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  <front>
    <journal-meta>
<journal-id journal-id-type="publisher">ACP</journal-id>
<journal-title-group>
<journal-title>Atmospheric Chemistry and Physics</journal-title>
<abbrev-journal-title abbrev-type="publisher">ACP</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Atmos. Chem. Phys.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1680-7324</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/acp-17-9067-2017</article-id><title-group><article-title>A wedge strategy for mitigation of urban warming<?xmltex \hack{\break}?> in future climate scenarios</article-title>
      </title-group><?xmltex \runningtitle{A wedge strategy for mitigation of urban warming in future climate scenarios}?><?xmltex \runningauthor{L. Zhao et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2 aff3">
          <name><surname>Zhao</surname><given-names>Lei</given-names></name>
          <email>lei.zhao@princeton.edu</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff3">
          <name><surname>Lee</surname><given-names>Xuhui</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Schultz</surname><given-names>Natalie M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-6269-2194</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Program in Science, Technology, and Environmental Policy (STEP),
Woodrow Wilson School of Public and International Affairs, Princeton
University, Princeton, New Jersey 08540, USA</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Yale-NUIST Center on Atmospheric Environment, Nanjing University of
Information Science and Technology, Nanjing, 210044, China</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>School of Forestry and Environmental Studies, Yale University, New
Haven, Connecticut 06511, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Lei Zhao (lei.zhao@princeton.edu)</corresp></author-notes><pub-date><day>27</day><month>July</month><year>2017</year></pub-date>
      
      <volume>17</volume>
      <issue>14</issue>
      <fpage>9067</fpage><lpage>9080</lpage>
      <history>
        <date date-type="received"><day>23</day><month>November</month><year>2016</year></date>
           <date date-type="rev-request"><day>16</day><month>January</month><year>2017</year></date>
           <date date-type="rev-recd"><day>3</day><month>May</month><year>2017</year></date>
           <date date-type="accepted"><day>28</day><month>June</month><year>2017</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://acp.copernicus.org/articles/17/9067/2017/acp-17-9067-2017.html">This article is available from https://acp.copernicus.org/articles/17/9067/2017/acp-17-9067-2017.html</self-uri>
<self-uri xlink:href="https://acp.copernicus.org/articles/17/9067/2017/acp-17-9067-2017.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/17/9067/2017/acp-17-9067-2017.pdf</self-uri>


      <abstract>
    <p>Heat stress is one of the most severe climate threats to human society in a future warmer world. The situation is further exacerbated
in urban areas by urban heat islands (UHIs). Because the majority of
world's population is projected to live in cities, there is a pressing need
to find effective solutions for the heat stress problem. We use a climate
model to investigate the effectiveness of various urban heat mitigation
strategies: cool roofs, street vegetation, green roofs, and reflective
pavement. Our results show that by adopting highly reflective roofs, almost
all the cities in the United States and southern Canada are transformed into
“white oases” – cold islands caused by cool roofs at midday, with an
average oasis effect of <inline-formula><mml:math id="M1" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>3.4 K in the summer for the period 2071–2100,
which offsets approximately 80 % of the greenhouse gas (GHG) warming
projected for the same period under the RCP4.5 scenario. A UHI mitigation
wedge consisting of cool roofs, street vegetation, and reflective pavement has
the potential to eliminate the daytime UHI plus the GHG warming.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>Heat stress associated with climate change is projected to cause a
substantial increase in human mortality (Patz et al., 2005; Huang et al.,
2011) and a large reduction in workplace productivity (Dunne et al., 2013;
Zander et al., 2015). These risks are further amplified for urban residents
because of the urban heat island (UHI) effect, a phenomenon in which surface
temperatures are higher in urban areas than in surrounding rural areas
(Grimmond, 2007). Because more than 50 % of the world's population
currently lives in cities, and that number is projected to increase to
70 % by year 2050 (Heilig, 2012), there is a pressing need to find
effective solutions for urban heat stress. In recent years, urban climate
agendas have broadened beyond carbon management, which brings marginal heat
relief to urban residents (Revi et al., 2014), to include urban climate adaptation.
It is now recognized that in addition to the traditional emphasis on
preparedness to cope with heat stress (Stone et al., 2012), urban adaptation
should include active modifications to the urban landscape to reduce urban
temperatures (Rizwan et al., 2008; Castleton et al., 2010; Santamouris,
2013; Bowler et al., 2010; Jacobson, 2009).</p>
      <p>Field experiments have demonstrated the cooling benefits of street
vegetation (Shashua-Bar and Hoffman, 2000; Mackey et al., 2012), bright
pavement (Rosenfeld et al., 1995; Mackey et al., 2012), green roofs (Jim and
Peng, 2012), solar roofs (Dominguez et al., 2011), and cool roofs (Ismail et
al., 2011) at the scale of individual buildings. Specifically, street
vegetation and green roofs provide localized cooling through enhanced
evaporation, and for street vegetation by increasing surface roughness and
therefore convection efficiency. Bright pavement and cool roofs, both
characterized by a higher albedo than traditional materials, cool the urban
environment by reflecting a higher portion of solar radiation away from the
surface. Solar roofs produce localized cooling through their conversion of
solar energy to electricity.</p>
      <p>Although it is financially challenging to conduct field experiments on these
methods at the city scale, modeling studies have evaluated the potential of
citywide implementation of these methods on temperature reduction. A
majority of the modeling studies deploy a mesoscale weather forecast model,
such as the Weather Research Forecasting Model (WRF; Skamarock et al.,
2008), and model simulations are performed for a business-as-usual case and
for one or more mitigation strategies, including tree planting (Stone et
al., 2013, 2014), green roof (Li et al., 2014; Stone et al.,
2014), cool roof (Georgescu et al., 2014), and rooftop solar panels
(Salamanca et al., 2016).</p>
      <p>The high computational demand of mesoscale modeling limits long-term and
large-scale simulations, with most of these studies restricting their
analysis to high-impact heatwaves in a single city (Rosenzweig et al., 2009;
Li et al., 2014). Recently, studies using a mesoscale modeling approach have
begun to scale up the geographic scope of analysis, comparing and evaluating
urban heat mitigation methods across multiple (up to 3) cities in
contrasting regional climates (Stone et al., 2014; Vargo et al., 2016) and
even over the continental United States (Georgescu et al., 2014).</p>
      <p>A second modeling strategy, using subgrid output from a global climate
model (GCM), overcomes the computational constraints of mesoscale models, allowing
for the continental or global-scale analysis of UHI and heat mitigation
strategies over climatological timescales (Oleson et al., 2010c; Hu et al.,
2016; Jacobson and Ten Hoeve, 2012). Although climate models cannot resolve
local-scale processes, such as advection between adjacent urban and rural
land in the same grid cell, they can capture the urban effects on the
large-scale dynamics of the atmosphere. Additionally, GCMs can simulate the
interactions of greenhouse gas (GHG)-induced warming and the biophysical drivers of urban
heat islands and heat mitigation methods. As urban heat mitigation is
becoming an integral part of the climate adaptation agenda, GCMs can provide
useful knowledge to city planners about the effectiveness of various
mitigation strategies across a range of climate conditions and under
different climate scenarios.</p>
      <p>In this study, we use an urban climate model to assess the effectiveness of
urban climate mitigation methods in future warmer climates. Our specific
objectives are to (1) investigate the urban heat island intensity under
current and future climate scenarios for three climate regions in the US
and southern Canada, (2) quantify the effectiveness of several mitigation
strategies (street vegetation, green roof, cool roof and bright pavement) on
offsetting urban warming, and (3) estimate aggregated temperature reduction
potential of these strategies using a UHI mitigation wedge approach. Our
research complements the studies by Georgescu et al. (2014), Rosenzweig et
al. (2009), and Stone et al. (2014) in that we are also interested in
quantifying the effectiveness of multiple UHI mitigation strategies, both
individually and collectively, across a diverse range of climate conditions.
Here, we expand the analysis to several climate scenarios and a large number
of cities (57 cities) to understand the interactions between the UHI
biophysical drivers, GHG-induced warming, and influence of local background
climate. We propose a new method to assess the mitigation strategies, which
is based on a theoretical understanding of the surface energy balance and is
unconstrained by computational demand.</p>
</sec>
<sec id="Ch1.S2">
  <title>Materials and methods</title>
      <p>We used a global climate model to simulate the UHI and to quantify the
cooling potential of urban heat mitigation strategies: cool roofs, street
vegetation, green roofs, and reflective pavement. As will be discussed in
more detail in the following subsections, the simplified representation of
urban areas in the model does not directly allow for online assessment of
each of the mitigation strategies. Therefore, in addition to the online
simulations to assess the mitigation potential of cool roofs, we used an
offline attribution method to quantify the mitigation potential of green
roofs and reflective pavement as well as a two-member interpolation method to
quantify the cooling potential of street vegetation (Table 1) for three
climate scenarios. The offline calculations are based on the diagnostic
variables of the surface energy balance produced by the model.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p>The simulations run and the methods used to assess the temperature
mitigation strategies. The online simulation method calculated the mitigation
potential of cool roofs as the difference between the WHT and CTR simulations
(WHT – CTR). The offline attribution and two-endmember interpolation
methods used diagnostic data from the CTR simulations.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.98}[.98]?><oasis:tgroup cols="8">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:colspec colnum="5" colname="col5" align="left"/>
     <oasis:colspec colnum="6" colname="col6" align="left"/>
     <oasis:colspec colnum="7" colname="col7" align="left"/>
     <oasis:colspec colnum="8" colname="col8" align="left"/>
     <oasis:thead>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="1">Model simulations</oasis:entry>

