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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-14-3521-2021</article-id><title-group><article-title>A spatially explicit approach to simulate urban heat mitigation with InVEST (v3.8.0)</article-title><alt-title>A spatially explicit approach to simulate urban heat islands</alt-title>
      </title-group><?xmltex \runningtitle{A spatially explicit approach to simulate urban heat islands}?><?xmltex \runningauthor{M.~Bosch et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Bosch</surname><given-names>Martí</given-names></name>
          <email>marti.bosch@epfl.ch</email>
        <ext-link>https://orcid.org/0000-0001-8735-9144</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Locatelli</surname><given-names>Maxence</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Hamel</surname><given-names>Perrine</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Remme</surname><given-names>Roy P.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0799-2319</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Chenal</surname><given-names>Jérôme</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8109-8358</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4 aff1">
          <name><surname>Joost</surname><given-names>Stéphane</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1184-7501</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Urban and Regional Planning Community, École Polytechnique Fédérale de Lausanne, Lausanne, Switzerland</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Asian School of the Environment, Nanyang Technological University, Singapore, Singapore</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Natural Capital Project, Stanford University, Stanford, USA</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Laboratory of Geographic Information Systems, École Polytechnique Fédérale de Lausanne, Lausanne, Switzerland</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Martí Bosch (marti.bosch@epfl.ch)</corresp></author-notes><pub-date><day>11</day><month>June</month><year>2021</year></pub-date>
      
