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  <front>
    <journal-meta><journal-id journal-id-type="publisher">CP</journal-id><journal-title-group>
    <journal-title>Climate of the Past</journal-title>
    <abbrev-journal-title abbrev-type="publisher">CP</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Clim. Past</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1814-9332</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/cp-17-1777-2021</article-id><title-group><article-title>Mid-Pliocene West African Monsoon rainfall as simulated<?xmltex \hack{\break}?> in the PlioMIP2 ensemble</article-title><alt-title>Mid-Pliocene West African Monsoon Rainfall</alt-title>
      </title-group><?xmltex \runningtitle{Mid-Pliocene West African Monsoon Rainfall}?><?xmltex \runningauthor{E. Berntell et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Berntell</surname><given-names>Ellen</given-names></name>
          <email>ellen.berntell@natgeo.su.se</email>
        <ext-link>https://orcid.org/0000-0002-2409-4035</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Zhang</surname><given-names>Qiong</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9137-2883</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Li</surname><given-names>Qiang</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6390-0343</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Haywood</surname><given-names>Alan M.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Tindall</surname><given-names>Julia C.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Hunter</surname><given-names>Stephen J.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4593-6238</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3 aff4">
          <name><surname>Zhang</surname><given-names>Zhongshi</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2354-1622</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Li</surname><given-names>Xiangyu</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7724-4025</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Guo</surname><given-names>Chuncheng</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-6276-6499</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5 aff6">
          <name><surname>Nisancioglu</surname><given-names>Kerim H.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5737-5765</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7">
          <name><surname>Stepanek</surname><given-names>Christian</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3912-6271</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7 aff8">
          <name><surname>Lohmann</surname><given-names>Gerrit</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2089-733X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff9 aff10">
          <name><surname>Sohl</surname><given-names>Linda E.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6673-2007</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff9 aff10">
          <name><surname>Chandler</surname><given-names>Mark A.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6548-227X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff11 aff12">
          <name><surname>Tan</surname><given-names>Ning</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff12">
          <name><surname>Contoux</surname><given-names>Camille</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8487-9275</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff12">
          <name><surname>Ramstein</surname><given-names>Gilles</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff13">
          <name><surname>Baatsen</surname><given-names>Michiel L. J.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff13 aff14">
          <name><surname>von der Heydt</surname><given-names>Anna S.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5557-3282</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff15">
          <name><surname>Chandan</surname><given-names>Deepak</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0756-754X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff15">
          <name><surname>Peltier</surname><given-names>William Richard</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5555-7661</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff16">
          <name><surname>Abe-Ouchi</surname><given-names>Ayako</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1745-5952</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff16">
          <name><surname>Chan</surname><given-names>Wing-Le</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5646-6104</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff17">
          <name><surname>Kamae</surname><given-names>Youichi</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-0461-5718</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff18 aff19">
          <name><surname>Williams</surname><given-names>Charles J. R.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1791-2463</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff18">
          <name><surname>Lunt</surname><given-names>Daniel J.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3585-6928</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff20">
          <name><surname>Feng</surname><given-names>Ran</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff21">
          <name><surname>Otto-Bliesner</surname><given-names>Bette L.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1911-1598</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff21">
          <name><surname>Brady</surname><given-names>Esther C.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7833-2249</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Department of Physical Geography and Bolin Centre for Climate
Research, Stockholm University, Stockholm, Sweden</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>School of Earth and Environment, University of Leeds, Woodhouse Lane, Leeds, West Yorkshire, UK</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Atmospheric Science, School of Environmental Studies,
China University of Geosciences, Wuhan, China</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>NORCE Norwegian Research Centre, Bjerknes Centre for Climate Research, Bergen, Norway</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Department of Earth Science, University of Bergen and Bjerknes Centre for Climate Research, Bergen, Norway</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Centre for Earth Evolution and Dynamics, University of Oslo, Oslo,
Norway</institution>
        </aff>
        <aff id="aff7"><label>7</label><institution>Alfred Wegener Institute – Helmholtz-Zentrum für Polar und
Meeresforschung, Bremerhaven, Germany</institution>
        </aff>
        <aff id="aff8"><label>8</label><institution>Institute for Environmental Physics, University of Bremen, Bremen,
Germany</institution>
        </aff>
        <aff id="aff9"><label>9</label><institution>Centre for Climate Systems Research, Columbia University, New York,
USA</institution>
        </aff>
        <aff id="aff10"><label>10</label><institution>NASA Goddard Institute for Space Studies, New York, USA</institution>
        </aff>
        <aff id="aff11"><label>11</label><institution>Key Laboratory of Cenozoic Geology and Environment, Institute of
Geology and Geophysics,<?xmltex \hack{\break}?> Chinese Academy of Sciences, Beijing, China</institution>
        </aff>
        <aff id="aff12"><label>12</label><institution>Laboratoire des Sciences du Climat et de l'Environnement, LSCE/IPSL, CEA-CNRS-UVSQ,<?xmltex \hack{\break}?> Université Paris-Saclay, Gif-sur-Yvette, France</institution>
        </aff>
        <aff id="aff13"><label>13</label><institution>Centre for Complex Systems Science, Utrecht University, Utrecht, the Netherlands</institution>
        </aff>
        <aff id="aff14"><label>14</label><institution>Institute for Marine and Atmospheric research Utrecht (IMAU),
Department of Physics,<?xmltex \hack{\break}?> Utrecht University, Utrecht, the Netherlands</institution>
        </aff>
        <aff id="aff15"><label>15</label><institution>Department of Physics, University of Toronto, Toronto, Ontario,
Canada</institution>
        </aff>
        <aff id="aff16"><label>16</label><institution>Centre for Earth Surface System Dynamics (CESD), Atmosphere and Ocean Research Institute (AORI),<?xmltex \hack{\break}?> University of Tokyo, Tokyo, Japan</institution>
        </aff>
        <aff id="aff17"><label>17</label><institution>Faculty of Life and Environmental Sciences, University of Tsukuba,
Tsukuba, Japan</institution>
        </aff>
        <aff id="aff18"><label>18</label><institution>School of Geographical Sciences, University of Bristol, Bristol, UK</institution>
        </aff>
        <aff id="aff19"><label>19</label><institution>NCAS, Department of Meteorology, University of Reading, Reading, UK</institution>
        </aff>
        <aff id="aff20"><label>20</label><institution>Department of Geosciences, University of Connecticut, Storrs, USA</institution>
        </aff>
        <aff id="aff21"><label>21</label><institution>Climate and Global Dynamics Laboratory, National Center for
Atmospheric Research, Boulder, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Ellen Berntell (ellen.berntell@natgeo.su.se)</corresp></author-notes><pub-date><day>27</day><month>August</month><year>2021</year></pub-date>
      
      <volume>17</volume>
      <issue>4</issue>
      <fpage>1777</fpage><lpage>1794</lpage>
      <history>
        <date date-type="received"><day>12</day><month>February</month><year>2021</year></date>
           <date date-type="rev-request"><day>26</day><month>February</month><year>2021</year></date>
           <date date-type="rev-recd"><day>20</day><month>July</month><year>2021</year></date>
           <date date-type="accepted"><day>21</day><month>July</month><year>2021</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2021 Ellen Berntell et al.</copyright-statement>
        <copyright-year>2021</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://cp.copernicus.org/articles/17/1777/2021/cp-17-1777-2021.html">This article is available from https://cp.copernicus.org/articles/17/1777/2021/cp-17-1777-2021.html</self-uri><self-uri xlink:href="https://cp.copernicus.org/articles/17/1777/2021/cp-17-1777-2021.pdf">The full text article is available as a PDF file from https://cp.copernicus.org/articles/17/1777/2021/cp-17-1777-2021.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e488">The mid-Pliocene warm period (mPWP; <?xmltex \hack{\mbox\bgroup}?><inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">3.2</mml:mn></mml:mrow></mml:math></inline-formula><?xmltex \hack{\egroup}?> million years ago) is seen as the most recent time period characterized by a
warm climate state, with similar to modern geography and <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">400</mml:mn></mml:mrow></mml:math></inline-formula> ppmv atmospheric CO<inline-formula><mml:math id="M3" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> concentration, and is therefore often considered
an interesting analogue for near-future climate projections.
