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  <front>
    <journal-meta><journal-id journal-id-type="publisher">ESD</journal-id><journal-title-group>
    <journal-title>Earth System Dynamics</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ESD</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Earth Syst. Dynam.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2190-4987</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/esd-13-133-2022</article-id><title-group><article-title>Atmospheric regional climate projections <?xmltex \hack{\break}?>for the Baltic Sea region until 2100</article-title><alt-title>Atmospheric regional climate projections for the Baltic Sea region until 2100</alt-title>
      </title-group><?xmltex \runningtitle{Atmospheric regional climate projections for the Baltic Sea region until 2100}?><?xmltex \runningauthor{O. B. Christensen et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Christensen</surname><given-names>Ole Bøssing</given-names></name>
          <email>obc@dmi.dk</email>
        <ext-link>https://orcid.org/0000-0002-9513-2588</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Kjellström</surname><given-names>Erik</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6495-1038</ext-link></contrib>
        <contrib contrib-type="author" deceased="yes" corresp="no" rid="aff2">
          <name><surname>Dieterich</surname><given-names>Christian</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Gröger</surname><given-names>Matthias</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9927-5164</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3 aff2">
          <name><surname>Meier</surname><given-names>Hans Eberhard Markus</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>National Centre for Climate Research (NCKF), Danish Meteorological Institute, Copenhagen, Denmark</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Research and Development Department, Swedish Meteorological <?xmltex \hack{\break}?> and Hydrological Institute, Norrköping,
Sweden</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Physical Oceanography and Instrumentation, Leibniz Institute for <?xmltex \hack{\break}?> Baltic Sea Research Warnemünde, Rostock,
Germany</institution>
        </aff><author-comment content-type="deceased"><p/></author-comment>
      </contrib-group>
      <author-notes><corresp id="corr1">Ole Bøssing Christensen (obc@dmi.dk)</corresp></author-notes><pub-date><day>24</day><month>January</month><year>2022</year></pub-date>
      
