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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-18-14059-2018</article-id><title-group><article-title>Impact of urban canopy meteorological forcing on <?xmltex \hack{\break}?>aerosol concentrations</article-title><alt-title>Impact of urban canopy on aerosols</alt-title>
      </title-group><?xmltex \runningtitle{Impact of urban canopy on aerosols}?><?xmltex \runningauthor{P. Huszar et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Huszar</surname><given-names>Peter</given-names></name>
          <email>huszarpet@gmail.com</email>
        <ext-link>https://orcid.org/0000-0003-2954-8347</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Belda</surname><given-names>Michal</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9514-4888</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Karlický</surname><given-names>Jan</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2936-0785</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Bardachova</surname><given-names>Tatsiana</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Halenka</surname><given-names>Tomas</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1584-791X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Pisoft</surname><given-names>Petr</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5034-9169</ext-link></contrib>
        <aff id="aff1"><institution>Department of Atmospheric Physics, Faculty of Mathematics and Physics, Charles University, <?xmltex \hack{\break}?>V Holešovičkách 2, 180 00 Prague 8, Czech Republic</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Peter Huszar (huszarpet@gmail.com)</corresp></author-notes><pub-date><day>4</day><month>October</month><year>2018</year></pub-date>
      
      <volume>18</volume>
      <issue>19</issue>
      <fpage>14059</fpage><lpage>14078</lpage>
      <history>
        <date date-type="received"><day>25</day><month>April</month><year>2018</year></date>
           <date date-type="rev-request"><day>18</day><month>June</month><year>2018</year></date>
           <date date-type="rev-recd"><day>11</day><month>September</month><year>2018</year></date>
           <date date-type="accepted"><day>18</day><month>September</month><year>2018</year></date>
      </history>
      <permissions>
        
        
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://acp.copernicus.org/articles/.html">This article is available from https://acp.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://acp.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/.pdf</self-uri>
      <abstract>
    <p id="d1e127">The regional climate model RegCM4 extended with the land surface model CLM4.5
was coupled to the chemistry transport model CAMx to analyze the impact of
urban meteorological forcing on surface fine aerosol (<inline-formula><mml:math id="M1" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)
concentrations for summer conditions over the 2001–2005 period, focusing on
the area of Europe. Starting with the analysis of the meteorological
modifications caused by urban canopy forcing, we found a significant increase
in urban surface temperatures (up to 2–3 K), a decrease of specific humidity (by
up to 0.4–0.6 <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">gkg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), a reduction of wind speed (up to <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">ms</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) and an enhancement of vertical turbulent diffusion coefficient
(up to 60–70 <inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>).</p>
    <p id="d1e198">These modifications translated into significant changes in surface aerosol
concentrations that were calculated by a “cascading” experimental approach.
First, none of the urban meteorological effects were considered. Then, the
temperature effect was added, then the humidity and the wind, and finally, the
enhanced turbulence was considered in the chemical runs. This facilitated the
understanding of the underlying processes acting to modify urban aerosol
concentrations. Moreover, we looked at the impact of the individual aerosol
components as well. The urbanization-induced temperature changes resulted in
a decrease of <inline-formula><mml:math id="M6" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> by <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, while decreased
urban winds resulted in increases by 1–2 <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. The enhanced
turbulence over urban areas resulted in decreases of <inline-formula><mml:math id="M11" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> by <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. The combined effect of all individual impact depends on
the competition between the partial impacts and can reach up to <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for some cities, especially when the temperature impact was stronger
in magnitude than the wind impact. The effect of changed humidity was found
to be minor. The main contributor to the temperature impact is the
modification of secondary inorganic aerosols, mainly nitrates, while the wind