Paleoenvironmental reconstructions indicate higher surface temperatures,
decreasing tropical deserts, and a more humid climate in West Africa
characterized by a strengthened West African Monsoon (WAM). Using model
results from the second phase of the Pliocene Modelling Intercomparison
Project (PlioMIP2) ensemble, we analyse changes of the WAM rainfall during
the mPWP by comparing them with the control simulations for the pre-industrial
period. The ensemble shows a robust increase in the summer rainfall over
West Africa and the Sahara region, with an average increase of 2.5 mm/d,
contrasted by a rainfall decrease over the equatorial Atlantic. An anomalous
warming of the Sahara and deepening of the Saharan Heat Low, seen in
<inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mi mathvariant="italic">&gt;</mml:mi><mml:mn mathvariant="normal">90</mml:mn></mml:mrow></mml:math></inline-formula> % of the models, leads to a strengthening of the WAM and
an increased monsoonal flow into the continent. A similar warming of the
Sahara is seen in future projections using both phase 3 and 5 of the
Coupled Model Intercomparison Project (CMIP3 and CMIP5). Though previous
studies of future projections indicate a west–east drying–wetting contrast
over the Sahel, PlioMIP2 simulations indicate a uniform rainfall increase in
that region in warm climates characterized by increasing greenhouse gas
forcing. We note that this effect will further depend on the long-term
response of the vegetation to the CO<inline-formula><mml:math id="M5" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> forcing.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<?pagebreak page1778?><sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e551">The mid-Pliocene warm period (mPWP; 3.264–3.025 Ma; also known as the
mid-Piacenzian warm period) is considered to be the most recent past warm
climate state, with average global temperatures several degrees above
pre-industrial (PI) levels (1.4–4.7 <inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C;
Haywood et al., 2020) and
atmospheric CO<inline-formula><mml:math id="M7" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> concentrations of <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">400</mml:mn></mml:mrow></mml:math></inline-formula> ppmv
(Badger
et al., 2013; Bartoli et al., 2011; Dowsett et al., 2010; Haywood et al.,
2020, 2013; de la Vega et al., 2020; Martínez-Botí et al., 2015;
Pagani et al., 2010; Raymo et al., 1996; Salzmann et al., 2013; Seki et al.,
2010; Tripati et al., 2009; Zhang et al., 2013). Paleoenvironmental
reconstructions indicate a warm and humid climate during the mPWP, with
elevated sea surface temperatures (SSTs) and surface air temperatures (SATs),
especially at high latitudes
(Dowsett et al., 2010; Salzmann et
al., 2013), forests and grassland expanding into areas that are
covered by tundra during more recent times, and savanna and woodland expanding at the expense of
deserts (Salzmann
et al., 2008). While much of the research on the mPWP climate focused on
global large-scale patterns and the high latitudes
(Haywood
et al., 2013, 2020; De Nooijer et al., 2020), several studies have
emphasized the implications of the warm climate state for tropical climate,
showing, e.g. an enhancement of the East Asian Summer Monsoon
(Wan et al., 2010) and a
drying of the Southern Hemisphere tropics and subtropics
(Pontes et al., 2020). Analysis based on, e.g. dust records of the
coast of West Africa, also indicates a strengthened West African Monsoon
(WAM) during the mPWP, as well as wetter conditions over West Africa and the
Sahara region
(Kuechler
et al., 2018; Salzmann et al., 2008).</p>
      <p id="d1e582">With a paleogeography and atmospheric CO<inline-formula><mml:math id="M9" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> concentrations similar to
today (Dowsett et al., 2010), the mPWP has long been considered
an interesting analogue for near-future climate projections
(Chandler
et al., 1994; Jiang et al., 2005) and has been the focus of many modelling
studies
(e.g.
Haywood and Valdes, 2004; Salzmann et al., 2008). To increase our
understanding of the dynamical drivers of the warm climate state, several
model simulations have been performed as part of the Pliocene Modelling
Intercomparison Project (PlioMIP;
Haywood
et al., 2010, 2011). Model–data comparisons between the PlioMIP1 (first
phase of PlioMIP) simulations and PRISM3 (PRISM – Pliocene Research
Interpretation and Synoptic Mapping) reconstructions
(Dowsett
et al., 2010, 2012, 2013) have shown an underestimation of the high-latitude
warming in the mPWP and an overestimation of the warming in the tropics
(Haywood
et al., 2013; Salzmann et al., 2013), which has influenced the
representation of the WAM within the models (Zhang et
al., 2016). PlioMIP1 was later followed up by a second phase (PlioMIP2),
representing a more narrow geological time window (marine isotope stage
KM5c, 3.205 Mya) to, e.g. facilitate data–model comparison
(Haywood et al., 2016), and though
some areas of concern still remain, results from the PlioMIP2 have shown a
widespread model–data agreement
(Haywood et al., 2020).</p>
      <p id="d1e594">While previous model studies have shown that the high-latitude warming has
reduced the Equator–pole temperature gradient
(Haywood
et al., 2013) and weakened tropical circulation such as the Hadley
Circulation (Corvec and Fletcher,
2017), the terrestrial warming during the mPWP has been shown to strengthen
the WAM and increase the summer rainfall over the Sahel region by more than
1 mm/d (Haywood et
al., 2020; Zhang et al., 2016). A similar rainfall increase over the Sahel is
seen in future projections for both CMIP3 and CMIP5 ensembles, though this is with a
drying located over western Sahel (Roehrig et
al., 2013). However, models have been shown to inaccurately capture past
rainfall variability and change over West Africa and the Sahel region
(Berntell et al., 2018; Roehrig
et al., 2013), and there is still little confidence in future projections of
the summer rainfall
(Biasutti et al.,
2008; Cook, 2008; Roehrig et al., 2013). West Africa is a region sensitive
to hydrological variability and experienced extended droughts during the
1970s and 1980s
(Berntell
et al., 2018; Held et al., 2005; Nicholson et al., 2000). There is a large
need to increase confidence in future projections in order to support
adaption strategies in the region.</p>
      <?pagebreak page1779?><p id="d1e597">The similarity to modern conditions, as well as the high amount of
paleogeological and environmental data from the mPWP, has made PlioMIP2 well
suited to both evaluate the models' ability to capture a warm climate state
and further our understanding of the effects of greenhouse gas forcing and
related feedbacks on the global climate system
(Haywood
et al., 2020; Haywood and Valdes, 2004). In this article we will evaluate
the representation of the WAM within the PlioMIP2 ensemble, qualitatively
compare it to palaeohydrological reconstructions, and discuss the
implications for the WAM in a near-future warm climate state with increasing
greenhouse gas forcing.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data and methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Participating PlioMIP2 models</title>
      <p id="d1e615">To examine the behaviour of the WAM during the mPWP, data produced by 17
different general circulation models as part of the PlioMIP2 were used (Table 1). Simulations produced within PlioMIP2 are run for at least 500 years
(Haywood et al., 2016) towards an
equilibrium state, and the last 100 years of the simulations are then used
for analysis. In the experimental set-up the CO<inline-formula><mml:math id="M10" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> levels are set to 400 ppmv, and the remaining concentrations of trace gases and aerosols are set
to pre-industrial levels (Haywood et
al., 2016). The simulations are run using standard or enhanced boundary
conditions from PRISM4 (Dowsett et al., 2016)
as described in Haywood et al. (2016), with changes to, e.g. the topography, bathymetry, and land ice cover.