         <oasis:entry rowsep="1" namest="col2" nameend="col3" align="center">Albedo </oasis:entry>

         <oasis:entry colname="col4"/>

         <oasis:entry rowsep="1" namest="col5" nameend="col8" align="center">Mitigation strategy method </oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">CTR</oasis:entry>

         <oasis:entry colname="col3">WHT</oasis:entry>

         <oasis:entry colname="col4"/>

         <oasis:entry colname="col5">Cool roofs</oasis:entry>

         <oasis:entry colname="col6">Street vegetation</oasis:entry>

         <oasis:entry colname="col7">Green roofs</oasis:entry>

         <oasis:entry colname="col8">Reflective pavement</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

         <oasis:entry colname="col1">Current (1972–2004)</oasis:entry>

         <oasis:entry colname="col2">default</oasis:entry>

         <oasis:entry colname="col3">0.88</oasis:entry>

         <oasis:entry colname="col4"/>

         <oasis:entry colname="col5">online simulations,</oasis:entry>

         <oasis:entry colname="col6">two-endmember</oasis:entry>

         <oasis:entry colname="col7">offline attribution</oasis:entry>

         <oasis:entry colname="col8">offline attribution</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">RCP 4.5 (2005–2100)</oasis:entry>

         <oasis:entry colname="col2">(0.18 – 0.37)</oasis:entry>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4"/>

         <oasis:entry colname="col5">offline attribution</oasis:entry>

         <oasis:entry colname="col6">interpolation</oasis:entry>

         <oasis:entry colname="col7"/>

         <oasis:entry colname="col8"/>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">RCP 8.5 (2005–2100)</oasis:entry>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4"/>

         <oasis:entry colname="col5"/>

         <oasis:entry colname="col6"/>

         <oasis:entry colname="col7"/>

         <oasis:entry colname="col8"/>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