and turbulence impact is most pronounced in the case of primary aerosol (primary
black and organic carbon and other fine particle matter). The overall as well
as individual impacts on secondary organic aerosol are very small, with the
increased turbulence acting as the main driver. The analysis of the vertical
extent of the aerosol changes showed that the perturbations caused by urban
canopy forcing, besides being large near the surface, have a secondary
maximum for turbulence and wind impact over higher model levels, which is
attributed to the vertical extent of the changes in turbulence over urban
areas. The validation of model data with measurements showed good agreement,
and we could detect a clear model improvement in some areas when including
the urban canopy meteorological effects in our chemistry simulations.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e347">Among the many types of impacts of urban areas on the environment, the
impact on the atmospheric environment is regarded to be the “most important
and most far-reaching” <xref ref-type="bibr" rid="bib1.bibx15" id="paren.1"/>. A major component of this impact
is the direct influence of the urban canopy on meteorological conditions: cities
are largely covered by artificial surfaces and they affect the physical
properties of the air above in a very specific way resulting in an increase
in temperatures, a reduction of winds, an increase in turbulence and other
meteorological modifications
<xref ref-type="bibr" rid="bib1.bibx45 bib1.bibx28 bib1.bibx31 bib1.bibx36" id="paren.2"/>.</p>
      <p id="d1e356">The most known aspect of urban influence on meteorological conditions is the
formation of the urban heat island<?pagebreak page14060?> (UHI), which has been the subject of a large
number of studies since the early 1980s <xref ref-type="bibr" rid="bib1.bibx55" id="paren.3"/>. UHI and other related
meteorological effects were studied by many authors, and impacts on
temperature, wind speed, turbulence and structure of the boundary layer were
identified <xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx16 bib1.bibx63 bib1.bibx37 bib1.bibx25 bib1.bibx1" id="paren.4"/>.
Cities further influence humidity, precipitation and the hydrological cycle
in general <xref ref-type="bibr" rid="bib1.bibx61 bib1.bibx64" id="paren.5"/>. With the introduction of urban canopy
parameterizations and models of different complexity, modeling approaches
describing the urban effects on meteorology and climate became widespread,
examining both local <xref ref-type="bibr" rid="bib1.bibx83 bib1.bibx25" id="paren.6"/> and regional scales
<xref ref-type="bibr" rid="bib1.bibx14 bib1.bibx76 bib1.bibx72 bib1.bibx28 bib1.bibx36" id="paren.7"/>.
<xref ref-type="bibr" rid="bib1.bibx28" id="text.8"/> showed that urbanization can contribute to regional
warming <xref ref-type="bibr" rid="bib1.bibx28" id="paren.9"><named-content content-type="pre">e.g.</named-content></xref> and determine the climate of whole regions
<xref ref-type="bibr" rid="bib1.bibx42" id="paren.10"/>, as the impact usually exceeds the geographical location
of the city itself and propagates to larger scales.</p>
      <p id="d1e386">Over urban areas, the meteorological conditions are thus largely perturbed.
Consequently, as air chemistry is strongly linked to meteorological
conditions, it is expected that modifications in meteorological parameters
will result in modifications in species concentrations as well, as has already been shown by many
regarding the climate-change-related meteorological
changes and their impact on air quality
<xref ref-type="bibr" rid="bib1.bibx26 bib1.bibx38 bib1.bibx34" id="paren.11"/>.</p>
      <p id="d1e392">In particular, the UHI triggers higher urban temperatures, modifies chemical
reaction rates and particle nucleation and also influences dry deposition
velocities and wet scavenging rates <xref ref-type="bibr" rid="bib1.bibx69" id="paren.12"/>. Further, <xref ref-type="bibr" rid="bib1.bibx23" id="text.13"/> and <xref ref-type="bibr" rid="bib1.bibx66" id="text.14"/>, e.g., showed that the UHI can generate
urban breeze circulation, resulting in pollutant transport from and to cities
depending on the time of day but also on the surrounding orography and/or the
presence of coasts <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx47" id="paren.15"/>. Urban surfaces, however, act in
the opposite direction a well: higher drag induces wind stilling and thus
suppresses the dispersion of urban emissions and secondary pollutants into
regional scales. Surface heterogeneities in urban areas further enhance
turbulence, and increased eddy transport helps pollutant transport to upper
layers of the urban boundary layer <xref ref-type="bibr" rid="bib1.bibx73" id="paren.16"><named-content content-type="pre">UBL;</named-content></xref>. In general, a very
strong link is identified between the state of the UBL and pollution
<xref ref-type="bibr" rid="bib1.bibx51" id="paren.17"/>.</p>
      <p id="d1e417">The above-listed effects act, however, simultaneously in a rather complex
manner, requiring coupled modeling approaches. Most of the work done focused