All model simulations are run using a mid-Pliocene land–sea mask, except for
HadGEM3 and MRI-CGCM 2.3, which use a modern land–sea mask. COSMOS uses
dynamic vegetation (Stepanek et
al., 2020), while the remaining 16 models use prescribed vegetation based on
Salzmann et al. (2008). As the models have different horizontal resolutions, the data from
the models were bilinearly interpolated onto a 1<inline-formula><mml:math id="M11" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M12" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid using the software CDO
(Climate Data Operators, Schulzweida, 2019) to
facilitate multi-model analysis.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e655">PlioMIP2 models used in this study. Spatial resolution of
the atmosphere model indicated by grid cell extent (in degrees longitude <inline-formula><mml:math id="M14" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> latitude) and
number of vertical layers (<inline-formula><mml:math id="M15" display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula>).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Model ID</oasis:entry>
         <oasis:entry colname="col2">Atmospheric resolution</oasis:entry>
         <oasis:entry colname="col3">Reference</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">CCSM4-NCAR</oasis:entry>
         <oasis:entry colname="col2">1.25 <inline-formula><mml:math id="M16" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.9, L26</oasis:entry>
         <oasis:entry colname="col3">Feng et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">CCSM4-Utrecht</oasis:entry>
         <oasis:entry colname="col2">2.5 <inline-formula><mml:math id="M17" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1.9, L26</oasis:entry>
         <oasis:entry colname="col3"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">CCSM4-UofT</oasis:entry>
         <oasis:entry colname="col2">1.25 <inline-formula><mml:math id="M18" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.9, L26</oasis:entry>
         <oasis:entry colname="col3">Peltier and Vettoretti (2014);</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">Chandan and Peltier (2017, 2018)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">CESM1.2</oasis:entry>
         <oasis:entry colname="col2">1.25? <inline-formula><mml:math id="M19" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.9, L30</oasis:entry>
         <oasis:entry colname="col3">Feng et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">CESM2</oasis:entry>
         <oasis:entry colname="col2">1.25 <inline-formula><mml:math id="M20" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.9, L32</oasis:entry>
         <oasis:entry colname="col3">Feng et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">COSMOS</oasis:entry>
         <oasis:entry colname="col2">T31 (<inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">3.75</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M22" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 3.75), L19</oasis:entry>
         <oasis:entry colname="col3">Stepanek et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">EC-Earth3-LR</oasis:entry>
         <oasis:entry colname="col2">T159 (<inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1.125</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M24" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1.125), L62</oasis:entry>
         <oasis:entry colname="col3">Q. Zhang et al. (2021)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">GISS-E2-1-G</oasis:entry>
         <oasis:entry colname="col2">2.0 <inline-formula><mml:math id="M25" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5, L40</oasis:entry>
         <oasis:entry colname="col3">Kelley et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">HadCM3</oasis:entry>
         <oasis:entry colname="col2">2.5 <inline-formula><mml:math id="M26" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 3.75, L19</oasis:entry>
         <oasis:entry colname="col3">Hunter et al. (2019)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">HadGEM3(-GC31-LL)</oasis:entry>
         <oasis:entry colname="col2">N96 (<inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1.875</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M28" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1.25), L85</oasis:entry>
         <oasis:entry colname="col3">Williams et al. (2021)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">IPSLCM6A-LR</oasis:entry>
         <oasis:entry colname="col2">2.5 <inline-formula><mml:math id="M29" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1.26, L79</oasis:entry>
         <oasis:entry colname="col3">Lurton et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">IPSLCM5A2</oasis:entry>
         <oasis:entry colname="col2">3.75 <inline-formula><mml:math id="M30" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1.9, L39</oasis:entry>
         <oasis:entry colname="col3">Tan et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">IPSLCM5A</oasis:entry>
         <oasis:entry colname="col2">3.75 <inline-formula><mml:math id="M31" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1.9, L39</oasis:entry>
         <oasis:entry colname="col3">Tan et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">MIROC4m</oasis:entry>
         <oasis:entry colname="col2">T42 (<inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">2.8</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M33" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.8), L20</oasis:entry>
         <oasis:entry colname="col3">Chan and Abe-Ouchi (2020)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">MRI-CGCM 2.3</oasis:entry>
         <oasis:entry colname="col2">T42 (<inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">2.8</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M35" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.8), L30</oasis:entry>
         <oasis:entry colname="col3">Kamae et al. (2016)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">NorESM-L</oasis:entry>
         <oasis:entry colname="col2">T31 (<inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">3.75</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M37" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 3.75), L26</oasis:entry>
         <oasis:entry colname="col3">Li et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">NorESM1-F</oasis:entry>
         <oasis:entry colname="col2">1.9 <inline-formula><mml:math id="M38" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5, L26</oasis:entry>
         <oasis:entry colname="col3">Li et al. (2020)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Methods</title>
      <p id="d1e1104">The rainfall and West African climate is analysed over the months
July–October (JASO), and the multi-model mean (MMM) represents the
unweighted average of the PlioMIP2 ensemble. The robustness of the signal
is evaluated using the methodology of
Mba et al. (2018), where the
signal is considered robust if at least 14 of the 17 models (<inline-formula><mml:math id="M39" display="inline"><mml:mo lspace="0mm">≥</mml:mo></mml:math></inline-formula> 80 %) agree on the sign of the anomaly and the MMM anomaly is equal to or
larger than the inter-model standard deviation. The models are evaluated
against their PI simulation, and the 1901–1930 climatology based on CRU TS
v4 (Climatic Research Unit gridded Time Series;
Harris et al., 2020) is included as a reference
for the observations. The seasonal cycle of the WAM is also examined over
two sub-regions, the Sahel (10–20<inline-formula><mml:math id="M40" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 20<inline-formula><mml:math id="M41" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–30<inline-formula><mml:math id="M42" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E)
and the coast of Guinea (5–10<inline-formula><mml:math id="M43" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 20<inline-formula><mml:math id="M44" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–30<inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E), representing regions characterized by a narrow and a wider or bimodal
rainfall season, respectively. A more narrow definition of the Sahel region
is also sometimes used (10<inline-formula><mml:math id="M46" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–10<inline-formula><mml:math id="M47" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, e.g.
Thorncroft et al., 2011), but our
analysis has shown no difference in the seasonal distribution of rainfall
compared to a wider region (20<inline-formula><mml:math id="M48" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–30<inline-formula><mml:math id="M49" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E). Given the
possible northward expansion of the WAM during the mPWP, the seasonal cycle
over the Sahara region (20–30<inline-formula><mml:math id="M50" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 20<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–30<inline-formula><mml:math id="M52" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E)
is also included.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Changes in seasonality</title>
      <p id="d1e1249">The progression of the WAM creates different seasonal cycles of rainfall
depending on the region, where northern latitudes in West Africa (south of the
Sahara) have one clear peak while more southern regions have a wider or
bimodal rainy season (Nicholson et al.,
2000). We have therefore divided West Africa into two sub-regions, the Sahel
(10–20<inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 20<inline-formula><mml:math id="M54" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–30<inline-formula><mml:math id="M55" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) and the coast of Guinea
(5–10<inline-formula><mml:math id="M56" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 20<inline-formula><mml:math id="M57" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–30<inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E), and shown the results
together with the seasonal cycle over the Sahara region (20–30<inline-formula><mml:math id="M59" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N,
20<inline-formula><mml:math id="M60" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–30<inline-formula><mml:math id="M61" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E). The seasonal cycle of terrestrial rainfall
is calculated for each ensemble member and presented together with the MMM
for the PI and mPWP simulations separately, as well as for the Pliocene
anomaly (mPWP-PI) (Fig. 1). The “modern” seasonal cycle is plotted
together with the PI cycle for reference, based on 1901–1930 CRU TS v4 data
(Harris et al., 2020).</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="d1e1336">Seasonal cycle of rainfall (unit: mm/d) over the Sahel <bold>(a, d, g)</bold>, the coast of Guinea <bold>(b, e, h)</bold>, and the Sahara region <bold>(c, f, i)</bold> for PI <bold>(a–c)</bold>, mPWP <bold>(d–f)</bold>, and mPWP anomalies (mPWP-PI, <bold>g–i</bold>). The multi-model mean MMM
(black) is shown together with the individual models, and the modern
conditions as derived from observations (Harris
et al., 2020) are included as a reference (red).</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1777/2021/cp-17-1777-2021-f01.png"/>

        </fig>

      <p id="d1e1364">In agreement with PI observations, the PI MMM shows a seasonal cycle with a
peak in rainfall in August over the Sahel at 3.1 mm/d. The individual models
mainly exhibit the same seasonal cycle; however, four models exhibit that the highest
level of rainfall shifted to July (HadCM3) or September (CCSM4-Utrecht,
NorESM-L and NorESM-F) rather than August. The magnitude of summer rainfall
seen in CESM1.2 and MIROC4m is 5.1 and 5.2 mm/d respectively and is comparable
to modern conditions (4.9 mm/d) (Fig. 1), while the other 15 ensemble
members remain within a span of 2–4 mm/d, which is considerably below
modern levels. The mPWP MMM shows an increase in monsoon rainfall, with the
maximum rainfall doubling and reaching 6.1 mm/d in August. The largest
increase is shown in EC-Earth3-LR at 7.3 and 7.5 mm/d in August and
September, making it reach a maximum of 9.2 mm/d in the Pliocene Sahel. As
with the PI, the highest level of Pliocene rainfall in the PlioMIP2 ensemble
is seen in MIROC4m, with 11.5 mm/d in August. All models show an increase
in rainfall in the July–October period, with the largest increase occurring
either in August, September, or October, resulting in a lengthening of the
WAM. We will therefore base our spatial analysis of the WAM on the
July–October (JASO) period, although this does not alter the spatial
patterns compared to a shorter monsoon season (July–September).</p>
      <?pagebreak page1780?><p id="d1e1368">Over the coast of Guinea, the PI simulations show higher levels of rainfall
through most of the Northern Hemisphere's spring, summer, and fall, with the
ensemble mean showing a maximum of 8.1 mm/d occurring in August (Fig. 1).