      <volume>14</volume>
      <issue>6</issue>
      <fpage>3521</fpage><lpage>3537</lpage>
      <history>
        <date date-type="received"><day>31</day><month>May</month><year>2020</year></date>
           <date date-type="rev-request"><day>13</day><month>July</month><year>2020</year></date>
           <date date-type="rev-recd"><day>29</day><month>March</month><year>2021</year></date>
           <date date-type="accepted"><day>21</day><month>April</month><year>2021</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2021 Martí Bosch et al.</copyright-statement>
        <copyright-year>2021</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021.html">This article is available from https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021.html</self-uri><self-uri xlink:href="https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021.pdf">The full text article is available as a PDF file from https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e147">Mitigating urban heat islands has become an important objective for many cities experiencing heat waves.
Despite notable progress, the spatial relationship between land use and/or land cover patterns and the distribution of air temperature remains poorly understood.
This article presents a reusable computational workflow to simulate the spatial distribution of air temperature in urban areas from their land use and/or land cover data.
The approach employs the InVEST urban cooling model, which estimates the cooling capacity of the urban fabric based on three biophysical mechanisms: tree shade, evapotranspiration and albedo.
An automated procedure is proposed to calibrate the parameters of the model to best fit air temperature observations from  monitoring stations.
In a case study in Lausanne, Switzerland, spatial estimates of air temperature obtained with the calibrated model show that the urban cooling model outperforms spatial regressions based on satellite data. This represents two major advances in urban heat island modeling.
First, unlike in black-box approaches, the calibrated parameters of the urban cooling model can be interpreted in terms of the physical mechanisms that they represent; therefore, they can help promote an understanding of how urban heat islands emerge in a particular context.
Second, the urban cooling model requires only land use and/or land cover and reference temperature data and can, therefore, be used to evaluate synthetic scenarios such as master plans, urbanization prospects and climate scenarios.
The proposed approach provides valuable insights into the emergence of urban heat islands which can serve to inform urban planning and assist the design of heat mitigation policies.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e159">Since the industrial revolution, the Earth has seen a global increase in temperature which has been especially prominent in urban areas <xref ref-type="bibr" rid="bib1.bibx35 bib1.bibx5 bib1.bibx16" id="paren.1"/>.
Such a trend concurs with the unprecedented growth of urban areas, making contemporary cities a major source of landscape changes and greenhouse gas emissions <xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx23 bib1.bibx54" id="paren.2"/>.
By modifying the energy and water balance processes and influencing the movement of air, urban surfaces alter local climatic characteristics, often resulting in warmer temperatures than their rural surroundings <xref ref-type="bibr" rid="bib1.bibx36" id="paren.3"/>. This phenomenon is known as the “urban heat island” (UHI) effect.</p>
      <p id="d1e171">The quantification of UHIs can be broadly divided into two main approaches <xref ref-type="bibr" rid="bib1.bibx42" id="paren.4"/>, namely the canopy-layer UHI, measured by the air temperature, usually at 2 m height <xref ref-type="bibr" rid="bib1.bibx50" id="paren.5"/>, and the surface UHI, measured by land surface temperatures (LSTs) derived from remote sensing data <xref ref-type="bibr" rid="bib1.bibx55" id="paren.6"/>.
The increasing availability of satellite raster datasets has fostered a large body of research on the spatial distribution of LSTs and their relationship with the spatial composition and configuration of urban landscapes <xref ref-type="bibr" rid="bib1.bibx55 bib1.bibx61" id="paren.7"/>, which contrasts with the spatial sparsity of meteorological stations that measure air temperature.
Despite exhibiting some correlations, air temperature and LST are essentially different physical quantities.
Air temperature is closer to thermal comfort felt by humans and can therefore be employed to evaluate the influence of UHIs on key matters such as the energy demand for air conditioning or human health.
Additionally,<?pagebreak page3522?> depending on the satellite overpass time, the differences between air temperature and LST can range from a few degrees (<inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C) up to tens of degrees <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx48" id="paren.8"/>, which calls for special caution when employing satellite-derived LST data for the study of UHIs.</p>
      <p id="d1e199">Although notable studies have explored the relationship between satellite-derived LST raster data and air temperature measurements to provide high-resolution insights into the canopy-layer UHI <xref ref-type="bibr" rid="bib1.bibx18 bib1.bibx43 bib1.bibx4 bib1.bibx46 bib1.bibx47" id="paren.9"/>, they have mostly focused on finding statistical relationships between UHIs and the spatial distribution of terrain features such as vegetation indices, without exploring how the observed patterns relate to the biophysical mechanisms that explain the canopy-layer UHI.
Such a limitation is important when models are used in simulations – for example, to examine the effect of urban planning scenarios on air temperatures.
As part of the Integrated Valuation of Ecosystem Services and Tradeoffs (InVEST) software, a suite of spatial models to quantify and value the goods and services from nature that sustain and fulfill human life <xref ref-type="bibr" rid="bib1.bibx45" id="paren.10"/>, an urban cooling model has been developed following recent research on the effects of surface materials and vegetation cover on UHIs <xref ref-type="bibr" rid="bib1.bibx39 bib1.bibx60" id="paren.11"/>.
The aim of the urban cooling model is to simulate the spatial distribution of UHIs based on three key mechanisms, namely the shade provided by trees, the evapotranspiration of urban vegetation and the albedo of the urban surface.
In a preliminary application of the model, <xref ref-type="bibr" rid="bib1.bibx25" id="text.12"/> showed its capability to represent the spatial pattern of nighttime air temperature of the 2003 heat waves in the Île-de-France region.</p>
      <p id="d1e214">The main objective of this study is to extend such preliminary experiments by proposing a reusable computational workflow to apply the InVEST urban cooling model to predict the spatial distribution of air temperature in a given study area. The validity of the simulated results is optimized by calibrating some key parameters to best fit a set of air temperature measurements from monitoring stations.
Additionally, the simulated spatial pattern of air temperature is compared with one obtained using an alternative approach, namely a spatial regression over features extracted from satellite data.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Materials and methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Study area</title>
      <p id="d1e232">Situated at the western end of the Swiss Plateau and on the shores of Lake Geneva, Lausanne is the fourth largest Swiss urban agglomeration with 420 757 inhabitants as of January 2019 <xref ref-type="bibr" rid="bib1.bibx52" id="paren.13"/>.
As the second most important student and research center in Switzerland (after Zurich), the urban agglomeration of Lausanne has experienced substantial growth during recent decades, which has mostly occurred in the form of suburbanization <xref ref-type="bibr" rid="bib1.bibx13" id="paren.14"/>.</p>
      <p id="d1e241">A notable geographic feature of Lausanne is its elevation difference of about 500 m between the lake shore at 372 m a.s.l. and the northeastern part of the agglomeration (see Fig. <xref ref-type="fig" rid="Ch1.F1"/>). The area is characterized by a continental temperate climate with mean annual temperatures of 10.9 <inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C and mean annual precipitation of 1100 mm, and a dominating vegetation of mixed broadleaf forest.</p>
<sec id="Ch1.S2.SS1.SSSx1" specific-use="unnumbered">
  <title>Spatial extent of the study</title>
      <p id="d1e260">In line with urban economics and regional sciences, many works rely on administrative boundaries to define the spatial extent of the study.
However, the way in which boundaries are constructed overlooks the characteristic scales at which landscape changes and environmental processes unfold, and might thus lead to equivocal results <xref ref-type="bibr" rid="bib1.bibx31 bib1.bibx37" id="paren.15"/>.
Considering such issues, the spatial extent for this study was determined quantitatively by following the method employed in the Atlas of Urban Expansion <xref ref-type="bibr" rid="bib1.bibx3" id="paren.16"/>. The core idea is that a pixel is considered part of the spatial extent depending on the proportion of built-up pixels that surround it. In this study, a pixel is considered part of the spatial extent when more than 15 % of the pixels that lay within a 500 m radius are built-up. Additionally, in order to evaluate how temperatures change across the urban–rural gradient, the spatial extent has been extended by a 1000 m buffer.
The above procedure has been applied to the rasterized land use and/or land cover (LULC) map by means of the Urban footprinter <xref ref-type="bibr" rid="bib1.bibx9" id="paren.17"/> Python library.
The obtained spatial extent, displayed in Fig. <xref ref-type="fig" rid="Ch1.F1"/>, has a surface of 112.46 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>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e285">Study area.
The upper left plot <bold>(A)</bold> shows the computed spatial extent (in orange) over the repartition of urban pixels (in black) derived from the rasterized cadastral survey <xref ref-type="bibr" rid="bib1.bibx6" id="paren.18"/>. The upper right plot <bold>(B)</bold> shows the locations of the air temperature measurement stations (see Appendix <xref ref-type="sec" rid="App1.Ch1.S1.SS2"/>).
The bottom row shows, for the computed spatial extent of the study, <bold>(C)</bold> the tree canopy map derived from the SWISSIMAGE orthomosaic <xref ref-type="bibr" rid="bib1.bibx20" id="paren.19"/> and <bold>(D)</bold> the altitude map derived from the free version of the digital height model of Switzerland <xref ref-type="bibr" rid="bib1.bibx19" id="paren.20"/>.
The basemap of plots <bold>(A)</bold>, <bold>(C)</bold> and <bold>(D)</bold> is based on the World Shaded Relief (© 2009 Esri).
The basemap tiles of plot <bold>(B)</bold> have been provided by Stamen Design (<uri>https://stamen.com</uri>, last access: 28 July 2020), under a Creative Commons BY 3.0 License (<uri>http://creativecommons.org/licenses/by/3.0</uri>, last access: 28 July 2020), with data from OpenStreetMap (<uri>https://openstreetmap.org</uri>, last access: 28 July 2020, © OpenStreetMap contributors 2021, distributed under a Creative Commons BY-SA License).</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021-f01.png"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Data</title>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>Land use and/or land cover data</title>
      <p id="d1e356">The LULC maps were obtained by rasterizing the vector geometries of the official cadastral survey of August 2019 to a 10 m resolution. Such a dataset is provided and maintained (i.e., updated weekly) by the cantonal administration of Vaud, and it features the whole spatial extent of the canton of Vaud <xref ref-type="bibr" rid="bib1.bibx6" id="paren.21"/>. The classification distinguishes 25 LULC classes that are relevant to the urban, rural and wild landscapes encountered in Switzerland <xref ref-type="bibr" rid="bib1.bibx17" id="paren.22"/>.
Moreover, a 1 m binary tree canopy mask was derived from the SWISSIMAGE orthomosaic <xref ref-type="bibr" rid="bib1.bibx20" id="paren.23"/>, by means of the DetecTree <xref ref-type="bibr" rid="bib1.bibx8" id="paren.24"/> Python library, which implements the methods proposed by <xref ref-type="bibr" rid="bib1.bibx57" id="text.25"/>.
The tree canopy mask of the spatial extent of the study is shown in Fig. <xref ref-type="fig" rid="Ch1.F1"/>.</p>
</sec>
<?pagebreak page3523?><sec id="Ch1.S2.SS2.SSS2">
  <label>2.2.2</label><title>Elevation data</title>
      <p id="d1e385">The elevation map for the study area, which is displayed in Fig. <xref ref-type="fig" rid="Ch1.F1"/>, is extracted from the free version of the digital height model of Switzerland <xref ref-type="bibr" rid="bib1.bibx19" id="paren.26"/>, provided at a 200 m resolution by the Federal Office of Topography.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS3">
  <label>2.2.3</label><title>Satellite data</title>
      <p id="d1e401">The satellite dataset consists of the eight Landsat 8 images in 2018 and 2019 that do not feature clouds over the study area and comprise days on which the maximum observed air temperature was over 25 <inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C (see the list of selected image tiles in Appendix <xref ref-type="sec" rid="App1.Ch1.S1.SS1"/>).
Data from Landsat 7 were excluded because of the scan line corrector malfunction.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS4">
  <label>2.2.4</label><title>Air temperature data</title>
      <p id="d1e423">A dataset of consistent air temperature measurements in the study area was assembled by combining data from 11 stations operated by various governmental and research sources, which are shown in Fig. <xref ref-type="fig" rid="Ch1.F1"/>.
The temporal resolution of the stations ranges from 10 to 30 min.
Given that the UHI effect in Switzerland reaches its maximal intensity around 21:00 CET <xref ref-type="bibr" rid="bib1.bibx15" id="paren.27"/>, the remainder of this study evaluates it based on the air temperature observations at the abovementioned time.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Simulation with the InVEST urban cooling model</title>
      <p id="d1e440">The simulation of the spatial distribution of UHIs employs the InVEST urban cooling model, version 3.8.0 <xref ref-type="bibr" rid="bib1.bibx45" id="paren.28"/>, which is based on the heat mitigation provided by shade, evapotranspiration and albedo.
The main inputs are a LULC raster map, a reference evapotranspiration raster and a biophysical table containing model information of each LULC class of the map. Each row of the biophysical table represents a LULC class and features the following columns:
<list list-type="bullet"><list-item>
      <p id="d1e448"><monospace>lucode</monospace> – the LULC class code as represented in the LULC raster map;</p></list-item><list-item>
      <p id="d1e454"><monospace>Shade</monospace> – a value between zero and one representing the proportion of tree cover in such a LULC class;</p></list-item><list-item>
      <p id="d1e460"><monospace>Kc</monospace> – the evapotranspiration coefficient;</p></list-item><list-item>