      <volume>13</volume>
      <issue>1</issue>
      <fpage>133</fpage><lpage>157</lpage>
      <history>
        <date date-type="received"><day>29</day><month>June</month><year>2021</year></date>
           <date date-type="rev-request"><day>17</day><month>August</month><year>2021</year></date>
           <date date-type="rev-recd"><day>1</day><month>December</month><year>2021</year></date>
           <date date-type="accepted"><day>10</day><month>December</month><year>2021</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Ole Bøssing Christensen et al.</copyright-statement>
        <copyright-year>2022</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022.html">This article is available from https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022.html</self-uri><self-uri xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022.pdf">The full text article is available as a PDF file from https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e139">The Baltic Sea region is very sensitive to climate change; it is a
region with spatially varying climate and diverse ecosystems, but it is also
under pressure due to a high population in large parts of the area. Climate
change impacts could easily exacerbate other anthropogenic stressors such as
biodiversity stress from society and eutrophication of the Baltic Sea
considerably. Therefore, there has been a focus on estimations of future
climate change and its impacts in recent research. In this overview paper,
we will concentrate on a presentation of recent climate projections from
12.5 km horizontal resolution atmosphere-only regional climate models from
Coordinated Regional Climate Downscaling Experiment – European domain (EURO-CORDEX).
Comparison will also be done with corresponding prior results
as well as with coupled atmosphere–ocean regional climate models. The recent
regional climate model projections strengthen the conclusions from previous
assessments. This includes a strong warming, in particular in the north in
winter. Precipitation is projected to increase in the whole region apart
from the southern half during summer. Consequently, the new results lend
more credibility to estimates of uncertainties and robust features of future
climate change. Furthermore, the larger number of scenarios gives
opportunities to better address impacts of mitigation measures. In
simulations with a coupled atmosphere–ocean model, the climate change signal
is locally modified relative to the corresponding stand-alone atmosphere
regional climate model. Differences are largest in areas where the coupled
system arrives at different sea-surface temperatures and sea-ice conditions.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e151">For many years, hundreds of global climate projections have been produced
according to various scenarios of future greenhouse gas emissions and other
forcing factors including changes in aerosols and land use. This has been
coordinated in model intercomparison projects (MIPs) that have provided
fundamental input to the Working Group I assessment reports of the
Intergovernmental Panel on Climate Change (IPCC; IPCC, 2001, 2007, 2013,
2021). The fifth IPCC Assessment Report (AR5; IPCC, 2013) was built on the
World Climate Research Programme's (WCRP) Coupled Model Intercomparison
Project phase 5 (CMIP5) multi-model data (Taylor et al., 2012). Many general
circulation models (GCMs) participated in simulations according to several
Representative Concentration Pathway (RCP) scenarios (van Vuuren et al.,
2011). The most recent, sixth, Assessment Report (IPCC, 2021; AR6) builds on
the successor, CMIP6 (Eyring et al., 2016), that involves a new set of Shared
Socioeconomic Pathway (SSP) scenarios (O'Neill et al., 2017). This<?pagebreak page134?> has,
however, not been addressed here as, at this point, downscaling activities
based on CMIP6 projections are still lacking.</p>
      <p id="d1e154">The Baltic Sea region is highly diverse with considerable spatial
variability over small distances compared to typical GCM resolutions.
Consequently, GCMs do not represent all relevant processes at adequate
scales and results are often biased (e.g. Graham et al., 2008).
High-resolution regional climate models, nested in the GCMs, have been shown
to add value to the GCM results and to promote detailed analysis on regional
to local scales (e.g. Giorgi and Gao, 2018). At the European level,
considerable efforts have therefore been undertaken to downscale GCM
simulations to a higher horizontal resolution with RCMs. The history of
coordinated RCM simulations started in the Prediction of Regional Scenarios and Uncertainties for Defining European Climate Change Risks and Effects (PRUDENCE) project with RCMs mostly
operated at 50 km spatial resolution (Christensen and Christensen, 2007),
continued with the  Ensemble-based Predictions of Climate Changes and their Impacts (ENSEMBLES) project (van der Linden and Mitchell, 2009;
Hanel and Buishand, 2011; Kyselý et al., 2011; Räisänen and Eklund,
2011; Déqué et al., 2012; Kjellström et al., 2013) and more
recently in the EURO-CORDEX initiative, which forms part of the Coordinated
Regional climate Downscaling EXperiment (CORDEX, <uri>https://cordex.org/</uri>, last access: 14 January 2022; e.g. Giorgi et al., 2006; Jacob et al., 2014; Kotlarski et al., 2014; Keuler et
al., 2016; Kjellström et al., 2018). Most recently, the European
Copernicus Climate Change Services has supported an extension of the
available CMIP5-driven RCM downscaling simulations in the EURO-CORDEX setup
with around 12 km spatial resolution (Vautard et al., 2021; Coppola et al.,
2021). This has led to the public availability of a large amount, currently
127, of different simulations following the RCP2.6, RCP4.5, and RCP8.5
scenarios (some simulations with known errors are not counted).</p>
      <p id="d1e160">Regional climate models have been used not only for downscaling of climate
change scenarios. Also, observation-based reanalysis datasets have been
extensively downscaled with RCMs in recent years (e.g. Feser et al., 2001;
Hagemann et al., 2004; Christensen et al., 2010; Samuelsson et al., 2011;
Kotlarski et al., 2014; Prein et al., 2015). These experiments are useful
for comparing RCM results and observational data for recent decades, and
thereby for evaluation of RCM models. The RCMs are found to capture many
features of the climate in a realistic way, albeit with some systematic
errors and biases (Wibig et al., 2015; Kjellström and Christensen,
2020). As a remedy, bias correction is sometimes applied to the results
(e.g. Dosio et al., 2016). Biases are generally larger when GCMs are
downscaled instead of reanalysis data, as these show systematic biases in
their representation of the atmospheric circulation at large scales, of
temperature, humidity, and sea-surface conditions. For an area like the
Baltic Sea region, this implies that sea-surface temperatures (SSTs) and sea
ice from the coarse-scale driving GCM may not be completely adequate as
input to an RCM; this constitutes an additional source of potential
uncertainty of the downscaled regional scenarios (Kjellström and
Ruosteenoja, 2007).</p>
      <p id="d1e163">During the past decades, a number of regional coupled
atmosphere–ocean–sea-ice models with focus on the Baltic Sea and adjacent
marginal seas have therefore been developed for climate studies (e.g.
Gustafsson et al., 1998; Döscher et al., 2002; Wang et al., 2015;
Dieterich et al., 2019; Primo et al., 2019; Kelemen et al., 2019; Akhtar et
al., 2019; Sein et al., 2020). In these models, prescribed boundary
conditions at the sea surface (i.e. sea ice and SST) were replaced by online
coupled ocean models allowing for a direct and more realistic representation
of air–sea thermal feedback mechanisms (see review by Gröger et al.,
2021b). These coupled models exhibit a different model solution for many
climate variables compared to their atmosphere stand-alone counterparts,
especially over the coupled region (Gröger et al., 2015; Ho-Hagemann et
al., 2017; Primo et al., 2019; Gröger et al., 2019, 2021a). The most
recent and largest ensemble of regional coupled climate change simulations
was provided by Dieterich et al. (2019) and Gröger et al. (2019, 2021a),
and is based on the Rossby Centre Regional Climate Model (RCA4) coupled interactively to the
Nucleus for European Modelling of the Ocean (NEMO).</p>
      <p id="d1e167">Available RCM literature describes extensive studies of possible future
climate conditions for many areas, including the Baltic Sea basin (see,
e.g. Lind and Kjellström, 2008; Kjellström and Lind, 2009; Benestad,
2011; Kjellström
et al., 2011; Nikulin et al., 2011; Christensen et al.,
2015a; Christensen and Kjellström, 2018; Coppola et al., 2021). Ensembles
of climate projection simulations have been used to obtain probabilistic
climate change information, both GCM (Lind and Kjellström, 2008;
Räisänen, 2010) and RCM ensembles (Buser et al., 2010; Donat et al.,
2011). In addition, the wider range of GCM scenarios has been used to set
regional scenarios in a broader context (Lind and Kjellström, 2008;
Kjellström et al., 2016, 2018).</p>
      <p id="d1e170">This work aims at presenting climate change in the area around the Baltic
Sea, as it is projected by the very large ensemble of EURO-CORDEX RCMs at 12 km
resolution. The spread in results between the projections is used to
discuss uncertainties in future climate change. In addition to the uncoupled
atmosphere-only EURO-CORDEX RCM ensemble, we will also assess changes in an
ensemble with the atmospheric regional model RCA4 coupled to the NEMO ocean
model. A comparison between results from the stand-alone atmospheric model
and the coupled model provides input to the assessment of uncertainties in
future climate change projections for the area.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data and methods</title>
      <p id="d1e181">We will focus on data of the most commonly studied fields: surface air
temperature, average total precipitation, mean<?pagebreak page135?> wind speed at 10 m height,
incoming short-wave radiation, and average winter snow and sea-ice cover.
The consequences of extreme weather events impact many aspects of society.
Extreme precipitation often results in flooding, which often causes
extensive damage as do extreme winds in connection with low-pressure
systems. Changes in these extremes as a result of anthropogenic climate
change have received considerable attention. We will therefore also report
on extremes of daily precipitation and 10 m wind speed.</p>
      <p id="d1e184">The main results of this study build on seasonal means from the publicly
available and accessible EURO-CORDEX data, which at the time of writing
consisted of the 124 simulations indicated in Table 1 out of a current total
of 127. Three different emission scenarios have been widely used for
downscaling within CORDEX. The RCP2.6 scenario is the most moderate and will
require a targeted emission reduction worldwide. The RCP8.5 scenario, in
contrast, is consistent with large future increases in emissions, little
emission mitigation, and a continued reliance on fossil fuels for many
decades. In the middle, the RCP4.5 scenario requires a considerable amount
of mitigation but is very unlikely to achieve the 2 % warming limit
relative to pre-industrial conditions, which the Paris Agreement targets.</p>
      <p id="d1e187">In this study, we will concentrate on the warmer RCP8.5 scenario. In the
analysis, we will analyse three periods: 1981–2010, 2041–2070, and 2071–2100.
Plots corresponding to the other scenarios can be found in the Supplement.
In general, the amplitude of regional climate change for varying
scenarios scales with temperature change, while the spatial pattern is
similar (see, e.g. Christensen et al., 2015b). This means that the RCP8.5
scenario will show expected patterns of climate change with a relative
minimum of noise from interannual variability of the simulations.
Furthermore, the largest of all three RCP ensembles is the RCP8.5 one (Table 1);
hence, the analysis of these scenario simulations allows the best
estimate of model uncertainties and internal variability.</p>
      <p id="d1e190">Not all EURO-CORDEX simulations have been analysed for every variable
considered here; two WRF361H simulations do not contain solar radiation, and
snow and sea ice from several simulations either do not exist in the archive
or have not been downloaded. Some simulations with the Convection-Resolving Climate Model (crCLIM) are missing winter (DJF)
2005–2006 due to a problem when handling the transition between historical
and scenario simulations; we have repeated DJF 2004–2005 in its place. All
simulations driven by Hadley Centre Global Environment Model version 2 Earth
system configuration (HadGEM2-ES) are missing the year 2100; for these
simulations, we have used 2070–2099 as the end-of-century period.</p>
      <p id="d1e194">The second Baltic Sea Experiment (BALTEX) Assessment of
Climate Change for the Baltic Sea basin (BACC) report from 2015 (BACC II Author Team, 2015) showed similar
maps to those presented here. These results were based on the ENSEMBLES
database (van der Linden and Mitchell, 2009), consisting of simulations
following the Special Report on Emissions Scenarios (SRES) (Nakićenović et al., 2000) A1B scenario performed
in 25 km grid resolution. The periods compared were 1961–1990 and 2071–2100.
The mean GCM global temperature change weighted with the number of RCM
simulations in the ensemble, for the EURO-CORDEX and ENSEMBLES simulations,
can be seen in Table 2. Note that the first reference period differs between
ENSEMBLES (1961–1990) and EURO-CORDEX (1981–2010).</p>
      <p id="d1e197">To a high extent, maps over the Baltic Sea catchment of climate change for
the weaker emission scenarios exhibit the same patterns as the RCP8.5
climate change normalized by global temperature change; maps are available
in the Supplement.</p>

<?xmltex \floatpos{p}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e203">Model simulations of the study. These constitute the entire set of
seasonal average fields available from the Earth System Grid Federation
(ESGF; <uri>http://esgf-data.dkrz.de</uri>, last access: 31 May 2021) archive  in May 2021. There are
72 ensemble members following RCP8.5, 22 following RCP4.5, and 30 following
RCP2.6.</p></caption>
  <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-t01.png"/>
</table-wrap>