This is, both in seasonal distribution and amount, comparable to the PI
observations that exhibit maximum rainfall of 7.9 mm/d in September.
However, while the observations show a slight bi-modal rainfall
distribution, with peaks in June and September, the PI MMM has a wider
distribution with a peak in August. 16 of the 17 members have maximum levels
of rainfall spanning between 5.9 and 9.8 mm/d, while MIROC4m again
exceeds the remaining models with rainfall reaching 11.9 mm/d in July. The
MMM of the mPWP simulations again shows an increase of monsoon rainfall
compared to the PI, with positive anomalies throughout the seasonal cycle,
but it shows the highest values in October and a secondary peak in July. However,
while no individual models showed negative anomalies during the monsoon
season in the Sahel, CCSM4-NCAR, MIROC4m, and NorESM1-F show a decrease in rainfall
over the coast of Guinea in July–September. The remaining models show both
increasing and decreasing rainfall during April–June but mainly positive
anomalies from July to November.</p>
      <p id="d1e1371">The rainfall over the Sahara region remains low for the PI observations and
PI simulations, with both PI observations and the PI MMM remaining
consistently below 0.2 mm/d throughout the year and 16 of the 17 models
staying between 0.0–0.5 mm/d (Fig. 1). MIROC4m again exhibits the highest
levels of rainfall, with a peak of 0.8 mm/d in May and a second peak of
0.7 mm/d in September. The mPWP simulations show a clear increase in
rainfall over Sahara in the later part of the WAM season, with the mPWP MMM
anomalies centred on September and the maximum rainfall reaching 0.8 mm/d. The largest increase is seen in EC-Earth3-LR and CCSM4-Utrecht at
2.3 mm/d in September and 2.6 and 2.7 mm/d in September and October,
respectively.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Changes in monsoon rainfall</title>
      <p id="d1e1382">To see the changes in the WAM rainfall during the mPWP we look at the JASO
rainfall anomalies (mPWP-PI, Fig. 2). The MMM shows a clear dipole pattern
with a latitudinal transition at 7<inline-formula><mml:math id="M62" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N stretching from the Atlantic
Ocean to the eastern part of northern Africa (Fig. 2a). The robust signal of
rainfall increase is centred on the Sahel and southern Sahara, covering most of
northern Africa and reaching from the coast of Guinea into the northern Sahara.
The negative anomalies cover an area stretching from 7<inline-formula><mml:math id="M63" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and
continuing<?pagebreak page1781?> south over the equatorial Atlantic, with the largest decrease
located along the Gulf of Guinea.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e1405">The mPWP July–August–September–October (JASO) rainfall anomalies
(mPWP-PI) for the MMM <bold>(a)</bold> and the individual models <bold>(b–r)</bold>, with all
panels using the same colour bar. Robust signals in <bold>(a)</bold> are indicated
with an x, where <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mi mathvariant="italic">&gt;</mml:mi><mml:mn mathvariant="normal">80</mml:mn></mml:mrow></mml:math></inline-formula> % of the models (14 out of 17) show the same
sign of anomaly and the anomaly is equal to or larger than the inter-model
standard deviation. Dots indicate that only the first criterion is
fulfilled. The pattern correlation between the MMM and individual model is
seen in the bottom-left corner of <bold>(b–r)</bold>. <bold>(s)</bold> The inter-model variability is
shown as the standard deviation (unit: mm/d).</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1777/2021/cp-17-1777-2021-f02.png"/>

        </fig>

      <p id="d1e1440">The large-scale features of the rainfall anomalies are consistent over the
individual models, with the rainfall increase centred at 10–15<inline-formula><mml:math id="M65" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N
and reaching up into the southern Sahara and negative values located over the
Gulf of Guinea (Fig. 2a and b–r). The results are less consistent along the
coast of Guinea, with models indicating slightly different locations of the
transition from negative to positive rainfall anomalies. Some models exhibit
a rainfall decrease reaching up to 9<inline-formula><mml:math id="M66" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N (MIROC4m, GISS-E2-1-G),
while other models limit the negative values to only cover the equatorial
Atlantic and Central Africa (CCSM4-UofT, HadCM3). EC-Earth3-LR, CCSM4-UofT,
CCSM4-NCAR, and HadCM3 show the highest pattern correlation to the MMM at
<inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.96</mml:mn></mml:mrow></mml:math></inline-formula> (EC-Earth3-LR) and <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.93</mml:mn></mml:mrow></mml:math></inline-formula> (other models), respectively, while
GISS-E2-1-G has the lowest correlation (<inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.52</mml:mn></mml:mrow></mml:math></inline-formula>). The different models show
the largest spread over the Sahel and southern Sahara (standard deviation of 2–4 mm/d, Fig. 2s). This is a region where all models indicate an increase in
rainfall, but the simulated magnitude differs largely, from over 8 mm/d in
EC-Earth3-LR and MIROC4m to around 1 mm/d for GISS-E2-1-G and IPSLCM5A2. A
spatial mean of the rainfall anomalies over the Sahel (Fig. 3) shows a similar
spread, with the highest values for EC-Earth3-LR and MIROC4m (6.1 and 5.0 mm/d) and the lowest for GISS-E2-1-G and IPSLCM5A2 (0.4 and 0.7 mm/d).
The remaining 13 models all show an increase of 1–4 mm/d over Sahel with a
MMM of 2.5 mm/d.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e1500">Mean July–October (JASO) Sahel (10–20<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N,
20<inline-formula><mml:math id="M71" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–30<inline-formula><mml:math id="M72" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) mPWP rainfall anomaly (mPWP-PI, unit:
mm/d) for the individual PlioMIP2 ensemble models, together with the
MMM.</p></caption>
          <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1777/2021/cp-17-1777-2021-f03.png"/>

        </fig>

      <?pagebreak page1783?><p id="d1e1536">Looking at the latitudinal mean JASO rainfall (Fig. 4) we can also see that
the rain belt, i.e. the latitudinal band of maximum rainfall during the WAM,
has shifted northward in the mPWP and is centred at 9.5<inline-formula><mml:math id="M73" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N with
the largest rainfall increase of 2.0–3.1 mm/d occurring between
9.5 and 17.5<inline-formula><mml:math id="M74" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N for the MMM. The ensemble does,
however, still exhibit a large spread, with three models showing a maximum
increase to the south of the MMM (IPSLCM5A, IPSLCM5A2 and IPSLCM6A), four
models showing an increase to the north (CCSM4-Utrecht, CESM1.2, NorESM-L and NorESM1-F), and two
models showing a substantially larger increase than the MMM (EC-Earth3-LR
and MIROC4m).</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="d1e1559"><bold>(a)</bold> Latitudinal mean terrestrial rainfall for MMM PI
(grey) and mPWP (blue), with dark blue where they overlap, and <bold>(b)</bold>
latitudinal mean July–October (JASO) rainfall anomalies (mPWP-PI) for the
individual models and for the MMM.</p></caption>
          <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1777/2021/cp-17-1777-2021-f04.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>The dynamics for the changes in WAM rainfall</title>
      <p id="d1e1581">To understand the dynamics behind the increased rainfall in West Africa
during the mPWP, the sea level pressure, horizontal wind at 850 hPa, and near-surface temperature anomalies (mPWP-PI) are analysed for each individual
model.</p>
      <p id="d1e1584">Sea level pressure anomalies for the monsoon season (JASO, mPWP-PI) are
shown in Fig. 5 for the individual PlioMIP2 models. All models except
MRI-CGCM 2.3 (Fig. 5n) show a deepening of the low-pressure area across the
Sahara region (negative anomalies) and a strengthening of the negative
latitudinal pressure gradients between the Sahara and the equatorial Atlantic.
