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  <front>
    <journal-meta><journal-id journal-id-type="publisher">GMD</journal-id><journal-title-group>
    <journal-title>Geoscientific Model Development</journal-title>
    <abbrev-journal-title abbrev-type="publisher">GMD</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Geosci. Model Dev.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1991-9603</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/gmd-12-1351-2019</article-id><title-group><article-title>A predictive algorithm for wetlands in deep <?xmltex \hack{\break}?> time paleoclimate models</article-title><alt-title>A predictive algorithm for wetlands in deep-time paleoclimate models</alt-title>
      </title-group><?xmltex \runningtitle{A predictive algorithm for wetlands in deep-time paleoclimate models}?><?xmltex \runningauthor{D. J. Wilton et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Wilton</surname><given-names>David J.</given-names></name>
          <email>d.j.wilton@shef.ac.uk</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff3 aff4">
          <name><surname>Badger</surname><given-names>Marcus P. S.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8195-5244</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Kantzas</surname><given-names>Euripides P.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7610-1874</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Pancost</surname><given-names>Richard D.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Valdes</surname><given-names>Paul J.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1902-3283</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Beerling</surname><given-names>David J.</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Department of Animal and Plant Sciences, The University of Sheffield, Sheffield, S10 2TN, UK</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>School of Environment, Earth and Ecosystem Sciences, The Open University, Milton Keynes, MK7 6AA, UK</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Organic Geochemistry Unit, The Cabot Institute, School of Chemistry, School of Earth Sciences,<?xmltex \hack{\break}?> The University of Bristol, Bristol, BS8 1TH, UK</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Bristol Research Initiative for the Dynamic Global Environment (BRIDGE), The Cabot Institute, <?xmltex \hack{\break}?> School of Geographical Sciences, The University of Bristol, BS8 1TH, UK</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">David J. Wilton (d.j.wilton@shef.ac.uk)</corresp></author-notes><pub-date><day>4</day><month>April</month><year>2019</year></pub-date>
      
      <volume>12</volume>
      <issue>4</issue>
      <fpage>1351</fpage><lpage>1364</lpage>
      <history>
        <date date-type="received"><day>30</day><month>August</month><year>2018</year></date>
           <date date-type="rev-request"><day>27</day><month>September</month><year>2018</year></date>
           <date date-type="rev-recd"><day>30</day><month>January</month><year>2019</year></date>
           <date date-type="accepted"><day>3</day><month>March</month><year>2019</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2019 David J. Wilton et al.</copyright-statement>
        <copyright-year>2019</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://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019.html">This article is available from https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019.html</self-uri><self-uri xlink:href="https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019.pdf">The full text article is available as a PDF file from https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e152">Methane is a powerful greenhouse gas produced in wetland
environments via microbial action in anaerobic conditions. If the location and extent of
wetlands are unknown, such as for the Earth many millions of years in the past, a model
of wetland fraction is required in order to calculate methane emissions and thus help
reduce uncertainty in the understanding of past warm greenhouse climates. Here we present
an algorithm for predicting inundated wetland fraction for use in calculating wetland
methane emission fluxes in deep-time paleoclimate simulations. For each grid cell in a
given paleoclimate simulation, the algorithm determines the wetland fraction predicted by
a nearest-neighbour search of modern-day data in a space described by a set of
environmental, climate and vegetation variables. To explore this approach, we first test
it for a modern-day climate with variables obtained from observations and then for an
Eocene climate with variables derived from a fully coupled global climate model
(HadCM3BL-M2.2; Valdes et al., 2017). Two independent dynamic vegetation models were used
to provide two sets of equivalent vegetation variables which yielded two different
wetland predictions. As a first test, the method, using both vegetation models,
satisfactorily reproduces modern day wetland fraction at a course grid resolution, similar to those used in
paleoclimate simulations. We then applied the method to an early Eocene climate, testing
its outputs against the locations of Eocene coal deposits. We predict global mean monthly
wetland fraction area for the early Eocene of <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mn mathvariant="normal">8</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mn mathvariant="normal">10</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> with a
corresponding total annual methane flux of 656 to 909 Tg <inline-formula><mml:math id="M4" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> yr<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>,
depending on which of the two different dynamic global vegetation models are used to
model wetland fraction and methane emission rates. Both values are significantly higher
than estimates for the modern day of <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> and around
190 Tg <inline-formula><mml:math id="M8" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> yr<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (Poulter et al., 2017; Melton et al., 2013).</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e274">Methane (<inline-formula><mml:math id="M10" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) is a powerful greenhouse gas. As well as absorbing infrared
radiation from the Earth's surface, it also contributes to additional indirect warming
through its photochemistry and oxidation to <inline-formula><mml:math id="M11" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in the atmosphere (IPCC, 2013).
Along with other trace gases, methane is therefore an important component of the Earth's
climate system; but for studies of the past, such as warm greenhouse paleoclimates, we
lack suitable geochemical or biological proxies for methane concentration. Therefore,
Earth system models used to reconstruct ancient climate or develop future climate
scenarios must either assume atmospheric methane concentrations as a boundary condition
and/or incorporate dynamic methane fluxes from natural sources and sinks (Beerling et
al., 2011). The main natural source of methane is wetland environments via microbial
action in anaerobic conditions (Whiticar, 1999), but methane fluxes from wetlands are
also<?pagebreak page1352?> modulated by climatic factors such as temperature (Westermann,
1993). Therefore, in order to model fluxes of methane to the atmosphere
both the extent and locations of wetlands need to be known. For the modern day, recent
past and near-future scenarios, maps of observed wetland extent (Prigent et al., 2007;
Papa et al., 2010; Schroeder et al., 2015; Poulter et al., 2017) can be used or wetland
extent can be calculated at a sub-grid level from fine-resolution topographical data (as
in the TOPMODEL approach of Beven and Kirkby, 1979; Lu and Zhuang, 2012; Stocker et al.,
2014), as wetlands only form where
the ground is relatively flat.</p>
      <p id="d1e299">For the study of deep-time paleoclimates (many millions of years in the past) there are
no direct observations of wetland extent, although we may use a proxy such as coal
deposit locations as we discuss in Sect. 3.2.1, and the topography is only known on