<?xmltex \floatpos{p}?><table-wrap id="Ch1.T2" specific-use="star"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e217">Average global warming from driving GCMs in each scenario, weighted
by the number of downscaling simulations of each. The warming is presented
relative to the reference period 1981–2010 for mid-century (2041–2070) and
end-of-century (2071–2100) conditions.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <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:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Project</oasis:entry>
         <oasis:entry colname="col2">Scenario</oasis:entry>
         <oasis:entry colname="col3">Ensemble size</oasis:entry>
         <oasis:entry colname="col4">Mid-century warming</oasis:entry>
         <oasis:entry colname="col5">End-of-century warming</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">ENSEMBLES</oasis:entry>
         <oasis:entry colname="col2">SRES A1B</oasis:entry>
         <oasis:entry colname="col3">13</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
         <oasis:entry colname="col5">3.00</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">EURO-CORDEX</oasis:entry>
         <oasis:entry colname="col2">RCP8.5</oasis:entry>
         <oasis:entry colname="col3">72</oasis:entry>
         <oasis:entry colname="col4">2.21</oasis:entry>
         <oasis:entry colname="col5">3.71</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">EURO-CORDEX</oasis:entry>
         <oasis:entry colname="col2">RCP4.5</oasis:entry>
         <oasis:entry colname="col3">22</oasis:entry>
         <oasis:entry colname="col4">1.67</oasis:entry>
         <oasis:entry colname="col5">2.13</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">EURO-CORDEX</oasis:entry>
         <oasis:entry colname="col2">RCP2.6</oasis:entry>
         <oasis:entry colname="col3">30</oasis:entry>
         <oasis:entry colname="col4">1.22</oasis:entry>
         <oasis:entry colname="col5">1.19</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e332">The maps below show results based on 72 regional climate change simulations
from the RCP8.5 EURO-CORDEX simulations listed in Table 1. Corresponding
plots for other scenarios and periods can be found in the Supplement. For each location, the median among ensemble members of the change
is shown together with the first and third quartiles. In the maps showing
the median, we only display grid points where 75 % of models agree on the
sign, i.e. where both quartile plots show the same sign; elsewhere, we
indicate in a white colour that the changes are not robust. We will discuss
only DJF and summer (JJA) in this study. The scatter plots below
show results for all simulations following the three commonly used scenarios
(Table 1). Where possible, we also include results from the ENSEMBLES project,
which were the basis of BACC II (Christensen et al., 2015a). In addition to
the average over the entire Baltic Sea catchment region including the Baltic
Sea, we divide the region into sea points and land points north and south of
60<inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N. In the Supplement (Tables S1–S20), tables of ensemble means
and ensemble standard deviations can be found for temperature and
precipitation, for both periods, all scenarios (including the BACC
II/ENSEMBLES SRES A1B scenario), and all five areas.</p>
      <p id="d1e345">We will also investigate the coupled-model ensemble with RCA4-NEMO. RCA4 is
set up for the EURO-CORDEX domain with a horizontal resolution of
<inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula> km and 40 vertical levels. NEMO simulates the
hydrodynamics of the Baltic Sea as well as the North Sea at <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">3.7</mml:mn></mml:mrow></mml:math></inline-formula> km resolution and 56 vertical levels (Gröger et al., 2015; Dieterich
et al., 2019). Air–sea fluxes are exchanged every 3 h between the
ocean and the atmosphere. The RCA4-NEMO ensemble consists of 22 downscaled
GCM simulations based on eight different global models for the historical period
and the RCP2.6, RCP4.5, and RCP8.5 scenarios. In addition, there is also a
reanalysis-driven simulation for the historical period.</p>
      <p id="d1e368">These results will be compared to the corresponding RCA4 atmosphere-only
simulations at 12.5 km resolution, which can be found in the EURO-CORDEX
archive. When possible, these simulations are included in the scatter
plots below.</p>
</sec>
<?pagebreak page137?><sec id="Ch1.S3">
  <label>3</label><title>Results and discussion</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Temperature</title>
      <p id="d1e386">According to the analysed EURO-CORDEX ensemble, we will see increasing air
temperature in the Baltic Sea area during the present century. According to
this ensemble, it is a robust result for all seasons, locations, simulations,
and scenarios.</p>
      <p id="d1e389">For both seasons analysed (winter and summer), the temperature change shows
spatial gradients with the strongest warming in the northeast (Fig. 1).
Winter warming is larger than summer warming and larger than the global
average warming of about 3.7 % (Table 2); in the northeast, it
approaches twice the global average warming. Larger warming than the global
average is generally expected for land areas, since land heats more quickly
than sea areas where also enhanced evaporation tends to reduce warming (e.g.
Sutton et al., 2007); it is most clearly seen in winter in the eastern part
of the area. The strong winter increase is also influenced by the feedback
mechanisms involving retreating snow and sea ice. There is a general pattern
of higher warming in the north than in the south, but there is a spread in
the magnitude of the change. This is illustrated in the columns of the
figures below. As only eight GCMs have been used for these RCP8.5 RCM
experiments, the spread between quartiles could be lower than what would
have come from an exhaustive downscaling of all CMIP5 global simulations;
Kjellström et al. (2016) compared nine GCMs, including the eight GCMs analysed
here, to 25 other CMIP5 GCMs and found the nine-member-ensemble spread over
Sweden to be comparable in summer but smaller than that in the larger GCM
ensemble in winter.</p>
      <p id="d1e392">Earlier studies have shown that the increase in winter temperatures is
strongest for the coldest episodes (Kjellström, 2004) as well as for
extreme daily maximum and minimum temperatures (Kjellström et al., 2007;
Nikulin et al., 2011). There is a significant decrease in the probability of
cold temperatures (Benestad, 2011). Warm summer extremes are projected to
become more pronounced; for example, Nikulin et al. (2011) used an ensemble
of six RCM simulations, all downscaling GCMs under the SRES A1B scenario;
the data indicate that warm extremes with a present-day (1961–1990) return
period of 20 years will be reached 4 times as often in Scandinavia by
2071–2100, with a frequency around once every 5 years in Scandinavia by
2071–2100.</p>
      <p id="d1e395">Summer warming in the Baltic Sea basin is smaller than winter warming, and
it is relatively homogeneous across the area. A tendency is seen for larger
warming over land areas in the northernmost parts of the Baltic Sea basin.
These areas are closest to the northern rim of Scandinavia and the Kola
Peninsula where warming in summer is as high as that projected for parts of
southernmost Europe (Kjellström et al., 2018). In the northeastern part
of the region, a large warming may be related to the larger temperature
increases further to the north in the Arctic, potentially connected with the
ice–albedo and other feedback mechanisms (IPCC, 2021). The strong warming in
the southeastern part of the Baltic Sea basin is related to the large-scale
pattern of warming in Europe, where the strongest summer warming is seen in
southern Europe. Similar results for other GCM–RCM combinations have been
reached in, e.g. Christensen and Christensen (2007), Kjellström et al. (2011),
and Vautard et al. (2014). A potential source of difference between
GCMs and RCMs is the different treatment of aerosols in these models. Many
of the RCMs do not include time-varying anthropogenic aerosols leading to
weaker future warming compared to GCMs (Boé et al., 2020). The
EURO-CORDEX-based results are consistent with the RCM results for 2021–2050
in Déqué et al. (2012). This study found that there is a significant
temperature response, even for the relatively short-term 2021–2050 time
frame, even though the total uncertainty related to the choice of model
combination (GCM–RCM) and sampling (natural variability) is large.
Similarly, Kjellström et al. (2013) showed early emergence already in
the first few decades of the 21st century of trends in both winter and
summer temperature despite large natural variability as represented in the
ENSEMBLES RCM projections used in BACC II.</p>
      <p id="d1e399">Corresponding changes in the daily minimum temperature and daily maximum
temperature (not shown) have the same patterns as the average temperature
change, with the expected larger magnitude of warming for minimum
temperature. A range of factors may be responsible for this decrease in
difference between minimum and maximum temperatures. This could involve
changes in the diurnal temperature range (e.g. Lindvall and Svensson, 2015)
or changes in the synoptic weather variability in combination with reduced
large-scale temperature gradients between the Atlantic Ocean and the
Eurasian continent (IPCC, 2021).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e404">Temperature change between 1981–2010 and 2071–2100 for 72
simulations from EURO-CORDEX according to the RCP8.5 scenario. <bold>(a–c)</bold>
Winter. <bold>(d–f)</bold> Summer. <bold>(a, d)</bold> Lowest quartile; <bold>(b, e)</bold> median
value; <bold>(c, f)</bold> higher quartile. In all the following figures,
panels <bold>(b, e)</bold>
depicting pointwise median values are only coloured when 75 % of the
simulations agree on the sign of the change. The Baltic Sea catchment is
indicated in yellow.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f01.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Precipitation</title>
      <p id="d1e440">The multi-model EURO-CORDEX ensemble relative precipitation change for
winter and summer is shown in Fig. 2. The ensemble is the same as that in Fig. 1.</p>
      <p id="d1e443">During winter, the relative increases are quite homogeneous, although there
are large differences between the lower and upper quartiles. These
differences are largest west of the Baltic Sea catchment (Norway) where the
amount of precipitation is particularly sensitive to different changes in
the large-scale circulation. For summer, there is a clear pattern of more
positive change in the north versus less positive change in the south. As
expected, winter increases are projected to be larger than those in summer.
Roughly, the winter increase is 25 %–35 % over most of the area in the
median, and the summer increase is 15 %–25 % for the northern part of the
area. This is consistent with the AR5 Climate Atlas, where median increases
of precipitation in the area are 10 %–20 % for the winter half year and
5 %–10 % for summer, as these<?pagebreak page138?> results correspond to the RCP4.5 scenario with
around 2.5 % of warming for the periods mapped, whereas the
EURO-CORDEX results correspond to a global warming of 3.8 <inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C.</p>
      <p id="d1e455">For summer, there is disagreement on the sign of climate change for most of
the southern half of the area, indicated by the masked-out area defined as
regions where at least 25 % of the models disagree on the sign with the
majority. Since the period mapped here consists of the three summer months of
June–August, whereas the AR5 Climate Atlas maps April–September, a
comparison of the position of the no-change area is difficult. In an
analysis of the older ENSEMBLES simulations (Déqué et al., 2012),
almost all land points in the Baltic Sea region showed significantly
positive summer precipitation signals.</p>
      <p id="d1e458">This general picture of change is not surprising. Climate models generally
project the global hydrological cycle to become more intense (e.g. Held and
Soden, 2006). For Europe, this corresponds to increasing precipitation in
northern Europe and decreasing precipitation in southern Europe, both in
winter and summer (Christensen et al., 2007). Between these areas of
projected increase and projected decrease, only small changes or changes in
different directions are projected (see, e.g. Kjellström et al., 2011).
The location of the transition zone depends on the season and is located
farther to the south in winter than in summer. In summer, this zone shifts
into the Baltic Basin: winter precipitation is projected to increase over
the entire Baltic Sea catchment, while summer precipitation is mostly
projected to only increase in the<?pagebreak page139?> northern half of the basin. In the south,
precipitation change is small for the ensemble mean, and there is a large
spread between different models with both increases and decreases.
Basically, both increases and decreases are possible in the future.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e464">Precipitation relative change (%) between 1981–2010 and
2071–2100 for 72 simulations from EURO-CORDEX according to the RCP8.5
scenario. <bold>(a–c)</bold> Winter. <bold>(d–f)</bold> Summer. <bold>(a, d)</bold> Lowest quartile; <bold>(b, e)</bold> median value; <bold>(c, f)</bold> higher quartile. In all following figures, panels <bold>(b, e)</bold> depicting
pointwise median values are only coloured when 75 % of simulations agree on
the sign of the change. The Baltic Sea catchment is indicated in red.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f02.png"/>

