (494)</oasis:entry>  
         <oasis:entry colname="col4">247 (232)</oasis:entry>  
         <oasis:entry colname="col5">183 (194)</oasis:entry>  
         <oasis:entry colname="col6">143 (140)</oasis:entry>  
         <oasis:entry colname="col7">1.35 (1.19)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">FS</oasis:entry>  
         <oasis:entry colname="col3">501 (498)</oasis:entry>  
         <oasis:entry colname="col4">197 (191)</oasis:entry>  
         <oasis:entry colname="col5">236 (247)</oasis:entry>  
         <oasis:entry colname="col6">111 (110)</oasis:entry>  
         <oasis:entry colname="col7">0.83 (0.77)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p>The daily maximum BR showed a strong gradient of increasing values towards
the south of the domain (Fig. <xref ref-type="fig" rid="Ch1.F6"/>a–c). Recall that when the value
is lower (higher) than 1, the latent heat flux (LE) is higher (lower) than
the sensible heat flux (H). Southern Europe is characterised by dry summers,
with a strong control of the soil moisture on the evapotranspiration
<xref ref-type="bibr" rid="bib1.bibx25" id="paren.59"/>, and thus lower LE than H. Large differences existed between
the three downscaling approaches, particularly for the continental part of
the domain. This is in agreement with the larger differences between the
simulation modes in 2 m temperature for the continental subdomains compared
to the southern subdomains. Therefore, the 2 m temperature is correlated to
evapotranspiration by the sensitivity of LE on the soil moisture
<xref ref-type="bibr" rid="bib1.bibx43" id="paren.60"/>.</p>
      <p>CON had relatively low BR values of 0 to 1 for the continental area, DRI
showed BR values of 0.5 to 1 and FS had the highest values of 2 to 3. The
larger values presented by FS were in agreement with the warm and dry summer
bias. Comparison with the FLUXNET observations showed a general
underestimation of BR for CON and DRI, whereas FS estimated well the BR for
most of the sites. The FLUXNET sites show typically a closure imbalance of
20 % <xref ref-type="bibr" rid="bib1.bibx47" id="paren.61"/>, whereas it was assumed that the BR is well
estimated by the eddy-covariance system <xref ref-type="bibr" rid="bib1.bibx36" id="paren.62"/>. Though this
validation was based on five summer periods only from 1996 to 2000, it was
still robust as indicated by the corresponding BR for the 10-year summer
period from 1991 to 2000 (Fig. <xref ref-type="fig" rid="Ch1.F6"/>d–f, Table <xref ref-type="table" rid="Ch1.T4"/>).
Considering the two FLUXNET sites Vielsalm and Collelongo, DRI indicates the
best agreement with the observed BR (Fig. <xref ref-type="fig" rid="Ch1.F6"/>b), with values of 0.78 and 1.35 compared to 1.12 and 1.32 respectively
(Table <xref ref-type="table" rid="Ch1.T4"/>). Despite higher BR values in FS, estimates corresponding
to Vielsalm and Collelongo were located in regions where the BR was
comparatively low, resulting in average values of 0.61 and 0.83 respectively
(Table <xref ref-type="table" rid="Ch1.T4"/>).</p>
      <p>The model performed well for the simulation of the daily cycle of the net
radiation (RN; not shown), even though the model underestimated the values of
RN by ca. 5–10 % (Table <xref ref-type="table" rid="Ch1.T4"/>). The model generally
underestimated H, and overestimated LE (Fig. <xref ref-type="fig" rid="Ch1.F7"/> and
Table <xref ref-type="table" rid="Ch1.T4"/>). The ground heat flux (G) showed improbably high values
compared to the observed ones (Table <xref ref-type="table" rid="Ch1.T4"/>). G is dependent on the
soil temperature, which was largely overestimated by the land surface model
(not shown). The standard version of ISBA, the nature tile of SURFEX,
aggregates soil and vegetation properties for each grid cell
<xref ref-type="bibr" rid="bib1.bibx38" id="paren.63"/>. The net radiation is directly transferred to the ground,
causing an inaccurate partitioning of the incoming energy into turbulent and
ground heat fluxes <xref ref-type="bibr" rid="bib1.bibx36" id="paren.64"/>. An additional parameterisation for the
leaf litter on the surface soil impacts this distribution <xref ref-type="bibr" rid="bib1.bibx48" id="paren.65"/>.
We suggest to include an explicit formulation of the canopy layer
<xref ref-type="bibr" rid="bib1.bibx36" id="paren.66"/> and potentially a parameterisation for the forest litter
layer <xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx48" id="paren.67"/>. The implementation of these explicit
formulations in ISBA outperformed the representation of the soil temperature
of the original ISBA model <xref ref-type="bibr" rid="bib1.bibx36" id="paren.68"/>. They showed that the original
ISBA model overestimated the G flux amplitude with several tens of
W m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> during both daytime and nighttime. However, using the distinct
surface energy budgets resolved part of the overestimated G by intercepting
most of the downward solar radiation, leaving more energy available for
turbulent fluxes. Consequently, less net radiation reaches the forest
surface, reducing the energy available for the soil conductance
<xref ref-type="bibr" rid="bib1.bibx36" id="text.69"/>.</p>
      <p>For Vielsalm, H was simulated well by DRI and FS during nighttime and
daytime, whereas CON underestimated H during daytime (Fig. <xref ref-type="fig" rid="Ch1.F7"/>a).
The daily maximum H by CON was only 118 W m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, as compared to 151 and
139 W m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for DRI and FS respectively (Table <xref ref-type="table" rid="Ch1.T4"/>). This
validation was only done for five summer periods from 1996 to 2000, but the
corresponding daily maximum values for the 10-year summer period from 1991 to 2000
indicate that the 5-year period was representative for the validation of the
fluxes (Table <xref ref-type="table" rid="Ch1.T4"/>). The LE was overestimated by all simulations, but
the difference in the observations was smallest for DRI, due to the
frequent land surface reinitialisations, compared to the highest values for CON.
The daily maximum BR was lower than 1 for all downscaling approaches
(Table <xref ref-type="table" rid="Ch1.T4"/>). This means that they all simulated a higher latent than
sensible heat flux. Still, DRI and FS showed higher values for BR than CON.