<sec id="Ch1.S2.SS1">
  <title>Climate model and simulations</title>
      <p>We used the Community Earth System Model (CESM; Hurrell et al., 2013) to
simulate the UHI for cities in the United States and southern Canada. The
land surface processes are represented by the Community Land Model (CLM,
version 4.0), which is the land component of CESM (Oleson et al., 2010b). In CLM 4.0,
the land surface heterogeneity is represented as a nested hierarchy of
subgrid levels. The model grid cell consists of up to five land units:
vegetated land, glacier, wetland, urban, and lake, all of which are driven
by the same atmospheric forcing. In the CESM architecture, fluxes and state
variables are computed at each land unit level and then area-weighted to
grid cell means before being passed to the atmosphere model. We use data
from the urban and vegetated land units in this analysis to represent urban
and rural land cover types, respectively. The urban land unit is represented
in a conceptual canyon structure that consists of a roof, sunlit wall, shaded
wall, and pervious (bare soil) and impervious (road, sidewalk, and parking
lot) ground (Oleson et al., 2010a). The thermal (such as heat capacity and
thermal conductivity), radiative (such as albedo and emissivity), and
morphological (such as height-to-width ratio, roof areal fraction, average
building height, and pervious ground fraction) characteristics of these
canyon components are provided by Jackson et al. (2010) for each grid cell.
The vegetated land unit is comprised of up to 15 natural plant functional
types and bare soil.</p>
      <p>The CLM was run under three climate scenarios: current climate,
Representative Concentration Pathway (RCP) 4.5, and RCP8.5. These three
simulations comprise the control (CTR) group of simulations, where all the
urban parameters were kept as the default values prescribed by the model. For
the current climate, the model was run for 33 years after a 60-year spin-up,
driven by a reconstructed climatology from 1972 to 2004 (Qian et al., 2006).
For the two future scenarios, the model was forced by atmospheric outputs
from fully coupled runs of the CESM and run for 96 years from 2005 to 2100
after a 600 year spin-up. Dynamic land surface input data corresponding to
each future scenario are used in the simulations. It should be noted here
that although the vegetated land unit changes dynamically in the climate
scenarios, the urban land is kept fixed in the default configuration of the
current version of CESM. This model setup is a shortcut to the fully coupled
mode and can be considered as a simplified retrieval of the surface climate
variables from the fully coupled runs. The results should be nearly identical
to those obtained from the coupled simulations because the impacts of
large-scale feedbacks represented in a coupled CESM, such as large-scale
dynamics and ocean–air feedbacks, are preserved by the atmospheric variables.
All the simulations were run at a horizontal resolution of <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">0.9</mml:mn><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">1.25</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> (latitude <inline-formula><mml:math id="M3" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> longitude).</p>
      <p>This model configuration cannot simulate the dynamic impact of changes to
the urban land on the atmosphere. However, because the urban land unit in
CLM comprises only a small areal fraction of each grid cell, changes in
urban temperature would lead to negligible changes in grid cell mean
temperature. Therefore, the dynamic feedbacks between changes in urban land
and the atmosphere are negligible. Studies that fully couple CLM to the
atmosphere conclude that modification of the urban albedo has negligible
effects on the regional and global climate (Hu et al., 2016; Zhang et al.,
2016).</p>
      <p>We used 33 years (1972–2004) of data in the current climate and
the last 30 years (2071–2100) of data in the two future scenarios to
compute climatological mean temperatures and the UHI intensity. We analyzed
the UHI intensity for 57 selected cities, representing three Köppen–Geiger
climate zones: temperate climate (24 cities, eastern and southern US),
continental climate (20 cities, northern US and southern Canada), and dry
climate (13 cities, arid and semiarid western US). These cities comprise
less than 20 % of the grid cell area. Model outputs at 13:00 and 01:00
local time were used to represent daytime and nighttime conditions,
respectively. These two times were selected for two reasons. First,
they are close to the times of the daily maximum and minimum temperature, thus
giving a better representation of the diurnal range of the UHI intensity
(<inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>). Second, the performance of both CLM and our offline
attribution method in estimating <inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> was validated against MODIS
observations at these two times (close to the MODIS overpassing times) in a
previous study (Zhao et al., 2014). Our analysis was restricted to summer
(June–August) results.</p>
      <p>In this analysis, we use the surface temperature instead of the
screen-height air temperature in our assessment of UHI and the temperature
mitigation potential of cooling strategies. In other words, the UHI
intensity is defined as the surface UHI, which is the difference in radiative surface
temperature between urban and nonurban subgrid land units in the grid cell
where the city is located. This is different from the air UHI which is
defined using screen-height air temperature. These two UHI definitions
differ in a variety of aspects. First, the air UHI can be affected by the
local air and landscape conditions and thus is susceptible to the
inhomogeneous urban landscape. The surface UHI, instead, is a spatial
average. Although the surface temperature does not necessarily match the
human experience of warmth while walking across the rural–urban boundary, it
is more stable as a metric of the city-scale microclimate and can be
directly validated against satellite observations over large areas,
especially when compared across different cities over diverse local climate
conditions. Second, the air UHI is more tightly related to heat stress and
heat exposure assessment (Oleson et al., 2015) than surface UHI. However,
the surface UHI has a firm theoretical basis that underpins the wedge method
for assessment of multiple mitigation strategies. It has been shown from the
surface energy balance principle that the overall surface UHI can be
estimated by linear supposition of different biophysical contributions (Zhao
et al., 2014). The linear supposition property, that the overall temperature
reduction due to simultaneous implementation of several mitigation methods
can be approximated by the sum of cooling benefits from implementation of
these methods one at a time, is the underlying basis for the UHI mitigation
wedge approach used in this study. In addition, this linear supposition
seems to be a robust property for the air UHI as well. We will present
evidence from published UHI mitigation studies using the air UHI (Taha et
al., 1997; Georgescu et al., 2014; Stone et al., 2014; Salamanca et al.,
2016).</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>Offline UHI attribution</title>
      <p>Defining UHI by surface temperature allows us to estimate the contribution
of different biophysical mechanisms to the overall surface UHI from surface
energy balance principles (Zhao et al., 2014). In addition to <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>,
the model also produces diagnostic variables of the surface energy balance.
In this analysis, these diagnostic data served two purposes. First, they
were used to attribute the UHI (<inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>) to contributions from changes in
surface biophysical parameters including albedo, evaporation, convection
efficiency, heat storage, and anthropogenic heat addition (Zhao et al.,
2014). This offline attribution analysis serves to examine the linear
supposition of different biophysical contributions, which is the basis
underlying the UHI mitigation wedge approach used in this study. Second,
they allowed us to estimate the cooling benefit of two of the four UHI
mitigation methods (green roof and reflective pavement; details described
below).</p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Temperature mitigation strategies</title>
<sec id="Ch1.S2.SS3.SSS1">
  <title>Cool roofs</title>
      <p>To investigate the mitigation potential of cool roofs, an additional set of
simulations was conducted for each of the three climate scenarios (including
current climate, RCP 4.5, and RCP 8.5). In this group of simulations (white roofs, here abbreviated as WHT),
the roof albedo was increased to 0.88, the value of the US EPA Energy Star
Solareflect coating material after 3 years of wear and aging (Georgescu
et al., 2014). This value is slightly lower than the initial albedo of 0.89,
indicating the material's high capability of maintaining high solar
reflectance
(<uri>https://downloads.energystar.gov/bi/qplist/roofs_prod_list.pdf?8ddd-02cf</uri>).
The cooling benefit of the cool roofs was determined by comparing the urban
surface temperature in the WHT simulation with that in the CTR simulation,
where the roof albedo was kept as the default value (0.18–0.37), under each
climate scenario.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><caption><p>Attribution of summer mean UHI intensity during 2071–2100
under the RCP 4.5 scenario for the control (CTR) run. <bold>(a, b, c, d)</bold> daytime; <bold>(e, f, g, h)</bold> nighttime. <bold>(a, e)</bold> dry climate; <bold>(b, f)</bold> continental climate; <bold>(c, g)</bold>
temperate climate; <bold>(d, h)</bold> all selected cities. The radiative forcing term
results mostly from albedo differences between urban and rural land in the
daytime and from small differences in surface emissivity at night. Error bars
are <inline-formula><mml:math id="M8" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>1 standard error.</p></caption>
            <?xmltex \igopts{width=298.753937pt}?><graphic xlink:href="https://acp.copernicus.org/articles/17/9067/2017/acp-17-9067-2017-f01.pdf"/>

          </fig>

      <p>The morphological properties were kept unchanged in the CTR and WHT
simulations. Of the 57 selected cities, the average prescribed roof areal
fraction in CLM 4.0 is 48.8 %, the average default roof albedo is 0.29,
and the average citywide albedo is 0.18. After the deployment of white
roofs, the average citywide albedo is increased to 0.47.</p>
      <p>To help the reader visualize the changes brought by the cool roofs to the
urban landscape, we created two animations using a 3-D point cloud and image
mosaic dataset acquired by an unmanned aerial vehicle over an urban
neighborhood in Switzerland (<uri>http://www.sensefly.com</uri>). In Animation
Movie S1 in the Supplement, the roof pixels retain their natural reflectance
values. In Animation Movie S2, these pixels were replaced with saturation
reflectance values to simulate the Solareflect coating material.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS2">
  <title>Street vegetation</title>
      <p>It is not possible to directly evaluate the cooling benefit of street
vegetation with CLM because vegetation is not explicitly represented in the
urban land unit in CLM. Here, we used a simple two-endmember interpolation
method to calculate the surface temperature change <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> associated
with street vegetation as
              <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M10" display="block"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mi>V</mml:mi><mml:mo>×</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M11" display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula> is the areal fraction of street vegetation in the urban land unit
and <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the UHI intensity from the CTR run. A negative
<inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> indicates cooling effect, and vice versa. This simple linear
method satisfies the two endmembers: at 0 % vegetation, there is no
temperature reduction, and the UHI intensity is the original <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>; at
100 % vegetation, the urban land would be completely converted to the
rural landscape, and thus the cooling benefit should totally offset the
original <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>. The calculation assumes that street vegetation consists
of native plant species having the same species compositions in the adjacent
rural land. In CLM, the average tree-to-grass ratios in the surrounding
rural land of selected cities are 1.8, 2.5, and 1.2 for the temperate,
continental, and dry climate zones, respectively. These numbers are in line
with the real urban forest-to-grass ratio estimated using remote sensing
techniques (Myeong et al., 2001; Nowak and Greenfield, 2012). For each of
the selected cities, <inline-formula><mml:math id="M16" display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula> is the areal fraction of pervious surface in the
urban land unit prescribed by the model. The average <inline-formula><mml:math id="M17" display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula> value for these
cities is 30 %.</p>
      <p>This method yields the net cooling of all the biophysical effects associated
with street vegetation, including changes in albedo, convection efficiency,
evaporation, and storage. It should be noted here that this method may
slightly overestimate the vegetation cooling benefit for two reasons. First,
the UHIs from the CTR simulations also include anthropogenic heat
contribution. According to the offline attribution results, the
anthropogenic heat contribution is about 20 % (Fig. 1). Second, street
vegetation is inherently not identical to its rural counterparts due to
the radiative trapping by urban canyons via the “canyon effect” (Wang,
2014; Ryu et al., 2016). Therefore, the same amount of vegetation inside urban
canyons may not induce as much cooling as it would in the adjacent rural
land.
<?xmltex \hack{\newpage}?></p>
</sec>
<sec id="Ch1.S2.SS3.SSS3">
  <title>Green roofs</title>
      <p>We calculated the cooling benefit of green roofs using the diagnostic
surface energy balance data as
              <disp-formula id="Ch1.E2" content-type="numbered"><mml:math id="M18" display="block"><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{9.2}{9.2}\selectfont$\displaystyle}?><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi>f</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced close=")" open="("><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>a</mml:mi></mml:mfenced><mml:msub><mml:mi>K</mml:mi><mml:mo>↓</mml:mo></mml:msub><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow><mml:mrow><mml:msup><mml:mfenced open="(" close=")"><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi>f</mml:mi></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced open="(" close=")"><mml:msubsup><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi><mml:mo>∗</mml:mo></mml:msubsup><mml:mo>-</mml:mo><mml:msub><mml:mi>Q</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>Q</mml:mi><mml:mi mathvariant="normal">AH</mml:mi></mml:msub></mml:mfenced><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>f</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:math></disp-formula>
            with