CCSM4-NCAR, EC-Earth3-LR, and CCSM4-UofT (Fig. 5b, f and q), the models with
some of the highest pattern correlation in rainfall to the ensemble mean,
all exhibit a clear north–south dipole pattern with negative sea level
pressure anomalies over the Sahara continuing northward into Europe and
positive anomalies over the Sahel, the coast of Guinea, and the equatorial
Atlantic. The same dipole pattern, with a latitudinal transition at approx.
17<inline-formula><mml:math id="M75" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, is also seen in seven additional ensemble members
(CCSM4-Utrecht, CESM2, GISS-E2-1-G, HadGEM3, MIROC4m, NorESM-L, and
NorESM1-F), but while MRI-CGCM 2.3 exhibits positive sea level pressure
anomalies south of 15<inline-formula><mml:math id="M76" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, the negative anomalies over the Sahara are
divided by positive anomalies over northern Africa and southern Europe,
centred on the Mediterranean region, resulting in a quadrupole-type pattern
(Fig. 5n). The three IPSL models (IPSLCM6A, IPSLCM5A and IPSLCM5A2) show
negative anomalies or weak positive anomalies south of 17<inline-formula><mml:math id="M77" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N,
forming a weaker enhancement of the latitudinal pressure gradient relative
to the other PlioMIP2 models.</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="d1e1616">July–October (JASO) mean sea level pressure (shading) and
850 hPa horizontal wind (vectors) anomalies for the PlioMIP2 ensemble
members <bold>(a–q)</bold>.</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1777/2021/cp-17-1777-2021-f05.png"/>

        </fig>

      <p id="d1e1629">Associated with the deepening of the Saharan Heat Low and strengthening of
the latitudinal pressure gradients is an anomalous cyclonic flow and
strengthened westerly and southwesterly horizontal winds at the 850 hPa level,
going from the equatorial Atlantic into the Sahel and Sahara (Fig. 5a–q). This
is seen in all models, albeit at different magnitudes, with the highest
increase in wind speed seen in CCSM4-Utrecht, EC-Earth3-LR, and MIROC4m (Fig. 5c, f and m) and the lowest in GISS-E2-1-G, IPSLCM5A, and
IPSLCM5A2 (Fig. 5g, j and k).</p>
      <?pagebreak page1784?><p id="d1e1632">The JASO near-surface temperature anomalies (<inline-formula><mml:math id="M78" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>SAT, mPWP-PI, Fig. 6)
show a strengthened north–south temperature gradient between the Sahara
Desert and the equatorial Atlantic for all models except MRI-CGCM 2.3 (Fig. 6n). The temperature increase either stretches relatively uniformly across the
Sahara, as in EC-Earth3-LR, COSMOS, and CCSM4-UofT, or exhibits two separate
centres, one in the western Sahara and one in the eastern Sahara, as in MIROC4m,
NorESM-L, and NorESM1-F. MRI-CGCM 2.3 (Fig. 6n) has positive temperature
anomalies located mainly outside the Sahara, centred along both the western
coast of the Sahara and over the eastern Sahara and the Arabian Peninsula. An area
of negative temperature anomalies is located over the Mediterranean region,
and its surrounding areas in the northern Sahara exhibit a weaker warming than
the neighbouring areas of the Sahara Desert. Nine models show clear
latitudinal bands of negative anomalies stretching across northern Africa at
approx. 15<inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N (COSMOS, CCSM4-NCAR, CCSM4-Utrecht, EC-Earth 3-LR,
HadCM3, MIROC4m, MRI-CGCM 2.3, NorESM-L, NorESM1-F), similar to the latitude
of maximum rainfall increase. CCSM4-UofT temperatures exhibit negative
anomalies more dispersed over northern Africa, located mainly along the
western coastline of the Sahara and over the central Sahel region.</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="d1e1653">July–October (JASO) mean near-surface temperature
anomalies (<inline-formula><mml:math id="M80" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>SAT, mPWP-PI) for the PlioMIP2
ensemble members <bold>(a–q)</bold>.</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1777/2021/cp-17-1777-2021-f06.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Discussion</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>The paleo-proxy evidence for WAM during the mid-Pliocene</title>
      <p id="d1e1688">The mPWP is often used as an analogue for near-future climate change due to
its similar-to-modern paleogeography and high concentrations of CO<inline-formula><mml:math id="M81" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> in
the atmosphere
(Corvec
and Fletcher, 2017; Dowsett et al., 2013; Sun et al., 2013), and both marine
and terrestrial proxy reconstructions indicate a climate with higher sea
surface and surface air temperatures than present
(Dowsett
et al., 2013; Salzmann et al., 2008). A model–data comparison using PlioMIP1
indicated that the models underestimated the high-latitude warming by up to
15 <inline-formula><mml:math id="M82" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, while overestimating the low-latitude temperatures by 1–6 <inline-formula><mml:math id="M83" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C
(Dowsett
et al., 2013; Haywood et al., 2013; Salzmann et al., 2013). A comparison of
atmosphere-only general circulation models (AGCMs) and coupled
ocean–atmosphere models (AOGCMs) showed that AGCMs, using prescribed SSTs
based on paleo-reconstructions, produce a much stronger WAM compared to
models using a coupled ocean–atmosphere configuration, believed to be due to
the overestimation of SST and SAT in the tropics in the PlioMIP1 AOGCMs
(Zhang et al., 2016). Analysis of the PlioMIP2
ensemble by Haywood et al. (2020) indicates a widespread model–data agreement for SSTs and little
systematic temperature bias in the tropics, suggesting a reduced
underestimation of the WAM in the PlioMIP2, but the relatively low
availability of palaeohydrological proxies covering West Africa makes it
difficult to perform a similar model–data comparison for the WAM and its
related rainfall
(Salzmann
et al., 2008, 2013). However, several studies of proxy reconstructions
across northern Africa indicate a more humid climate during the
mid-Pliocene. Palynological data records suggest a higher density of tree
cover and an expansion of woodland and savanna in northern Africa at the
expense of deserts
(Bonnefille,
2010; Salzmann et al., 2008). Multi-proxy studies analysing, e.g. plant wax
and dust records in marine sediment cores taken offshore of West Africa,
indicate wetter conditions during the mid-Pliocene
(deMenocal,
2004; Feakins et al., 2005; Kuechler et al., 2018), which is qualitatively
consistent with the results from the PlioMIP2 ensemble (Fig. 2). The
expansion of forest into the Sahara region is also seen in the results from
COSMOS (Stepanek et al., 2020),
which is the only member of the PlioMIP2 ensemble that is run with dynamic
vegetation. It is also important to note that the PlioMIP2 ensemble is
designed to simulate the Marine Isotope Stage KM5c (MIS KM5c; 3.205 Ma) within the mPWP
(Haywood
et al., 2020, 2016), and while it<?pagebreak page1786?> represents a useful comparison to modern
conditions it might not represent the full climate variability within the
mPWP, possibly affecting model–data comparisons
(Prescott
et al., 2014; Samakinwa et al., 2020).</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>WAM – PI and mid-Pliocene</title>
      <p id="d1e1726">High pattern correlations of JAS rainfall over West Africa (<inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mi mathvariant="italic">&gt;</mml:mi><mml:mn mathvariant="normal">0.90</mml:mn></mml:mrow></mml:math></inline-formula>; Table 2) between the PI simulations and climatologies based on
observational data (CRU: 1901–1930;Harris et
al., 2020) for all models (<inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.97</mml:mn></mml:mrow></mml:math></inline-formula> for MMM) indicate that the models are
able to sufficiently reproduce the WAM rainfall pattern. However, looking at
the absolute values (Fig. 1) it is clear that while they capture the general
seasonal cycle with rainfall peaking in July–September, most models still
underestimate the magnitude of the modern summer rainfall over the Sahel by 1–3 mm/d, the only exceptions being CESM1.2 and MIROC4m with <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mi mathvariant="italic">&gt;</mml:mi><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> mm/d of rainfall in August. This is consistent with our general
understanding that models struggle to capture West African rainfall
(e.g. Roehrig et al., 2013).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e1766">Pattern correlation of July–September mean rainfall over
West Africa (0–25<inline-formula><mml:math id="M87" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 30<inline-formula><mml:math id="M88" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–30<inline-formula><mml:math id="M89" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) between
PlioMIP2 PI simulations, including the MMM and observational data (CRU TS
v4.: 1901–1930 mean).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="18">
     <oasis:colspec colnum="1" colname="col1" align="center"/>
     <oasis:colspec colnum="2" colname="col2" align="center"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:colspec colnum="6" colname="col6" align="center"/>