relatively coarse resolutions of around 0.5<inline-formula><mml:math id="M12" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> at best. Therefore, any model
calculation of wetland extent must either rely on using approximate knowledge of the
topography or not rely on the topography at all. Previous studies (Beerling et al., 2011;
Valdes et al., 2005), the only current model-based approach for deep-time paleoclimates,
classified grid cells as either producing or not producing methane, based on either (i) a
month being within a defined melt season for grid cells where mean monthly temperature
drops below 0 <inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C for at least 1 month of the year, or (ii) precipitation being
greater than evapotranspiration. They then scaled emissions by empirically derived
functions of the variance or standard deviation of orography at the best resolution
available. The scaling effectively reduces methane emission rates in grid cells where
elevation varies significantly and are therefore unlikely to have substantial wetlands
within them, but relies on what may be quite coarse-resolution topography not able to
resolve sub-grid-scale variations. The goal of this paper is to explore other
methodologies for calculating wetland extent in the context of a deep-time paleoclimates.</p>
      <p id="d1e320">In this work we develop a nearest-neighbour-based algorithm to predict the fraction of a
specified area that is wetland (FW). We base this on a modern-day reference data set of
FW and corresponding environmental variables, empirically associating the FW observations
with corresponding observed climate data and vegetation data calculated using one of two
dynamic global vegetation models (DGVMs), the Sheffield Dynamic Global Vegetation Model
(Woodward et al., 1995; Beerling and Woodward, 2001) and the
Lund-Postdam-Jenna model (Wania et al., 2009). Wetland is defined in the same manner as
for our reference data (Poulter et al., 2017), discussed in the following section. It
includes both permanently and seasonally flooded soils but excludes lakes, reservoirs,
rivers, areas of rice cultivation, saline estuaries and salt marshes. We demonstrate its
application by predicting FW and <inline-formula><mml:math id="M14" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> fluxes for an early Eocene (52 Ma) model
climate, an interval of greenhouse warming (Zachos et al., 2008) when sedimentary records
indicate the existence of large areas of wetlands (Sloan et al., 1992; Beerling et al.,
2009). For the Eocene, the same climate variables are obtained from a fully coupled
global climate model and vegetation variables are derived from the same DGVMs. We then
predict FW for the Eocene by analysis and comparison to the modern-day reference data. We
note that different reference sets, vegetation models or climate models will likely yield
different results and these should be explored in future work; but our aim here is to
demonstrate this approach and its potential rather than to produce a model–model
intercomparison.</p>
      <p id="d1e334">In the “Data and methods” section we first describe modern-day wetland data at
0.5<inline-formula><mml:math id="M15" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> spatial resolution and a monthly time step for a mean modern-day year, along
with climate and vegetation data which we later use as a reference data set. We then
describe two test data sets at lower spatial resolution, equivalent to that used in
paleoclimate models, again for a single year. The first of these is for the modern day
and derived by interpolation of the reference data, and the second is derived from a
paleoclimate model of the early Eocene. We briefly describe unsuccessful attempts to
model FW through analysis of the reference data set. The main conclusion of these
unsuccessful attempts being to indicate that any relationship between FW and various
environmental variables must be quite complex. We then introduce the nearest-neighbour
method we later found to be successful and finally in that section describe the model
used to calculate wetland methane emissions.</p>
      <p id="d1e347">In the “Results and discussion” section we first discuss model results for the
modern-day test data set where we expect the nearest-neighbour method should perform
well, since the test data are simply a version of the reference data interpolated to
lower spatial resolution; these results, therefore, serve to demonstrate whether or not
some form of the nearest-neighbour method could be successfully applied to prediction of
FW for a climate very different to the modern day. We then apply this method to
prediction of FW for the Eocene, and show that we can tune it by using the locations of
coal deposits as wetland proxies.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data and methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Modern-day reference data</title>
      <p id="d1e365">We use a modern-day reference data set of observed FW, the term observed being used to
distinguish this from our later model results, with corresponding environmental data to
develop an algorithm for the prediction of FW in the past, i.e. we assume that there
exists a relationship between FW and the environmental variables compiled in the
reference data and then apply that relationship to predicting FW in the past. We use the
recently developed SWAMPS-GLWD (Poulter et al., 2017), which improves on the Surface
Water Microwave Product Series (SWAMPS; Schroeder et al., 2015) using the static
inventory of wetland area from the Global Lakes and Wetlands Database (GLWD; Lehner<?pagebreak page1353?> and
Doll, 2004), correcting the SWAMPS data set in regions where this satellite-derived data
set fails to detect water beneath closed canopies. We calculated the average monthly FW
at each 0.5<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M17" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.5<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid cell for the years 2000 to 2012 on a
monthly time step to give a modern-day FW (FW<inline-formula><mml:math id="M19" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:math></inline-formula>; annual max shown in
Fig. 1). Corresponding climate data on the same spatial and temporal resolution were
obtained from CRU-NCEP v4.0 (Wei et al., 2014) and averaged to give monthly values for a
mean modern-day year over the same time interval. The climate data for this mean year
were then used to drive two DGVMs: the Sheffield Dynamic Global Vegetation Model (SDGVM;
Woodward et al., 1995; Beerling and Woodward, 2001) and the Lund-Postdam-Jenna model
(LPJ; Wania et al., 2009) to produce corresponding vegetation data. The combination of
these yielded a reference data set of FW, climate (temperature and precipitation) and
vegetation (leaf area index, net primary productivity, transpiration, evapotranspiration,
soil water content and surface runoff) variables (either SDGVM or LPJ) for a set of
0.5<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M21" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.5<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> spatial and monthly temporal resolution sites for a
single modern-day average year. Some variables, such as transpiration and
evapotranspiration, are available from both climate and vegetation models. In such cases
we use those from the vegetation model as they will be calculated from a more advanced
vegetation scheme. To ensure that wetlands in areas dominated by agriculture or areas where one
of our vegetation models, SDGVM, predicts bare land did not bias our FW predictions,
such grid cells were removed from the reference data. For the latter, this was done
simply by removing those grid cells that SDGVM predicted to be bare land. For the former,
we removed those that were 50 % or more, by cover, classed as cultivated and managed
or mosaic cropland (Global Land Cover 2000 database, 2003).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><label>Figure 1</label><caption><p id="d1e430">Annual monthly maximum observed FW from the SWAMPS-GLWD data set
(Poulter et al., 2017), mean of 2000 to 2012. Grey shading indicates bare
land, as predicted by SDGVM, or <inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> % cultivated (Global Land
Cover 2000 database, 2003).</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019-f01.png"/>