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M19" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E3"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msubsup><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi><mml:mo>∗</mml:mo></mml:msubsup><mml:mo>=</mml:mo><mml:mfenced open="(" close=")"><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi>a</mml:mi></mml:mfenced><mml:msub><mml:mi>K</mml:mi><mml:mo>↓</mml:mo></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mo>↓</mml:mo></mml:msub><mml:mo>-</mml:mo><mml:mfenced close=")" open="("><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="italic">ε</mml:mi></mml:mfenced><mml:msub><mml:mi>L</mml:mi><mml:mo>↓</mml:mo></mml:msub><mml:mo>-</mml:mo><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="italic">σ</mml:mi><mml:msubsup><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msubsup><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E4"><mml:mtd/><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>f</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mi>p</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced open="(" close=")"><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi mathvariant="italic">β</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E5"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>f</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mi>p</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="italic">β</mml:mi></mml:mrow><mml:mrow><mml:msup><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where <inline-formula><mml:math id="M20" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> is the surface temperature, <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the local climate sensitivity
(<inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="italic">σ</mml:mi><mml:msup><mml:mi>T</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M23" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> is the energy redistribution
factor, <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:msubsup><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi><mml:mo>∗</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> is the apparent net radiation, <inline-formula><mml:math id="M25" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula> is the air density,
<inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>p</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the specific heat of air at constant pressure, <inline-formula><mml:math id="M27" 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 aerodynamic
resistance to heat diffusion, <inline-formula><mml:math id="M28" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula> is the Bowen ratio, <inline-formula><mml:math id="M29" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> is the surface
albedo, <inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mo>↓</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula> is the incoming solar radiation, <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mo>↓</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula> is the
incoming longwave radiation, <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the stored heat, <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msub><mml:mi>Q</mml:mi><mml:mi mathvariant="normal">AH</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the
anthropogenic heat release, <inline-formula><mml:math id="M34" display="inline"><mml:mi mathvariant="italic">ε</mml:mi></mml:math></inline-formula> is the surface emissivity, <inline-formula><mml:math id="M35" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>
is the Stefan–Boltzmann constant, and <inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the air temperature at the blending
height. Equation (2) is obtained by differentiating the surface temperature
solution given in Lee et al. (2011).</p>
      <p>The Bowen ratio of green roofs was the average Bowen ratio value for
grassland calculated at the subgrid level by the CLM for the grass plant
functional type with its own soil column (Schultz et al., 2016). This
implies that the water-conserving native grass is used for green roofs. The
citywide Bowen ratio change was the area-weighted average of the green roof
Bowen ratio and the Bowen ratio of other surface components in the urban
land unit. The Bowen ratio change (<inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="italic">β</mml:mi></mml:mrow></mml:math></inline-formula>) was the difference in
Bowen ratio between urban land units with and without green roof
installation.</p>
      <p>The green roofs were assigned the average warm-season grassland albedo value
of 0.20 (Bonan, 2008). The citywide albedo was the area-weighted average of
the green roof albedo and the albedo of other surface components in the
urban land unit. The albedo change (<inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:math></inline-formula>) was the difference
between the city with and without green roof installation. The average
<inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:math></inline-formula> of the 57 cities was 0.01.</p>
      <p>The change in surface roughness induced by green roofs is minimal and thus
was omitted in this analysis.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS4">
  <title>Reflective pavement</title>
      <p>The same offline method was used to calculate the effect of reflective
pavement as
              <disp-formula id="Ch1.E6" content-type="numbered"><mml:math id="M40" display="block"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi>f</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced open="(" close=")"><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>a</mml:mi></mml:mfenced><mml:msub><mml:mi>K</mml:mi><mml:mo>↓</mml:mo></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:math></inline-formula> is the citywide albedo change associated with the use
of reflective pavement. Only the impervious surface in each urban land unit is
considered for conversion into reflective pavement. We increased the pavement
albedo from the default value of 0.13 to 0.25 as recommended by Akbari et
al. (2012). The areal fraction of pavement was on average 20.2 %. The
average citywide albedo of the 57 cities was increased by 0.04. In order to
further confirm the validity of the offline method, we conducted another
side simulation to directly simulate the cooling benefits of reflective
pavements under current climate. In this simulation, the albedos of
impervious surface in each urban land unit of the 57 cities were raised to
0.25.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Results and discussion</title>
<sec id="Ch1.S3.SS1">
  <title>Offline UHI diagnostics</title>
      <p>An example of the attribution result is given in Fig. 1 for the period
2071–2100 under RCP4.5. The offline <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> (the sum of the component
contributions) shows good agreement with the online <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> (the surface
temperature difference between the urban and the vegetation land unit
computed directly by the model). The offline <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> is slightly lower
than the online <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> because high-order terms are ignored in the
linearization of the surface long-wave radiation term of the energy balance
equation, and nonlinear interactions among the component contributions are
omitted (Zhao et al., 2014). Good agreement was also obtained for the
current climate conditions (Zhao et al., 2014), implying that nonlinear
interactions among the various UHI contributors are small.</p>
      <p>This linear supposition property of different biophysical contributions is
the theoretical basis underpinning the wedge approach that we use to
quantify the overall effectiveness of multiple UHI mitigation strategies.
Different mitigation strategies affect the urban surface temperature through
these biophysical contributions. Combining different UHI abatement actions
is actually adding up the perturbed biophysical contributions in the process
level. Linear supposition of various biophysical contributions states that
different mitigation strategies add up linearly as well. Therefore, good
agreement between online <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> and offline <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> (Fig. 1)
supports the idea that different UHI mitigation strategies, as long as their
deployments are not mutually exclusive, act nearly linearly when quantified
collectively.<?xmltex \hack{\newpage}?></p>
      <p>The validity of our offline method is further supported by the excellent
agreement between the online and offline <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> for a total of 18
combinations of climate zone, roof choice, and climate scenarios (Fig. 2).
In the offline calculation, changes in the citywide albedo from CTR to WHT
were computed from the modeled reflected solar radiation and the incident
solar radiation in the urban land unit. The citywide albedo changes were
then substituted into Eq. (6) (the offline method for cool roof is
equivalent to the method for reflective pavement). Other component
contribution terms were kept unchanged in the offline UHI attribution
equation, because cool roofs only alter the radiation contribution to
<inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> in the surface energy balance. The <inline-formula><mml:math id="M50" 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> value of the linear
correlation between the two sets of <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> calculations is 0.99 and the
mean bias (offline <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> minus online <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>) is 0.1 K. Similarly,
the online simulated and offline estimated <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> for reflective
pavements also show an excellent agreement with the <inline-formula><mml:math id="M55" 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> value of 0.98
and the mean difference of 0.3 K.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><caption><p>Scatter plot between the daytime UHI intensity computed
online with the CLM and that calculated offline using the surface energy
balance diagnostic data. Filled and open symbols denote results from control
(CTR) and white roof (WHT) simulations, respectively. Red, green, and blue
colors denote dry (dry), continental (cont) and temperate (temp) climate
regions, respectively. Circle, triangle, and square symbols denote current
climate (cur), RCP4.5 (RCP45), and RCP8.5 (RCP85) scenarios, respectively.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/17/9067/2017/acp-17-9067-2017-f02.pdf"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS2">
  <title>Future UHI under RCP scenarios</title>
      <p>We find strong urban climate change signals under both RCP scenarios. Near
the end of this century, the average summer daytime <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> is projected
to increase by 0.9 <inline-formula><mml:math id="M57" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2 K (mean <inline-formula><mml:math id="M58" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1 standard error) and the
nighttime <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> by 1.5 <inline-formula><mml:math id="M60" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2 K under the RCP4.5 scenario
(Fig. 3a and b). This is in addition to the GHG-induced summer surface
temperature increase of 4.2 and 2.6 K from the current temperature of
32.7 and 18.0 <inline-formula><mml:math id="M61" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C in the daytime and nighttime,
respectively, for years 2071–2100. The increase in <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> is partly the
result of higher anthropogenic heat release, primarily from air-conditioning
(AC) energy use to cope with the GHG-induced warming (Table 2; Hu et al.,
2016; Oleson et al., 2011). The contribution of anthropogenic heat to the UHI
intensity in the current climate is 0.4 and 0.02 K in the daytime and
nighttime, respectively, and is increased to 0.8 and 0.7 K, respectively,
in the RCP4.5 scenario. This conclusion is supported by the offline UHI
attribution analysis described by Zhao et al. (2014). The larger increase in
the nighttime <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> than the daytime <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> confirms the
well-established fact that anthropogenic heat is a dominant contributor to
urban warming at night (Oke, 1982).</p>
      <p>In the current climate, the spatial variations of daytime <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> across
the climate zones are controlled by the precipitation regime, being lowest
in the dry climate and highest in the humid temperate climate (Zhao et al.,
2014). This zonation is preserved in the future warmer world (Fig. 3a).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p>Urban heat island intensity from the control (CTR; <bold>a, b</bold>)
and white roof (WHT; <bold>c, d</bold>) simulations. <bold>(a, c)</bold> daytime; <bold>(b, d)</bold> nighttime. Red,
green, and blues bars denote dry, continental, and temperate climate zones,
respectively. Error bars are <inline-formula><mml:math id="M66" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>1 standard error.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/17/9067/2017/acp-17-9067-2017-f03.pdf"/>