Therefore, the partitioning of the surface energy fluxes was better
represented by DRI and FS for the station of Vielsalm.</p>
      <p>For Collelongo, the model underestimated H during daytime and overestimated H
during nighttime, except for DRI, which demonstrated a good agreement with the
observations. Consequently, the model overestimated LE during daytime, except
for DRI. The daily maximum H for DRI of 247 W m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> was close to the
observed value of 253 W m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, whereas CON and FS simulated much lower
values of 159 and 197 W m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> respectively (Table <xref ref-type="table" rid="Ch1.T4"/>). CON
showed the largest LE bias. Regarding BR, the simulation by DRI with a value
of 1.35 was in very good agreement with the observations. The DRI simulation
resulted in the least biased partitioning of the surface energy fluxes at
Collelongo. However, FS showed that frequent atmospheric reinitialisations
can add value.</p>
      <p>In summary, the model presented a good spatial variability of BR, and the
agreement with observations was highest for FS. However, when focusing on the
sites that represent at least 50 % of the land cover at the corresponding
model grid cell, it was DRI that performed well for H at Vielsalm and for LE
at Collelongo. For Collelongo, this resulted in the least biased simulation
of the partitioning of the surface energy fluxes, translating into a better BR
estimate. The use of a daily reinitialised atmosphere and land surface
improved the correct partitioning of the surface energy fluxes, whereas the
continuous land surface initialisation as in FS could not improve the
representation of the surface energy fluxes. The high values of G were caused
by the large overestimation of the soil temperature and could be solved by
implementing additional parameterisations for the canopy layer and soil
surface layer. This implementation could alter the energy budget available
for the turbulent fluxes, but this lies outside the scope of this study.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusions</title>
      <p>An assessment of three downscaling approaches has been performed using the
regional climate model ALARO-0 coupled to the land surface model SURFEXv5,
with lateral and initial boundary conditions from ERA-Interim. The
simulations were applied for a 10-year period from 1991 to 2000, for a
western European domain. The performance of ALARO-0 with SURFEX has already
been validated for NWP applications <xref ref-type="bibr" rid="bib1.bibx22" id="paren.70"/>, and here we present an
evaluation for long-term climate simulations.</p>
      <p>We compared the commonly used approach of a continuous climate simulation
with two alternative methods of frequently reinitialising the RCM boundary
conditions, combined with either a daily reinitialised or continuous land
surface. The use of a daily reinitialised atmosphere outperformed the
continuous (CON) approach for winter and summer 2 m temperature, and
deteriorated the summer precipitation. However, the use of a continuous land
surface (FS) with a daily reinitialised atmosphere improved the summer
precipitation relative to the full continuous approach. Furthermore, it
improved the winter 2 m temperature, whereas it resulted in a neutral impact
on the summer 2 m temperature and the winter precipitation, despite a slight
deterioration over the Mediterranean. The SSTs were reinitialised daily
together with the atmosphere, as compared to the monthly updated SSTs in the
continuous approach.</p>
      <p>The seasonal cycle of the 2 m temperature and precipitation was different for
three selected subdomains that covered large climate variability. Both the
temperate climate of mid-Europe and the continental climate of eastern Europe
indicated more seasonal variability than the Mediterranean climate of the
Iberian Peninsula. The simulation of the 2 m temperature had improved when
applying daily reinitialised atmosphere with continuous land surface, despite
an overestimation of the summer 2 m temperature. Precipitation biases were
larger and are perhaps associated with the tendency for ERA-Interim to be
wetter than E-OBS, and the low spatial coverage by the observations in some
regions. It was clear that the agreement for the precipitation between the
model and the observations was highest during summer, while other seasons
showed stronger deviations.</p>
      <p>During summer, the interaction between the land surface and the overlaying
atmosphere is largest. The 2 m temperature interacts with the soil moisture
and influences the partitioning of the surface energy fluxes. The daily
reinitialisation of the atmosphere improved the correct partitioning of the
latent and sensible heat flux, although the biases were still quite large to
be conclusive. Still, this approach outperformed the use of a continuous
simulation. For a more comprehensive analysis, future research will consider
including more FLUXNET stations. A more in-depth analysis on the interaction
between 2 m temperature, precipitation and surface energy fluxes can reveal
soil–moisture–temperature coupling <xref ref-type="bibr" rid="bib1.bibx25" id="paren.71"/>, but this lies outside
the scope of this study.</p>
      <p>In conclusion, this study demonstrated that the approach of a daily
reinitialised atmosphere was superior over the full continuous approach. The
use of a continuous surface next to a daily reinitialised atmosphere improved
the winter temperature and summer precipitation. We recommend using FS in a
set-up with GCM forcing for climate simulations with ALARO-0.</p>
</sec>
<sec id="Ch1.S6">
  <title>Code and data availability</title>
      <p>The used ALADIN codes, along with all related intellectual property rights,
are owned by the members of the ALADIN consortium. Access to the ALADIN
System, or elements thereof, can be granted upon request and for research
purposes only. The used SURFEX codes are freely available, together with the
ECOCLIMAP database, at
<uri>http://www.cnrm-game-meteo.fr/surfex///spip.php?rubrique8</uri>.</p>
      <p>This study is based on large datasets written in .FA and .lfi format. The
relevant output is exported to R datasets. Due to licensing restrictions,
this model output is not made publicly available. However, for the purpose of
the review, the data can be made available for the editor and reviewer upon
request by contacting Julie Berckmans.</p>
</sec>

      
      </body>
    <back><notes notes-type="authorcontribution">

      <p>J. Berckmans performed the model simulations CON, DRI, and FS
and analysed the results. J. Berckmans drafted the manuscript. O. Giot and
R. De Troch designed R tools for the analysis. O. Giot designed the
experiment CON. R. Hamdi designed the experiment DRI and FS and developed the
model code for the implementation of SURFEX within ALARO-0. P. Termonia and
R. Ceulemans provided overall guidance during the project. R. Ceulemans and
R. Hamdi were the project contractors. All co-authors contributed to the
writing and the revising of the manuscript.</p>
  </notes><ack><title>Acknowledgements</title><p>We acknowledge the E-OBS dataset from the EU-FP6 project ENSEMBLES
(<uri>http://ensembles-eu.metoffice.com</uri>) and the data providers in the
ECA&amp;D project (<uri>http://www.ecad.eu</uri>). This work used eddy-covariance
data acquired and shared by the FLUXNET community. The validation data have
been collected and prepared by the individual site PIs and their teams. We
would like to thank Marc Aubinet (Vielsalm), Giorgio Matteucci (Collelongo),
Reinhart Ceulemans, Ivan Janssens (Brasschaat), Eddy Moors (Loobos),
Christian Bernhofer (Tharandt), Bernard Longdoz (Hesse) and Denis Loustau (Le
Bray) for contributing data to this study. This research was funded by the
Belgian Federal Science Policy Office under the BRAIN.be program as MASC
contract no. BR/121/A2 and supported by the research project no.
BR/132/A1/FORBIOCLIMATE. The authors thank A. L. Hirsch and the anonymous
referee for their valuable suggestions to improve the manuscript notably. The
authors also like to thank Annelies Duerinckx (Royal Meteorological Institute
of Belgium, Brussels) for the fruitful discussions.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?> Edited by: D. Lawrence<?xmltex \hack{\newline}?> Reviewed by:
A. L. Hirsch and one anonymous referee</p></ack><ref-list>
    <title>References</title>

      <ref id="bib1.bibx1"><label>ALADIN International Team(1997)</label><mixed-citation>
ALADIN International Team: The ALADIN project: Mesoscale modelling seen as
a basic tool for weather forecasting and atmospheric research, WMO Bulletin,
46, 317–324, 1997.</mixed-citation></ref>
      <ref id="bib1.bibx2"><label>Anthes et al.(1989)</label><mixed-citation>
Anthes, R. A., Kuo, Y.-H., Hsie, E.-Y., Low-Nam, S., and Bettge, T. W.:
Estimation skill and uncertainty in regional numerical models, Q. J. Roy.