        </fig>

      <p id="d1e449"><?xmltex \hack{\newpage}?>Many of the methods that can be used to analyse the reference data and predict FW require
that the data are scaled so that each variable covers a similar range of values.
Therefore, we scaled the values of each environmental variable, <inline-formula><mml:math id="M24" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula>, using their global
mean, <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and global standard deviation, <inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, i.e. for a given grid cell,
<inline-formula><mml:math id="M27" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>, each variable was scaled as
            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M28" display="block"><mml:mrow><mml:msup><mml:mi>X</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mfenced close=")" open="("><mml:mi>J</mml:mi></mml:mfenced><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>X</mml:mi><mml:mfenced open="(" close=")"><mml:mi>J</mml:mi></mml:mfenced><mml:mo>-</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          This scales all variables such that they have a global mean of 0 and standard deviation
of 1.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Test data sets</title>
      <p id="d1e537">A modern-day test data set was made by interpolating the reference climate
data to 2.5<inline-formula><mml:math id="M29" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M30" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 3.75<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, the spatial resolution
often used for paleoclimate models. The DGVM simulations were driven by
this interpolated data to yield the vegetation outputs. All climate and
vegetation variables were scaled in the same way as the reference data,
using the global means and standard deviations of the reference data. The
paleoclimatic assessment of our model was performed using an early Eocene
test data set made using a single year of output, on a monthly time step,
from a three-dimensional fully dynamic coupled ocean–atmosphere global
climate model HadCM3BL-M2.2 (Valdes et al., 2017), on a 2.5<inline-formula><mml:math id="M32" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> latitude
by 3.75<inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> longitude grid. To simulate the early Eocene a
Ypresian paleogeography and high <inline-formula><mml:math id="M34" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration (4 times modern; 1120 ppm; Anagnostou et
al., 2016) was used. SDGVM and LPJ were both run with these model-simulated
climate data to produce the vegetation variables required, as was done for
the reference data set, whereas temperature and precipitation were derived
directly from the climate model. All variables were again scaled using the
means and standard deviations of the reference data. Therefore, for each
climate, modern day and early Eocene, we have two test data sets for a mean
year on a monthly time step at 2.5<inline-formula><mml:math id="M35" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M36" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 3.75<inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> spatial
resolution and both with the same climate data, one with SDGVM vegetation data
and one with LPJ vegetation data. Predictions for each test data set were
made with the corresponding vegetation model's reference data set. The
reference and test data sets are summarised in Table 1.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><label>Table 1</label><caption><p id="d1e623">Summary of reference and test data sets used combining data from
dynamic global vegetation models SDGVM (Woodward et al., 1995; Beerling and
Woodward, 2001) and LPJ (Wania et al., 2009) with climate data from CRU-NCEP
v4.0 (Wei et al., 2014) for the modern day, and HadCM3BL-M2.2 (Valdes et
al., 2017) for the early Eocene.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <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:colspec colnum="4" colname="col4" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Data set</oasis:entry>
         <oasis:entry colname="col2">Time</oasis:entry>
         <oasis:entry colname="col3">Climate data source</oasis:entry>
         <oasis:entry colname="col4">DGVM used</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">SDGVM reference</oasis:entry>
         <oasis:entry colname="col2">modern day</oasis:entry>
         <oasis:entry colname="col3"><italic>CRU-NCEP v4.0</italic></oasis:entry>
         <oasis:entry colname="col4">SDGVM</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">LPJ reference</oasis:entry>
         <oasis:entry colname="col2">modern day</oasis:entry>
         <oasis:entry colname="col3"><italic>CRU-NCEP v4.0</italic></oasis:entry>
         <oasis:entry colname="col4">LPJ</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SDGVM modern test</oasis:entry>
         <oasis:entry colname="col2">modern day</oasis:entry>
         <oasis:entry colname="col3">Interpolated <italic>CRU-NCEP v4.0</italic></oasis:entry>
         <oasis:entry colname="col4">SDGVM</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">LPJ modern test</oasis:entry>
         <oasis:entry colname="col2">modern day</oasis:entry>
         <oasis:entry colname="col3">Interpolated <italic>CRU-NCEP v4.0</italic></oasis:entry>
         <oasis:entry colname="col4">LPJ</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SDGVM Eocene test</oasis:entry>
         <oasis:entry colname="col2">early Eocene</oasis:entry>
         <oasis:entry colname="col3"><italic>HadCM3BL-M2.2</italic></oasis:entry>
         <oasis:entry colname="col4">SDGVM</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">LPJ Eocene test</oasis:entry>
         <oasis:entry colname="col2">early Eocene</oasis:entry>
         <oasis:entry colname="col3"><italic>HadCM3BL-M2.2</italic></oasis:entry>
         <oasis:entry colname="col4">LPJ</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Initial unsuccessful models of wetland fraction</title>
      <p id="d1e768">Before discussing the model we employed to predict paleoclimate FW, it is
useful to describe briefly other strategies that we attempted but did not
yield robust predictions when evaluated against modern-day data. The first of
these was to examine FW vs. individual environmental variables graphically
from the reference data to ascertain if we could define ranges for those
variables that corresponded to predominantly low or high FW; this is similar
to the approach of Shindell et al. (2004), who proposed threshold values of
standard deviation of topography, ground temperature, ground<?pagebreak page1354?> wetness and
downward shortwave flux for wetland development. However, this proved
unsuccessful, revealing only the rather obvious relationship that wetlands do
not usually occur when mean monthly temperature is below 0 <inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C.
Although we expected to identify relationships for FW with other
environmental variables (i.e. ground wetness), none were found. This is due
to the combined effects of wetland occurrence being the function of multiple
factors and the fact that most grid cells have <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mi mathvariant="normal">FW</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> for
all months of the year and the number of grid cells with significantly
non-zero FW is quite small. Therefore, environmental variables associated
with high values of FW also tend to be associated with <inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:mi mathvariant="normal">FW</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>. Poor correlation of FW with environmental variables is also due to the
important control exerted by the topography; regardless of climate, wetlands
cannot form in landscapes where excess water flows away rather than remaining
in situ. Collectively, these factors caused significant overlap in the range
of environmental variables associated with both low and high FW.</p>
      <p id="d1e804">Another approach was a multiple linear regression using the reference data
in order to derive an equation for FW in terms of linear functions of
multiple environmental variables. However, this yielded equations that
predicted a widespread occurrence of very low FW, including those areas
where FW<inline-formula><mml:math id="M41" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:math></inline-formula> is very high either seasonally or throughout the year.
Similarly, poor predictive models were obtained whether derived for all
sites or just those restricted to specific plant functional types. These
outcomes likely occur because linear regression optimises a function by
minimising the error between predicted and observed values. As most grid
cells have <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:mi mathvariant="normal">FW</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> (Fig. 1), the “best” regression equation is one
that predicts FW to be very low almost everywhere, since in the majority of cases
this is quite accurate. Efforts were made to use other optimisation criteria
with customised functions that attempted to put more weight on predicting
high FW correctly at the expense of larger errors where FW is low. However,
these simply over-predicted FW. Therefore, we were unable to find any
satisfactory solution based on linear regression. The fact that we did not find a
satisfactory regression equation for FW on the reference data suggests that
any relationship between FW and the environmental variables must be complex
and therefore another approach is required if we are to be able to predict FW.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>FW predicted by a nearest-neighbour search</title>
      <p id="d1e836">Given that we were unable to find simple mathematical formula with which to
predict FW, we must consider another approach. Nearest-neighbour searches can
be used to predict a property for a query by comparing data for that query
to similar such data from a reference data set. We find the entry in the
reference data set that is most similar to, i.e. the nearest neighbour of,
the query, and predict the query has the same value in the property of
interest as its nearest neighbour. The reference data set of FW and
environmental variable sites, on a 0.5<inline-formula><mml:math id="M43" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid at a monthly time
step, can be viewed as a set of data points yielding FW at many different
locations in a multi-dimensional space. The eight dimensions of that space
are the two climate and six vegetation variables; temperature,
precipitation, leaf area index, net primary productivity, transpiration,
evapotranspiration, soil water content and surface runoff. If we have the
same environmental variables for a site of unknown FW, we can search the
reference data set for its nearest neighbour and then predict it would have
the same FW as that nearest neighbour, as illustrated below.
<list list-type="order"><list-item>
      <p id="d1e850">The set of <inline-formula><mml:math id="M44" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> environmental variables, suitably scaled, <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>...<inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>N</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> defines an <inline-formula><mml:math id="M48" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula>-dimensional
space.</p></list-item><list-item>
      <p id="d1e901">The Euclidean distance between two points, <inline-formula><mml:math id="M49" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M50" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>, in this space is given by
<inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mrow><mml:mi>I</mml:mi><mml:mi>J</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>,<disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M52" display="block"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mrow><mml:mi>I</mml:mi><mml:mi>J</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mi>N</mml:mi></mml:mrow></mml:munder><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mi>I</mml:mi></mml:mfenced><mml:mo>-</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mi>J</mml:mi></mml:mfenced></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p></list-item><list-item>
      <p id="d1e989">We calculate <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mrow><mml:mi>I</mml:mi><mml:mi>J</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> for site <inline-formula><mml:math id="M54" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula> of unknown FW and all sites, <inline-formula><mml:math id="M55" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>, in the
reference data set for each of which we know FW(<inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mi>J</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>.</p></list-item><list-item>
      <p id="d1e1031">We find <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the nearest neighbour, which gives the lowest
<inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mrow><mml:mi>I</mml:mi><mml:mi>J</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>.</p></list-item><list-item>
      <p id="d1e1060">We then predict FW (<inline-formula><mml:math id="M59" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>) = FW (<inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>.</p></list-item><list-item>
      <p id="d1e1084">If site <inline-formula><mml:math id="M61" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula> is classed as bare land by the DGVM, thereby having all vegetation
variables <inline-formula><mml:math id="M62" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0, we predict FW(<inline-formula><mml:math id="M63" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>) <inline-formula><mml:math id="M64" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.</p></list-item></list>
This nearest-neighbour (NN) method can, if necessary, be extended whereby rather than
predicting FW based solely on the single nearest neighbour we instead consider some
function of the <inline-formula><mml:math id="M65" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> nearest neighbours, which we hereafter refer to as
<inline-formula><mml:math id="M66" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>NN.</p>
</sec>
<?pagebreak page1355?><sec id="Ch1.S2.SS5">
  <label>2.5</label><title>Calculating wetland methane emissions</title>
      <p id="d1e1139">The aim of this study was to derive an algorithm for predicting wetland
fraction that can then be used to calculate methane emissions. For the
latter, we use the empirical method described by Cao et al. (1996), where
methane production, mp, and methane oxidation, mo, rates for a specific grid
cell and month (both in units of g <inline-formula><mml:math id="M67" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M68" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> month<inline-formula><mml:math id="M69" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) are given by