        </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><caption><p>The mean anthropogenic heat flux for all the selected
cities and the cities in the three climate zones in the current climate, RCP
4.5, and RCP 8.5 scenarios from both the control (CTR) and the white roof (WHT)
simulations. (Units: W m<inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></p></caption><oasis:table frame="topbot"><oasis:tgroup cols="10">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="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="left"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:colspec colnum="10" colname="col10" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry namest="col1" nameend="col10" align="center">Daytime </oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry rowsep="1" namest="col2" nameend="col5" align="center">CTR </oasis:entry>  
         <oasis:entry colname="col6"/>  
         <oasis:entry rowsep="1" namest="col7" nameend="col10" align="center">WHT </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">Dry</oasis:entry>  
         <oasis:entry colname="col3">Continental</oasis:entry>  
         <oasis:entry colname="col4">Temperate</oasis:entry>  
         <oasis:entry colname="col5">All</oasis:entry>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7">Dry</oasis:entry>  
         <oasis:entry colname="col8">Continental</oasis:entry>  
         <oasis:entry colname="col9">Temperate</oasis:entry>  
         <oasis:entry colname="col10">All</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Current</oasis:entry>  
         <oasis:entry colname="col2">8.9</oasis:entry>  
         <oasis:entry colname="col3">2.3</oasis:entry>  
         <oasis:entry colname="col4">56.8</oasis:entry>  
         <oasis:entry colname="col5">26.8</oasis:entry>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7">1.6</oasis:entry>  
         <oasis:entry colname="col8">1.9</oasis:entry>  
         <oasis:entry colname="col9">18.3</oasis:entry>  
         <oasis:entry colname="col10">8.7</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">RCP 4.5</oasis:entry>  
         <oasis:entry colname="col2">39.3</oasis:entry>  
         <oasis:entry colname="col3">7.9</oasis:entry>  
         <oasis:entry colname="col4">84.1</oasis:entry>  
         <oasis:entry colname="col5">47.1</oasis:entry>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7">11.8</oasis:entry>  
         <oasis:entry colname="col8">4.5</oasis:entry>  
         <oasis:entry colname="col9">39.9</oasis:entry>  
         <oasis:entry colname="col10">21.1</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">RCP 8.5</oasis:entry>  
         <oasis:entry colname="col2">55.1</oasis:entry>  
         <oasis:entry colname="col3">14.6</oasis:entry>  
         <oasis:entry colname="col4">95.2</oasis:entry>  
         <oasis:entry colname="col5">57.8</oasis:entry>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7">21.8</oasis:entry>  
         <oasis:entry colname="col8">7.3</oasis:entry>  
         <oasis:entry colname="col9">60.4</oasis:entry>  
         <oasis:entry colname="col10">32.9</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry namest="col1" nameend="col10" align="center">Nighttime </oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry rowsep="1" namest="col2" nameend="col5" align="center">CTR </oasis:entry>  
         <oasis:entry colname="col6"/>  
         <oasis:entry rowsep="1" namest="col7" nameend="col10" align="center">WHT </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">Dry</oasis:entry>  
         <oasis:entry colname="col3">Continental</oasis:entry>  
         <oasis:entry colname="col4">Temperate</oasis:entry>  
         <oasis:entry colname="col5">All</oasis:entry>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7">Dry</oasis:entry>  
         <oasis:entry colname="col8">Continental</oasis:entry>  
         <oasis:entry colname="col9">Temperate</oasis:entry>  
         <oasis:entry colname="col10">All</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Current</oasis:entry>  
         <oasis:entry colname="col2">5.0</oasis:entry>  
         <oasis:entry colname="col3">3.7</oasis:entry>  
         <oasis:entry colname="col4">16.9</oasis:entry>  
         <oasis:entry colname="col5">9.5</oasis:entry>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7">4.6</oasis:entry>  
         <oasis:entry colname="col8">2.7</oasis:entry>  
         <oasis:entry colname="col9">17.2</oasis:entry>  
         <oasis:entry colname="col10">9.2</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">RCP 4.5</oasis:entry>  
         <oasis:entry colname="col2">14.2</oasis:entry>  
         <oasis:entry colname="col3">6.7</oasis:entry>  
         <oasis:entry colname="col4">33.0</oasis:entry>  
         <oasis:entry colname="col5">19.5</oasis:entry>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7">12.4</oasis:entry>  
         <oasis:entry colname="col8">5.3</oasis:entry>  
         <oasis:entry colname="col9">27.3</oasis:entry>  
         <oasis:entry colname="col10">16.2</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">RCP 8.5</oasis:entry>  
         <oasis:entry colname="col2">23.4</oasis:entry>  
         <oasis:entry colname="col3">11.8</oasis:entry>  
         <oasis:entry colname="col4">47.8</oasis:entry>  
         <oasis:entry colname="col5">29.6</oasis:entry>  
         <oasis:entry colname="col6"/>  
         <oasis:entry colname="col7">21.0</oasis:entry>  
         <oasis:entry colname="col8">9.1</oasis:entry>  
         <oasis:entry colname="col9">41.8</oasis:entry>  
         <oasis:entry colname="col10">25.6</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S3.SS3">
  <title>Effectiveness of the mitigation strategies</title>
<sec id="Ch1.S3.SS3.SSS1">
  <title>Cool roof</title>
      <p>Adoption of the bright, reflective Solareflect roof material transforms
almost all the cities into cold islands in both the current and the future
climates, as indicated by the negative daytime <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> (Figs. 3c and 4c).
In other words, these cities become isolated “white oases” surrounded by a
hot landscape. Under the RCP4.5 scenario, the average daytime surface
temperature reduction in the WHT simulation is 6.5 <inline-formula><mml:math id="M69" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 K for the
period 2071–2100, in reference to the CTR simulation for the same period
(Table S1 in the Supplement). There is a discernible spatial pattern in the
oasis effect, which follows the climatological wetness gradient across the
continent (Fig. 4c). The strongest oases are located in the dry region where
the urban land is 6.2 <inline-formula><mml:math id="M70" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.4 K cooler than the surrounding rural land
(Figs. 3c and 4c). For comparison, the average oasis effect for the cities in
the humid temperate region is <inline-formula><mml:math id="M71" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.6 <inline-formula><mml:math id="M72" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.5 K. The average <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>
of all the cities is <inline-formula><mml:math id="M74" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>3.4 <inline-formula><mml:math id="M75" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 K, enough to offset 80 % of the
GHG warming. The cooling benefit of reflective roofs is similar under the
RCP8.5 scenario (Table S1, Fig. 3c).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p>Maps of summer mean urban heat island intensity during
2071–2100 under the RCP4.5 scenario. <bold>(a)</bold> daytime control (CTR) simulation; <bold>(b)</bold>
nighttime CTR simulation; <bold>(c)</bold> daytime white roof (WHT) simulation; <bold>(d)</bold>
nighttime WHT simulation. Red and blue symbols denote positive and negative
UHIs, respectively.</p></caption>
            <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/17/9067/2017/acp-17-9067-2017-f04.pdf"/>