on gas-phase chemistry, especially ozone (<inline-formula><mml:math id="M16" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and nitrogen oxide
(<inline-formula><mml:math id="M17" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) changes due to urban land surface forcing. <xref ref-type="bibr" rid="bib1.bibx50" id="text.18"/>
and <xref ref-type="bibr" rid="bib1.bibx67" id="text.19"/> each focused on one single city, Athens and Paris, and found
a significant impact on pollutant concentrations, mainly due to changed
turbulence when urban surfaces are considered. <xref ref-type="bibr" rid="bib1.bibx6" id="text.20"/>, using a
bulk approach for the description of urban surfaces, predicted a considerable
increase in the episode maximum 8 h average <inline-formula><mml:math id="M18" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration due to
future urbanization. <xref ref-type="bibr" rid="bib1.bibx72" id="text.21"/> looked at the southern Poland region
and found a reduction of primary pollutants (<inline-formula><mml:math id="M19" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M20" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>) due to
enhanced vertical mixing. Recently, <xref ref-type="bibr" rid="bib1.bibx13" id="text.22"/> analyzed ozone
changed after urban greening utilization and found <inline-formula><mml:math id="M21" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> reduction due
to temperature mitigation, but increases of primary pollutants due to the
associated decreased mixing. A large number of authors focused on Chinese
cities and urban areas <xref ref-type="bibr" rid="bib1.bibx79 bib1.bibx80 bib1.bibx84 bib1.bibx90" id="paren.23"/>. They
calculated an ozone concentration increase due to urbanization which has a
similar magnitude to future emission changes and changed climate,
emphasizing the importance of considering urban canopy effects in air quality
modeling. <xref ref-type="bibr" rid="bib1.bibx48" id="text.24"/> investigated how different urban canopy
parameterizations influence the air quality prediction for a Chinese
agglomeration. Sulfur dioxide (<inline-formula><mml:math id="M22" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) changes due to urbanization were
modeled by <xref ref-type="bibr" rid="bib1.bibx4" id="text.25"/> who found significant decreases of this important
primary pollutant over urban areas, caused mainly by increased vertical mixing
over the urban canopy. <xref ref-type="bibr" rid="bib1.bibx65" id="text.26"/> and <xref ref-type="bibr" rid="bib1.bibx66" id="text.27"/> modeled the urbanization impact
on ozone concentrations over Seoul, South Korea, and identified a strong urban breeze
circulation greatly affecting ozone concentrations, and this was found to be
further modulated by the effect of anthropogenic heat released from the city.
Regarding aerosols, <xref ref-type="bibr" rid="bib1.bibx90" id="text.28"/> investigated the impact of the change of
land use from natural to artificial due to urban expansion on coarse particle
matter (PM<inline-formula><mml:math id="M23" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>) and found decreases driven mainly by enhanced vertical
eddy transport. Increases of planetary boundary layer (PBL) height and turbulence over urban areas were
the main reason for decreases of primary pollutant concentration near the
surface in <xref ref-type="bibr" rid="bib1.bibx85" id="text.29"/> and <xref ref-type="bibr" rid="bib1.bibx46" id="text.30"/>. Over Toulouse, France,
<xref ref-type="bibr" rid="bib1.bibx51" id="text.31"/> analyzed how fine-mode aerosols interact with the urban
boundary layer and found a strong role of vertical dispersion in modulating
their concentration. Recently, <xref ref-type="bibr" rid="bib1.bibx8" id="text.32"/> found that the application
of urban canopy models instead of simple “bulk” approaches has a positive
impact on model accuracy for both gaseous species (<inline-formula><mml:math id="M24" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M25" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and <inline-formula><mml:math id="M26" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. For fine aerosol they found that the main
driver for changes is the lower wind in urban areas that is closer to
observed values than that modeled with simple approaches or without
considering urban surfaces at all. For Paris, France, <xref ref-type="bibr" rid="bib1.bibx40" id="text.33"/> showed
that when using an urban canopy model that triggers stronger vertical mixing in
the model over urban areas, <inline-formula><mml:math id="M27" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations are lower and
agree better with observations. The important consequences that land use changes
and, particularly, urbanization have on PM concentrations were noted by
<xref ref-type="bibr" rid="bib1.bibx74" id="text.34"/> too.</p>
      <p id="d1e602">The listed studies point to different meteorological changes occurring over
urban areas that influence local and regional air pollution, often in an
opposite manner. Indeed,<?pagebreak page14061?> when evaluating the integrated chemical effect of
urban canopy meteorological forcing, one encounters a number of difficulties.