      <p id="d1e466"><monospace>Albedo</monospace> – a value between zero and one representing the proportion of solar radiation directly reflected by the LULC class;</p></list-item><list-item>
      <p id="d1e472"><monospace>Green_area</monospace> – whether the LULC class should be considered a green area or not;</p></list-item><list-item>
      <p id="d1e478"><monospace>Building_intensity</monospace> – a value between zero and one representing the ratio between floor area and land area (for nighttime simulations).</p></list-item></list></p>
<?pagebreak page3524?><sec id="Ch1.S2.SS3.SSS1">
  <label>2.3.1</label><title>Model description</title>
      <p id="d1e490">The data inputs described above are used to compute the cooling capacity index, which is based on the physical mechanisms that contribute to cooling urban temperatures. More precisely, the cooling capacity index used in the InVEST urban cooling model builds upon the indices proposed by <xref ref-type="bibr" rid="bib1.bibx60" id="text.29"/>, which are based on shading and evapotranspiration, and extends them by adding a factor to account for the albedo.
For each pixel <inline-formula><mml:math id="M5" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> of the LULC raster map, the cooling capacity index is computed as follows:
              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M6" display="block"><mml:mrow><mml:msub><mml:mtext>CC</mml:mtext><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">S</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">AL</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:msub><mml:mtext>AL</mml:mtext><mml:mi>i</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">ET</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:msub><mml:mtext>ETI</mml:mtext><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:msub><mml:mtext>AL</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:msub><mml:mtext>ETI</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> represent the respective tree shading, albedo and evapotranspiration values of pixel <inline-formula><mml:math id="M10" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> as defined in the biophysical table, and <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">S</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">AL</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">ET</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> represent the weights attributed to each respective component.
The values of <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msub><mml:mtext>AL</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are retrieved from the biophysical table according to the LULC class <inline-formula><mml:math id="M16" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> of the pixel <inline-formula><mml:math id="M17" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> (see Appendix <xref ref-type="sec" rid="App1.Ch1.S1.SS3"/>).
The tree shading is computed by overlaying the binary tree canopy mask with the rasterized LULC map so that for each LULC class <inline-formula><mml:math id="M18" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>, the shade coefficient <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> corresponds to the average proportion of tree cover over all the LULC pixels of class <inline-formula><mml:math id="M20" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>, as follows:
              <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M21" display="block"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mo>|</mml:mo><mml:msub><mml:mi mathvariant="normal">Ω</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>|</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>∈</mml:mo><mml:msub><mml:mi mathvariant="normal">Ω</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:munder><mml:msub><mml:mi>x</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            Here, <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">Ω</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the set of pixels of the tree canopy mask whose location corresponds to class <inline-formula><mml:math id="M23" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> in the LULC raster, and <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the value of pixel <inline-formula><mml:math id="M25" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> of the tree canopy mask, i.e., one if <inline-formula><mml:math id="M26" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> corresponds to a tree and zero otherwise.
The albedo coefficients are based on the local climate zone classification by <xref ref-type="bibr" rid="bib1.bibx51" id="text.30"/>.</p>
      <p id="d1e792">The evapotranspiration index ETI is computed as a normalized value of the potential evapotranspiration as follows:
              <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M27" display="block"><mml:mrow><mml:mtext>ETI</mml:mtext><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:msub><mml:mi mathvariant="normal">ET</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="normal">ET</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the evapotranspiration coefficient, <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">ET</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the reference evapotranspiration raster for the period and area of interest, and <inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">ET</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the maximum evapotranspiration value observed in the area of interest.</p>
      <p id="d1e861">In line with the studies of <xref ref-type="bibr" rid="bib1.bibx33" id="text.31"/>, <xref ref-type="bibr" rid="bib1.bibx34" id="text.32"/> and <xref ref-type="bibr" rid="bib1.bibx32" id="text.33"/>, the evapotranspiration coefficients are attributed to each LULC class by distinguishing four cases, namely the crop coefficient for single crops for vegetation LULC classes, the water evaporation coefficient for surface water, the rock and soil evaporation coefficient for bare soils and rocks, and evaporation coefficients for artificial LULC classes (e.g., urban areas).
The evapotranspiration coefficients attributed to the LULC classes of the Swiss cadastral survey are listed in Table <xref ref-type="sec" rid="App1.Ch1.S1.SS3"/>.</p>
      <p id="d1e875">Following the recommendations of <xref ref-type="bibr" rid="bib1.bibx1" id="text.34"/>, the daily evapotranspiration <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">ET</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (in mm/d) was estimated for each pixel using the Hargreaves equation <xref ref-type="bibr" rid="bib1.bibx26" id="paren.35"/> as follows:
              <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M32" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="normal">ET</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0023</mml:mn><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">avg</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">17.8</mml:mn><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:msup><mml:mo>⋅</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">avg</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> correspond to the average, maximum and minimum <inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (in <inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C) of each day, respectively, and <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the extraterrestrial radiation (in mm/d), which is estimated for the latitude of Lausanne (i.e., 46.519833<inline-formula><mml:math id="M39" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>) for each date following the methods of <xref ref-type="bibr" rid="bib1.bibx1" id="text.36"><named-content content-type="post">Eq. 21</named-content></xref>.
The temperature values of each day have been extracted from the inventory of gridded datasets provided by the Federal Office of Meteorology and Climatology (MeteoSwiss), which feature the minimum, average and maximum daily <inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for the extent of the whole country at a resolution of 1 km. Such a dataset is obtained by interpolating 100 <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> stations across Switzerland (including the MeteoSwiss Pully station in Fig. <xref ref-type="fig" rid="Ch1.F1"/>) based on nonlinear thermal profiles of major basins and non-Euclidean distance weighting that accounts for terrain effects <xref ref-type="bibr" rid="bib1.bibx21" id="paren.37"/>.</p>
      <p id="d1e1064">In order to account for the cooling effect of large green spaces, the computed cooling capacity index of pixels that are part of large green areas (<inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> ha) is adjusted as follows:
              <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M43" display="block"><mml:mrow><mml:msubsup><mml:mtext>CC</mml:mtext><mml:mi>i</mml:mi><mml:mi mathvariant="normal">green</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>∈</mml:mo><mml:msub><mml:mi mathvariant="normal">Ω</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:munder><mml:msub><mml:mi>g</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:msub><mml:mtext>CC</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mstyle scriptlevel="+1"><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">cool</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is one when the pixel <inline-formula><mml:math id="M45" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> is a green area and zero otherwise (as defined in the biophysical table), <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the distance between pixels <inline-formula><mml:math id="M47" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M48" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">cool</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is a parameter that defines the distance over which a green space has a cooling effect, and <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">Ω</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the set of pixels whose distance to <inline-formula><mml:math id="M51" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> is lower than <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">cool</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e1239">A heat mitigation (HM) index is then computed as follows:
              <disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M53" display="block"><mml:mrow><mml:msub><mml:mtext>HM</mml:mtext><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mfenced open="{" close=""><mml:mtable class="array" columnalign="left left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mtext>CC</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext> if </mml:mtext><mml:mi>i</mml:mi><mml:mtext> is part of a large green area</mml:mtext></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mtext> or </mml:mtext><mml:msub><mml:mtext>CC</mml:mtext><mml:mi>i</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:msubsup><mml:mtext>CC</mml:mtext><mml:mi>i</mml:mi><mml:mi mathvariant="normal">green</mml:mi></mml:msubsup></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msubsup><mml:mtext>CC</mml:mtext><mml:mi>i</mml:mi><mml:mi mathvariant="normal">green</mml:mi></mml:msubsup></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext> otherwise</mml:mtext><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced></mml:mrow></mml:math></disp-formula>
            In order to simulate the spatial distribution of <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the model requires two additional inputs. The first is the rural reference temperature <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, where the UHI effect is not observed, e.g.,<?pagebreak page3525?> in the rural surroundings of the city. The second is the magnitude of the UHI effect <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">UHI</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, namely the difference between the rural reference temperature and the maximum <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> observed in the city center.
The two parameters are combined with <inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:msub><mml:mtext>HM</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> to compute the <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for each pixel <inline-formula><mml:math id="M60" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> of the study area as follows:
              <disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M61" display="block"><mml:mrow><mml:msubsup><mml:mi>T</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mi mathvariant="normal">no</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">mix</mml:mi></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mtext>HM</mml:mtext><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:msub><mml:mi mathvariant="normal">UHI</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            Finally, the <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values of each pixel <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:msubsup><mml:mi>T</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mi mathvariant="normal">no</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">mix</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> are spatially averaged using a Gaussian function with a kernel radius <inline-formula><mml:math id="M64" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> defined by the user.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS2">
  <label>2.3.2</label><title>Calibration and evaluation of the model</title>
      <p id="d1e1476">To compare the InVEST urban cooling model with the spatial regression based on satellite features, the urban cooling model is used to simulate the spatial distribution of <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for the same eight dates used to train the spatial regression model, i.e., the dates of the selected Landsat images.
It is implicitly assumed that no significant LULC changes have occurred throughout study period (i.e., from May 2018 to August 2019); therefore, all simulations depart from the same LULC raster, i.e., the rasterized cadastral survey of the canton of Vaud as described above.
Given the rugged terrain of the study area, the <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> was set as the minimum average <inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> observed among the monitoring stations, while <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">UHI</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> was set as the difference between the maximum average <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> observed among the monitoring stations and <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. The values of <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">UHI</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for the 8 d considered in this study are displayed in Fig. <xref ref-type="fig" rid="App1.Ch1.S1.F7"/>.</p>
      <p id="d1e1570">Although the documentation of the InVEST urban cooling model <xref ref-type="bibr" rid="bib1.bibx45" id="paren.38"/> provides some suggested values for several parameters of the model, their suitability depends strongly on the local geographic conditions of the study area.