          </fig>

      <p>Our results indicate a stronger cooling effect of reflective roofs than
those estimated by previous research. Studies using the WRF model showed a
cooling effect of 0.2–2.0 K in screen-height air temperature with
reflective roof materials of different albedos (Georgescu et al., 2014; Li
et al., 2014; Stone et al., 2014). A case study of the California South
Coast Air Basin area using a mesoscale model coupled with an urban airshed
model showed that a citywide albedo increase by 0.30 can reduce the air
temperature by up to 4.5 K in the mid-afternoon (Taha et al., 1997).
However, Rosenzweig et al. (2009) reported very modest cooling effects (0.3–0.6 K) from cool roofs with albedo of 0.5 in New York City using a
regional climate model. Studies using global climate models also report
local cooling effects, ranging from a global average of 0.02 K (Jacobson and
Ten Hoeve, 2012) to 0.4 K (Oleson et al., 2010c) decrease in air temperature
with different prescribed cool roof albedos. Apparently, these estimates
vary with the choice of cool roof albedo as well as the roof space
available for cool roof installation (Akbari et al., 2012; Rosenzweig et
al., 2009).</p>
      <p>There are three reasons why we observe a stronger cooling effect compared to
previous studies. First, the albedo of the cool roof in our study (0.88) is
at the higher end of the range (0.3–0.9) used in previous modeling
studies. Second, we define <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> using radiative surface temperature
rather than screen-height air temperature. The radiative surface temperature
is more sensitive to the surface radiation balance than the air temperature.
Using a mesoscale weather model, Li et al. (2014) showed that, when measured
by radiative surface temperature, the cooling effect of cool roofs was 3–4 K, which is
much higher than that of 0.5 K measured by 2 m air temperature. These
results are consistent with observational studies using radiative surface
temperature. Using LANDSAT satellite albedo and radiative temperature observations,
Mackey et al. (2012) detected a surface cooling effect of 5.0 K with an
albedo increase of 0.16. Gaffin et al. (2012) tested three generic white
membranes in New York City and found that the radiative temperature of the
white surfaces was on average 23.6 K lower than a black surface during peak
sunlight times. Third, our analysis and results are restricted to midday
hours (13:00 local time) and summer months (June–August), rather than the
annual mean values as reported in previous studies. The rationale behind
this restriction is that heat stress mitigation is a more pressing need in
the summer (Rosenzweig et al., 2009). Because surface incoming solar
radiation peaks in the summer noon time, the reflected solar radiation by
cool roofs would peak as well. The cooling effect induced by cool roofs
increases as the reflected solar radiation increases. Therefore, the
reductions in <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> reported here are likely the maximum potential of
urban heat mitigation by cool roofs.</p>
      <p>Our results are based on the albedo value of roof coating material after
3 years of use. The long-term weathering and aging problem of the
reflective material has not been taken into account. Although the albedo of
the Solareflect coating material decreases only slightly from 0.89 to 0.88
after 3 years, its long-term performance of retaining solar reflectance
is unknown. In addition, none of the current roofing materials can last
96 years (2005–2100) while preserving high albedos. Re-coating or reroofing
seems necessary for long-term use. Therefore, our results should be
interpreted as an upper bound of the cooling potential of the cool roof
strategy.</p>
</sec>
<sec id="Ch1.S3.SS3.SSS2">
  <title>Street vegetation</title>
      <p>Street vegetation is less effective than cool roofs in terms of temperature
reduction. The daytime surface temperature reduction is 1.3 <inline-formula><mml:math id="M78" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2 K in
the temperate climate and 0.3 <inline-formula><mml:math id="M79" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.1 K in the dry climate under the
RCP4.5 scenario. The cooling under the RCP8.5 scenario is 1.1 <inline-formula><mml:math id="M80" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.1 K
in the temperate climate and 0.3 <inline-formula><mml:math id="M81" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.1 K in the dry climate
(Table S1). The cooling effect is weaker in the dry climate compared to that
in the temperate climate. One factor that limits the mitigation potential is
the area available for vegetation planting. In the model domain, the pervious
surface that can be converted to vegetation cover occupies 25 to
45 % of the urban land. Our calculation assumes that street vegetation
consists of native species that have adapted to local soil moisture
conditions and can grow without additional water supply. Enhanced cooling
brought by irrigation is not considered.</p>
      <p>As mentioned previously, our method for calculating the cooling potential of
street vegetation may slightly overestimate the cooling benefit because of
the anthropogenic heat contribution to the UHI and the radiative trapping
effects by urban canyons. Our offline attribution results show that
anthropogenic heat contribution is about 20 % (Fig. 1). Ryu et al.
(2016) showed that the trees in the urban canyon decreased the sensible heat
flux and increased the latent heat flux by roughly a similar amount. Another
potential source of uncertainty to this method is the street vegetation
composition. Cities that have different vegetation composition from their
surrounding rural landscapes may generate slightly different cooling than
predicted here. However, integrating all these considerations into our
results would not change the point that street vegetation reduces urban
surface temperature less effectively in comparison to cool roofs.</p>
      <p>The cooling effects of street vegetation estimated in this study are
generally consistent with previous studies. Rosenzweig et al. (2009) found
that planting trees in open spaces and along streets reduces the
mid-afternoon air temperature by 0.2–0.6 K in neighborhoods of New York
City. Luley and Bond (2002) reported that in their maximum scenario, in
which all urban grass is replaced by trees, an up to 1.0 K reduction in air
temperature is expected in Manhattan, New York City, on a summer afternoon.
By forcing a mesoscale weather forecast model with atmospheric conditions
generated by a global climate model, Stone et al. (2014) found that, under
the business-as-usual climate change scenario, increasing green
vegetation in urban public areas reduces the urban daily average air
temperature by 0.1–0.3 K. Consistent with our results, they also reported
a weaker vegetation cooling effect over a city in the dry climate compared
to the cities in the temperate climate. In extreme scenarios, in which the
urban center of Atlanta, Georgia, is fully substituted by forest, Stone et
al. (2013) found a reduction in air temperature of 0.5–1.5 K. Generally,
the cooling benefit varies with different cities because of the area
available for tree planting. Our estimates fall at the higher end of the
range reported previously, partly because the temperature difference is
measured by surface radiative temperature.</p>
</sec>
<sec id="Ch1.S3.SS3.SSS3">
  <title>Green roof</title>
      <p>Green roofs generate modest cooling. The average daytime surface temperature
reduction is 1.6 <inline-formula><mml:math id="M82" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2 K for the 57 cities under the RCP4.5 and RCP8.5
scenarios (Fig. S1c and g; Table S1). According to our offline UHI
attribution, the albedo effect of green roofs is negligible (Table S1). Even
though the albedo of green roofs (0.20, the average warm-season grassland
albedo; Bonan, 2008) is lower than the average default roof value (0.29), the
citywide albedo is decreased only slightly (by 0.01) in comparison to the CTR
simulations. This is in sharp contrast to the WHT simulations where the
citywide albedo is increased by an average amount of 0.29. Therefore, the