        </fig>

      <p id="d1e492">In Fig. 3, we show scatter plots where the relative change between 1981–2010 and
2071–2100 of precipitation is plotted against the corresponding
change of temperature for each model and each scenario. Ensemble means for
the three scenarios are indicated by the three larger symbols. This
calculation has been performed for various subsets of the Baltic Sea
catchment (see Fig. 1): the entire region; only land points; only sea
points; only land points north and south of 60<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, respectively.</p>
      <p id="d1e504">There is a strong correlation between temperature and precipitation in
winter with significant regression slopes of around five percentage points per
degree and squared correlation coefficients of 0.5 to 0.6 depending on the
sub-area. This is an indication of an approximate common sensitivity of
precipitation change to local temperature change. This correspondence breaks
down for summer, where the plots contain much more noise, indicating large
model-dependent influences on the precipitation signal. The north–south
gradient in summer precipitation change is apparent in the model averages
(compare the northern and southern land point plots), but the inter-model
spread is large.</p>
      <p id="d1e507">Due to the roughly 20 % higher average global warming in the current
RCP8.5 ensemble than in the GCMs underlying BACC II (see Table 2), we would
have expected general climate change to be around 20 % larger for
EURO-CORDEX RCP8.5 than those presented in BACC II. It is noteworthy that
this difference is not generally seen in Fig. 3, where we have plotted
temperature and precipitation change for the BACC II simulations (BACC II
Author Team, 2015) along with the three scenarios of the present analysis.
The BACC II results correspond to the RCP8.5 results both with respect to
temperature and precipitation change apart from land areas in summer where
the BACC II change is only about 80 % of the RCP8.5 result (<inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">6.5</mml:mn></mml:mrow></mml:math></inline-formula> % vs.
<inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">8.2</mml:mn></mml:mrow></mml:math></inline-formula> %).</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e532">Relative change 1981–2010 to 2071–2100 of precipitation against
temperature change for individual models and all scenarios. Scenario means
are indicated by larger black symbols. Blue squares: RCP2.6; pink triangles:
RCP4.5; red diamonds: RCP8.5; green crosses: the ENSEMBLES simulations
analysed in BACC II (2015). Plus signs in colours corresponding to the
scenario: the RCA4-NEMO atmosphere–ocean coupled simulations. Calculation
performed for subsets of the Baltic catchment: the entire catchment; sea
points; land points north and south of 60<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, respectively.
Panels <bold>(a)</bold>–<bold>(d)</bold> show winter; panels <bold>(e)</bold>–<bold>(h)</bold> show summer. The lines, with quoted slope
and squared correlation coefficient, are best fits to all EURO-CORDEX and
ENSEMBLES data but do not include coupled-model results.</p></caption>
          <?xmltex \igopts{width=384.112205pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f03.png"/>