Meteor. Soc., 115, 763–806, 1989.</mixed-citation></ref>
      <ref id="bib1.bibx3"><label>Aubinet et al.(1999)</label><mixed-citation>
Aubinet, M., Grelle, A., Ibrom, A., Rannik, U., Moncrieff, J., Foken, T.,
Kowalski, A. S., Martin, P. H., Berbigier, P., Bernhofer, Ch., Clement, R.,
Elbers, J., Granier, A., Grünwald, T., Morgenstern, K., Pilegaard, K.,
Rebmann, C., Snijders, W., Valentini, R., and Vesala, T.: Estimates of the
annual net carbon and water exchange of forests: the EUROFLUX methodology,
Adv. Ecol. Res., 30, 113–175, 1999.</mixed-citation></ref>
      <ref id="bib1.bibx4"><label>Baldocchi et al.(2001)</label><mixed-citation>
Baldocchi, D., Falge, E., Lianhong, G., Olson, R., Hollinger, D., Running,
S., Anthoni, P., Bernhofer, Ch., Davis, K., Evans, R., Fuentes, J.,
Goldstein, A., Katul, G., Law, B., Lee, X., Malhi, Y., Meyers, T., Munger,
W., Oechel, W., Paw, K. T., Pilegaard, K., Schmid, H. P., Valentini, R.,
Verma, S., Vesala, T., Wilson, K., and Wofsy, S.: FLUXNET: a new tool to
study the temporal and spatial variability of ecosystem-scale carbon dioxide,
water vapor and energy flux densities, B. Am. Meteorol. Soc., 82, 2415–2435,
2001.</mixed-citation></ref>
      <ref id="bib1.bibx5"><label>Best et al.(2004)</label><mixed-citation>
Best, M. J., Beljaars, A., Polcher, J., and Viterbo, P.: A proposed structure
for coupling tiled surfaces with the planetary boundary layer, J.
Hydrometeorol., 5, 1271–1278, 2004.</mixed-citation></ref>
      <ref id="bib1.bibx6"><label>Boone and Wetzel(1999)</label><mixed-citation>
Boone, A. and Wetzel, P. J.: A simple method for modeling sub-grid soil
texture variability for use in an atmospheric climate model, J. Meteorol.
Soc. Jpn., 77, 317–333, 1999.</mixed-citation></ref>
      <ref id="bib1.bibx7"><label>Bowen(1926)</label><mixed-citation>
Bowen, I. S.: The ratio of heat losses by conduction and by evaporation from
any water surface, Phys. Rev. Lett., 27, 779–787, 1926.</mixed-citation></ref>
      <ref id="bib1.bibx8"><label>Bubnová et al.(1995)</label><mixed-citation>
Bubnová, R., Hello, G., Bénard, P., and Geleyn, J.-F.: Integration of the
fully elastic equations cast in the hydrostatic pressure terrain-following
coordinate in the framework of the ARPEGE/Aladin NWP system, Mon. Weather
Rev., 123, 515–535, 1995.</mixed-citation></ref>
      <ref id="bib1.bibx9"><label>Christensen et al.(2007)</label><mixed-citation>
Christensen, J. H., Carter, T. R., Rummukainen, M., and Amanatidis, G.:
Evaluating the performance and utility of regional climate models: the
PRUDENCE project, Climate Change, 81, 1–6, 2007.</mixed-citation></ref>
      <ref id="bib1.bibx10"><label>Davies(1976)</label><mixed-citation>
Davies, H. C.: A lateral boundary formulation for multi-level prediction
models, Q. J. Roy. Meteor. Soc., 102, 405–418,
1976.</mixed-citation></ref>
      <ref id="bib1.bibx11"><label>De Troch et al.(2013)</label><mixed-citation>
De Troch, R., Hamdi, R., Van De Vyver, H., Geleyn, J.-F., and Termonia, P.:
Multiscale performance of the ALARO-0 Model for simulating extreme summer
precipitation climatology in Belgium, J. Climate, 26, 8895–8915,
2013.</mixed-citation></ref>
      <ref id="bib1.bibx12"><label>Dee et al.(2011)</label><mixed-citation>
Dee, D. P., Uppala, S. M., Simmons, A. J., Berrisford, P., Poli, P., Kobayashi,
S., Andrae, U., Balmaseda, M. A., Balsamo, G., Bauer, P., Bechtold, P.,
Beljaars, A. C. M., van de Berg, L., Bidlot, J., Bormann, N., Delsol, C.,
Dragani, R., Fuentes, M., Geer, A. J., Haimberger, L., Healy, S. B.,
Hersbach, H., Hólm, E. V., Isaksen, L., Kållberg, P., Köhler, M.,
Matricardi, M., McNally, A. P., Monge-Sanz, B. M., Morcrette, J.-J., Park,
B.-K., Peubey, C., de Rosnay, P., Tavolato, C., Thépaut, J.-N., and
Vitart, F.: The ERA-Interim reanalysis: configuration and performance of the
data assimilation system, Q. J. Roy. Meteor. Soc., 137, 553–597, 2011.</mixed-citation></ref>
      <ref id="bib1.bibx13"><label>Dickinson et al.(1989)</label><mixed-citation>
Dickinson, R. E., Errico, R. M., Giorgi, F., and Bates, G. T.: A regional
climate model for the Western United States, Clim. Change, 15, 383–422,
1989.</mixed-citation></ref>
      <ref id="bib1.bibx14"><label>Faggian(2015)</label><mixed-citation>
Faggian, P.: Climate Change Projections for Mediterranean Region with Focus
over Alpine Region and Italy, J. Environ. Sci.
Eng., 4, 482–500, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx15"><label>Gerard(2007)</label><mixed-citation>
Gerard, L.: An integrated package for subgrid convection, clouds and
precipitation compatible with the meso-gamma scales, Q. J. Roy. Meteor. Soc.,
133, 711–730, 2007.</mixed-citation></ref>
      <ref id="bib1.bibx16"><label>Gerard and Geleyn(2005)</label><mixed-citation>
Gerard, L. and Geleyn, J.-F.: Evolution of a subgrid deep convection
parametrization in a limited area model with increasing resolution, Q. J.