contribution of green roofs to the temperature reduction comes from enhanced
evaporation. Once again, we assume in our calculation that water-conserving
native grass is planted on the roofs to minimize irrigation demand; this is a
fair assumption because water will be a scarce resource in future cities
(McDonald et al., 2011). Cities that can afford rooftop irrigation (Georgescu
et al., 2014; Bass et al., 2003) are expected to gain more cooling than
predicted here.</p>
      <p>These results are comparable with the green roof cooling effects reported by
previous studies. Building-scale observational studies have shown a
relatively large range of temperature reduction. A case study evaluating the
“green” and “white” policy in Chicago, Illinois, found that green roofs
can reduce the building-top temperature by 0.3–2.6 K according to the
LANDSAT satellite observations (Mackey et al., 2012). Ismail et al. (2011)
used an experimental approach on a test building in Malaysia and showed a
4.6 K reduction in the surface temperature around noontime between a green
roof and a black bare roof. Mesoscale modeling studies have also shown
cooling estimates ranging from 0.2 to 0.8 K if measured by air temperature
(Rosenzweig et al., 2009; Stone et al., 2014) and 3 to 4 K if measured by
surface temperature (Li et al., 2014). All these results, together with our
study, confirm that a major factor in determining the mitigation potential of
green roof is water availability.</p>
</sec>
<sec id="Ch1.S3.SS3.SSS4">
  <title>White oasis effect</title>
      <p>Our results favor cool roofs as the preferred method for urban heat
mitigation. Although empirical data are not yet available to validate the
white oasis effect, some lessons can be drawn from studies of green oases.
Local cooling has been observed for green oases as small as several hectares
in area (Kai et al., 1997). A typical green oasis effect ranges from <inline-formula><mml:math id="M83" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1
to <inline-formula><mml:math id="M84" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>7 K (Potchter et al., 2008), comparable in magnitude to the white
oasis effect reported here. The strongest green oasis effect is also found in
dry climates (Potchter et al., 2008). In the case of green oases, surface
cooling by evaporation typically results in a stable inversion air layer
above the ground, which would severely limit air pollution dispersion and
worsen air quality. In contrast, unstable lapse conditions generally prevail
over white oases (Fig. S2). In other words, implementation of cool roofs may
decrease the dispersion capacity of urban air due to a reduction in the mixed
layer depth (Georgescu et al., 2012), but not nearly to the extent of a
stable stratification brought by the green oasis effect.</p>
      <p>An explanation to this phenomenon can be achieved using the big-leaf model
(Sellers et al., 1996) solution of surface temperature shown below:
              <disp-formula id="Ch1.E7" content-type="numbered"><mml:math id="M85" display="block"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>d</mml:mi></mml:msub><mml:msub><mml:mi>c</mml:mi><mml:mi>p</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>⋅</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">γ</mml:mi><mml:mfenced close=")" open="("><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi>G</mml:mi></mml:mfenced><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>d</mml:mi></mml:msub><mml:msub><mml:mi>c</mml:mi><mml:mi>p</mml:mi></mml:msub><mml:mi>D</mml:mi><mml:mo>/</mml:mo><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:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="italic">γ</mml:mi><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:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">a</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="M86" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the surface temperature, <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the air temperature at a
reference height, <inline-formula><mml:math id="M88" 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 aerodynamic resistance, and <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the surface
resistance; <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the net radiation; <inline-formula><mml:math id="M91" display="inline"><mml:mi>G</mml:mi></mml:math></inline-formula> is the storage heat; <inline-formula><mml:math id="M92" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> is the water vapor
pressure deficit; <inline-formula><mml:math id="M93" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula> is the slope of the saturation vapor pressure
curve; and
<inline-formula><mml:math id="M94" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula> is the psychrometric constant. Equation (7) shows that the sign of
(<inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is determined by the sign of the second numerator on the
right-hand side,<inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>d</mml:mi></mml:msub><mml:msub><mml:mi>c</mml:mi><mml:mi>p</mml:mi></mml:msub><mml:mi>D</mml:mi><mml:mo>/</mml:mo><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:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>. In green oases in dry climates, <inline-formula><mml:math id="M97" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> is a large number and the
surface resistance is small due to irrigation, with both factors combined
yielding a negative sign of the numerator of the term on the right side of the
equation. Therefore, an inversion (<inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) typically prevails in the
surface layer over a green oasis. Over white oases, the available energy
<inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi>G</mml:mi></mml:mrow></mml:math></inline-formula>) is reduced somewhat, but, because the surface
resistance is very large in urban land, the numerator of the term on the
right-hand side of Eq. (7) stays positive. Therefore, unstable lapse
conditions (<inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> should be expected over white oases.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS4">
  <title>Mitigation wedges</title>
      <p>On the global (Pacala and Socolow, 2004) and urban (Creutzig et al., 2015)
scales, the highest carbon mitigation potential is achieved by using the
strategy of mitigation wedges or combining the incremental benefits of a
number of abatement actions. Because nonlinear interactions among the various
biophysical UHI contributors are small (Zhao et al., 2014; Fig. 1), a similar
strategy can be used to estimate the aggregated potential of multiple urban
temperature reduction methods. Figure 5 shows the additive benefit of three
UHI mitigation wedges: cool roofs (or green roofs), street vegetation, and
reflective pavement. Because cool roofs and green roofs are mutually exclusive
under the assumption of a 100 % penetration rate, we did not combine the
cooling benefit of cool roofs and green roofs in a single scenario. The urban
daytime surface temperature is on average 2.4 K greater than the rural
background temperature in the current climate. Near the end of the century,
the urban temperature will be 7.3 K greater under the RCP4.5 scenario than
the current background temperature due to the GHG warming (4.2 K) and the
UHIs (3.1 K). The combined wedges with cool roofs (Fig. 5a) provide greater
cooling benefit than the ones with green roofs (Fig. 5b). The total cooling
effect of the three mitigation wedges with cool roofs is 8.0 K, essentially
eliminating all the UHI effect plus the GHG warming.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><caption><p>A UHI strategy consisting of three mitigation wedges
under the RCP4.5 scenario. <bold>(a)</bold> cool roof, street vegetation, and reflective
pavement; <bold>(b)</bold> green roof, street vegetation, and reflective pavement. The
horizontal line marks the mean midday rural surface temperature of all
57 cities in the current climate conditions, and other temperatures are mean
values relative to this rural background.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/17/9067/2017/acp-17-9067-2017-f05.pdf"/>