First of all, the individual meteorological components (like temperature
changes, modifications of turbulence etc.) often counteract each other. Enhanced
urban temperatures trigger higher reaction rates for production as well as
chemical destruction of secondary pollutants. Decreases in wind speeds block
pollutants from dispersing into larger scales; however this is also true for
their precursors which stay close to sources and can trigger their
destruction, like in the case of ozone–<inline-formula><mml:math id="M28" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> interaction. However, at the same
time, enhanced vertical mixing contributes to their removal, which decreases
the concentrations. Another complexity in the urban meteorology–air chemistry
interaction is presented by the fact that the urbanization-induced meteorological
features as well as emissions are not uniformly distributed in time and their
daily cycles have specific features. Maximums and minimums in their peaks
sometimes occur simultaneously, leading to the amplifications of the effects.
In the case of secondary aerosols, the situation is even more complicated as
their concentrations are influenced not only directly via the urban
meteorological effects, but also via changes in their gas-phase precursors.
The overall impact on aerosol concentration is then the complex combination
of the impact on individual aerosol components, which, in the case of secondary
aerosols, is largely modulated by the impact on the source precursors. It is
clear that an integrated meteorology and air quality modeling framework is an
inevitable tool to analyze the changes of air pollutants due to urban canopy
land surface forcing in detail.</p>
      <p id="d1e616">Here, we introduce a model estimate of the impact of the urban canopy
meteorological forcing on fine aerosol (PM<inline-formula><mml:math id="M29" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>) concentrations over European
urban areas. This study is a follow-up to <xref ref-type="bibr" rid="bib1.bibx31" id="text.35"/> in which the impact
was analyzed from the perspective of gas-phase chemistry, focusing especially
on <inline-formula><mml:math id="M30" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and ozone. Here, we make a further step and look at
aerosols' concentrations and as a novelty, our study, as one of the first to do so, will
investigate each component of <inline-formula><mml:math id="M31" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, as it is expected that
different components of aerosol respond differently to urban meteorological
forcing. Another novelty of the study is that instead of modeling selected
short periods (although interesting from a meteorological perspective), we
perform continuous long-term simulations in order to capture the long-term
average impact. Our study is motivated by the appreciation that urban fine
aerosol still represents a substantial threat to the public in large cities
<xref ref-type="bibr" rid="bib1.bibx5" id="paren.36"/> and represents an important aspect of cities' air pollution
<xref ref-type="bibr" rid="bib1.bibx29" id="paren.37"/>. In order to implement measures for its reduction, proper knowledge
of the contributors to pollution levels is crucial and this has
to include the potential contribution from land use changes related to
urbanization as well.</p>
</sec>
<sec id="Ch1.S2">
  <title>Experimental setup</title>
<sec id="Ch1.S2.SS1">
  <title>Models</title>
      <p id="d1e671">Models used in this study were introduced and used with a very similar setup
to that used in <xref ref-type="bibr" rid="bib1.bibx29 bib1.bibx30 bib1.bibx31" id="text.38"/>. Here we provide a
rather brief but self-consistent description of them. The regional climate
model RegCM (version 4.4) was used as a meteorological driver
<xref ref-type="bibr" rid="bib1.bibx20" id="paren.39"/>. For convective- and large-scale precipitation, the Grell