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M70" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E3"><mml:mtd><mml:mtext>3</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi mathvariant="normal">mp</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:msub><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E4"><mml:mtd><mml:mtext>4</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi mathvariant="normal">mo</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="normal">mp</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi mathvariant="normal">GPP</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">GPP</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is absolute soil respiration and absolute GPP is gross primary
productivity (both in units of g C m<inline-formula><mml:math id="M72" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> month<inline-formula><mml:math id="M73" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and obtained from the respective
vegetation model). GPP<inline-formula><mml:math id="M74" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:math></inline-formula> is the maximum value of GPP for that grid cell for
any month of the year. <inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is a function that scales for air temperature,
TMP, in degrees Celcius.
            <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M76" display="block"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">exp</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0.04055</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">TMP</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn mathvariant="normal">3.375</mml:mn></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>
          This is capped at a maximum value of 1. In principle there would also be a
scaling function for water table depth, but this is defined as 1 for
inundated wetlands and we are only modelling inundated wetland fraction, as
that is how the SWAMPS-GLWD FW data set is defined.</p>
      <p id="d1e1328">Methane emission rate, me, is then the difference between methane produced and
methane oxidised, scaled by the wetland fraction for that grid cell and month:
            <disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M77" display="block"><mml:mrow><mml:mi mathvariant="normal">me</mml:mi><mml:mo>=</mml:mo><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="normal">mp</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">mo</mml:mi></mml:mrow></mml:mfenced><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">FW</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results and discussion</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Modern-day test data set</title>
      <p id="d1e1369">The modern-day test set explained in Sect. 2.2 was used as a first, simple, test of the
nearest-neighbour algorithm for predicting FW described in Sect. 2.4. Since the
modern-day test set is simply the reference climate data interpolated from 0.5<inline-formula><mml:math id="M78" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
to the courser HadCM3BL-M2.2 model grid of 2.5<inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> by 3.75<inline-formula><mml:math id="M80" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (with vegetation
from the DGVMs), we expect the NN algorithm to yield predicted FW reasonably consistent
with a similar downscaling of the SWAMPS-GLWD observed FW. If the NN predicted FW does
not achieve this, then that would indicate that the NN algorithm has failed to predict FW
sufficiently accurately. Therefore this test is primarily designed to indicate that a
nearest-neighbour algorithm either does or does not have the potential to be applied to
paleoclimates.</p>
      <p id="d1e1399">Figure 2 shows maps of seasonal, June–July–August and December–January–February,
average FW from the observed SWAMPS-GLWD data interpolated to
2.5<inline-formula><mml:math id="M81" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M82" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 3.75<inline-formula><mml:math id="M83" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> along with the predicted FW using either SDGVM or
LPJ vegetation data test sets. For both vegetation models, the predicted FW maps are
similar to the interpolated, observed data. Sparse patches of high FW occur in the tropics,
especially the Amazon, throughout the year, and large areas of seasonal summer wetlands
occur in Alaska, Canada, and Siberia. The monthly variation in FW north and south of
30<inline-formula><mml:math id="M84" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, i.e. essentially comparing boreal and tropical wetlands is shown in
Fig. 3. We split the global values into these two zones because there are virtually no
Southern Hemisphere boreal wetlands, and any division based purely on latitude is
arbitrary. The nearest-neighbour algorithm generates the correct seasonal FW pattern in
boreal regions and, as expected, a relatively constant monthly FW in the tropics.
However, SDGVM consistently underestimates the amount of tropical wetland, whilst LPJ
agrees reasonably well with observations: mean monthly values are <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.11</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>,
<inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.47</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.90</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M88" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> for the observed, SDGVM and LPJ
data, respectively. This is due to the fact that SDGVM classes some grid cells as bare
land, assumed to have FW <inline-formula><mml:math id="M89" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0 in our algorithm, even though some of these have
non-zero FW in the SWAMPS-GLWD database. LPJ does not classify these grid cells as bare
land but instead treats them as very low amounts of vegetation, therefore yielding higher
global FW that is more consistent with observations. If we exclude those grid cells SDGVM
predicts as bare land from the observed data, then the SDGVM prediction matches better
the observed data and LPJ predictions (Table 2). These results give confidence to the
fact that a nearest-neighbour algorithm is able to reproduce acceptable FW based on these
specific climate and vegetation variables.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><label>Figure 2</label><caption><p id="d1e1500">Seasonal mean FW: observed interpolated to model grid;
<bold>(a)</bold> June–July–August and <bold>(b)</bold> December–January–February. The 1NN
prediction by SDGVM <bold>(c)</bold> June–July–August and
<bold>(d)</bold> December–January–February. The 1NN prediction by LPJ
<bold>(e)</bold> June–July–August and <bold>(f)</bold> December–January–February.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019-f02.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><label>Figure 3</label><caption><p id="d1e1531">Monthly zonal variations in FW calculated for the mean 2000–2012
climate on a <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">3.75</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M91" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid; <bold>(a)</bold> north of
30<inline-formula><mml:math id="M92" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and <bold>(b)</bold> south of 30<inline-formula><mml:math id="M93" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019-f03.png"/>