     <oasis:colspec colnum="7" colname="col7" align="center"/>
     <oasis:colspec colnum="8" colname="col8" align="center"/>
     <oasis:colspec colnum="9" colname="col9" align="center"/>
     <oasis:colspec colnum="10" colname="col10" align="center"/>
     <oasis:colspec colnum="11" colname="col11" align="center"/>
     <oasis:colspec colnum="12" colname="col12" align="center"/>
     <oasis:colspec colnum="13" colname="col13" align="center"/>
     <oasis:colspec colnum="14" colname="col14" align="center"/>
     <oasis:colspec colnum="15" colname="col15" align="center"/>
     <oasis:colspec colnum="16" colname="col16" align="center"/>
     <oasis:colspec colnum="17" colname="col17" align="center"/>
     <oasis:colspec colnum="18" colname="col18" align="center"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <?xmltex \rotentry?><oasis:entry colname="col1">COSMOS</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col2">CCSM4-NCAR</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col3">CCSM4-Utrecht</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col4">CESM1.2</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col5">CESM2</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col6">EC-Earth3-LR</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col7">GISS-E2-1-G</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col8">HadGEM3</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col9">IPSLCM5A2</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col10">IPSLCM5A</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col11">IPSL-CM6A-LR</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col12">HadCM3</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col13">MIROC4m</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col14">MRI-CGCM2.3</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col15">NorESM1-F</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col16">NorESM-L</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col17">CCSM4-UofT</oasis:entry>
         <?xmltex \rotentry?><oasis:entry colname="col18">MMM</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">0.95</oasis:entry>
         <oasis:entry colname="col2">0.98</oasis:entry>
         <oasis:entry colname="col3">0.97</oasis:entry>
         <oasis:entry colname="col4">0.96</oasis:entry>
         <oasis:entry colname="col5">0.98</oasis:entry>
         <oasis:entry colname="col6">0.90</oasis:entry>
         <oasis:entry colname="col7">0.95</oasis:entry>
         <oasis:entry colname="col8">0.95</oasis:entry>
         <oasis:entry colname="col9">0.93</oasis:entry>
         <oasis:entry colname="col10">0.90</oasis:entry>
         <oasis:entry colname="col11">0.93</oasis:entry>
         <oasis:entry colname="col12">0.95</oasis:entry>
         <oasis:entry colname="col13">0.96</oasis:entry>
         <oasis:entry colname="col14">0.94</oasis:entry>
         <oasis:entry colname="col15">0.96</oasis:entry>
         <oasis:entry colname="col16">0.97</oasis:entry>
         <oasis:entry colname="col17">0.97</oasis:entry>
         <oasis:entry colname="col18">0.97</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e1985">The MMM shows a clear increase in summer rainfall in the Sahel region and
(to a lesser extent) over the Sahara region, consistent with a
strengthened WAM during the mPWP (Fig. 1). The anomalies are centred on mid-summer
to late summer (August–September), which indicates a later withdrawal of the
WAM and a lengthened monsoon season. The monsoonal rainfall over the
(terrestrial) Coast of Guinea also exhibits larger positive anomalies over
the later months of the summer rainfall, further suggesting an
intensification of<?pagebreak page1787?> the WAM rainfall towards the end of the monsoon season as
well as a later withdrawal during the mid-Pliocene.</p>
      <p id="d1e1989">There is a large consistency within the ensemble regarding the general
features of the mPWP WAM (Fig. 2). All models show a JASO rainfall
increase over the Sahel reaching up into the Sahara and negative anomalies over the
Equatorial Atlantic, indicating an intensification and northward shift as
well as expansion of the WAM. The changes are statistically robust and
consistent with previous studies on both PlioMIP1 and 2, where the tropics,
particularly the Northern Hemisphere monsoon region, is identified as a
region with a robust rainfall signal during the mid-Pliocene
(Haywood
et al., 2020; Li et al., 2018; Pontes et al., 2020; Zhang et al., 2016). A
model–proxy comparison by Feng et al. (2021) has also shown that the wetter conditions seen over the Sahel and West
Africa in PlioMIP2 (Fig. 2) are consistent with the available qualitative
indicators of mPWP hydroclimate, although the magnitude of change cannot be
obtained from these proxy datasets and therefore not compared quantitatively
to the PlioMIP2 results.</p>
      <p id="d1e1992">The signal is markedly stronger in the PlioMIP2 compared to PlioMIP1, where
the MMM shows a doubling of the rainfall increase over Sahel from 1–2 mm/d
in PlioMIP1 (Zhang et al., 2016) to 2–4 mm/d in
PlioMIP2 (Fig. 2). Note that the use of June–August as the monsoon season in
Zhang et al. (2016) might also have contributed to
the discrepancy, especially given the rainfall increase seen in our results
over the later part of the monsoon season (Fig. 1). The updated boundary
conditions from PRISM3 to PRISM4 might have contributed to this enhancement,
where a sensitivity study by
(Samakinwa et al., 2020)
using COSMOS has shown that the updated paleogeography played the largest
role in the changes to the global large-scale climate between PlioMIP1 and
PlioMIP2. However, these changes appear to be more pronounced in high latitudes than in
low latitudes (Samakinwa et
al., 2020), and HadGEM3 and MRI-CGCM 2.3, which did not implement the
enhanced boundary conditions, still exhibit a precipitation response over
West Africa within 1 SD of the MMM (Fig. 2).
Haywood et al. (2020) instead
suggest that the sensitivity of the individual ensemble members to the
mid-Pliocene boundary conditions is mostly related to the model
parameterization and initial conditions, with model improvements between the
two phases also playing a role. Within model families, later model versions,
run with the same boundary and initial conditions, tend to be more sensitive
than earlier versions (Haywood et
al., 2020). This is also consistent with our results, where CESM2
exhibits larger rainfall anomalies than CESM1.2 and IPSLCM6A exhibits larger
rainfall anomalies than IPSLCM5A and IPSLCM5A2, for example (Fig. 3).</p>
      <p id="d1e1995">The precipitation response of the models over West Africa is also in many
ways similar to their global response, where, for example, the weakest rainfall
increase in the Sahel is seen in GISS-E2-1-G (Fig. 2), consistent with the
model's low global rainfall response to the mid-Pliocene boundary conditions
(Haywood et al., 2020). Models
that were identified as having a larger land–sea rainfall anomaly contrast,
with a larger rainfall enhancement over land compared to the ocean
(Haywood et al., 2020), are also
the models that show a larger rainfall increase in the Sahel (EC-Earth3-LR,
HadCM3, MIROC4m, NorESM1-F, NorESM-L and CCSM4-UofT). However, COSMOS, which
did not show a clear land rainfall enhancement globally, exhibits similarly
strong levels of rainfall increase in the Sahel, even slightly more than
NorESM1-F (2.3 and 2.0 mm/d respectively).</p>
      <p id="d1e1998">Haywood et al. (2020) also
suggest that, in general, models exhibiting large SAT sensitivity (i.e.
high global mean <inline-formula><mml:math id="M90" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>SAT) also exhibit a larger rainfall change
(globally), but there is still uncertainty in changes in more regional
patterns. While this finding is consistent with the results from
EC-Earth3-LR, which has one of the highest increases in both Sahel rainfall
and global SAT (De Nooijer et al., 2020), there is less
consistency within the remaining ensemble. MIROC4m and IPSLCM6A both exhibit
similar global <inline-formula><mml:math id="M91" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>SAT (De Nooijer et al., 2020), but
their rainfall change differs by close to a factor of 3 (Fig. 3). The
PlioMIP2 models, however, show a consistent JASO warming of the Sahara Desert
(Fig. 6), and if the analysis is limited to the Sahara (10<inline-formula><mml:math id="M92" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–10<inline-formula><mml:math id="M93" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, 20–30<inline-formula><mml:math id="M94" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N), a clear link between the <inline-formula><mml:math id="M95" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>SAT
and the rainfall increase can be observed (Fig. 7, <inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.42</mml:mn></mml:mrow></mml:math></inline-formula>, 90 %
significance, and if only looking at JAS: <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.50</mml:mn></mml:mrow></mml:math></inline-formula>, 95 % significance). The
warming of the Sahara and strengthened latitudinal temperature
gradient between the Sahara region and<?pagebreak page1788?> the equatorial Atlantic leads to a
deepening of the thermally induced Saharan Heat Low (Fig. 5)
(Lavaysse et al., 2009).