        </fig>

      <p>The example given in Fig. 5 is the most optimistic scenario. Because roof
space is a “precious” resource that must accommodate other competing
needs, a 100 % conversion to white roofs is probably impractical. However,
we can linearly scale the endmember results (Table S1) to
estimate the cooling benefits of other wedge combinations. For example, a
wedge strategy consisting of 50 % cool roof, 50 % green roof, 100 %
street vegetation, and 100 % reflective pavement will bring a total
temperature reduction of 5.7 K (cool roof 3.3 K <inline-formula><mml:math id="M101" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> green roof 0.8 K <inline-formula><mml:math id="M102" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> street vegetation 0.9 K <inline-formula><mml:math id="M103" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> reflective pavement 0.7 K).</p>
      <p>Conversion of roof space to solar photovoltaics (PVs) can also cool the urban
air (Hu et al., 2016; Salamanca et al., 2016). A typical solar PV has an
albedo of 0.10 and a futuristic electricity conversion efficiency of 25 %
(Hu et al., 2016), giving a heat removal rate equivalent to having a surface
albedo of 0.33, which is 0.04 more than the average default roof albedo
value. Scaling the WHT simulation result proportionally by the albedo
increase, we estimate that the solar PV will lower the surface temperature
by an average amount of 1.2 K in the daytime. This estimate is made using
the offline energy balance diagnostics and Eq. (6), where <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:math></inline-formula> is
the citywide equivalent albedo change associated with the use of solar PV roofs.
The aggregated potential of 100 % solar PV roof, 100 % street
vegetation,
and 100 % reflective pavement is 2.8 K under the RCP4.5 scenario.</p>
      <p>The above discussion focuses on mitigation of the daytime temperature.
Unfortunately, none of the strategies are effective in eliminating the
nighttime UHI. Conversion to cool roofs reduces building storage of solar
radiation in the daytime and subsequent heat release at night, contributing
to nighttime cooling by an average amount of 0.7 <inline-formula><mml:math id="M105" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.03 K (Figs. 3d
and 4d). This is not nearly enough to offset the UHI (3.0 <inline-formula><mml:math id="M106" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.1 K;
Figs. 3b and 4b) or the GHG warming (2.6 <inline-formula><mml:math id="M107" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 K) expected near the
end of the century under the RCP4.5 scenario. The lack of nighttime cooling
underscores the importance of increasing resilience and preparedness to cope
with heat stress (Stone et al., 2012; Revi et al., 2014), in addition to
re-engineering the city landscape to achieve daytime temperature reduction.
In CLM, AC is switched on when the interior temperature of a building is
greater than 24.5 <inline-formula><mml:math id="M108" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. The daytime AC energy saving in the WHT
simulations is 26.0 and 24.8 W m<inline-formula><mml:math id="M109" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, or 55 and 43 % under the
RCP4.5 and RCP8.5 scenarios, respectively, in comparison to the CTR
simulations, which is more than enough to support the AC energy use for
cooling at night (Table 2).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><caption><p>Comparison between combined cooling benefit (combined
simulation results) and sum of the components (sum of individual simulation
results). Both are measured by screen-height air temperature. Black symbols: cool roof <inline-formula><mml:math id="M110" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> solar panel roof; green symbols: cool
roof <inline-formula><mml:math id="M111" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> green roof; circles: Salamanca et al. (2016); squares: Taha et al.
(1997); stars: Stone et al. (2014); triangles: Georgescu et al. (2014)</p></caption>
          <?xmltex \igopts{width=184.942913pt}?><graphic xlink:href="https://acp.copernicus.org/articles/17/9067/2017/acp-17-9067-2017-f06.pdf"/>

        </fig>

      <p>The above wedge strategy is applied to the surface UHI. To find out if the
linear supposition can also be extended to air UHI, we also conducted a
meta-analysis based on the published studies that presented modeled air UHI
results of both combined mitigation strategies and individual strategies. We
calculated the sum of the cooling benefit from each simulation of individual
strategy (as is shown in the <inline-formula><mml:math id="M112" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis of Fig. 6) and compared it with the
total cooling benefit from the combined simulation (as is shown in the <inline-formula><mml:math id="M113" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis
of Fig. 6). These data collected from the literature include simulations of
cool roofs, green roofs, and solar PVs. For example, Georgescu et al. (2014)
showed that if cool roofs and green roofs are implemented individually in
California, the cooling benefit is 1.45 and 0.24 K, respectively. The linear
supposition principle estimates that if both methods are put in place, the
overall cooling is the sum of the individual benefit which is 1.69 K
(1.45 K <inline-formula><mml:math id="M114" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> 0.24 K). For comparison, the simulated cooling for the simultaneous
implementation of these two mitigation methods is 1.66 K. Figure 6
demonstrates that the UHI mitigation wedge method (linear supposition) holds
valid for the air UHI as well. This confirms that the wedge idea can provide
a reasonable estimate of the maximum potential cooling benefit of multiple
strategies collectively. Although not directly related to heat exposure, the
surface UHI yields robust conclusions and implications when used as a
universal metric consistently across different cities.</p>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <title>Conclusions</title>
      <p>The UHI intensity is projected to increase in future warmer climates, partly
due to higher anthropogenic heat release from AC energy use to cope with the
GHG-induced warming. Our modeling analyses favor cool roofs as the preferred
method for urban heat mitigation in comparison to green roofs, street
vegetation, and reflective pavement. By adopting highly reflective roofs
citywide, almost all the selected cities in the USA and in southern Canada
are transformed into white oases. Cool roofs also bring large daytime AC
energy savings in future climate scenarios. A UHI mitigation wedge strategy
consisting of 50 % cool roof, 50 % green roof, street vegetation, and
reflective pavement has the potential to reduce the urban daytime surface
temperature by 5.7 K in the summer from the unmitigated urban scenario.
Unfortunately, none of the UHI mitigation methods are effective in
eliminating the nighttime UHI.</p>
      <p>Cities are in fact engineered landscapes. The above UHI wedge strategies
amount to a re-engineering of these landscapes (Animation
Movies S1 and S2). A key distinction between urban engineering and
geoengineering is the scale. Unlike planetary-scale geoengineering, urban
engineering impacts a much smaller areal extent (about 2.7 % of the
terrestrial land; Schneider et al., 2009). Planetary albedo modification can
temporarily cool the global climate but at potentially large environmental
costs (Mcnutt et al., 2015). In contrast, re-engineering of the urban land
should have minimal negative consequences. Reorientation of the discussion
from the global-scale albedo intervention to the small-scale temperature
modification can motivate local actions because the payback is immediate and
direct.</p>
</sec>

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

      <p>Data used in this study are CESM simulation results
conducted by Lei Zhao on the US National Center for Atmospheric Research's
cluster “Yellowstone” and can be provided upon request to the
corresponding author, Lei Zhao (lei.zhao@princeton.edu).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p><bold>The Supplement related to this article is available online at <inline-supplementary-material xlink:href="https://doi.org/10.5194/acp-17-9067-2017-supplement" xlink:title="zip">https://doi.org/10.5194/acp-17-9067-2017-supplement</inline-supplementary-material>.</bold></p></supplementary-material>
        </app-group><notes notes-type="competinginterests">

      <p>The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p>This research was supported by the Ministry of Education of China (grant
PCSIRT), a Princeton STEP Postdoctoral Fellowship (to Lei Zhao), and a Yale
University Graduate Fellowship (to Natalie Schultz). We thank Chang Cao for making the
animation movies. We acknowledge high-performance computing support from
Yellowstone (ark:/85065/d7wd3xhc) provided by NCAR's Computational and
Information Systems Laboratory, sponsored by the US National Science
Foundation.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Yun Qian<?xmltex \hack{\newline}?>
Reviewed by: three anonymous referees</p></ack><ref-list>
    <title>References</title>

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    <!--<article-title-html>A wedge strategy for mitigation of urban warming in future climate scenarios</article-title-html>
<abstract-html><p class="p">Heat stress is one of the most severe climate threats to human society in a future warmer world. The situation is further exacerbated
in urban areas by urban heat islands (UHIs). Because the majority of
world's population is projected to live in cities, there is a pressing need
to find effective solutions for the heat stress problem. We use a climate
model to investigate the effectiveness of various urban heat mitigation
strategies: cool roofs, street vegetation, green roofs, and reflective
pavement. Our results show that by adopting highly reflective roofs, almost
all the cities in the United States and southern Canada are transformed into
<q>white oases</q> – cold islands caused by cool roofs at midday, with an
average oasis effect of −3.4 K in the summer for the period 2071–2100,
which offsets approximately 80 % of the greenhouse gas (GHG) warming
projected for the same period under the RCP4.5 scenario. A UHI mitigation
wedge consisting of cool roofs, street vegetation, and reflective pavement has
the potential to eliminate the daytime UHI plus the GHG warming.</p></abstract-html>
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