Therefore, calibration of the parameters is required in order to better understand how the physical mechanisms beyond the emergence of UHIs take place in the context of Lausanne.
Following the manual calibration approach drafted by <xref ref-type="bibr" rid="bib1.bibx25" id="text.39"/>, the target parameters are the weights attributed to the tree shading (<inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">S</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), albedo (<inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and evapotranspiration (<inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">ET</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), the distance over which green spaces have a cooling effect (<inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">cool</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and the <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> mixing radius (<inline-formula><mml:math id="M78" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula>).
As an additional contribution, this article implements an automated calibrated procedure based on simulated annealing optimization <xref ref-type="bibr" rid="bib1.bibx29" id="paren.40"/> that aims at the minimization of the <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> between the <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values observed in the monitoring stations and those predicted by the model<fn id="Ch1.Footn1"><p id="d1e1668">The calibration module has been designed as a reusable open-source Python package (see <uri>https://github.com/martibosch/invest-ucm-calibration</uri>; last access: 11 September 2020)</p></fn>.
The parameter values suggested in the documentation of the model are set as the initial state of the simulation annealing procedure, which corresponds to a <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> mixing radius of <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> m, a green area cooling distance of <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">cool</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> m, and weights attributed to tree shading, albedo and evapotranspiration of <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">S</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">ET</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula>, respectively. The number of calibration iterations is set to 100.</p>
      <p id="d1e1759">Given that the <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">UHI</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> parameters in this study were obtained from observations from each simulated day, metrics such as the mean absolute error (MAE) and the root mean squared error (RMSE) are effectively constrained to the <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msub><mml:mi mathvariant="normal">UHI</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> range, which affects the interpretation of these metrics.
Therefore, in order to evaluate the ability of the InVEST urban cooling model to spatially simulate UHIs, the coefficient of adjustment <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, MAE and RMSE of the calibrated model are compared with those computed in two additional experiments.
The first experiment consisted of randomly sampling the <inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values from a uniform distribution over the <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msub><mml:mi mathvariant="normal">UHI</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> range of each date.
In the second experiment, the <inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values of each date were randomly sampled from a normal distribution with the mean and standard deviation of the <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> measurements of the monitoring stations.
For both experiments, the three evaluation metrics are reported as their average over 10 runs.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Spatial regression of air temperature based on satellite data</title>
      <p id="d1e1881">The spatial regression to predict <inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> from features derived from satellite data is performed over a raster dataset on a per-pixel basis. A regression model is then trained to fit the observed <inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> measurements by minimizing the error at the pixels that correspond to the locations of the monitoring stations.</p>
      <p id="d1e1906">The regression operates in each pixel with the <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> as the target variable, and the elevation, the LST and the normalized difference water index (NDWI) <xref ref-type="bibr" rid="bib1.bibx22" id="paren.41"/> as independent variables.
Additionally, to account for the influence of the temperature and moisture surface conditions of each pixel, the LST and NDWI are spatially averaged over a series of circular neighborhoods with radii of 200, 400, 600 and 800 m, thereby reckoning eight supplementary features.
Based on previous research on the sensitivity of the landscape pattern–UHI relationships to the spatial resolution <xref ref-type="bibr" rid="bib1.bibx56 bib1.bibx49" id="paren.42"/>, the target resolution was set to 200 m.</p>
<sec id="Ch1.S2.SS4.SSS1">
  <label>2.4.1</label><title>Computation of satellite-derived features</title>
      <p id="d1e1933">The estimation of the LST from Landsat 8 images followed the methods of <xref ref-type="bibr" rid="bib1.bibx7" id="text.43"/>. On the one hand, the data from the near-infrared (NIR) and red bands of Landsat 8 (i.e., bands 4 and 5, respectively) were used to compute the normalized difference vegetation index (NDVI), which was then used to estimate the ground emissivity (<inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>). On the other hand, following the Landsat 8 Data Users Handbook <xref ref-type="bibr" rid="bib1.bibx59" id="paren.44"/>, the data from the thermal band of Landsat 8 (i.e., band 10) were first converted to top-of-atmosphere spectral radiance (<inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), from which brightness temperature (BT) was estimated (in <inline-formula><mml:math id="M100" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C) as follows:
              <disp-formula id="Ch1.E8" content-type="numbered"><label>8</label><mml:math id="M101" display="block"><mml:mrow><mml:mtext>BT</mml:mtext><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mrow><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>K</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:mn mathvariant="normal">273.15</mml:mn><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            Here, <inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are band-specific thermal conversion constants embedded in the Landsat image metadata. Finally, the ground emissivity (<inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and the brightness temperature (BT) were used to compute the LST by inversion of Planck's Law:
              <disp-formula id="Ch1.E9" content-type="numbered"><label>9</label><mml:math id="M105" display="block"><mml:mrow><mml:mtext>LST</mml:mtext><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mtext>BT</mml:mtext><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:mtext>BT</mml:mtext><mml:mo>/</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="italic">λ</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.438</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> m K is a constant computed as a product of the Boltzmann constant and Planck's constants divided by the velocity of the light, and <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">10.895</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> is the average of the limiting wavelengths of the thermal band.</p>
      <p id="d1e2152">The NDWI is computed from the green and near-infrared (NIR) bands of Landsat 8 (i.e., bands 3 and 5, respectively) as follows:
              <disp-formula id="Ch1.E10" content-type="numbered"><label>10</label><mml:math id="M108" display="block"><mml:mrow><mml:mtext>NDWI</mml:mtext><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">green</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">NIR</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">green</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">NIR</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
</sec>
<sec id="Ch1.S2.SS4.SSS2">
  <label>2.4.2</label><title>Model selection and evaluation</title>
      <p id="d1e2202">Based on the work of <xref ref-type="bibr" rid="bib1.bibx27" id="text.45"/>, three regression models have been considered, namely a multiple linear regression model, a support-vector machine (SVM) model and a random forest model.
The accuracy of each regression model is assessed by means of a <inline-formula><mml:math id="M109" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-fold cross-validation procedure, where the regression samples are first shuffled and partitioned into three folds. For each fold <inline-formula><mml:math id="M110" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>, a regression model is then trained using the other two folds, and it is validated using the samples of the <inline-formula><mml:math id="M111" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> fold.
Finally, the model that shows the best validation score (i.e., the <inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> averaged over 10 repetitions of the <inline-formula><mml:math id="M113" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-fold procedure) is selected.
Additionally, the MAE and RMSE are computed in order to evaluate the deviations between the observed <inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the predictions of each model.</p>
      <p id="d1e2259">The importance of each feature is also evaluated by computing its permutation importance <xref ref-type="bibr" rid="bib1.bibx14" id="paren.46"/>, namely the average decrease in the regression accuracy when a feature is randomly shuffled.
The training of the regression models, the cross-validation and the permutation feature importance described above have been implemented by means of the Scikit-learn library <xref ref-type="bibr" rid="bib1.bibx38" id="paren.47"/>.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Spatial regression of air temperature based on satellite data</title>
      <p id="d1e2285">When including all of the samples, the <inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> for the linear regression, SVM and random forest are 0.832, 0.014 and 0.960, respectively, with a respective MAE of 1.198, 2.671 and 0.580 <inline-formula><mml:math id="M116" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, and a respective RMSE of 1.508, 3.652 and 0.738 <inline-formula><mml:math id="M117" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C.
The coefficients suggest that SVM is not well suited for such a regression in this study area, whereas the linear regression and random forest models obtain a very strong fit – with the latter achieving the best performance.
Nevertheless, the average cross-validation scores suggest that the linear regression (average score <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.733</mml:mn></mml:mrow></mml:math></inline-formula>) is more robust to missing data and also less likely to over-fit the observations than the random forest regressor (average score <inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.658</mml:mn></mml:mrow></mml:math></inline-formula>).
Thus, the remainder of the article only considers the results obtained with a linear regression model trained with all of the samples.</p>
      <p id="d1e2347">The importance of features of the chosen linear regression model can be evaluated by means of an <inline-formula><mml:math id="M120" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> test, as implemented in the statsmodels <xref ref-type="bibr" rid="bib1.bibx44" id="paren.48"/> Python library (see Table <xref ref-type="table" rid="App1.Ch1.S2.T1"/>).
With a significance level of <inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>, the results of the <inline-formula><mml:math id="M122" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> test suggest that the most significant variable for the linear regression is the NDWI spatially averaged over a 800, 600 and 400 m radius (in decreasing order of significance). The following most significant variable is the NDWI spatially averaged over a 200 m radius (<inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.071</mml:mn></mml:mrow></mml:math></inline-formula>) and without spatial averaging (<inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.231</mml:mn></mml:mrow></mml:math></inline-formula>), and the LST spatially averaged over a 400 m radius (<inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.277</mml:mn></mml:mrow></mml:math></inline-formula>). With a significance level of <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.420</mml:mn></mml:mrow></mml:math></inline-formula>, the elevation does not appear to be significant in this particular regression.
The low significance obtained for the LST features in this study might be attributable to the large time lag between the acquisition time of the Landsat images (which ranges from 11:15 to 11:23 CET) and the time of the <inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> measurements (i.e. 21:00 CET).</p>
      <p id="d1e2441">The relationship between the predicted and the observed values is displayed in Fig. <xref ref-type="fig" rid="App1.Ch1.S2.F8"/>.
The respective MAE and RMSE values of 1.198 and 1.508 <inline-formula><mml:math id="M128" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C demonstrate a stronger fit than the values of 1.82 and 2.31 <inline-formula><mml:math id="M129" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C obtained in the study of <xref ref-type="bibr" rid="bib1.bibx27" id="text.49"/> in Vancouver.
The two plots in Fig. <xref ref-type="fig" rid="Ch1.F2"/> show the relationship between the elevation and <inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of each sample and the regression errors. While there is no discernable relationship regarding the elevation of the samples (i.e., the elevation of the monitoring stations), the regression errors seem to be negatively correlated with <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.
This pattern, which was also noted by <xref ref-type="bibr" rid="bib1.bibx27" id="text.50"/>, indicates that high-temperature samples are systematically underestimated by the regression model, whereas low-temperature samples are consistently overestimated.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e2498">Scatterplot of the spatial regression residuals (<inline-formula><mml:math id="M132" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis) against the elevation of the monitoring station (<inline-formula><mml:math id="M133" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis of panel <bold>a</bold>) and the observed <inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M135" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis of panel <bold>b</bold>), colored by the sample date. See Appendix B.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021-f02.png"/>