        </fig>

      <p id="d1e563">In Christensen et al. (2019), a thorough comparison of change patterns of
mean temperature and precipitation has been performed for the PRUDENCE
simulations behind the first BACC report (BACC Author Team, 2008), the
ENSEMBLES simulations behind the second report (BACC II Author Team, 2015),
and the EURO-CORDEX data behind the present report. This analysis used
patterns of change scaled with global temperature change and is therefore
useful for pinpointing differences between the BACC reports extraneous to
the variations of general scenario strength, i.e. differences in local
sensitivity and/or change patterns apart from those due to differences in
emission scenarios. The most important differences between BACC II and the
current simulations are a slightly reduced winter warming per unit of global
warming in EURO-CORDEX compared to BACC II; a smaller wintertime
precipitation increase but a slightly larger increase of summer
precipitation over the Baltic Sea. These conclusions do not contradict the
results from Fig. 3, since a scaling with global warming would increase both
local precipitation and local temperature changes for the BACC II ENSEMBLES
results relative to RCP8.5.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Extreme precipitation</title>
      <p id="d1e574">The water-holding capacity of the atmosphere increases with increasing
temperature. Therefore, precipitation extremes are projected to increase with
climate warming (e.g. Lenderink and van Meijgaard, 2010). Several studies,
some of which are described in the following, indicate that extreme
precipitation is likely to increase in the future, even in areas and
seasons, where the average precipitation does not increase. One example is
the IPCC Special Report on extreme events (Seneviratne et al., 2012), where
it was shown that higher extremes of precipitation consistently show larger
increases than lower extremes, and higher increases than averages.</p>
      <p id="d1e577">Already simulations from the PRUDENCE project (Christensen and Christensen,
2003) showing a considerable decrease in average summer precipitation in
large parts of southern Europe at the same time showed an increased
probability of very extreme precipitation in that area as well as in the
north, where average precipitation was not projected to decrease. Quite
generally, more intense precipitation can be expected on all timescales,
from single rain showers to synoptic-scale precipitation.</p>
      <p id="d1e580">Nikulin et al. (2011) investigated an ensemble of RCM simulations following
the SRES A1B scenario with the RCA model; they showed that the 20-year
return value of precipitation extremes in Scandinavia in the period
1961–1990 was projected to decrease to 6–10 years in 2071–2100 for summer
over northern Europe and to 2–4 years in winter. Similarly, Larsen et al. (2009)
analysed a high-resolution RCM integration and reported that the
return period for 20-year rainfall events at hourly duration decreased to
about 4 years for Sweden.</p>
      <p id="d1e583">Collected results from 90 of the models from the EURO-CORDEX project are
illustrated in Fig. 4, along with results from the coupled models discussed
below. For data availability reasons at the time of writing, not all
simulations have been analysed for extreme precipitation. We will here use
the 10-year return value as representative of extreme precipitation. This is
defined as the daily precipitation amount, which is only exceeded once every
10 years on average. The model-median signal has a consistently positive
sign across the domain for the areas where more than 75 % of the model
results have the same sign. The temperature dependence of the increases in
the Baltic Sea basin (slopes in Fig. 4) are generally larger in summer than
in winter with the southern land points as an exception, the same area where
the average precipitation (Figs. 2–3) decreases. The inter-model spread is
considerably larger in summer than in winter, illustrating the greater
influence of local processes in this season; it should be noted<?pagebreak page140?> that the
increase from 19 to 90 in the number of models analysed, compared to Christensen and
Kjellström (2018), results in a considerably more robust
positive signal in the summer 10-year return value.</p>
      <p id="d1e587">The relative changes of extreme precipitation in winter (Fig. 4 upper panels)
are quite similar to the relative change in average precipitation (Fig. 2),
indicating no change in the shape of the intensity distribution function.
For summer, however, the projected change in extreme precipitation is
consistently more positive than the change in average precipitation. While
the temperature sensitivities (slopes in Figs. 3 and 4) for winter average
precipitation and winter extreme precipitation are almost identical, the
sensitivity of extremes in summer is larger than that for winter, while it is
insignificant for the average precipitation in summer. This feature is,
however, less apparent in the EURO-CORDEX results than in the PRUDENCE
results of BACC (BACC Author Team, 2008) and the ENSEMBLES results described
in BACC II (BACC II Author Team, 2015). It is not clear if this difference
is due to the fact that the RCMs are run at different horizontal resolutions
in the three projects (i.e. 50, 25, and 12.5 km, respectively), or if it is a
consequence of different model formulations in the projects or of the
large-scale climate change signal as imposed by the underlying GCMs that
also differs between the experiments.</p>
      <?pagebreak page142?><p id="d1e590">Recently, several research institutes have started employing
convection-permitting regional models (CPMs). Such models are able to run in much
higher resolution, where traditional hydrostatic RCMs with fully
parameterized convective precipitation release may produce convective
precipitation explicitly as well as parameterized, CPMs avoid this possible
double counting at high resolution. With CPMs grid distances below the
“grey zone” of 3–5 km are possible. In Lind et al. (2020), results are
presented with the CPM HIRLAM ALADIN Regional Mesoscale
Operational NWP in Europe -Climate version (HARMONIE-Climate; HCLIM), produced in a common Nordic
model collaboration (NorCP) with participation from Sweden, Norway, Denmark,
and Finland. Comparing a CPM version of HCLIM in 3 km resolution with a
non-CPM version in 12 km, it was concluded that the high-resolution model
showed better results for precipitation intensity distribution, including
extreme precipitation at subdaily timescales, for the summer precipitation
diurnal cycle, and for snow in mountains. Such better agreement now shown
for the Nordic region has previously been shown for other regions in
Europe and elsewhere (e.g. Kendon et al., 2014; Lind et al., 2016; Gao et
al., 2020).</p>
      <p id="d1e593">Based on convection-permitting models, it has been argued that changes in
precipitation extremes of a shorter duration may be larger than those for
longer timescales (e.g. Kendon et al., 2014; Lenderink and van Meijgaard, 2010).
However, other results indicate (Ban et al., 2015) that
convection-permitting models may give roughly the same increase also for
shorter durations, consistent with the Clausius–Clapeyron scaling of around
6 %–7 % per degree of warming. In a study of idealized warming experiments
repeating present-day observed weather under warmer and moister conditions
with the HCLIM model, Lenderink et al. (2019) showed that the increase in
precipitation extremes is strongly dependent on moisture availability.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e598">Relative change 1981–2010 to 2071–2100 of the 10-year return value
of daily precipitation against temperature change for individual models and
all scenarios. Scenario means are indicated by larger black symbols. Blue
squares: RCP2.6; pink triangles: RCP4.5; red diamonds: RCP8.5; green
crosses: the ENSEMBLES simulations analysed in BACC II (2015). Plus signs in
colours corresponding to the scenario: the RCA4-NEMO atmosphere–ocean
coupled simulations. Calculation performed for subsets of the Baltic
catchment: the entire catchment; sea points; land points north and south of
60<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, respectively. Panels <bold>(a)</bold>–<bold>(d)</bold> show winter; panels <bold>(e)</bold>–<bold>(h)</bold> show
summer. The lines, with quoted slope and squared correlation coefficient,
are best fits to all EURO-CORDEX and ENSEMBLES data but do not include
coupled-model results.</p></caption>
          <?xmltex \igopts{width=384.112205pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f04.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Wind speed</title>
      <p id="d1e636">Changes in the climatology of 10 m wind speed are even more uncertain
than is the case for the precipitation climate, both for seasonal mean
conditions and for extremes on shorter timescales (e.g. Kjellström et
al., 2011, 2018; Nikulin et al., 2011).</p>
      <p id="d1e639">In a study by Donat et al. (2011), annual 98th percentile daily maximum wind
speed changes in RCM simulations from the ENSEMBLES project were analysed,
for the middle of the century as well as the end of the century. The
ensemble average, like the driving GCMs, increased in a region from the
British Isles to the Baltic Sea and  decreased in the Mediterranean area.
Nikulin et al. (2011) found increasing wind speed extremes (20-year return
periods of annual maximum 10 m wind speed) over the Baltic Sea in five
out of six simulations, based on an ensemble of one RCM downscaling six
different GCMs under the A1B scenario.</p>
      <p id="d1e642">In BACC II (BACC II Author Team, 2015), an analysis of 13 ENSEMBLES
simulations showed a very small insignificant median increase in the
southern part of the Baltic Sea area; the signal is consistent with the
findings by Donat et al. (2011) but with a large spread between models.</p>
      <p id="d1e645">Figure 5 shows average changes over the Baltic Sea for the 72 EURO-CORDEX
RCP8.5 simulations, the 22 RCP4.5 simulations, and the 30 RCP2.6
simulations, which were used (Table 1). In Figs. S13–S18, we show median and
quartile maps for summer and winter for each of the three RCP scenarios.
There is very little agreement between the models about even the direction
of change for winter in the Baltic Sea area unlike the tendency for reduced
average wind speed outside of the study area over the North Atlantic (not
shown). Over the northernmost part of the Baltic Sea basin, the Bothnian
Bay, there is an indication of larger wind speed increase (or less decrease)
over the sea than over surrounding land areas. This feature has previously
been pointed out by Kjellström et al. (2011), Meier et al. (2011), and
Tobin et al. (2016), and has been related to decreases in sea ice in the
future warmer climate, leading to consequent changes in stability conditions
of the lower atmosphere. See also the comparison between regional coupled
and uncoupled simulations in Fig. 12, where the probably more consistent
treatment of ice–albedo feedback leads to a slightly larger increase in
winter. As seen in Fig. 5b, the slight increase in mean wind over the Baltic Sea in BACC II is not projected in the current
simulations.</p>
      <p id="d1e649">Summer results show consistent but small reductions of wind over land of
about 2 %–6 %. Again, in summer, there are differences between land and
ocean areas with generally larger increases, or smaller decreases, over the
Baltic Sea than its surrounding land areas.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e654">Relative change 1981–2010 to 2071–2100 of 10 m wind speed against
temperature change for individual models and all scenarios. Scenario means
are indicated by larger black symbols. Blue squares: RCP2.6; pink triangles:
RCP4.5; red diamonds: RCP8.5; green crosses: the ENSEMBLES simulations
analysed in BACC II (2015). Plus signs in colours corresponding to the
scenario: the RCA4-NEMO atmosphere–ocean coupled simulations. Calculation
performed for subsets of the Baltic catchment: the entire catchment; sea
points; land points north and south of 60<inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, respectively.
Panels <bold>(a–d)</bold> show winter; panels <bold>(e–h)</bold> show summer. The lines, with quoted slope
and squared correlation coefficient, are best fits to all EURO-CORDEX and
ENSEMBLES data but do not include coupled-model results.</p></caption>
          <?xmltex \igopts{width=384.112205pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f05.png"/>