This deepened Saharan Heat Low induces low-level convergence and strengthens
the southwesterly flow, bringing moisture from the equatorial Atlantic into
the continent, leading to increased moisture availability and rainfall over
Sahel and parts of Sahara and, in summary, indicating a strengthened WAM
(Fig. 5).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e2076">Sahel (10–20<inline-formula><mml:math id="M98" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 20<inline-formula><mml:math id="M99" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–30<inline-formula><mml:math id="M100" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E)
rainfall and Sahara (20–30<inline-formula><mml:math id="M101" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 10<inline-formula><mml:math id="M102" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–10<inline-formula><mml:math id="M103" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E)
near-surface temperature anomalies (mPWP <inline-formula><mml:math id="M104" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula> PI). Filled markers and the black line
show JASO anomalies and least-squares fit, while non-filled markers and
the dashed line show JAS anomalies and least-squares fit.</p></caption>
          <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1777/2021/cp-17-1777-2021-f07.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>Role of mid-Pliocene forcing and boundary conditions</title>
      <p id="d1e2155">The warming of the Sahara region and subsequent strengthening of the WAM is
similar to what we see during other warm climates, such as the mid-Holocene
and last interglacial period
(Gaetani et al., 2017; Otto-Bliesner
et al., 2021), but given the boundary conditions in the mid-Pliocene
simulations this warming over Sahara is most likely driven by the changes in
the atmospheric CO<inline-formula><mml:math id="M105" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> concentration, topography, and related vegetation
changes over West Africa. Studies of model simulations as well as
observational data has shown that greenhouse gas forcing leads to a
land–ocean warming contrast, with a larger temperature increase over land
(Byrne
and O'Gorman, 2013; Haywood et al., 2020; Lambert et al., 2011). The
contrast is a result of the lower moisture availability over land
influencing the lapse rate and leading to a higher warming compared to the
ocean (Byrne and O'Gorman, 2013), which is
consistent with the strong response over the arid Sahara region (Fig. 6).
Studies show that this land–ocean warming contrast is present in both
equilibrium and transient simulations
(Lambert et al., 2011), and future
scenarios of climate change show a continued land–ocean contrast and warming
of the Sahara region
(Boer, 2011; Sutton et
al., 2007), leading to strengthened latitudinal temperature gradients.</p>
      <p id="d1e2167">In addition to the CO<inline-formula><mml:math id="M106" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> forcing, the majority of the PlioMIP2 ensemble
members were forced by the PRISM4 boundary conditions, with reconstructed
distributions of topography, bathymetry, land ice cover, vegetation, and
land–sea mask being amongst the major changes compared to modern geography
(Dowsett et al.,
2016; Haywood et al., 2016). While the PlioMIP2 set-up, with orography and
vegetation being changed together, makes it difficult to distinguish between
the impact of the two boundary conditions, the sensitivity simulations by
COSMOS indicate that the mid-Pliocene paleogeography still contributes to
the increased rainfall over West Africa in mPWP
(Stepanek et al., 2020). The
enhanced topography with closed Arctic gateways has been shown to strengthen
the Atlantic meridional overturning circulation (AMOC), contributing to the
warming in the North Atlantic seen in PlioMIP2, as well as the reduced
model–proxy mismatch between PlioMIP1 and 2 (Z. Zhang et
al., 2021). However, although the strength of the AMOC has been linked to
rainfall variability over the Sahel (Mulitza et al., 2008),
HadGEM3, which did not include the enhanced topography and instead exhibits a
weakening of the AMOC (Z. Zhang et al., 2021​​​​​​​), still
exhibits a rainfall increase over West Africa close to (within 1 SD) the MMM (Fig. 2). These findings indicate that other
mid-Pliocene boundary conditions remain important related to rainfall
changes over West Africa.</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="d1e2181">Prescribed PRISM4 <bold>(a)</bold> high and <bold>(b)</bold> low vegetation used as
boundary conditions for PlioMIP2 simulations
(Dowsett et al., 2016), sourced from
Salzmann et
al. (2008).</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1777/2021/cp-17-1777-2021-f08.png"/>

        </fig>

      <p id="d1e2197">Land surface changes are also known to impact rainfall over West Africa,
where, e.g. expansion of vegetation into the Sahara region at the expense
of desert leads to a decrease of the surface albedo and an increase in
equivalent potential temperature, further strengthening the Saharan Heat Low
and subsequently the WAM, leading to a vegetation–albedo feedback
(Charney, 1975). Additionally, later modelling studies
have emphasized the role of soil moisture
(Patricola and Cook, 2008) and
evapotranspiration (Rachmayani et al., 2015) in the
vegetation–precipitation feedback due to their effect on low-level moist
static energy, convective instability, and surface latent heat flux
anomalies. These feedback mechanisms have been shown to strengthen the
response of the WAM to external forcing in other past climates
(e.g. Braconnot et al.,
1999; Chandan and Peltier, 2020; Claussen and Gayler, 1997; Messori et al.,
2019; Rachmayani et al., 2015), and the enhanced vegetation in the PlioMIP2
ensemble
(Haywood
et al., 2020; Salzmann et al., 2008) is likely to have contributed to the
strengthening of the mPWP WAM and West African summer rainfall. While
vegetation and orography are changed together in PlioMIP2, making it
difficult to separate the impact of the two boundary conditions, sensitivity
experiments indicate that they play a large role in the mPWP rainfall
increase over West Africa
(Chan
and Abe-Ouchi, 2020; Hunter et al., 2019; Kamae et al., 2016). Studies by
Feng et al. (in review, Sci. Adv.) further indicate
that the enhanced vegetation drives the mPWP hydroclimatological changes
over the Sahel to a larger extent than the enhanced topography. In PlioMIP2 the
enhanced vegetation is used as a boundary condition (Fig. 8), but a
northward expansion of vegetation is also seen in the dynamic vegetation
model COSMOS (Stepanek et
al., 2020, Fig. 25e, f), indicating that the mPWP rainfall increase over
West Africa and Sahel of 2.5 mm/d for the MMM and 2.3 mm/d for COSMOS
(Fig. 3) can support the enhanced vegetation cover seen in the PRISM4.</p>
      <p id="d1e2200">As the latitudinal land–ocean temperature gradient is central to the
development and strength of the WAM through the development of the Saharan
Heat Low (Lavaysse et al.,
2009), the results have strong implications for future scenarios. Unlike the
results in PlioMIP2, and previously in PlioMIP1
(Zhang et al., 2016), which exhibit a uniform
rainfall increase over West Africa, both CMIP3 (SRES A2) and CMIP5 (RCP8.5)
model ensembles show a drying over the western Sahel and a rainfall increase
over the central and eastern Sahel (Roehrig et
al., 2013). As analysis of both CMIP3 and CMIP5 ensembles show a large
spread in projected rainfall change in the Sahel region, which weakens its
confidence in future projections (Roehrig et
al., 2013), our<?pagebreak page1789?> results support a future strengthening of the WAM and
rainfall increase over West Africa and the Sahel in a high CO<inline-formula><mml:math id="M107" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> scenario.