Roy. Meteor. Soc., 131, 2293–2312, 2005.</mixed-citation></ref>
      <ref id="bib1.bibx17"><label>Gerard et al.(2009)</label><mixed-citation>
Gerard, L., Piriou, J.-M., Brozková, R., Geleyn, J.-F., and Banciu, D.:
Cloud and precipitation parameterization in a meso-gamma-scale operational
weather prediction model, Mon. Weather Rev., 137, 3960–3977, 2009.</mixed-citation></ref>
      <ref id="bib1.bibx18"><label>Giorgi(2006)</label><mixed-citation>
Giorgi, F.: Regional climate modeling: status and perspectives, J. Physics,
139, 101–118, 2006.</mixed-citation></ref>
      <ref id="bib1.bibx19"><label>Giorgi and Mearns(1999)</label><mixed-citation>
Giorgi, F. and Mearns, L. O.: Introduction to special section: regional
climate modeling revisited, J. Geophys. Res., 104, 6335–6352, 1999.</mixed-citation></ref>
      <ref id="bib1.bibx20"><label>Giot et al.(2016)</label><mixed-citation>Giot, O., Termonia, P., Degrauwe, D., De Troch, R., Caluwaerts, S., Smet, G.,
Berckmans, J., Deckmyn, A., De Cruz, L., De Meutter, P., Duerinckx, A.,
Gerard, L., Hamdi, R., Van den Bergh, J., Van Ginderachter, M., and Van
Schaeybroeck, B.: Validation of the ALARO-0 model within the EURO-CORDEX
framework, Geosci. Model Dev., 9, 1143–1152, <ext-link xlink:href="http://dx.doi.org/10.5194/gmd-9-1143-2016" ext-link-type="DOI">10.5194/gmd-9-1143-2016</ext-link>,
2016.</mixed-citation></ref>
      <ref id="bib1.bibx21"><label>Hamdi et al.(2012)</label><mixed-citation>
Hamdi, R., Van de Vyver, H., and Termonia, P.: New cloud and microphysics
parameterisation for use in high-resolution dynamical downscaling:
application for summer extreme temperature over Belgium, Int. J. Climatol.,
32, 2051–2065, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx22"><label>Hamdi et al.(2014)</label><mixed-citation>Hamdi, R., Degrauwe, D., Duerinckx, A., Cedilnik, J., Costa, V., Dalkilic,
T., Essaouini, K., Jerczynki, M., Kocaman, F., Kullmann, L., Mahfouf, J.-F.,
Meier, F., Sassi, M., Schneider, S., Vána, F., and Termonia, P.:
Evaluating the performance of SURFEXv5 as a new land surface scheme for the
ALADINcy36 and ALARO-0 models, Geosci. Model Dev., 7, 23–39,
<ext-link xlink:href="http://dx.doi.org/10.5194/gmd-7-23-2014" ext-link-type="DOI">10.5194/gmd-7-23-2014</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx23"><label>Haylock et al.(2008)</label><mixed-citation>Haylock, M. R., Hofstra, N., Klein Tank, A. M. G., Klok, E. J., Jones, P. D.,
and New, M.: A European daily high-resolution gridded data set of surface
temperature and precipitation for 1950-2006, J. Geophys. Res., 113, D20119,
<ext-link xlink:href="http://dx.doi.org/10.1029/2008JD010201" ext-link-type="DOI">10.1029/2008JD010201</ext-link>, 2008.</mixed-citation></ref>
      <ref id="bib1.bibx24"><label>Jacob et al.(2014)</label><mixed-citation>
Jacob, D., Petersen, J., Eggert, B., Alias, A., Christensen, O. B., Bouwer,
L. M., Braun, A., Colette, A., Déqué, M., Georgievski, G.,
Georgopoulou, E., Gobiet, A., Menut, L., Nikulin, G., Haensler, A.,
Hempelmann, N., Jones, C., Keuler, K., Kovats, S., Kröner, N., Kotlarski,
S., Kriegsmann, A., Martin, E., van Meijgaard, E., Moseley, C., Pfeifer,
S., Preuschmann, S., Radermacher, C., Radtke, K., Rechid, D., Rounsevell, M.,
Samuelsson, P., Somot, S., Soussana, J.-F., Teichmann, C., Valentini, R.,
Vautard, R., Weber, B., and Yiou, P.: EURO-CORDEX: new high-resolution
climate change projections for European impact research, Reg. Environ.
Change, 14, 563–578, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx25"><label>Jaeger et al.(2009)</label><mixed-citation>
Jaeger, E. B., Stöckli, R., and Seneviratne, S. I.: Analysis of planetary
boundary layer fluxes and land-atmosphere coupling in the regional climate
model CLM, J. Geophys. Res., 114, 1–15, 2009.</mixed-citation></ref>
      <ref id="bib1.bibx26"><label>Koster and Suarez(2001)</label><mixed-citation>
Koster, R. D. and Suarez, M. J.: Soil moisture memory in climate models, J.
Hydrometeorology, 2, 558–570, 2001.</mixed-citation></ref>
      <ref id="bib1.bibx27"><label>Kotlarski et al.(2012)</label><mixed-citation>
Kotlarski, S., Hagemann, S., Krahe, P., Podzun, R., and Jacob, D.: The Elbe
river flooding 2002 as seen by an extended regional climate model, J.