        </fig>

      <p id="d1e2546">The series of predicted <inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> maps for the eight dates as well as the prediction errors at the locations of the monitoring stations are displayed in Fig. <xref ref-type="fig" rid="Ch1.F3"/>.
While the range of temperatures exhibits important differences throughout the dates, the spatial distribution of <inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is seemingly consistent.
The highest temperatures persistently occur in the most urbanized areas, whereas the lowest temperatures take place at higher elevations located in the east and northeast of the map.
Finally, there seems to be no discernable pattern in space nor time regarding the prediction errors at the monitoring stations.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e2575">Maps of the <inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> predicted by the spatial regression for the eight dates. The points in the map correspond to the location of the monitoring stations and are colored according to the regression errors. </p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021-f03.png"/>

        </fig>

</sec>
<?pagebreak page3527?><sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Simulation with the InVEST urban cooling model</title>
      <p id="d1e2603">The parameters of the model that result in the best fit of the station measurements are a <inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> mixing radius of <inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">236.02</mml:mn></mml:mrow></mml:math></inline-formula> m, a green area cooling distance of <inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">cool</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">89.21</mml:mn></mml:mrow></mml:math></inline-formula> m, and weights attributed to tree shading, albedo and evapotranspiration of <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">S</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.59</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.24</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">ET</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.17</mml:mn></mml:mrow></mml:math></inline-formula>, respectively (see Appendix B).
The <inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, MAE and RMSE of the calibrated model are 0.903, 0.955 and 1.144 <inline-formula><mml:math id="M146" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, respectively; these values suggest better model performance than randomly sampling from the station measurements. Random sampling from the station measurements yields a respective <inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, MAE and RMSE of 0.573, 1.947 and 2.405 <inline-formula><mml:math id="M148" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C when sampling from a uniform distribution and 0.550, 1.952 and 2.468 <inline-formula><mml:math id="M149" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C when sampling from a normal distribution.
Furthermore, the values of <inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, MAE and RMSE obtained with the calibrated parameters reveal a stronger fit than the spatial regression reported above.</p>
      <?pagebreak page3528?><p id="d1e2751">The relationship between the <inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values at the monitoring stations simulated with the calibrated parameters and the actual observed measurements is shown in Fig. <xref ref-type="fig" rid="App1.Ch1.S2.F9"/>.
The differences between <inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> simulated at the monitoring stations and the observed values are plotted against the elevation and the observed temperatures (<inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) in Fig. <xref ref-type="fig" rid="Ch1.F4"/>.
The pattern of such relationships is very similar to that observed in the spatial regression. Conversely, there is no clear relationship between the prediction error of the urban cooling model and elevation.
Moreover, the prediction errors exhibit a negative correlation with the observed temperature, denoting a systematic tendency to both underestimate high temperatures and overestimate low temperatures – with the former being more prominent in this case, as is noticeable from the asymmetry of the <inline-formula><mml:math id="M154" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis in Fig. <xref ref-type="fig" rid="Ch1.F4"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e2803">Scatterplot of the differences between the <inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> simulated by the InVEST urban cooling model and the values observed at the monitoring stations (<inline-formula><mml:math id="M156" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis) against the elevation of the monitoring station (<inline-formula><mml:math id="M157" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis of panel <bold>a</bold>) and the observed <inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M159" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis of panel <bold>b</bold>), colored by the sample date.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021-f04.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e2865">Maps of the <inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> simulated by the InVEST urban cooling model for the eight dates. The points on the map correspond to the location of the monitoring stations and are colored according to the simulation errors.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021-f05.png"/>