However, given the role of the enhanced vegetation in the strengthening of
the mPWP WAM, this will also depend on the future vegetation changes in the
region which still remain elusive (Bathiany
et al., 2014).</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusion</title>
      <p id="d1e2222">The PlioMIP2 ensemble shows a clear rainfall increase over West Africa, with
the largest increase located over Sahel, and a strengthening of the WAM
leading to the rainfall reaching farther in over the continent. These
results are consistent with geological evidence which suggests a more humid
climate during the mid-Pliocene
(Kuechler
et al., 2018; Salzmann et al., 2008). Some regional differences occur among
the ensemble members, mainly along the coast of the Gulf of Guinea, where
some models indicate drier conditions while<?pagebreak page1790?> other models indicate a rainfall
increase. The largest inter-model variability is centred along the Sahel, where
the magnitude of the rainfall increase varies largely between the models.
The strengthened WAM is driven by the warming of the Sahara region and
subsequent deepening of the Saharan Heat Low, most likely due to the
greenhouse gas forcing, vegetation changes, and land–ocean warming contrast.
The deepened Saharan Heat Low leads to anomalous cyclonic flow and increased
moisture flux into the Sahel region, resulting in a northward shift and
intensification of the rainbelt. Given the potential for using the PlioMIP2
as an analogue for near-future scenarios, these results suggest a more
uniform rainfall increase over West Africa and the Sahel region, unlike the
east–west contrast seen in both CMIP3 and CMIP5 future projections
(Roehrig et al., 2013). Alternatively, these
results suggest that the extent of analogue between mid-Pliocene and future
climate in the context of rainfall over West Africa may depend on the
long-term response of vegetation to the CO<inline-formula><mml:math id="M108" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> forcing and on the speed
with which climate adapts to future carbon dioxide burden – CMIP simulations
of a transient climate and mid-Pliocene simulations of a quasi-equilibrium
climate representing endmembers of potential future conditions.</p>
</sec>

      
      </body>
    <back><notes notes-type="codedataavailability"><title>Code and data availability</title>

      <p id="d1e2238">The model data can be downloaded from PlioMIP2 data server located at the
School of Earth and Environment of the University of Leeds; an email can be
sent to Alan Haywood (a.m.haywood@leeds.ac.uk) for access.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e2244">EB and QZ designed the work. EB did the
analysis and wrote the manuscript. QZ, QL, AMH, JCT, SJH, ZZ, XL, CG, KHN, CS, GL, LES, MAC, NT, CC, GR, MLJB, ASvdH, DC, WRP, AAO, WLC, YK, CJRW, DJL, RF, BLOB, and ECB provided the PlioMIP2 experiments and contributed to the discussion of the results.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e2250">The authors declare that they have no conflict of interest.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e2256">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><notes notes-type="sistatement"><title>Special issue statement</title>

      <p id="d1e2262">This article is part of the special issue “PlioMIP Phase 2: experimental design, implementation and scientific results”. It does not belong to a conference.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e2268">The
model simulations with EC-Earth3 and data analysis were performed by
resources provided by ECMWF's computing and archive facilities and the
Swedish National Infrastructure for Computing (SNIC) at the National
Supercomputer Centre (NSC).</p><p id="d1e2270">Gerrit Lohmann and Christian Stepanek acknowledge computational resources from the Computing and Data
Centre of the Alfred-Wegener-Institute – Helmholtz-Centre for Polar and
Marine Research. Gerrit Lohmann and CS acknowledge funding via the Helmholtz Climate
Initiative REKLIM and the Alfred Wegener Institute's research programme
“Changing Earth – Sustaining our Future”.</p><p id="d1e2272">Bette L. Otto-Bliesner, Esther C. Brady and Ran Feng acknowledge that
material for their participation is based upon work supported by the
National Center for Atmospheric Research, which is a major facility
sponsored by the National Science Foundation (NSF) (cooperative agreement
no. 1852977 and NSF OPP grant no. 1418411). Ran Feng is also supported by
NSF grant no. 1903650. The CESM project is supported primarily by the
National Science Foundation. Computing and data storage resources, including
the Cheyenne supercomputer (<ext-link xlink:href="https://doi.org/10.5065/D6RX99HX" ext-link-type="DOI">10.5065/D6RX99HX</ext-link>), were provided
by the Computational and Information Systems Laboratory (CISL) at NCAR. NCAR
is sponsored by the National Science Foundation.</p><p id="d1e2277">Wing-Le Chan and Ayako Abe-Ouchi acknowledge funding from JSPS (KAKENHI grant no. 17H06104 and
MEXT KAKENHI grant no. 17H06323) and computational resources from the Earth
Simulator at JAMSTEC, Yokohama, Japan.</p><p id="d1e2279">The NorESM simulations benefitted from resources provided by UNINETT Sigma2
– the National Infrastructure for High Performance Computing and Data
Storage in Norway</p><p id="d1e2281">William Richard Peltier and Deepak Chandan were supported by Canadian NSERC Discovery Grant A9627, and they
wish to acknowledge the support of SciNet HPC Consortium for providing
computing facilities. SciNet is funded by the Canada Foundation for
Innovation under the auspices of Compute Canada, the Government of Ontario,
the Ontario Research Fund – Research Excellence, and the University of
Toronto.</p><p id="d1e2283">Charles J. R. Williams and Daniel J. Lunt acknowledge the financial support of the UK Natural Environment
Research Council (NERC)-funded SWEET project (research grant no. NE/P01903X/1).</p><p id="d1e2285">Development of GISS-E2.1 was supported by the NASA Modeling, Analysis, and
Prediction (MAP) Program. CMIP6 simulations with GISS-E2.1 were made
possible by the NASA High-End Computing (HEC) Program through the NASA
Center for Climate Simulation (NCCS) at Goddard Space Flight Center.</p><p id="d1e2287">The PRISM4 reconstruction and boundary conditions used in PlioMIP2 were
funded by the U.S. Geological Survey Climate and Land Use Change Research
and Development Program. Any use of trade, firm, or product names is for
descriptive purposes only and does not imply endorsement by the U.S.
Government.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e2292">This research has been supported by the Vetenskapsrådet (grant nos. 2013-06476 and 2017-04232).<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>The article processing charges for this open-access <?xmltex \notforhtml{\newline}?> publication were covered by Stockholm University.</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <?pagebreak page1791?><p id="d1e2303">This paper was edited by Martin Claussen and reviewed by Matthias Prange and one anonymous referee.</p>
  </notes><ref-list>
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    <!--<article-title-html>Mid-Pliocene West African Monsoon rainfall as simulated in the PlioMIP2 ensemble</article-title-html>
<abstract-html><p>The mid-Pliocene warm period (mPWP; <span style="" class="text"> ∼ 3.2</span> million years ago) is seen as the most recent time period characterized by a
warm climate state, with similar to modern geography and  ∼ 400&thinsp;ppmv atmospheric CO<sub>2</sub> concentration, and is therefore often considered
an interesting analogue for near-future climate projections.
Paleoenvironmental reconstructions indicate higher surface temperatures,
decreasing tropical deserts, and a more humid climate in West Africa
characterized by a strengthened West African Monsoon (WAM). Using model
results from the second phase of the Pliocene Modelling Intercomparison
Project (PlioMIP2) ensemble, we analyse changes of the WAM rainfall during
the mPWP by comparing them with the control simulations for the pre-industrial
period. The ensemble shows a robust increase in the summer rainfall over
West Africa and the Sahara region, with an average increase of 2.5&thinsp;mm/d,
contrasted by a rainfall decrease over the equatorial Atlantic. An anomalous
warming of the Sahara and deepening of the Saharan Heat Low, seen in
<i>&gt;</i>90&thinsp;% of the models, leads to a strengthening of the WAM and
an increased monsoonal flow into the continent. A similar warming of the
Sahara is seen in future projections using both phase 3 and 5 of the
Coupled Model Intercomparison Project (CMIP3 and CMIP5). Though previous
studies of future projections indicate a west–east drying–wetting contrast
over the Sahel, PlioMIP2 simulations indicate a uniform rainfall increase in
that region in warm climates characterized by increasing greenhouse gas
forcing. We note that this effect will further depend on the long-term
response of the vegetation to the CO<sub>2</sub> forcing.</p></abstract-html>
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