        </fig>

      <p id="d1e678">The relative change in extreme wind speed is shown in Fig. 6 as the relative
change of the 10-year return value of daily maximum wind speed for the
EURO-CORDEX RCP-based and the BACC II SRES-based simulations considered, as
well as for the coupled RCA4-NEMO simulations. The correlation between
temperature and extreme wind is quite small, which indicates that there is
no significant signal.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e683">Relative change 1981–2010 to 2071–2100 of the 10-year return value
of 10 m daily maximum wind speed against temperature change for individual
models and all scenarios. Scenario means are indicated by larger black
symbols. Blue squares: RCP2.6; pink triangles: RCP4.5; red diamonds: RCP8.5;
green crosses: the ENSEMBLES simulations analysed in BACC II (2015). Plus
signs in colours corresponding to the scenario: the RCA4-NEMO
atmosphere–ocean coupled simulations. Calculation performed for subsets of
the Baltic catchment: the entire catchment; sea points; land points north
and south of 60<inline-formula><mml:math id="M11" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, respectively. Panels <bold>(a)</bold>–<bold>(d)</bold>
show winter; panels <bold>(e)</bold>–<bold>(h)</bold> show summer. The lines, with quoted slope and squared correlation
coefficient, are best fits to all EURO-CORDEX and ENSEMBLES data but do not
include coupled-model results.</p></caption>
          <?xmltex \igopts{width=384.112205pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f06.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e716">Average incoming surface solar radiation relative change between
1981–2010 and 2071–2100 for 70 simulations from EURO-CORDEX according to the
RCP8.5 scenario. <bold>(a–c)</bold> Winter; <bold>(d–f)</bold> summer. <bold>(a, d)</bold> Lowest
quartile; <bold>(b, e)</bold> median value; <bold>(c, f)</bold> higher quartile. For the
medians, only points where 75 % of models agree on the sign are shown. The
Baltic Sea catchment is indicated in white.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f07.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS5">
  <label>3.5</label><title>Solar irradiation</title>
      <?pagebreak page146?><p id="d1e749">In Fig. 7, we study the change in incoming solar radiation in the ensemble.
In winter, most of the area shows a considerable relative reduction of the
order of 10 %. This has been proposed to be linked to the more extensive
cloud cover in northern Europe in most EURO-CORDEX RCMs for the future
(Coppola et al., 2021). It should be noted (Bartók et al., 2017) that
global and regional models frequently disagree considerably about the change
in incoming radiation in a changing climate, with global models having a
more positive trend; this discrepancy is connected to different projections
of cloud cover, with GCMs frequently projecting a decrease, while RCMs
frequently show no significant change. We repeat here that the different
treatment of aerosols in GCMs and RCMs plays a role as many of the RCMs do
not include time-varying anthropogenic aerosols as in GCMs (Boé et al.,
2020). It has also been suggested that reduced snow cover (see Sect. 3.6
below) could contribute to attenuate gross downward solar radiation flux as
the reduced surface albedo reduces multiple reflection between the surface
and the clouds (Ruosteenoja and Räisänen, 2013).</p>
</sec>
<sec id="Ch1.S3.SS6">
  <label>3.6</label><title>Snow and sea ice</title>
      <p id="d1e760">Future snow cover is expected to decrease with climate warming, both because
more precipitation is projected to fall as rain, and because snowmelt
accelerates. As an indicator of less cold conditions, Coppola et al. (2021)
show that the number of frost days decrease by more than 2 months in large
parts of the Baltic Sea basin comparing a set of EURO-CORDEX RCMs under
RCP8.5 for 2071–2100 with 1981–2010. Simultaneously, there is an increase in
winter precipitation in Scandinavia, which may partly compensate for these
effects.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e765">Relative change 1981–2010 to 2071–2100 of average winter (DJF) snow
amount (kg/m<inline-formula><mml:math id="M12" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>) against temperature change for 84 individual model
simulations from all scenarios. Scenario means are indicated by larger
symbols. Squares: RCP2.6; triangles: RCP4.5; diamonds: RCP8.5. Purple
colour: the RCA4-NEMO atmosphere–ocean coupled simulations. Calculation
performed for subsets of land points in the Baltic catchment: the entire
catchment; land points north and south of 60<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, respectively.
The lines, with quoted slope and squared correlation coefficient, are best
fits to all EURO-CORDEX data but do not include coupled-model results.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f08.png"/>

        </fig>

      <p id="d1e792">Räisänen and Eklund (2011) analysed data from RCM simulations from
the ENSEMBLES project. The study found a decrease of snow volume across all
of Europe in the future with the only exception that the Scandinavian
mountain areas may experience a slight and statistically insignificant
increase. Räisänen (2021) found a widespread future decrease in
northern Europe for snow water equivalents also for a set of EURO-CORDEX
RCMs. It was shown that a smaller snowfall fraction together with larger
reduction of snow on the ground more than compensated for increasing
precipitation, as seen in several of the RCMs. In relative numbers, the
decrease was found to be larger in southern<?pagebreak page147?> warmer parts of Scandinavia,
while changes in absolute numbers are larger in the north. Similarly, the
results were ambiguous for the most high-altitude parts of the Scandinavian
mountains where some models indicate increasing snow water and others a
decrease. A potential increase in the latter region was also proposed by
Schuler et al. (2006) in a detailed study for Norway based on two RCM
simulations with different GCM drivers. The study concluded that the maximum
amount of snow in extreme years could be greater than in extreme years of
the recent past in spite of decreasing average snow amount.</p>
      <p id="d1e796">Winter snow cover is one of the most drastically changed climatological
quantities (Fig. 8). There is agreement between models about a reduction of
average wintertime snow amount of around 50 % on average for land grid
points north of 60<inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N for the RCP8.5 scenario, and almost 80 %
reduction for land grid points south of this latitude. Northern grid points
probably have a lower reduction due to the generally colder climate and
smaller amount of solar radiation. In addition, there is a significant
amount of mountain grid points, where the warming temperature does not reach
the freezing point as frequently as in lower-lying regions even if the
frequency is increasing in a warmer climate (Nilsen et al., 2021). The
reduction in snow amount is slightly larger than in BACC II (BACC II Author
Team, 2015). This is consistent both with the fact that the RCP8.5
scenario on average projects larger warming than the SRES A1B scenario used
in BACC II and that the precipitation increase is smaller in the RCP8.5
scenario than in SRES A1B, at least north of 60<inline-formula><mml:math id="M15" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N (see Fig. 3c).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><?xmltex \def\figurename{Figure}?><label>Figure 9</label><caption><p id="d1e819"><bold>(a–c)</bold> Average winter sea-ice cover relative change between
1981–2010 and 2071–2100 for the simulations from EURO-CORDEX according to
the RCP8.5 scenario driven by the GCMs where RCA4-NEMO simulations exist.
These values have been interpolated before the RCM simulations from the
driving coupled GCM; note that several simulations have sea ice in the
Baltic Sea in the present-day period but not in the Bothnian Bay. For
comparison, in panels <bold>(d–f)</bold>, we also show the corresponding fields from the
corresponding five coupled RCA4-NEMO simulations where sea-ice cover is
calculated inside the regional model. <bold>(a, d)</bold> Lowest quartile;
<bold>(b, e)</bold> median value; <bold>(c, f)</bold> higher quartile. For the medians, only
points where 75 % of models agree on the sign are shown.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f09.png"/>