        </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2"><label>Table 2</label><caption><p id="d1e1591">Modern-day monthly mean FW area (10<inline-formula><mml:math id="M94" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:math></inline-formula> km<inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> for observed
data interpolated to the 2.5<inline-formula><mml:math id="M96" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M97" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 3.75<inline-formula><mml:math id="M98" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid or calculated
by vegetation model.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M100" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M102" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N</oasis:entry>
         <oasis:entry colname="col4">Global</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">FW</oasis:entry>
         <oasis:entry colname="col3">FW</oasis:entry>
         <oasis:entry colname="col4">FW</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Observed</oasis:entry>
         <oasis:entry colname="col2">1.84</oasis:entry>
         <oasis:entry colname="col3">2.11</oasis:entry>
         <oasis:entry colname="col4">3.95</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Observed excluding</oasis:entry>
         <oasis:entry colname="col2">1.47</oasis:entry>
         <oasis:entry colname="col3">1.41</oasis:entry>
         <oasis:entry colname="col4">2.88</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SDGVM bare land</oasis:entry>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SDGVM</oasis:entry>
         <oasis:entry colname="col2">1.53</oasis:entry>
         <oasis:entry colname="col3">1.47</oasis:entry>
         <oasis:entry colname="col4">3.00</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">LPJ</oasis:entry>
         <oasis:entry colname="col2">1.95</oasis:entry>
         <oasis:entry colname="col3">1.90</oasis:entry>
         <oasis:entry colname="col4">3.86</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e1794"><?xmltex \hack{\newpage}?>Figure 4 shows the monthly variation in wetland methane emissions for boreal and tropical
areas, calculated using the observed or predicted FW, both vegetation model outputs and
Eqs. (3) to (6). The annual methane emission totals are summarised in Table 3, along
with other recent estimates from model intercomparisons. The annual and monthly zonal
methane emissions are broadly similar for a given vegetation model regardless of whether
the observed or predicted FW is used. SDGVM gives global emissions in line with the other
modelling studies, whereas those from LPJ are somewhat lower. This is mainly due to
differences in tropical emissions. SDGVM yields higher tropical emissions than LPJ but
slightly lower emissions north of 30<inline-formula><mml:math id="M103" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N. The main factors influencing the
modelled methane emissions (other than FW) are, according to Eqs. (3) to (5), temperature
(which is the same for both vegetation models), soil respiration (<inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and
gross primary productivity (GPP), the latter two differing between the two vegetation
models. It appears that differences in <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> lead to the different zonal methane
totals. South of 30<inline-formula><mml:math id="M106" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, SDGVM and LPJ model annual total <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of
46 000 and 35 000 Tg C yr<inline-formula><mml:math id="M108" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively, and, using the same observed FW,
SDGVM and LPJ model annual methane emissions of 123 and 69 Tg <inline-formula><mml:math id="M109" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> yr<inline-formula><mml:math id="M110" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>,
respectively. Th<?pagebreak page1357?>erefore, in the tropics the differences in the predicted methane
emissions seem to be due to differences in calculated <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. North of
30<inline-formula><mml:math id="M112" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N both DGVMs have similar <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, 20 000 and
22 000 Tg C yr<inline-formula><mml:math id="M114" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively, for SDGVM and LPJ, and similar values of methane
emissions, 64 and 65 Tg <inline-formula><mml:math id="M115" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> yr<inline-formula><mml:math id="M116" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><label>Figure 4</label><caption><p id="d1e1956">Monthly zonal variations in wetland <inline-formula><mml:math id="M117" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions
(Tg <inline-formula><mml:math id="M118" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) calculated from DGVM model data and observed or modelled FW
for the mean 2000–2012 climate on a <inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">3.75</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M120" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
grid. <bold>(a)</bold> SDGVM north of 30<inline-formula><mml:math id="M121" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, <bold>(b)</bold> LPJ north of
30<inline-formula><mml:math id="M122" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, <bold>(c)</bold> SDGVM south of 30<inline-formula><mml:math id="M123" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and
<bold>(d)</bold> LPJ south of 30<inline-formula><mml:math id="M124" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N.</p></caption>
          <?xmltex \igopts{width=384.112205pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019-f04.png"/>

        </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3"><label>Table 3</label><caption><p id="d1e2064">Modern-day annual total wetland <inline-formula><mml:math id="M125" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emission (Tg <inline-formula><mml:math id="M126" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> yr<inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>,
calculated by vegetation model using either observed
FW data (interpolated to the 2.5<inline-formula><mml:math id="M128" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M129" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 3.75<inline-formula><mml:math id="M130" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid) or
model predicted FW, compared with other modelling studies.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.93}[.93]?><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>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M140" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M142" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N</oasis:entry>
         <oasis:entry colname="col5">Global</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Model</oasis:entry>
         <oasis:entry colname="col2">FW data</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M143" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M144" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M145" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">SDGVM</oasis:entry>
         <oasis:entry colname="col2">observed</oasis:entry>
         <oasis:entry colname="col3">64.32</oasis:entry>
         <oasis:entry colname="col4">122.69</oasis:entry>
         <oasis:entry colname="col5">187.01</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">predicted</oasis:entry>
         <oasis:entry colname="col3">57.95</oasis:entry>
         <oasis:entry colname="col4">108.63</oasis:entry>
         <oasis:entry colname="col5">166.58</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">LPJ</oasis:entry>
         <oasis:entry colname="col2">observed</oasis:entry>
         <oasis:entry colname="col3">65.43</oasis:entry>
         <oasis:entry colname="col4">68.60</oasis:entry>
         <oasis:entry colname="col5">134.03</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">predicted</oasis:entry>
         <oasis:entry colname="col3">73.11</oasis:entry>
         <oasis:entry colname="col4">83.78</oasis:entry>
         <oasis:entry colname="col5">156.89</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GCP-CH4<inline-formula><mml:math id="M146" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">observed 0.5<inline-formula><mml:math id="M147" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">184</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">WETCHIMP<inline-formula><mml:math id="M149" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">model specific</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:mn mathvariant="normal">51</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">15</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:mn mathvariant="normal">126</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">31</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:mn mathvariant="normal">190</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">39</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table><table-wrap-foot><p id="d1e2130"><inline-formula><mml:math id="M131" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula> GCP-CH4 (Poulter et al., 2017) results are the mean
of 11 different methane<?xmltex \hack{\\}?>emission models with the same observed wetland data
as used to produce Fig. 1 here.<?xmltex \hack{\\}?>They are quoted as means over specific
ranges of years: 2000–2006 <inline-formula><mml:math id="M132" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mn mathvariant="normal">184.0</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">21.1</mml:mn></mml:mrow></mml:math></inline-formula>, 2007–2012 <inline-formula><mml:math id="M134" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:mn mathvariant="normal">183.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">23.1</mml:mn></mml:mrow></mml:math></inline-formula> and 2012 <inline-formula><mml:math id="M136" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mn mathvariant="normal">185.7</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">23.2</mml:mn></mml:mrow></mml:math></inline-formula>. As our results are for a single<?xmltex \hack{\\}?>mean 2000–2012 year we therefore only quote an approximate value from this
source<?xmltex \hack{\\}?>for comparison. <inline-formula><mml:math id="M138" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula> WETCHIMP (Melton et al., 2013) results
are the mean of<?xmltex \hack{\\}?>8 different models, 1993–2004, each of which used their
own definition of wetland<?xmltex \hack{\\}?>extent rather than observed data.</p></table-wrap-foot></table-wrap>