        </fig>

      <p id="d1e2885">The simulated <inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> maps for the eight dates and the prediction errors at the monitoring stations are shown in Fig. <xref ref-type="fig" rid="Ch1.F5"/>.
As in the spatial regression, the temperature ranges show important differences across dates, yet the same spatial pattern of <inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> persists.
The simulated distribution of <inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> shows its highest values in the center of Lausanne and along the most urbanized (and hence less forested) zones along the main transportation axes, whereas the lowest temperatures are found in the forested areas located in the eastern and western extremes of the upper half of the study area.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Model comparison</title>
      <p id="d1e2931">A comparison of the maps predicted by the spatial regression and the urban cooling model is displayed in Fig. <xref ref-type="fig" rid="Ch1.F6"/>.
In line with the temporal consistency of the spatial patterns predicted by the respective two approaches, the comparison maps also show a spatial distribution of <inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> that persists throughout the dates.
Such a spatial pattern is strongly reminiscent of the elevation maps (see Fig. <xref ref-type="fig" rid="Ch1.F1"/> above) and reflects the fact that elevation is explicitly considered in the spatial regression but not in the urban cooling model.
The overall distribution of the <inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> pixel differences between the two approaches follows a normal distribution that ranges from <inline-formula><mml:math id="M166" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9.620</mml:mn></mml:mrow></mml:math></inline-formula> to 11.929 <inline-formula><mml:math id="M167" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C (reflecting the lower and higher temperatures predicted in the spatial regression, respectively), which is a considerably large range when compared with the small overall MAE and RMSE of both approaches.
Nonetheless, the way in which the histogram is centered around 0 <inline-formula><mml:math id="M168" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C suggests that the differences between the two approaches follow no particular correlation other than the spatial regression predicting more extreme <inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values, which is not surprising considering that the range of <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is systematically bounded in the urban cooling model by the <inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">UHI</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> parameters.</p><?xmltex \hack{\newpage}?><?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e3035">Maps comparing the difference between the <inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> predicted by the spatial regression <inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>T</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi mathvariant="normal">sr</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the InVEST urban cooling model <inline-formula><mml:math id="M175" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>T</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi mathvariant="normal">ucm</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for the eight dates (see Appendix B).</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021-f06.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Discussion</title>
      <p id="d1e3092">The results obtained in this study suggest that both the spatial regression based on satellite data and the InVEST urban cooling model are capable of predicting the spatial distribution of air temperature with a large degree of statistical determination.
Furthermore, the fact that a similar spatial pattern is predicted by both models suggests that the biophysical mechanisms embedded in the urban cooling model are well represented.
If that is the case, the urban cooling model presents two central advantages with respect to the spatial regression.</p>
      <p id="d1e3095">The first advantage is that, in contrast to regressions and black-box approaches, the biophysical mechanisms that drive the emergence of UHIs are represented explicitly; this allows for a physical interpretation of the parameters of the model.
For example, in a comparative study of the relationship between the LST and the spatial configuration of trees in Baltimore and Sacramento, <xref ref-type="bibr" rid="bib1.bibx62" id="text.51"/> suggested that the distinctive results observed in each city might be related to how the shading of trees and evapotranspiration contribute differently to urban cooling in the climatic context of each city.
More precisely, the abovementioned study suggested that in the dry climate of Sacramento, large patches of trees ameliorate the efficiency of the evapotranspiration, whereas the gains from the tree shading are likely more important in the humid climate of Baltimore.
The urban cooling model provides a suitable means to quantitatively address such matters – i.e., by calibrating the model in the two cities, we can explore the weights obtained for each factor to support such a hypothesis.
In the case study of Lausanne reported above, the weight attributed to the tree shading (<inline-formula><mml:math id="M176" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">S</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.59</mml:mn></mml:mrow></mml:math></inline-formula>) is higher than that attributed to the evapotranspiration (<inline-formula><mml:math id="M177" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">ET</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.17</mml:mn></mml:mrow></mml:math></inline-formula>). This is consistent with the local climatic conditions being more similar in Lausanne and Baltimore than in Sacramento; however, the weights obtained in this study might be partly determined by the initial solution provided.
Nonetheless, to further understand this issue, validation and calibration of the InVEST urban cooling model in a broader variety of cities is required.
Overall, the way in which the calibrated parameters differ from the recommendations in the documentation of the model are in consonance with the particular characteristics of Lausanne.
More precisely, the smaller mixing radius and cooling distances are consistent with the uneven relief of the study area.</p>
      <p id="d1e3131">The second major advantage of the urban cooling model is that once the model is calibrated for a given city, it can be used to evaluate synthetic scenarios, such as those stemming from master plans, urbanization prospects or the like, and to spatially design solutions.
This kind of spatially explicit evaluation of the impacts of alternative scenarios on ecosystem services is in fact one of the central purposes of the InVEST suite of models <xref ref-type="bibr" rid="bib1.bibx53" id="paren.52"/>.
Statistical models like the spatial regression are not well suited to such a<?pagebreak page3529?> purpose, as they rely on features, such as the LST, that are hard to obtain other than empirically.</p>
      <p id="d1e3137">The approach proposed in this article is nevertheless subject to some limitations that merit thoughtful consideration.
On the one hand, as acknowledged in its user guide <xref ref-type="bibr" rid="bib1.bibx45" id="paren.53"/>, the design of the InVEST urban cooling model presents a number of limitations, the most relevant to this study being the simplified and homogeneous way in which the air is mixed and the cooling effects of large green spaces. In complex terrains such as the Lausanne agglomeration, models with uniform weighting of space show considerable deviations from the observed distribution of air temperature <xref ref-type="bibr" rid="bib1.bibx21" id="paren.54"/>.
On the other hand, the relationship between the calibration parameters and the resulting <inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> is likely to define a complex optimization landscape with multiple local optima.
As a metaheuristic that strongly depends on random<?pagebreak page3530?> decisions, the simulated annealing procedure is susceptible to convergence to local optima, arbitrarily leading to different solutions in each run.
A sensitivity analysis of the parameters of the urban cooling model as undertaken preliminarily by <xref ref-type="bibr" rid="bib1.bibx25" id="text.55"/> for the Île-de-France region could serve as a basis to improve the simulated annealing procedure by careful design of an appropriate neighborhood search and annealing schedule.
Finally, the approach of the present study is based on observations at the moment of maximal UHI intensity (i.e., 21:00 CET in Switzerland); however, the factors that influence UHIs are likely to operate differently across the diurnal UHI cycle.
In fact, several studies point to distinct relationships between the spatial patterns of vegetation and daytime and nighttime UHIs <xref ref-type="bibr" rid="bib1.bibx4 bib1.bibx46 bib1.bibx47 bib1.bibx25" id="paren.56"/>.
Considering the nature of the implications of UHIs, e.g., energy consumption, work productivity or human health <xref ref-type="bibr" rid="bib1.bibx30 bib1.bibx41 bib1.bibx58" id="paren.57"/>, a sound understanding of the full diurnal UHI cycle becomes crucial towards the design of robust solutions.</p>
      <p id="d1e3168">Nevertheless, the limitations on how the urban cooling model represents the spatial air mixing and the cooling effects of green spaces seem hard to overcome with the current spatial sparsity of monitoring stations.
Such a major shortcoming, which contrasts with the growing availability of high-resolution LST datasets, is one of the main reasons why most UHI studies have focused on the latter <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx61" id="paren.58"/>.
As illustrated in this article, spatial regressions based on remote sensing features such as the LST and NDWI do not necessarily replicate the air temperature measurements better than biophysical models such as the InVEST urban cooling model.
Therefore, improving the spatial density of the monitoring network becomes imperative for further enlightenment with respect to the UHI phenomena.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d1e3183">The present article presents a spatially explicit approach to simulate UHIs with the InVEST urban cooling model, which is based on three biophysical mechanisms, namely tree shade, evapotranspiration and albedo. The proposed approach shows how LULC and air temperature data can be combined to calibrate the parameters of the model to best fit measurements from monitoring stations by means of an automated procedure.
The simulations performed for the urban agglomeration of Lausanne show that the InVEST urban cooling model can outperform spatial regressions based on satellite-derived features such as LST, NDWI and<?pagebreak page3531?> elevation.
The way in which both approaches consistently predict the highest temperatures in the most urbanized parts of the agglomeration suggests that the enhancement of green infrastructure can be an effective heat mitigation strategy; however, further exploration in other climatic contexts is required to fully understand this issue.
To that end, the reusability of the computational workflow paves the way for further application of the urban cooling model to a broad variety of cities, which can serve to improve the understanding of the UHI phenomena and support the design of heat mitigation strategies.</p><?xmltex \hack{\clearpage}?>
</sec>