Hydrology, 472–473, 169–183, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx28"><label>Kotlarski et al.(2014)</label><mixed-citation>Kotlarski, S., Keuler, K., Christensen, O. B., Colette, A., Déqué,
M., Gobiet, A., Goergen, K., Jacob, D., Lüthi, D., van Meijgaard, E.,
Nikulin, G., Schär, C., Teichmann, C., Vautard, R., Warrach-Sagi, K., and
Wulfmeyer, V.: Regional climate modeling on European scales: a joint standard
evaluation of the EURO-CORDEX RCM ensemble, Geosci. Model Dev., 7,
1297–1333, <ext-link xlink:href="http://dx.doi.org/10.5194/gmd-7-1297-2014" ext-link-type="DOI">10.5194/gmd-7-1297-2014</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx29"><label>Leung et al.(2003)</label><mixed-citation>
Leung, L. R., Mearns, L. O., Giorgi, F., and Wilby, R. L.: Regional climate
research, B. Am. Meteorol. Soc., 84, 89–95, 2003.</mixed-citation></ref>
      <ref id="bib1.bibx30"><label>Lindstedt et al.(2015)</label><mixed-citation>
Lindstedt, D., Lind, P., Kjellström, E., and Jones, C.: A new regional
climate model operating at the meso-gamma scale: performance over Europe,
Tellus, 67, 1–23, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx31"><label>Lo et al.(2008)</label><mixed-citation>
Lo, J. C.-F., Yang, Z.-L., and Pielke Sr., R. A.: Assessment of three
dynamical climate downscaling methods using the Weather Research and
Forecasting (WRF) model, J. Geophys. Res., 113, 1–16, 2008.</mixed-citation></ref>
      <ref id="bib1.bibx32"><label>Lucas-Picher et al.(2013)</label><mixed-citation>
Lucas-Picher, P., Boberg, F., Christensen, J. H., and Berg, P.: Dynamical
downscaling with reinitializations: a method to generate finescale climate
datasets suitable for impact studies, J. Hydrometeorol., 14, 1159–1174,
2013.</mixed-citation></ref>
      <ref id="bib1.bibx33"><label>Masson(2000)</label><mixed-citation>
Masson, V.: A physically-based scheme for the urban energy budget in
atmospheric models, Bound.-Lay. Meteorol., 94, 357–397, 2000.</mixed-citation></ref>
      <ref id="bib1.bibx34"><label>Masson et al.(2003)</label><mixed-citation>
Masson, V., Champeaux, J.-L., Chauvin, F., Meriguet, C., and Lacaze, R.: A
global database of land surface parameters at 1 km resolution in
meteorological and climate models, J. Climate, 16, 1261–1282, 2003.</mixed-citation></ref>
      <ref id="bib1.bibx35"><label>Masson et al.(2013)</label><mixed-citation>Masson, V., Le Moigne, P., Martin, E., Faroux, S., Alias, A., Alkama, R.,
Belamari, S., Barbu, A., Boone, A., Bouyssel, F., Brousseau, P., Brun, E.,
Calvet, J.-C., Carrer, D., Decharme, B., Delire, C., Donier, S., Essaouini,
K., Gibelin, A.-L., Giordani, H., Habets, F., Jidane, M., Kerdraon, G.,
Kourzeneva, E., Lafaysse, M., Lafont, S., Lebeaupin Brossier, C., Lemonsu,
A., Mahfouf, J.-F., Marguinaud, P., Mokhtari, M., Morin, S., Pigeon, G.,
Salgado, R., Seity, Y., Taillefer, F., Tanguy, G., Tulet, P., Vincendon, B.,
Vionnet, V., and Voldoire, A.: The SURFEXv7.2 land and ocean surface platform
for coupled or offline simulation of earth surface variables and fluxes,
Geosci. Model Dev., 6, 929–960, <ext-link xlink:href="http://dx.doi.org/10.5194/gmd-6-929-2013" ext-link-type="DOI">10.5194/gmd-6-929-2013</ext-link>, 2013.
</mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bibx36"><label>Napoly et al.(2016)</label><mixed-citation>
Napoly, A., Boone, A., Samuelsson, P., Gollvik, S., Martin, E., Seferian, R.,
Carrer, D., Decharme, B., and Jarlan, L.: The Interactions between
Soil-Biosphere-Atmosphere (ISBA) land surface model Multi-Energy Balance
(MEB) option in SURFEX – Part 2: Model evaluation for local scale forest
sites, Geosci. Model Dev. Discuss., doi:10.5194/gmd-2016-270, in review,
2016.</mixed-citation></ref>
      <ref id="bib1.bibx37"><label>Noilhan and Mahfouf(1996)</label><mixed-citation>
Noilhan, J. and Mahfouf, J.-F.: The ISBA land surface parameterisation
scheme, Global Planet. Change, 13, 145–159, 1996.</mixed-citation></ref>
      <ref id="bib1.bibx38"><label>Noilhan and Planton(1989)</label><mixed-citation>
Noilhan, J. and Planton, S.: A simple parameterization of land surface
processes for meteorological models, Mon. Weather Rev., 117, 536–549, 1989.</mixed-citation></ref>
      <ref id="bib1.bibx39"><label>Phillips(1956)</label><mixed-citation>
Phillips, N. A.: The general circulation of the atmosphere: a numerical
experiment, Q. J. Roy. Meteor. Soc., 82, 123–164, 1956.</mixed-citation></ref>
      <ref id="bib1.bibx40"><label>Qian et al.(2003)</label><mixed-citation>
Qian, J.-H., Seth, A., and Zebiak, S.: Reinitialized versus continuous
simulations for regional climate downscaling, Mon. Weather Rev., 131,
2857–2874, 2003.</mixed-citation></ref>
      <ref id="bib1.bibx41"><label>Rauscher et al.(2010)</label><mixed-citation>
Rauscher, S. A., Coppola, E., Piani, C., and Giorgi, F.: Resolution effects
on regional climate model simulations of seasonal precipitation over Europe,
Clim. Dynam., 35, 685–711, 2010.</mixed-citation></ref>
      <ref id="bib1.bibx42"><label>Ritter and Geleyn(1992)</label><mixed-citation>
Ritter, B. and Geleyn, J.-F.: A comprehensive radiation scheme for numerical
weather prediction models with potential applications in climate simulations,
Mon. Weather Rev., 120, 303–325, 1992.</mixed-citation></ref>
      <ref id="bib1.bibx43"><label>Seneviratne et al.(2006)</label><mixed-citation>
Seneviratne, S. I., Lüthi, D., Litschi, M., and Schär, C.:
Land-atmosphere coupling and climate change in Europe, Nature, 443, 205–209,
2006.</mixed-citation></ref>
      <ref id="bib1.bibx44"><label>Seneviratne et al.(2010)</label><mixed-citation>
Seneviratne, S. I., Corti, T., Davin, E. L., Hirschi, M., Jaeger, E. B.,
Lehner, I., Orlowsky, B., and Teuling, A. J.: Investigating soil
moisture-climate interactions in a changing climate: A review, Earth-Sci.