      <p id="d1e2504"><?xmltex \hack{\newpage}?>We stress that this was a simple test for a nearest-neighbour approach for
reasons outlined at the beginning of this section, and the satisfactory
results obtained here merely indicate that this is an approach that has potential
to be useful in predicting FW for a paleoclimate.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Early Eocene climate</title>
      <p id="d1e2516">In the previous section we have shown that a NN method can reproduce FW for a modern-day
climate, justifying its application to the early Eocene climate described in Sect. 2.2.
However, as noted at the end of Sect. 2.4, a NN method can be extended to <inline-formula><mml:math id="M153" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>NN, whereby
we predict FW based on some function of the FW of <inline-formula><mml:math id="M154" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> nearest neighbours (noting that in
Sect. 3.1, NN is simply 1NN, i.e. <inline-formula><mml:math id="M155" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>NN with <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>). A 1NN algorithm that works well to
predict modern-day FW may not work as well for a paleoclimate of many millions of years
in the past. The reference data set we use, Sect. 2.1, is very similar to the modern-day
test set, the latter's climate data are simply obtained by interpolating the former to a
courser spatial grid. Therefore, we expected and observed a high correlation between
modern-day FW predicted from the nearest neighbour in the reference data and the actual
FW. The early Eocene test data has significant differences to the reference data since
the climate of the early Eocene is obviously not the same as the modern day. Therefore,
it will be harder for a nearest-neighbour-based method, searching a space described by
climate and vegetation data, to find a nearest neighbour in the modern-day reference data
with the correct early Eocene FW, whatever that may be. It may be that for a high FW
early Eocene grid cell, the nearest neighbour happens to have quite low FW and vice
versa. Figure 1 shows that FW can change from very high to almost zero over relatively
small distances, for example in the Amazon basin, and therefore that sites with similar
climate and<?pagebreak page1358?> vegetation can have very different FW. The greater the degree of difference
between the early Eocene and the modern-day reference data sets, the more likely it is
that the first nearest neighbour does not have the correct FW.</p>
      <p id="d1e2552">FW calculated for the early Eocene using the exact same 1NN method as used for the
modern-day test set yields a value of global monthly mean wetland area of <inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:mn mathvariant="normal">4.07</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M158" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> using SDGVM. This is around 33 % higher than that for the
modern-day value, <inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.00</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M160" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>, from Table 2. However, this includes a
contribution of <inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.53</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M162" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> from areas south of 30<inline-formula><mml:math id="M163" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, which
have an almost negligible contribution for the modern day, so the tropics and northern
boreal regions actually have lower FW for the early Eocene. Given that the early Eocene
was significantly warmer and wetter than the modern day (Carmicheal et al., 2017), we
expect greater wetland area than the modern day. Beerling et al. (2011) reported global
wetland area for an early Eocene climate using SDGVM; employing their method to our early
Eocene climate, so as to eliminate differences arising from the specific HadCM3 model
climate and spatial resolution, yields a global monthly mean FW area of <inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:mn mathvariant="normal">16.29</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M165" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>, 4 times higher than the value we would calculate from a 1NN method.
Therefore, based on a comparison with both the modern-day studies and a previous Eocene
study, it appears that a 1NN method may be unsuitable for a paleoclimate that is very
different to our modern-day reference climate, and we consider <inline-formula><mml:math id="M166" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>NN with higher
values of <inline-formula><mml:math id="M167" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>.</p>
<sec id="Ch1.S3.SS2.SSS1">
  <label>3.2.1</label><?xmltex \opttitle{Maximum of $K$ nearest-neighbour FW prediction}?><title>Maximum of <inline-formula><mml:math id="M168" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> nearest-neighbour FW prediction</title>
      <?pagebreak page1359?><p id="d1e2690">If indeed the 1NN results are too low then that implies that for some hypothetical high
FW sites from the early Eocene, the first nearest neighbours in the reference data have
very low FW. Therefore, if we consider higher values of <inline-formula><mml:math id="M169" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> we may improve our estimate
by predicting FW to be the maximum FW of <inline-formula><mml:math id="M170" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> nearest neighbours (max<inline-formula><mml:math id="M171" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>NN) in the
reference data. However, applying this approach will yield increasingly higher FW as <inline-formula><mml:math id="M172" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>
increases, requiring a data-constrained optimisation of <inline-formula><mml:math id="M173" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>. Clearly there are no
observations of Eocene wetland distributions with which to properly train any predictive
algorithm, but we may utilise a suitable proxy for wetlands to try and obtain such a
constraint. Here we use the distribution of coal deposits in the Eocene (Boucot et al.,
2013), shown in Fig. 5 as such constraints. There are some limitations to this approach.
Coal is formed in wetlands, but can also form in other settings such as lakes; and of
course, these data sets do not document where wetlands were present but the sedimentary
record is missing or has not been published. In the tropics, coal may not have formed in
wetland environments due to a very high rate of carbon cycling and in northern latitudes
subsequent glaciations could have eroded coal deposits away. Moreover, data will be
sparse or non-existent for remote or inaccessible modern-day regions, such as under the
Antarctic ice sheet. We also note that precise age and location, especially when
comparing to low-resolution climate simulations, could cause disagreement for
grid-by-grid comparisons. A final and critical complication is that FW is a number
between 0 and 1, corresponding to the fraction of a site that is wetland, whereas the
coal data are a binary measure: either a grid cell has or does not have a coal deposit
within it. For all of these reasons, data–model comparisons must be done cautiously;
nonetheless, these data are useful for identifying the most effective <inline-formula><mml:math id="M174" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> value for
reconstructing likely wetlands.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><label>Figure 5</label><caption><p id="d1e2738">Locations of Eocene coal deposits plotted on our Eocene model land mask. The <inline-formula><mml:math id="M175" display="inline"><mml:mi mathvariant="italic">□</mml:mi></mml:math></inline-formula> symbols indicate an Eocene coal
deposit location (Boucot et al., 2013).</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019-f05.png"/>

          </fig>

      <p id="d1e2754">We defined two functions to assess how well a model FW matched the locations
of Eocene coal deposits. Firstly, <italic>f1</italic> is defined as the mean distance, in kilometres,
of a coal deposit location to a grid cell with model FW predicted to be
<inline-formula><mml:math id="M176" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula>. The choice of 0.2 representing significant FW is arbitrary
but the analysis was repeated with other values and the same conclusions
were found. Secondly, <italic>f2</italic> is defined as the mean FW of the grid cell closest to
each coal deposit location, providing that site is within 2 grid points of
that coal deposit location, to allow some leeway with regard to different
projected locations of land masses in the early Eocene. Again the choice of
a 2-pixel limit is arbitrary but the analysis was repeated with other limits
and the same conclusions found.</p>
      <p id="d1e2774">Figure 6 shows the values of <italic>f1</italic> and <italic>f2</italic> for max<inline-formula><mml:math id="M177" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>NN predictions of FW
with increasing <inline-formula><mml:math id="M178" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> for both the SDGVM and LPJ early Eocene data sets, compared to a data
set of coal deposit locations. As explained, since FW increases with <inline-formula><mml:math id="M179" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> then, by
extension, so does the likelihood of a site with a coal deposit in or close to it
coinciding with a site of significant FW. Therefore, we do not seek to find the value of
<inline-formula><mml:math id="M180" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> that will give the lowest value of <italic>f1</italic> and highest value of <italic>f2</italic> as
that would simply be <inline-formula><mml:math id="M181" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> equal to the size of the entire reference data set. Instead, we
try to find the lowest value of <inline-formula><mml:math id="M182" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> that gives a “good” prediction for both <italic>f1</italic>
and <italic>f2</italic>. Although “good” is a subjective measure, we define it based on where
increases in <inline-formula><mml:math id="M183" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> result in marginal improvements in <italic>f1</italic> and <italic>f2</italic>. For both
vegetation models as <inline-formula><mml:math id="M184" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> increases from 1 to 3 <italic>f1</italic> decreases significantly and
<italic>f2</italic> increases significantly. For <inline-formula><mml:math id="M185" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> the decrease in <italic>f1</italic> levels out
and the increase in <italic>f2</italic> also declines. Therefore, we conclude that based on
comparison of predicted FW and locations of coal deposits, <inline-formula><mml:math id="M186" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> is a reasonable choice
to make predictions for our early Eocene climate via a max<inline-formula><mml:math id="M187" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>NN algorithm.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F6" specific-use="star"><label>Figure 6</label><caption><p id="d1e2905">Variations of statistics for a match between Eocene max<inline-formula><mml:math id="M188" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>NN predicted high FW
and coal locations (Boucot et al., 2013). The <italic>f1</italic> is the mean distance of a coal
location to site with <inline-formula><mml:math id="M189" display="inline"><mml:mrow><mml:mi mathvariant="normal">FW</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula> for model based on <bold>(a)</bold> SDGVM and
<bold>(b)</bold> LPJ. The <italic>f2</italic> is the mean FW of sites within 2 pixels of a coal
location for model based on <bold>(c)</bold> SDGVM and <bold>(d)</bold> LPJ data.</p></caption>
            <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019-f06.png"/>