      
      </body>
    <back><app-group>

<?pagebreak page3532?><app id="App1.Ch1.S1">
  <?xmltex \currentcnt{A}?><label>Appendix A</label><title>Data</title>
<sec id="App1.Ch1.S1.SS1">
  <label>A1</label><title>Landsat tiles</title>
      <p id="d1e3205">The list of product identifiers for the Landsat image tiles are available as a comma-separated value (CSV) file at <uri>https://zenodo.org/record/4384675/files/landsat-tiles.csv</uri> (last access: 13 July 2020).</p>
</sec>
<sec id="App1.Ch1.S1.SS2">
  <label>A2</label><title>Monitoring stations</title>
      <p id="d1e3219">The list of monitoring stations with their operator and their elevation in meters above sea level is available as a CSV file at <uri>https://zenodo.org/record/4384675/files/station-tair.csv</uri> (last access: 13 July 2020). The operators are Agrometeo, the Federal Roads Office (ASTRA), the Federal Office for the Environment (BAFU), the general directorate for the environment of the canton of Vaud (DGE), and the Federal Institute of Forest, Snow and Landscape Research (WSL) <xref ref-type="bibr" rid="bib1.bibx40" id="paren.59"/>.</p>
</sec>
<sec id="App1.Ch1.S1.SS3">
  <label>A3</label><title>Biophysical table</title>
      <p id="d1e3236">The biophysical table used in the computational workflow is available as a CSV file at <uri>https://zenodo.org/record/4384675/files/biophysical-table.csv</uri> (last access 13 July 2020). The crop and water coefficients are based on Allen et al. (1998), whereas rock, soil and urban coefficients are derived from the results of Grimmond and Oke (1999) in the city of Chicago. Given that the evapotranspiration of the vegetation and crops is subject to seasonal changes in temperate zones such as Switzerland (Allen et al., 1998), the values
correspond to the mid-season estimation (June to August) in Nistor (2016). The albedo values are based on the work of Stewart and Oke (2012). The shade column, which represents
the proportion of tree cover of each LULC class, has been computed with a high-resolution tree canopy map of Lausanne and is, therefore, specific to the study area. Rows with a dash (–) in the shade column denote that the corresponding LULC class is not present in the study area.</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="App1.Ch1.S1.SS4">
  <label>A4</label><title>Reference temperatures and UHI magnitude</title>

      <?xmltex \floatpos{h!}?><fig id="App1.Ch1.S1.F7"><?xmltex \currentcnt{A1}?><?xmltex \def\figurename{Figure}?><label>Figure A1</label><caption><p id="d1e3253">Reference temperatures <inline-formula><mml:math id="M179" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (i.e., minimum <inline-formula><mml:math id="M180" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> at 21:00 CET among the monitoring stations) and magnitude of the UHI <inline-formula><mml:math id="M181" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">UHI</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (i.e., difference between <inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the maximum <inline-formula><mml:math id="M183" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> at 21:00 CET among the monitoring stations) for the eight dates considered in this study.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021-f07.png"/>

        </fig>

<?xmltex \hack{\clearpage}?>
</sec>
</app>

<?pagebreak page3533?><app id="App1.Ch1.S2">
  <?xmltex \currentcnt{B}?><label>Appendix B</label><title>Results</title>
<sec id="App1.Ch1.S2.SS1">
  <label>B1</label><title>Tables</title>

<?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S2.T1"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{B1}?><label>Table B1</label><caption><p id="d1e3339"><inline-formula><mml:math id="M184" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> test of variable significance of the linear regression.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left" colsep="1"/>
     <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:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Feature</oasis:entry>
         <oasis:entry colname="col2">Coefficient</oasis:entry>
         <oasis:entry colname="col3">SE</oasis:entry>
         <oasis:entry colname="col4">t</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M185" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>&gt;</mml:mo><mml:mo>|</mml:mo><mml:mi>t</mml:mi><mml:mo>|</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">[0.025</oasis:entry>
         <oasis:entry colname="col7">0.975]</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">const</oasis:entry>
         <oasis:entry colname="col2">1.1760</oasis:entry>
         <oasis:entry colname="col3">3.369</oasis:entry>
         <oasis:entry colname="col4">0.349</oasis:entry>
         <oasis:entry colname="col5">0.728</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M186" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5.534</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7">7.886</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">lst_0</oasis:entry>
         <oasis:entry colname="col2">0.4944</oasis:entry>
         <oasis:entry colname="col3">0.584</oasis:entry>
         <oasis:entry colname="col4">0.846</oasis:entry>
         <oasis:entry colname="col5">0.400</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M187" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.669</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7">1.658</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ndwi_0</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6.1852</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">5.127</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M189" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.206</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">0.231</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">16.396</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7">4.026</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">lst_200</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.3267</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">0.885</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.369</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">0.713</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2.089</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7">1.435</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ndwi_200</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">28.5531</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">15.581</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.833</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">0.071</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">59.585</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7">2.479</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">lst_400</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M197" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.9332</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">1.765</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M198" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.095</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">0.277</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M199" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5.449</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7">1.583</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ndwi_400</oasis:entry>
         <oasis:entry colname="col2">124.2456</oasis:entry>
         <oasis:entry colname="col3">46.749</oasis:entry>
         <oasis:entry colname="col4">2.658</oasis:entry>
         <oasis:entry colname="col5">0.010</oasis:entry>
         <oasis:entry colname="col6">31.138</oasis:entry>
         <oasis:entry colname="col7">217.353</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">lst_600</oasis:entry>
         <oasis:entry colname="col2">1.0526</oasis:entry>
         <oasis:entry colname="col3">2.963</oasis:entry>
         <oasis:entry colname="col4">0.355</oasis:entry>
         <oasis:entry colname="col5">0.723</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4.849</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7">6.955</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ndwi_600</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M201" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">156.7220</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">55.931</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M202" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2.802</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">0.006</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">268.119</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M204" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">45.325</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">lst_800</oasis:entry>
         <oasis:entry colname="col2">1.7306</oasis:entry>
         <oasis:entry colname="col3">1.685</oasis:entry>
         <oasis:entry colname="col4">1.027</oasis:entry>
         <oasis:entry colname="col5">0.308</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M205" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.626</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7">5.087</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ndwi_800</oasis:entry>
         <oasis:entry colname="col2">85.4412</oasis:entry>
         <oasis:entry colname="col3">22.732</oasis:entry>
         <oasis:entry colname="col4">3.759</oasis:entry>
         <oasis:entry colname="col5">0.000</oasis:entry>
         <oasis:entry colname="col6">40.167</oasis:entry>
         <oasis:entry colname="col7">130.715</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">elev</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.0026</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">0.003</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M207" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.810</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">0.420</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M208" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.009</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7">0.004</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="App1.Ch1.S2.SS2">
  <label>B2</label><title>Figures</title>