        </fig>

      <p id="d1e842">It is only in high-altitude parts of central and northern Scandinavia that
changes are limited with relatively large amounts of snow also in the
future. At high altitude, the increase of winter precipitation may be
compensating for the increase in melting with higher temperature. Also the
fact that increasing temperatures may not reach the melting point is
significant; see, e.g. Gröger et al. (2021a) Fig. 12b. However, also in
these high-altitude regions, the warmer future climate results in a shorter
snow season with accumulation starting later and spring melt starting
earlier, which acts to reduce the total amount of snow (Räisänen,
2021).</p>
      <p id="d1e845">Sea-ice cover is not a product of the RCM but rather an input originating
from the driving GCM. We will show the changes in interpolated sea-ice field
for the RCP8.5 scenario in Fig. 9, as these changes are large and are
decisive for the change in climate between the periods. In order to<?pagebreak page148?> compare
to a more consistent description of sea ice, we also show in Fig. 10 the
corresponding figures for the eight-member RCA4-NEMO coupled regional
simulations. The main difference is that the present-day simulations with
the coupled model have some extent of coastal sea ice in the southern Baltic
Sea, which is disappearing in the future.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Effects of model coupling</title>
      <p id="d1e857">Here, we take a more detailed look at RCM simulations driven by the five
GCMs, which have been downscaled both by the stand-alone atmosphere
EURO-CORDEX ensemble and by the 24 km RCA4-NEMO coupled-model version (all
coloured squares in Table 1 for the  RCA4 RCM).</p>
      <p id="d1e860">For near-surface air temperature (Fig. 10), the large-scale anomaly pattern
is fairly coherent in the two ensembles but differences are found over the
northern Baltic Sea where the coupled model shows a systematically stronger
winter warming than the uncoupled model. Over land, the coupled model
displays systematically lower warming. By contrast, during summer the
coupled model shows a weaker warming over the entire Baltic Sea, while land
temperatures increase more than in the stand-alone RCA.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><?xmltex \def\figurename{Figure}?><label>Figure 10</label><caption><p id="d1e865">Temperature change between 1981–2010 and 2071–2100 for five
atmosphere-only RCA4 simulations from EURO-CORDEX according to the RCP8.5
scenario <bold>(a, d)</bold> and for the coupled single-model RCA4-NEMO ensemble
with the same driving GCMs <bold>(b, e)</bold>; pointwise median values, only
coloured when 75 % of simulations agree on the sign of the change.
Difference between the two (<bold>c</bold>, <bold>f</bold>; coupled minus uncoupled; <inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C).
<bold>(a–c)</bold> Winter; <bold>(d–f)</bold> summer.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f10.png"/>

      </fig>

      <p id="d1e903">Due to its higher effective heat capacity, the Baltic Sea acts as a thermal
buffer, which dampens the seasonal amplitude compared to the surrounding
land areas. As a result, the Baltic Sea is warmer than the overlying
atmosphere during winter and releases heat to the atmosphere. Hence, in
regions not covered by sea ice, the SST significantly<?pagebreak page149?> influences the
sea-to-air heat flux. Consequently, in the uncoupled model, the prescribed SSTs from
the driving atmosphere–ocean GCM (AOGCM) serve as a restoring term for the air temperature. By
contrast, in the coupled model, SSTs are simultaneously modelled by the ocean
model and so the air-to-sea heat transfer acts to cool SSTs until a new
equilibrium would be reached. Despite these different dynamics in thermal
coupling, over the southern Baltic Sea, the solution of the two models is
quite similar compared to the northern Baltic (Fig. 10).</p>
      <p id="d1e906">In the northern Baltic Sea, the reduction of sea ice has to be considered.
In the future climate, areas which today are covered by sea ice will get
more tightly thermally coupled to the water body of the Baltic Sea (Dutheil
et al., 2022). As shown by Gröger et al. (2015, 2021a, b), the
ocean-to-atmosphere heat transfer is largely affected by small-scale
vertical mixing in the layered ocean because wind-induced mixing transports
warm waters from deeper water layers to the surface. These small-scale
processes are most likely not well represented in the prescribed SST from
the driving global ocean GCM. Furthermore, changes in the mean and turbulent
wind stress due to local climate change in RCA have no impact on
wind-induced mixing in the ocean in the RCA stand-alone simulations. This further
influences the local sea-ice cover and thus may explain the stronger warming
over the northern Baltic Sea in the coupled model compared to the uncoupled
version of RCA, which according to Fig. 9 generally starts out with less sea
ice in the present-day period and therefore experiences less sea-ice loss.
In the atmosphere, a stronger thermal coupling to the water body  not
only changes near-surface temperatures but also modifies atmospheric stability and
thereby mixing of heat, moisture, and momentum with potential impacts on
temperature, precipitation, and winds.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><?xmltex \currentcnt{11}?><?xmltex \def\figurename{Figure}?><label>Figure 11</label><caption><p id="d1e911">Precipitation relative change (%) between 1981–2010 and
2071–2100 for five atmosphere-only RCA4 simulations from EURO-CORDEX according
to the RCP8.5 scenario <bold>(a, d)</bold> and for the coupled single-model
RCA4-NEMO ensemble with the same driving GCMs <bold>(c, f)</bold>; pointwise
median values, only coloured when 75 % of simulations agree on the sign of
the change. Difference between the two (<bold>c</bold>, <bold>f</bold>; coupled minus
uncoupled; %). <bold>(a–c)</bold> Winter; <bold>(d–f)</bold> summer.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f11.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12" specific-use="star"><?xmltex \currentcnt{12}?><?xmltex \def\figurename{Figure}?><label>Figure 12</label><caption><p id="d1e941">Average wind speed relative change (%) between 1981–2010 and
2071–2100 for five atmosphere-only RCA4 simulations from EURO-CORDEX according
to the RCP8.5 scenario <bold>(a, d)</bold> and for the coupled single-model
RCA4-NEMO ensemble with the same driving GCMs <bold>(c, f)</bold>; pointwise
median values, only coloured when 75 % of simulations agree on the sign of
the change. Difference between the two (<bold>c</bold>, <bold>f</bold>; coupled minus
uncoupled; %). <bold>(a–c)</bold> Winter; <bold>(d–f)</bold> summer.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f12.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F13" specific-use="star"><?xmltex \currentcnt{13}?><?xmltex \def\figurename{Figure}?><label>Figure 13</label><caption><p id="d1e972">Average incoming solar radiation relative change (%) between
1981–2010 and 2071–2100 for five atmosphere-only RCA4 simulations from
EURO-CORDEX according to the RCP8.5 scenario <bold>(a, d)</bold> and for the
coupled single-model RCA4-NEMO ensemble with the same driving GCMs <bold>(c, f)</bold>;
pointwise median values, only coloured when 75 % of simulations
agree on the sign of the change. Difference between the two (<bold>c</bold>, <bold>f</bold>;
coupled minus uncoupled; %). <bold>(a–c)</bold> Winter; <bold>(d–f)</bold>
summer.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://esd.copernicus.org/articles/13/133/2022/esd-13-133-2022-f13.png"/>