Rev., 99, 125–161, 2010.</mixed-citation></ref>
      <ref id="bib1.bibx45"><label>Voldoire et al.(2013)</label><mixed-citation>
Voldoire, A., Sanchez-Gomez, E., Salas y Mélia, D., Decharme, B., Cassou,
C., Sénési, S., Valcke, S., Beau, I., Alias, A., Chevalier, M.,
Déqué, M., Deshayes, J., Douville, H., Fernandez, E., Madec, G.,
Maisonnave, E., Moine, M.-P., Planton, S., Saint-Martin, D., Szopa, S.,
Tyteca, S., Alkama, R., Belamari, S., Braun, A., Coquart, L., and Chauvin,
F.: The CNRM-CM5.1 global climate model: description and basic evaluation,
Clim. Dynam., 40, 2091–2121, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx46"><label>von Storch et al.(2000)</label><mixed-citation>
von Storch, H., Langenberg, H., and Feser, F.: A spectral nudging technique
for dynamical downscaling purposes, Mon. Weather Rev., 128, 3664–3673, 2000.</mixed-citation></ref>
      <ref id="bib1.bibx47"><label>Wilson et al.(2002)</label><mixed-citation>
Wilson, K., Goldstein, A., Falge, E., Aubinet, M., Baldocchi, D., Berbigier,
P., Bernhofer, C., Ceulemans, R., Dolman, H., Field, C., Grelle, A., Ibrom,
A., Law, B. E., Kowalski, A., Meyers, T., Moncrieff, J., Monson, R., Oechel,
W., Tenhunen, J., Valentini, R., and Verma, S.: Energy balance closure at
FLUXNET sites, Agr. Forest Meteorol., 113, 223–243, 2002.</mixed-citation></ref>
      <ref id="bib1.bibx48"><label>Wilson et al.(2012)</label><mixed-citation>
Wilson, T. B., Meyers, T. P., Kochendorfer, J., Anderson, M. C., and Heuer,
M.: The effect of soil surface litter residue on energy and carbon fluxes in
a deciduous forest, Agr. Forest Meteorol., 161, 134–147, 2012.</mixed-citation></ref>

  </ref-list><app-group content-type="float"><app><title/>

    </app></app-group></back>
    <!--<article-title-html>Reinitialised versus continuous regional climate simulations using ALARO-0 coupled to the land surface model SURFEXv5</article-title-html>
<abstract-html><p class="p">Dynamical downscaling in a continuous approach using initial and boundary
conditions from a reanalysis or a global climate model is a common method for
simulating the regional climate. The simulation potential can be improved by
applying an alternative approach of reinitialising the atmosphere, combined
with either a daily reinitialised or a continuous land surface. We evaluated
the dependence of the simulation potential on the running mode of the
regional climate model ALARO coupled to the land surface model
Météo-France SURFace EXternalisée (SURFEX), and driven by the
ERA-Interim reanalysis. Three types of downscaling simulations were carried
out for a 10-year period from 1991 to 2000, over a western European domain at
20 km horizontal resolution: (1) a continuous simulation of both the
atmosphere and the land surface, (2) a simulation with daily
reinitialisations for both the atmosphere and the land surface and (3) a
simulation with daily reinitialisations of the atmosphere while the land
surface is kept continuous. The results showed that the daily
reinitialisation of the atmosphere improved the simulation of the 2 m
temperature for all seasons. It revealed a neutral impact on the daily
precipitation totals during winter, but the results were improved for the
summer when the land surface was kept continuous. The behaviour of the three
model configurations varied among different climatic regimes. Their seasonal
cycle for the 2 m temperature and daily precipitation totals was very
similar for a Mediterranean climate, but more variable for temperate and
continental climate regimes. Commonly, the summer climate is characterised by
strong interactions between the atmosphere and the land surface. The results
for summer demonstrated that the use of a daily reinitialised atmosphere
improved the representation of the partitioning of the surface energy fluxes.
Therefore, we recommend using the alternative approach of the daily
reinitialisation of the atmosphere for the simulation of the regional
climate.</p></abstract-html>
<ref-html id="bib1.bib1"><label>ALADIN International Team(1997)</label><mixed-citation>
ALADIN International Team: The ALADIN project: Mesoscale modelling seen as
a basic tool for weather forecasting and atmospheric research, WMO Bulletin,
46, 317–324, 1997.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>Anthes et al.(1989)</label><mixed-citation>
Anthes, R. A., Kuo, Y.-H., Hsie, E.-Y., Low-Nam, S., and Bettge, T. W.:
Estimation skill and uncertainty in regional numerical models, Q. J. Roy.
Meteor. Soc., 115, 763–806, 1989.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>Aubinet et al.(1999)</label><mixed-citation>
Aubinet, M., Grelle, A., Ibrom, A., Rannik, U., Moncrieff, J., Foken, T.,
Kowalski, A. S., Martin, P. H., Berbigier, P., Bernhofer, Ch., Clement, R.,
Elbers, J., Granier, A., Grünwald, T., Morgenstern, K., Pilegaard, K.,
Rebmann, C., Snijders, W., Valentini, R., and Vesala, T.: Estimates of the
annual net carbon and water exchange of forests: the EUROFLUX methodology,
Adv. Ecol. Res., 30, 113–175, 1999.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>Baldocchi et al.(2001)</label><mixed-citation>
Baldocchi, D., Falge, E., Lianhong, G., Olson, R., Hollinger, D., Running,
S., Anthoni, P., Bernhofer, Ch., Davis, K., Evans, R., Fuentes, J.,
Goldstein, A., Katul, G., Law, B., Lee, X., Malhi, Y., Meyers, T., Munger,
W., Oechel, W., Paw, K. T., Pilegaard, K., Schmid, H. P., Valentini, R.,
Verma, S., Vesala, T., Wilson, K., and Wofsy, S.: FLUXNET: a new tool to
study the temporal and spatial variability of ecosystem-scale carbon dioxide,
water vapor and energy flux densities, B. Am. Meteorol. Soc., 82, 2415–2435,
2001.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>Best et al.(2004)</label><mixed-citation>
Best, M. J., Beljaars, A., Polcher, J., and Viterbo, P.: A proposed structure
for coupling tiled surfaces with the planetary boundary layer, J.
Hydrometeorol., 5, 1271–1278, 2004.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>Boone and Wetzel(1999)</label><mixed-citation>
Boone, A. and Wetzel, P. J.: A simple method for modeling sub-grid soil
texture variability for use in an atmospheric climate model, J. Meteorol.
Soc. Jpn., 77, 317–333, 1999.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>Bowen(1926)</label><mixed-citation>
Bowen, I. S.: The ratio of heat losses by conduction and by evaporation from
any water surface, Phys. Rev. Lett., 27, 779–787, 1926.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>Bubnová et al.(1995)</label><mixed-citation>
Bubnová, R., Hello, G., Bénard, P., and Geleyn, J.-F.: Integration of the
fully elastic equations cast in the hydrostatic pressure terrain-following
coordinate in the framework of the ARPEGE/Aladin NWP system, Mon. Weather
Rev., 123, 515–535, 1995.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>Christensen et al.(2007)</label><mixed-citation>
Christensen, J. H., Carter, T. R., Rummukainen, M., and Amanatidis, G.:
Evaluating the performance and utility of regional climate models: the
PRUDENCE project, Climate Change, 81, 1–6, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>Davies(1976)</label><mixed-citation>
Davies, H. C.: A lateral boundary formulation for multi-level prediction
models, Q. J. Roy. Meteor. Soc., 102, 405–418,
1976.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>De Troch et al.(2013)</label><mixed-citation>
De Troch, R., Hamdi, R., Van De Vyver, H., Geleyn, J.-F., and Termonia, P.:
Multiscale performance of the ALARO-0 Model for simulating extreme summer
precipitation climatology in Belgium, J. Climate, 26, 8895–8915,
2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>Dee et al.(2011)</label><mixed-citation>
Dee, D. P., Uppala, S. M., Simmons, A. J., Berrisford, P., Poli, P., Kobayashi,
S., Andrae, U., Balmaseda, M. A., Balsamo, G., Bauer, P., Bechtold, P.,
Beljaars, A. C. M., van de Berg, L., Bidlot, J., Bormann, N., Delsol, C.,
Dragani, R., Fuentes, M., Geer, A. J., Haimberger, L., Healy, S. B.,
Hersbach, H., Hólm, E. V., Isaksen, L., Kållberg, P., Köhler, M.,
Matricardi, M., McNally, A. P., Monge-Sanz, B. M., Morcrette, J.-J., Park,
B.-K., Peubey, C., de Rosnay, P., Tavolato, C., Thépaut, J.-N., and
Vitart, F.: The ERA-Interim reanalysis: configuration and performance of the
data assimilation system, Q. J. Roy. Meteor. Soc., 137, 553–597, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>Dickinson et al.(1989)</label><mixed-citation>
Dickinson, R. E., Errico, R. M., Giorgi, F., and Bates, G. T.: A regional
climate model for the Western United States, Clim. Change, 15, 383–422,
1989.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>Faggian(2015)</label><mixed-citation>
Faggian, P.: Climate Change Projections for Mediterranean Region with Focus
over Alpine Region and Italy, J. Environ. Sci.