          </fig>

</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <label>3.2.2</label><title>FW predicted by max3NN</title>
      <p id="d1e2960">Figure 7 shows annual maximum FW (i.e. for each pixel the highest of the 12 monthly
values) calculated by a max3NN model using SDGVM or LPJ vegetation data, as described
above, with the locations of early Eocene coal deposits also shown. The annual maximum FW
is shown here as FW might only need to be high at some point during the year to give rise
to coal deposits. The areas of predicted high FW are much larger than for the modern day
(Fig. 1); moreover, at this spatial resolution there are often abrupt changes from
low to medium (yellow) to much higher (red) values leading to some isolated patches of high
FW. The approach makes it difficult to interrogate specific factors that drive the
increase in Eocene FW compared to today but given the wetter climate of the early Eocene,
higher FW than the modern day is to be expected. The patchiness is partly a consequence
of using annual maximum FW but also reflects the challenge of predicting a characteristic
of a paleoenvironment based on modern-day reference data. Considering zonal total FW and
seasonal average FW maps, i.e. averaging out some of the small-scale spatial and temporal
variability, is likely a better approach for understanding ancient methane cycling and
these are discussed later.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F7" specific-use="star"><label>Figure 7</label><caption><p id="d1e2965">Annual maximum FW calculated by the max3NN method by <bold>(a)</bold> SDGVM and
<bold>(b)</bold> LPJ for the Eocene climate, compared with coal deposit locations.</p></caption>
            <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019-f07.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><label>Figure 8</label><caption><p id="d1e2982">Monthly variations in total wetland area calculated for the Eocene climate by
SDGVM and LPJ for <bold>(a)</bold> all areas north of 30<inline-formula><mml:math id="M190" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, <bold>(b)</bold> all areas
between 30<inline-formula><mml:math id="M191" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and 30<inline-formula><mml:math id="M192" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and <bold>(c)</bold> all areas south of
30<inline-formula><mml:math id="M193" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019-f08.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9"><label>Figure 9</label><caption><p id="d1e3040">Monthly variations in wetland <inline-formula><mml:math id="M194" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions (Tg <inline-formula><mml:math id="M195" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) calculated
from predicted FW for the Eocene climate by SDGVM and LPJ, for <bold>(a)</bold> all areas
north of 30<inline-formula><mml:math id="M196" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, <bold>(b)</bold> all areas between 30<inline-formula><mml:math id="M197" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and 30<inline-formula><mml:math id="M198" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N
and <bold>(c)</bold> all areas south of 30<inline-formula><mml:math id="M199" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019-f09.png"/>

          </fig>

      <?pagebreak page1361?><p id="d1e3117">The maps of predicted FW are quite different for the two vegetation models,
but the greatest differences are in areas with very little or no coal
deposits, e.g. the tropics, north-eastern North America and Antarctica,
making it difficult to critically evaluate them against the data. However,
the monthly variations given by the two vegetation models in total FW
(Fig. 8) and methane emissions (Fig. 9) for the three latitudinal zones
are reasonably similar with respect to seasonal variations in that both
have their highest values in the late spring and summer months for zones
north of 30<inline-formula><mml:math id="M200" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and south of 30<inline-formula><mml:math id="M201" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and no clear seasonal
variation in the tropics. In the tropical zone, predictions of monthly FW
area are similar in magnitude for the two vegetation models, with SDGVM
usually predicting higher FW than LPJ. However, in the zone north of
30<inline-formula><mml:math id="M202" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N LPJ predicts much higher FW than SDGVM throughout June to
October with a peak in September, whereas SDGVM peaks in May. A similar but
less striking pattern occurs for the zone south of 30<inline-formula><mml:math id="M203" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S where
again LPJ predicts higher summer FW area than SDGVM. These differences
between the two vegetation models are also evident in maps of seasonal
average predicted FW (Fig. 10). In June to August, SDGVM predicts very
little wetland area in the Northern Hemisphere, whereas LPJ predicts
moderate to high FW areas over much of the land north of around
50<inline-formula><mml:math id="M204" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N. In December to February both models predict almost zero FW
north of around 50<inline-formula><mml:math id="M205" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N. In the tropics and the Southern Hemisphere,
the two models predict similar amounts of wetland area, but with SDGVM
predicting slightly higher FW overall between 30<inline-formula><mml:math id="M206" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and
30<inline-formula><mml:math id="M207" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and LPJ predicting slightly higher FW south of 30<inline-formula><mml:math id="M208" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><label>Figure 10</label><caption><p id="d1e3204">Seasonal mean FW predicted for the Eocene climate by SDGVM and
LPJ using the max3NN <bold>(a)</bold> SDGVM June–July–August, <bold>(b)</bold> SDGVM
December–January–February, <bold>(c)</bold> LPJ June–July–August and <bold>(d)</bold> LPJ
December–January–February.</p></caption>
            <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019-f10.png"/>

          </fig>

      <p id="d1e3225">This differs from the modern-day distribution of wetlands (Fig. 1) and likely arises from
a variety of method-dependent factors. First, the coarser resolution leads to a more patchy
distribution, as is evident in the modern-day data in Figs. 1 and 2a and b at
0.5<inline-formula><mml:math id="M209" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:mo>×</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M211" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and 2.5<inline-formula><mml:math id="M212" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M213" 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="M214" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> spatial
resolutions, respectively. This is particularly true for the tropics where wetlands do occur in small
areas. Secondly, the<?pagebreak page1362?> nature of the nearest-neighbour algorithm relies on the principle
that a grid cell in a paleoclimate with specific values of environmental variables will
have the same FW as a grid cell in a modern-day reference data set with similar values
for those environmental variables; however, other factors influence wetland fraction,
such as the topography. Therefore, a nearest-neighbour method predicting FW for a
paleoclimate from a modern-day reference data may well have errors for a given grid cell
and month. These errors should reduce when averaged over latitudinal zones or seasonal
averages.</p>
      <p id="d1e3282">The differences between methane emissions from the two vegetation models likely arise
from their respective impacts on soil water balance, via the magnitude of
evapotranspiration (EVT) relative to precipitation (PRC). As the vegetation model, used
to calculate EVT, and climate model, used to calculate PRC, are not dynamically coupled,
PRC will be the same in all Eocene simulations, but EVT will vary; thus, vegetation
models that yield elevated EVT in a given grid cell are more likely to yield a negative
water balance (PRC <inline-formula><mml:math id="M215" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula> EVT) and low FW. Figure 11 shows the June to August mean PRC <inline-formula><mml:math id="M216" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>
EVT for SDGVM and LPJ, revealing that it is negative in most places north of
30<inline-formula><mml:math id="M217" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N for SDGVM but is slightly positive or at least much closer to zero for
LPJ. Therefore, SDGVM will generally predict lower FW by identifying modern-day nearest
neighbours where PRC <inline-formula><mml:math id="M218" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> EVT and unlikely to be wetland. The lack of extensive of coal
deposits in the high northern latitudes, especially where the LPJ-based approach predicts
wetlands, could indicate that the LPJ approach has over-predicted FW. However, we caution
that this could be a data limitation issue and future work is required to interrogate the
forecasts of these two methods. Regardless, both models yield broadly similar results on
global and zonal terms (Table 4) indicating that the <inline-formula><mml:math id="M219" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>NN algorithm could be a useful
complementary approach for interrogating ancient wetland extent and methane emissions.
Global monthly mean FW for the Eocene is <inline-formula><mml:math id="M220" display="inline"><mml:mrow><mml:mn mathvariant="normal">8.5</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M221" display="inline"><mml:mrow><mml:mn mathvariant="normal">10.3</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M222" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> predicted by SDGVM and LPJ, respectively. Both of these values are
larger than for the modern-day value of <inline-formula><mml:math id="M223" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.0</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M224" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>, as we would have
expected.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><label>Figure 11</label><caption><p id="d1e3389">June–July–August mean precipitation minus evapotranspiration
for the Eocene climate, using evapotranspiration from <bold>(a)</bold> SDGVM or <bold>(b)</bold> LPJ.</p></caption>
            <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/12/1351/2019/gmd-12-1351-2019-f11.png"/>