      </fig>

      <p id="d1e1000">During summer when the Baltic Sea takes up heat from the atmosphere, the
air–sea heat exchange is greatly influenced by the water bodies' thermocline
layer, which is of the order of 10–30 m thick (e.g. Gröger et
al., 2019). Thermocline dynamics is likely much more realistically
represented when explicitly modelled by a coupled high-resolution ocean RCM
rather than reflected in prescribed SST taken from a<?pagebreak page150?> global GCM of coarse
resolution and only a few vertical layers (Gröger et al., 2015).</p>
      <p id="d1e1003">Winter precipitation (Fig. 11) displays a fairly coherent spatial pattern of
change for the coupled and uncoupled RCA projections. However, the coupled
model simulates systematically lower increases in precipitation than the
uncoupled model. This is seen for both winter and summer. The differences
are most prominent over western Scandinavia and the Bothnian Sea especially
during summer.</p>
      <p id="d1e1006">A prominent feature of winter wind speed changes (Fig. 12) is the strong
decrease along the Norwegian coast seen in the coupled RCA model. This is
also notable but less pronounced in the uncoupled runs. However, in those
regions with steep topographic gradients, the differences can be likely
attributed to the differing grid resolutions though coupling effects cannot
be excluded. For most other land regions, winds are slightly weakened in the
lower and slightly strengthened in the higher quartile, and a consequently
high uncertainty is seen for median winds (not shown). This is probably an
effect of the different resolution of the two ensembles. A noteworthy
difference between coupled and uncoupled simulations during winter is the
stronger increase in wind speeds over the Bothnian Bay. This points to local
coupled feedback processes probably related to the vanishing sea ice, higher
sea-surface temperatures, and altered atmospheric static stability. A larger
decrease in sea ice and a stronger coupling between the atmosphere and the
water body leads to a stronger heat flux to the atmosphere and thereby
reduced vertical stability. This, in turn, leads to a more efficient
downward mixing of momentum in the lower atmosphere and consequently higher
wind speed close to the sea surface.</p>
      <p id="d1e1009">The changes between future and present climate conditions in solar
irradiation (Fig. 13) are closely linked to changes in cloud cover. Both RCA
versions simulate a generally less pronounced reduction in solar radiation
during winter than the average reduction seen in the entire EURO-CORDEX
ensemble (Fig. 7). Strongest reductions are found over the Bothnian Bay in
winter where vanishing sea ice exposes open water to the atmosphere formerly
isolated by sea ice. Compared to the coupled version, the uncoupled<?pagebreak page151?> RCA
reveals a stronger reduction, in particular over the Bothnian Sea (Fig. 13).</p>
      <p id="d1e1012">To fully understand the different responses, detailed process analyses
including the respective ocean dynamics would be necessary to draw general
conclusions. In addition, the here-described systematic coupled vs.
uncoupled differences may be specific with regard to the employed RCA
regional atmosphere model and the coupled NEMO ocean RCM. Also, the
atmospheric part of the model, RCA, is run with different resolutions in the
coupled and uncoupled simulations, which may have an impact on the results.
Hence, the here-found systematic differences should be tested in coordinated
experiments also including those with other coupled and uncoupled systems.</p>
      <p id="d1e1016">Finally, we note that the coupling area comprising the North Sea and Baltic
Sea only is relatively small compared to entire EURO-CORDEX domain, and there
is indication that coupling effects may be more important if other seas,
such as the Mediterranean or the NE Atlantic, are included (e.g. Kelemen et
al., 2019; Primo et al., 2019; Akhtar et al., 2019; Gröger et al.,
2021b). The potential of different coupling techniques to influence the
response of atmospheric large-scale circulation to climate change has been
found to be most important during the winter season.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d1e1028">Since the previous BACC reports from 2008 and 2015, a very large amount of
high-resolution regional climate model simulations have been performed over
Europe, mostly downscaling global simulations from CMIP5. We have presented
ensemble model results here, and we have compared the climate change results
to those of BACC II (BACC II Author Team, 2015). The regional climate model
simulations of BACC II were using a different emission scenario (SRES A1B)
and a different set of GCMs than the currently used RCP scenarios from
CMIP5. We have therefore chosen to compare the results as a function of
local temperature change.</p>
      <?pagebreak page152?><p id="d1e1031">The results, illustrated for seasonal mean precipitation (Fig. 3) and wind
speed (Fig. 5), do not indicate any significant change in the relation of
these fields to local temperature change since BACC II. However, the much
larger ensemble of scenario simulations allows for a more reliable
assessment of future climate change compared to earlier studies. This is
illustrated in the figures showing how the increase in the number of
simulations, particularly the many more global models considered, has given
much more robust estimates of uncertainty. This is the case both for local
climate sensitivity, as illustrated by the different temperature change
values for downscaling of each individual emission scenario, and for the
intervariable relations, as illustrated with the general scatter of the
points. Also, the addition of several emission scenarios enables a better
foundation for estimating effects of, e.g. emission mitigation.</p>
      <p id="d1e1034">The local winter temperature increases of current RCP8.5 simulations are
close to the A1B results of BACC II, in spite of the stronger average global
warming in the underlying RCP8.5 GCM ensemble compared to that in the A1B
GCM ensemble. According to the two suites of GCMs, the difference in global
mean by the end of the century is 0.7 K, i.e. about 25 %. For summer, the
differences are larger, and it cannot be generally concluded whether or not
the regional sensitivity to global climate change is different from what it
was in BACC II, or whether this is just caused by the concrete selections of
models included in the two model suites.</p>
      <p id="d1e1037">The expected anthropogenic climate change for the Baltic Sea area is
corroborated by the present results: temperature will increase, in step with
global warming and with a north–south gradient. In the northern part of the
area in winter, the warming approaches twice the average global warming.</p>
      <p id="d1e1041">Precipitation increases over the entire area in winter, somewhat less in
summer in the northern part of the domain, and it does not change
significantly in summer in the southern part. Extreme precipitation, here
the 10-year return value, increases systematically, particularly in summer,
in the entire domain, with some simulations showing more than 50 %
increase.</p>
      <?pagebreak page153?><p id="d1e1044">The large ensemble of simulations does not indicate a significant change in
wind speed. However, individual model simulations show distinct differences.
Consequently, there is a large uncertainty related to future wind speed
change in the area.</p>
      <p id="d1e1047">Solar irradiation at the surface is not projected to change in summer, but
the RCM simulations show some decrease in winter connected to more extensive
cloud cover and potentially also less snow in the future. There is, however,
a large uncertainty related to this, since many GCMs show the opposite sign
of the trend.</p>
      <p id="d1e1050">Snow cover, measured as the average amount of snow on the ground in winter
(DJF), is reduced drastically, particularly in the south of the Baltic Sea
catchment area, where the relative decrease is close to 80 %.</p>
      <p id="d1e1053">With respect to coupled vs. uncoupled models, we find a stronger warming in
the coupled model during winter which is most pronounced in areas that today
are seasonally affected by sea ice. During summer, the coupled model shows
weaker warming compared to the uncoupled model. The comparison between
coupled and uncoupled versions of a small subset of projections with the
RCA4 and RCA4-NEMO models generally confirms results by Gröger et al. (2021b),
who found coupling effects for changes in most climate indices, most
clearly over the interactively coupled open sea area. Notable differences
outside the coupled region occur over regions of topographically elevated
terrain likely as an artefact of different model resolution.</p>
</sec>

      
      </body>
    <back><notes notes-type="codeavailability"><title>Code availability</title>

      <p id="d1e1060">All data manipulations in this study are straightforward and described in
the paper.</p>
  </notes><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e1066">All data used in this publication are publicly available through the Earth System Grid Federation (ESGF)
network, e.g. <uri>http://esgf-data.dkrz.de</uri> (DKRZ, 2022).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e1072">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/esd-13-133-2022-supplement" xlink:title="pdf">https://doi.org/10.5194/esd-13-133-2022-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e1081">OBC, as the main author, has coordinated the writing, contributed to all parts of the paper, constructed figures and supplementary material.
EK has contributed to all parts of the paper, mainly regarding introduction and the atmospheric simulations.
MM, MG and CD have contributed to all parts of the paper, with their main focus on the comparison of atmospheric models with ocean–atmosphere coupled regional models.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e1087">The contact author has declared that neither they nor their co-authors have any competing interests.</p>
  </notes><notes notes-type="sistatement"><title>Special issue statement</title>

      <p id="d1e1093">This article is part of the special issue “The Baltic Earth Assessment Reports (BEAR)”.
It is not associated with a conference.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e1099">Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e1105">The research presented in this study is part of the Baltic Earth Assessment
Reports project of the Baltic Earth programme (Earth System Science of the
Baltic Sea Region, <uri>https://baltic.earth</uri>, last access: 14 January 2022). The authors would
like to thank the EURO-CORDEX network and WCRP CORDEX for ensuring
availability of CORDEX data.</p><p id="d1e1110">It is with great sadness that we received the news that our co-author,
Christian Dieterich, passed away during the review of this paper.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e1115">This study has been partly funded by the Copernicus Climate Change Service.
ECMWF implements this service on behalf of the European Commission. Part of
the funding is by the Danish state through the National Centre for Climate
Research (NCKF).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e1122">This paper was edited by Marcus Reckermann and reviewed by Jouni Räisänen and two anonymous referees.</p>
  </notes><ref-list>
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