Eng., 4, 482–500, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>Gerard(2007)</label><mixed-citation>
Gerard, L.: An integrated package for subgrid convection, clouds and
precipitation compatible with the meso-gamma scales, Q. J. Roy. Meteor. Soc.,
133, 711–730, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>Gerard and Geleyn(2005)</label><mixed-citation>
Gerard, L. and Geleyn, J.-F.: Evolution of a subgrid deep convection
parametrization in a limited area model with increasing resolution, Q. J.
Roy. Meteor. Soc., 131, 2293–2312, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>Gerard et al.(2009)</label><mixed-citation>
Gerard, L., Piriou, J.-M., Brozková, R., Geleyn, J.-F., and Banciu, D.:
Cloud and precipitation parameterization in a meso-gamma-scale operational
weather prediction model, Mon. Weather Rev., 137, 3960–3977, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>Giorgi(2006)</label><mixed-citation>
Giorgi, F.: Regional climate modeling: status and perspectives, J. Physics,
139, 101–118, 2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>Giorgi and Mearns(1999)</label><mixed-citation>
Giorgi, F. and Mearns, L. O.: Introduction to special section: regional
climate modeling revisited, J. Geophys. Res., 104, 6335–6352, 1999.
</mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>Giot et al.(2016)</label><mixed-citation>
Giot, O., Termonia, P., Degrauwe, D., De Troch, R., Caluwaerts, S., Smet, G.,
Berckmans, J., Deckmyn, A., De Cruz, L., De Meutter, P., Duerinckx, A.,
Gerard, L., Hamdi, R., Van den Bergh, J., Van Ginderachter, M., and Van
Schaeybroeck, B.: Validation of the ALARO-0 model within the EURO-CORDEX
framework, Geosci. Model Dev., 9, 1143–1152, <a href="http://dx.doi.org/10.5194/gmd-9-1143-2016" target="_blank">doi:10.5194/gmd-9-1143-2016</a>,
2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>Hamdi et al.(2012)</label><mixed-citation>
Hamdi, R., Van de Vyver, H., and Termonia, P.: New cloud and microphysics
parameterisation for use in high-resolution dynamical downscaling:
application for summer extreme temperature over Belgium, Int. J. Climatol.,
32, 2051–2065, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>Hamdi et al.(2014)</label><mixed-citation>
Hamdi, R., Degrauwe, D., Duerinckx, A., Cedilnik, J., Costa, V., Dalkilic,
T., Essaouini, K., Jerczynki, M., Kocaman, F., Kullmann, L., Mahfouf, J.-F.,
Meier, F., Sassi, M., Schneider, S., Vána, F., and Termonia, P.:
Evaluating the performance of SURFEXv5 as a new land surface scheme for the
ALADINcy36 and ALARO-0 models, Geosci. Model Dev., 7, 23–39,
<a href="http://dx.doi.org/10.5194/gmd-7-23-2014" target="_blank">doi:10.5194/gmd-7-23-2014</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>Haylock et al.(2008)</label><mixed-citation>
Haylock, M. R., Hofstra, N., Klein Tank, A. M. G., Klok, E. J., Jones, P. D.,
and New, M.: A European daily high-resolution gridded data set of surface
temperature and precipitation for 1950-2006, J. Geophys. Res., 113, D20119,
<a href="http://dx.doi.org/10.1029/2008JD010201" target="_blank">doi:10.1029/2008JD010201</a>, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>Jacob et al.(2014)</label><mixed-citation>
Jacob, D., Petersen, J., Eggert, B., Alias, A., Christensen, O. B., Bouwer,
L. M., Braun, A., Colette, A., Déqué, M., Georgievski, G.,
Georgopoulou, E., Gobiet, A., Menut, L., Nikulin, G., Haensler, A.,
Hempelmann, N., Jones, C., Keuler, K., Kovats, S., Kröner, N., Kotlarski,
S., Kriegsmann, A., Martin, E., van Meijgaard, E., Moseley, C., Pfeifer,
S., Preuschmann, S., Radermacher, C., Radtke, K., Rechid, D., Rounsevell, M.,
Samuelsson, P., Somot, S., Soussana, J.-F., Teichmann, C., Valentini, R.,
Vautard, R., Weber, B., and Yiou, P.: EURO-CORDEX: new high-resolution
climate change projections for European impact research, Reg. Environ.
Change, 14, 563–578, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>Jaeger et al.(2009)</label><mixed-citation>
Jaeger, E. B., Stöckli, R., and Seneviratne, S. I.: Analysis of planetary
boundary layer fluxes and land-atmosphere coupling in the regional climate
model CLM, J. Geophys. Res., 114, 1–15, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>Koster and Suarez(2001)</label><mixed-citation>
Koster, R. D. and Suarez, M. J.: Soil moisture memory in climate models, J.
Hydrometeorology, 2, 558–570, 2001.
</mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>Kotlarski et al.(2012)</label><mixed-citation>
Kotlarski, S., Hagemann, S., Krahe, P., Podzun, R., and Jacob, D.: The Elbe
river flooding 2002 as seen by an extended regional climate model, J.
Hydrology, 472–473, 169–183, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>Kotlarski et al.(2014)</label><mixed-citation>
Kotlarski, S., Keuler, K., Christensen, O. B., Colette, A., Déqué,
M., Gobiet, A., Goergen, K., Jacob, D., Lüthi, D., van Meijgaard, E.,
Nikulin, G., Schär, C., Teichmann, C., Vautard, R., Warrach-Sagi, K., and
Wulfmeyer, V.: Regional climate modeling on European scales: a joint standard
evaluation of the EURO-CORDEX RCM ensemble, Geosci. Model Dev., 7,
1297–1333, <a href="http://dx.doi.org/10.5194/gmd-7-1297-2014" target="_blank">doi:10.5194/gmd-7-1297-2014</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>Leung et al.(2003)</label><mixed-citation>
Leung, L. R., Mearns, L. O., Giorgi, F., and Wilby, R. L.: Regional climate
research, B. Am. Meteorol. Soc., 84, 89–95, 2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>Lindstedt et al.(2015)</label><mixed-citation>
Lindstedt, D., Lind, P., Kjellström, E., and Jones, C.: A new regional
climate model operating at the meso-gamma scale: performance over Europe,
Tellus, 67, 1–23, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>Lo et al.(2008)</label><mixed-citation>
Lo, J. C.-F., Yang, Z.-L., and Pielke Sr., R. A.: Assessment of three
dynamical climate downscaling methods using the Weather Research and
Forecasting (WRF) model, J. Geophys. Res., 113, 1–16, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>Lucas-Picher et al.(2013)</label><mixed-citation>
Lucas-Picher, P., Boberg, F., Christensen, J. H., and Berg, P.: Dynamical
downscaling with reinitializations: a method to generate finescale climate
datasets suitable for impact studies, J. Hydrometeorol., 14, 1159–1174,
2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>Masson(2000)</label><mixed-citation>
Masson, V.: A physically-based scheme for the urban energy budget in
atmospheric models, Bound.-Lay. Meteorol., 94, 357–397, 2000.
</mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>Masson et al.(2003)</label><mixed-citation>
Masson, V., Champeaux, J.-L., Chauvin, F., Meriguet, C., and Lacaze, R.: A
global database of land surface parameters at 1 km resolution in
meteorological and climate models, J. Climate, 16, 1261–1282, 2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>Masson et al.(2013)</label><mixed-citation>
Masson, V., Le Moigne, P., Martin, E., Faroux, S., Alias, A., Alkama, R.,
Belamari, S., Barbu, A., Boone, A., Bouyssel, F., Brousseau, P., Brun, E.,
Calvet, J.-C., Carrer, D., Decharme, B., Delire, C., Donier, S., Essaouini,
K., Gibelin, A.-L., Giordani, H., Habets, F., Jidane, M., Kerdraon, G.,
Kourzeneva, E., Lafaysse, M., Lafont, S., Lebeaupin Brossier, C., Lemonsu,
A., Mahfouf, J.-F., Marguinaud, P., Mokhtari, M., Morin, S., Pigeon, G.,
Salgado, R., Seity, Y., Taillefer, F., Tanguy, G., Tulet, P., Vincendon, B.,
Vionnet, V., and Voldoire, A.: The SURFEXv7.2 land and ocean surface platform
for coupled or offline simulation of earth surface variables and fluxes,
Geosci. Model Dev., 6, 929–960, <a href="http://dx.doi.org/10.5194/gmd-6-929-2013" target="_blank">doi:10.5194/gmd-6-929-2013</a>, 2013.

</mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>Napoly et al.(2016)</label><mixed-citation>
Napoly, A., Boone, A., Samuelsson, P., Gollvik, S., Martin, E., Seferian, R.,
Carrer, D., Decharme, B., and Jarlan, L.: The Interactions between
Soil-Biosphere-Atmosphere (ISBA) land surface model Multi-Energy Balance
(MEB) option in SURFEX – Part 2: Model evaluation for local scale forest
sites, Geosci. Model Dev. Discuss., doi:10.5194/gmd-2016-270, in review,
2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>Noilhan and Mahfouf(1996)</label><mixed-citation>
Noilhan, J. and Mahfouf, J.-F.: The ISBA land surface parameterisation
scheme, Global Planet. Change, 13, 145–159, 1996.
</mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>Noilhan and Planton(1989)</label><mixed-citation>
Noilhan, J. and Planton, S.: A simple parameterization of land surface
processes for meteorological models, Mon. Weather Rev., 117, 536–549, 1989.
</mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>Phillips(1956)</label><mixed-citation>
Phillips, N. A.: The general circulation of the atmosphere: a numerical
experiment, Q. J. Roy. Meteor. Soc., 82, 123–164, 1956.
</mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>Qian et al.(2003)</label><mixed-citation>
Qian, J.-H., Seth, A., and Zebiak, S.: Reinitialized versus continuous
simulations for regional climate downscaling, Mon. Weather Rev., 131,
2857–2874, 2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>Rauscher et al.(2010)</label><mixed-citation>
Rauscher, S. A., Coppola, E., Piani, C., and Giorgi, F.: Resolution effects
on regional climate model simulations of seasonal precipitation over Europe,
Clim. Dynam., 35, 685–711, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>Ritter and Geleyn(1992)</label><mixed-citation>
Ritter, B. and Geleyn, J.-F.: A comprehensive radiation scheme for numerical
weather prediction models with potential applications in climate simulations,
Mon. Weather Rev., 120, 303–325, 1992.
</mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>Seneviratne et al.(2006)</label><mixed-citation>
Seneviratne, S. I., Lüthi, D., Litschi, M., and Schär, C.:
Land-atmosphere coupling and climate change in Europe, Nature, 443, 205–209,
2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>Seneviratne et al.(2010)</label><mixed-citation>
Seneviratne, S. I., Corti, T., Davin, E. L., Hirschi, M., Jaeger, E. B.,
Lehner, I., Orlowsky, B., and Teuling, A. J.: Investigating soil
moisture-climate interactions in a changing climate: A review, Earth-Sci.
Rev., 99, 125–161, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>Voldoire et al.(2013)</label><mixed-citation>
Voldoire, A., Sanchez-Gomez, E., Salas y Mélia, D., Decharme, B., Cassou,
C., Sénési, S., Valcke, S., Beau, I., Alias, A., Chevalier, M.,
Déqué, M., Deshayes, J., Douville, H., Fernandez, E., Madec, G.,
Maisonnave, E., Moine, M.-P., Planton, S., Saint-Martin, D., Szopa, S.,
Tyteca, S., Alkama, R., Belamari, S., Braun, A., Coquart, L., and Chauvin,
F.: The CNRM-CM5.1 global climate model: description and basic evaluation,
Clim. Dynam., 40, 2091–2121, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>von Storch et al.(2000)</label><mixed-citation>
von Storch, H., Langenberg, H., and Feser, F.: A spectral nudging technique
for dynamical downscaling purposes, Mon. Weather Rev., 128, 3664–3673, 2000.
</mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>Wilson et al.(2002)</label><mixed-citation>
Wilson, K., Goldstein, A., Falge, E., Aubinet, M., Baldocchi, D., Berbigier,
P., Bernhofer, C., Ceulemans, R., Dolman, H., Field, C., Grelle, A., Ibrom,
A., Law, B. E., Kowalski, A., Meyers, T., Moncrieff, J., Monson, R., Oechel,
W., Tenhunen, J., Valentini, R., and Verma, S.: Energy balance closure at
FLUXNET sites, Agr. Forest Meteorol., 113, 223–243, 2002.
</mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>Wilson et al.(2012)</label><mixed-citation>
Wilson, T. B., Meyers, T. P., Kochendorfer, J., Anderson, M. C., and Heuer,
M.: The effect of soil surface litter residue on energy and carbon fluxes in
a deciduous forest, Agr. Forest Meteorol., 161, 134–147, 2012.
</mixed-citation></ref-html>--></article>