          </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4"><label>Table 4</label><caption><p id="d1e3407">Eocene monthly mean max3NN modelled FW area (10<inline-formula><mml:math id="M225" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:math></inline-formula> km<inline-formula><mml:math id="M226" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>).</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="right"/>
     <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">FW model</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M228" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N</oasis:entry>
         <oasis:entry colname="col3">30<inline-formula><mml:math id="M229" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S to 30<inline-formula><mml:math id="M230" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M232" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S</oasis:entry>
         <oasis:entry colname="col5">Global</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">SDGVM</oasis:entry>
         <oasis:entry colname="col2">2.82</oasis:entry>
         <oasis:entry colname="col3">4.11</oasis:entry>
         <oasis:entry colname="col4">1.53</oasis:entry>
         <oasis:entry colname="col5">8.48</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">LPJ</oasis:entry>
         <oasis:entry colname="col2">4.84</oasis:entry>
         <oasis:entry colname="col3">3.39</oasis:entry>
         <oasis:entry colname="col4">2.06</oasis:entry>
         <oasis:entry colname="col5">10.29</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Conclusions</title>
      <p id="d1e3566">We have presented a nearest-neighbour method by which FW can be calculated at sites on
the Earth's surface for an Eocene paleoclimate based on a set of environmental variables
obtained from climate and vegetation models and a<?pagebreak page1363?> comparison of these to a modern-day
reference data set. This has been used as an offline tool using data obtained from
climate and vegetation models, rather than by embedding this within existing Earth system
models, as the goal of this work was to explore and improve on methods of predicting FW
for deep-time paleoclimates. The precise formulation of the nearest- neighbour approach
was determined through comparison to locations of Eocene coal deposits and indicated that
a max3NN method was best suited in this case. That should not be taken to imply that a
max3NN would be the best in general; for another paleoclimate a similar analysis to that
performed here would be required to determine the optimum implementation of <inline-formula><mml:math id="M233" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>NN. It
would therefore be of interest in future work to apply this methodology to other
paleoclimates to see if similar results are obtained, perhaps using different
environmental variables to those we have used to find nearest neighbours and perhaps
other proxies for paleo-FW, should they become available. The predicted distributions of
FW are much higher than those of today, as we would expect. We have assessed this using
two different global vegetation models, and whilst these do yield some geographical
differences in FW arising from different evapotranspiration estimates, they are broadly
similar when considering zonal means. For both vegetation models, global monthly mean
modelled FW area is less than, around half to two-thirds, that of Beerling et al. (2011),
as are the values of the wetland methane emissions. However, our new method does not rely
on the standard deviation of orography, a variable which is only known to a relatively
coarse resolution for deep paleoclimates.</p>
</sec>

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

      <p id="d1e3581">This study presents a methodology using existing data and climate
and vegetation models. Information relating to these is already included in this article.
Code implementing the max<inline-formula><mml:math id="M234" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>NN prediction of FW is included in the Supplement.</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e3591">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/gmd-12-1351-2019-supplement" xlink:title="zip">https://doi.org/10.5194/gmd-12-1351-2019-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e3600">DJW and DJB planned the work with advice from all co-authors. DJW carried
out most of the experimental work with MB providing the HadCM3BL-M2.2 data and
EPK the LPJ model data. DJW prepared the manuscript with contributions from
all co-authors.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e3606">The authors declare that they have no conflict of
interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e3612">Funding was provided by the Natural Environmental Research Council (NERC)
grant NE/J00748X/1. The authors would like to thank Chris Scotese for access
to and advice on Eocene coal deposit data. We also thank two anonymous
referees for their comments and advice on improving this manuscript.</p></ack><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e3617">This paper was edited by David Lawrence and reviewed by two anonymous referees.</p>
  </notes><ref-list>
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    <!--<article-title-html>A predictive algorithm for wetlands in deep  time paleoclimate models</article-title-html>
<abstract-html><p>Methane is a powerful greenhouse gas produced in wetland
environments via microbial action in anaerobic conditions. If the location and extent of
wetlands are unknown, such as for the Earth many millions of years in the past, a model
of wetland fraction is required in order to calculate methane emissions and thus help
reduce uncertainty in the understanding of past warm greenhouse climates. Here we present
an algorithm for predicting inundated wetland fraction for use in calculating wetland
methane emission fluxes in deep-time paleoclimate simulations. For each grid cell in a
given paleoclimate simulation, the algorithm determines the wetland fraction predicted by
a nearest-neighbour search of modern-day data in a space described by a set of
environmental, climate and vegetation variables. To explore this approach, we first test
it for a modern-day climate with variables obtained from observations and then for an
Eocene climate with variables derived from a fully coupled global climate model
(HadCM3BL-M2.2; Valdes et al., 2017). Two independent dynamic vegetation models were used
to provide two sets of equivalent vegetation variables which yielded two different
wetland predictions. As a first test, the method, using both vegetation models,
satisfactorily reproduces modern day wetland fraction at a course grid resolution, similar to those used in
paleoclimate simulations. We then applied the method to an early Eocene climate, testing
its outputs against the locations of Eocene coal deposits. We predict global mean monthly
wetland fraction area for the early Eocene of 8×10<sup>6</sup> to 10×10<sup>6</sup>&thinsp;km<sup>2</sup> with a
corresponding total annual methane flux of 656 to 909&thinsp;Tg&thinsp;CH<sub>4</sub>&thinsp;yr<sup>−1</sup>,
depending on which of the two different dynamic global vegetation models are used to
model wetland fraction and methane emission rates. Both values are significantly higher
than estimates for the modern day of 4×10<sup>6</sup>&thinsp;km<sup>2</sup> and around
190&thinsp;Tg&thinsp;CH<sub>4</sub>&thinsp;yr<sup>−1</sup> (Poulter et al., 2017; Melton et al., 2013).</p></abstract-html>
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279–283, <a href="https://doi.org/10.1038/nature06588" target="_blank">https://doi.org/10.1038/nature06588</a>, 2008.
</mixed-citation></ref-html>--></article>