      <?xmltex \floatpos{h!}?><fig id="App1.Ch1.S2.F8"><?xmltex \currentcnt{B1}?><?xmltex \def\figurename{Figure}?><label>Figure B1</label><caption><p id="d1e3909">Scatterplot of the <inline-formula><mml:math id="M209" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> predicted by the linear regression model trained with all of the samples (<inline-formula><mml:math id="M210" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis) versus the observed measurements (<inline-formula><mml:math id="M211" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis).</p></caption>
          <?xmltex \hack{\hsize\textwidth}?>
          <?xmltex \igopts{width=227.622047pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021-f08.png"/>

        </fig>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{h!}?><fig id="App1.Ch1.S2.F9"><?xmltex \currentcnt{B2}?><?xmltex \def\figurename{Figure}?><label>Figure B2</label><caption><p id="d1e3948">Scatterplot of the <inline-formula><mml:math id="M212" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values simulated with the InVEST urban cooling model (<inline-formula><mml:math id="M213" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis) versus the observed measurements (<inline-formula><mml:math id="M214" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis).</p></caption>
          <?xmltex \hack{\hsize\textwidth}?>
          <?xmltex \igopts{width=227.622047pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/14/3521/2021/gmd-14-3521-2021-f09.png"/>

        </fig>

<?xmltex \hack{\clearpage}?>
</sec>
</app>
  </app-group><notes notes-type="codeavailability"><title>Code availability</title>

      <p id="d1e3991">The code materials used in this article are available at <ext-link xlink:href="https://doi.org/10.5281/zenodo.4916285" ext-link-type="DOI">10.5281/zenodo.4916285</ext-link> <xref ref-type="bibr" rid="bib1.bibx12" id="paren.60"/> and are maintained in a GitHub repository at <uri>https://github.com/martibosch/lausanne-heat-islands</uri> (last access: 22 December 2020).</p>

      <p id="d1e4003">The code for the spatial regression of air temperature from satellite data is available as a Jupyter Notebook (IPYNB) at <uri>https://github.com/martibosch/lausanne-heat-islands/blob/gmd-published/notebooks/spatial-regression.ipynb</uri> (last access: 9 June 2021).</p>

      <p id="d1e4009">The code of the spatial simulation of air temperature with the InVEST urban cooling model is available as a Jupyter Notebook (IPYNB) at <uri>https://github.com/martibosch/lausanne-heat-islands/blob/gmd-published/notebooks/invest-urban-cooling-model.ipynb</uri> (last access: 9 June 2021).</p>

      <p id="d1e4015">The code used for the comparison of the spatial regression and simulation of air temperature is available as a Jupyter Notebook (IPYNB) at <uri>https://github.com/martibosch/lausanne-heat-islands/blob/gmd-published/notebooks/comparison.ipynb</uri> (last access: 9 June 2021).</p>
  </notes><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e4024">The source files for the biophysical table, list of landsat tiles, reference evapotranspiration, station locations and station temperature measurements for the reference dates can be found in a dedicated archive at <uri>https://zenodo.org/record/4384675</uri> (last access: 13 July 2020). The reference evapotranspiration raster is obtained using the minimum, average and maximum temperature datasets of the copyrighted Spatial Climate Analyses of MeteoSwiss (Frei, 2014). The temperature observations correspond to monitoring stations operated by Agrometeo, the Federal Roads Office (ASTRA), the Federal Office for the Environment (BAFU), the general directorate for the environment of the Canton of Vaud (DGE), and the Federal Institute of Forest, Snow and Landscape Research (WSL) (Rebetez et al., 2018).</p>

      <p id="d1e4030">The source files for the spatial extent of the study area and the respective land use and/or land cover raster map can be found at a dedicated archive at <ext-link xlink:href="https://doi.org/10.5281/zenodo.4311544" ext-link-type="DOI">10.5281/zenodo.4311544</ext-link> (last access: 15 July 2020; <xref ref-type="bibr" rid="bib1.bibx10" id="altparen.61"/>). The obtained extent is based on the official cadastral survey of the canton of Vaud whose exclusive owner is the Canton of Vaud, with the use conditions disclosed in the norm OIT 8401.</p>

      <p id="d1e4039">The tree canopy map can be found at a dedicated archive at <ext-link xlink:href="https://doi.org/10.5281/zenodo.4310112" ext-link-type="DOI">10.5281/zenodo.4310112</ext-link> <xref ref-type="bibr" rid="bib1.bibx11" id="paren.62"/>. The map has been obtained based on the SWISSIMAGE 2016 aerial imagery dataset.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e4051">MB and ML designed the study and conducted the analysis with technical input from PH and RPR and overall supervision from JC and SJ. MB developed the code and wrote the paper. All authors provided comments and contributed to the final version of the paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e4057">The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e4063">This research has been supported by the École Polytechnique Fédérale de Lausanne (EPFL). The authors gratefully thank Yves Kazemi and Martin Schlaepfer for their help with the study design, Rémi Jaligot for his careful review of the paper before submission, Bethanna Jackson for editing the article as well as Daniel Rodrigues and Rubianca Benavidez for reviewing it.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e4068">This research has been supported by the École Polytechnique Fédérale de Lausanne (EPFL).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e4074">This paper was edited by Bethanna Jackson and reviewed by Daniel Rodrigues and Rubianca Benavidez.</p>
  </notes><ref-list>
    <title>References</title>

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    <!--<article-title-html>A spatially explicit approach to simulate urban heat mitigation with InVEST (v3.8.0)</article-title-html>
<abstract-html><p>Mitigating urban heat islands has become an important objective for many cities experiencing heat waves.
Despite notable progress, the spatial relationship between land use and/or land cover patterns and the distribution of air temperature remains poorly understood.
This article presents a reusable computational workflow to simulate the spatial distribution of air temperature in urban areas from their land use and/or land cover data.
The approach employs the InVEST urban cooling model, which estimates the cooling capacity of the urban fabric based on three biophysical mechanisms: tree shade, evapotranspiration and albedo.
An automated procedure is proposed to calibrate the parameters of the model to best fit air temperature observations from  monitoring stations.
In a case study in Lausanne, Switzerland, spatial estimates of air temperature obtained with the calibrated model show that the urban cooling model outperforms spatial regressions based on satellite data. This represents two major advances in urban heat island modeling.
First, unlike in black-box approaches, the calibrated parameters of the urban cooling model can be interpreted in terms of the physical mechanisms that they represent; therefore, they can help promote an understanding of how urban heat islands emerge in a particular context.
Second, the urban cooling model requires only land use and/or land cover and reference temperature data and can, therefore, be used to evaluate synthetic scenarios such as master plans, urbanization prospects and climate scenarios.
The proposed approach provides valuable insights into the emergence of urban heat islands which can serve to inform urban planning and assist the design of heat mitigation policies.</p></abstract-html>
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