and SUBEX schemes were invoked, respectively <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx59" id="paren.40"/>. The
planetary boundary layer processes were modeled using the Holtslag scheme
<xref ref-type="bibr" rid="bib1.bibx24" id="paren.41"/>. Radiative transfer calculations were conducted using the
NCAR Community Climate Model Version 3 <xref ref-type="bibr" rid="bib1.bibx39" id="paren.42"><named-content content-type="pre">CCM3;</named-content></xref>.</p>
      <p id="d1e691">The Community Land Model version 4.5
<xref ref-type="bibr" rid="bib1.bibx44 bib1.bibx58" id="paren.43"><named-content content-type="pre">CLM4.5;</named-content></xref> was chosen to describe the
land-cover processes. CLM4.5 provides a more comprehensive description of
land surface processes compared to the simple BATS land surface model which
is originally included in the RegCM model <xref ref-type="bibr" rid="bib1.bibx9" id="paren.44"/>. CLM4.5
further contains the CLMU (Community Land Model Urban) urban canopy scheme <xref ref-type="bibr" rid="bib1.bibx56" id="paren.45"/> based on the
traditional canyon representation of urban areas. The canyon consists of
roofs, walls and the canyon floor. Trapping of solar and long-wave radiation
within the canyon is taken into account. Momentum fluxes are calculated for
the urban land unit using roughness lengths and displacement heights typical
for the canyon. Anthropogenic heat from air conditioning and heating is
computed online within the CLMU from the heat conduction equation, with interior
boundary conditions represented by the interior temperature of the building. Another heat flux is added to
this anthropogenic heat flux that accounts for the waste heat from air heating/conditioning. It is parameterized directly
from the amount of energy required to keep the internal building temperature
between prescribed maximum and minimum values, assuming 50 % efficiency of
the heating/cooling systems <xref ref-type="bibr" rid="bib1.bibx57" id="paren.46"/>.</p>
      <p id="d1e708">We have chosen to use the CLM4.5 scheme as it produces a stronger and more
realistic UHI compared to the BATS scheme and gives a more emphasized wind speed
decrease <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx31" id="paren.47"><named-content content-type="pre">see</named-content></xref>. It further reduces the
overestimation of evaporation in summer seen in the BATS scheme and hence
models precipitation with a higher accuracy, which was already concluded by
<xref ref-type="bibr" rid="bib1.bibx81" id="text.48"/> who compared these two schemes.</p>
      <p id="d1e719">For chemical simulations, the chemistry transport model (CTM) CAMx version
6.30 <xref ref-type="bibr" rid="bib1.bibx12" id="text.49"/> was coupled offline to the regional climate model.
CAMx is an Eulerian photochemical CTM implementing multiple gas-phase
chemistry mechanism options (CBV, CB6, SAPRC07TC). In this study, the CBV
scheme <xref ref-type="bibr" rid="bib1.bibx86" id="paren.50"/> is invoked. CAMx further implements static two-mode treatment<?pagebreak page14062?> as well as multisectional particle size treatment and wet and dry
deposition of gases and particles, and it calculates the composition and phase
state of the ammonia–sulfate–nitrate–chloride–sodium–water inorganic aerosol
system in equilibrium with gas-phase precursors using the ISORROPIA
thermodynamic equilibrium model <xref ref-type="bibr" rid="bib1.bibx53" id="paren.51"/> activated in our setup. For
aerosol, we invoked the two-mode particle size treatment, and the
semi-volatile equilibrium scheme called SOAP <xref ref-type="bibr" rid="bib1.bibx71" id="paren.52"/> for the
formation of secondary organic aerosol (SOA) was used.</p>
      <p id="d1e735">As an offline couple, no feedbacks from the simulated species concentration
changes on RegCM radiation/microphysical processes (cloud/rain) were taken
into account. <xref ref-type="bibr" rid="bib1.bibx30" id="text.53"/> showed minor effects of these feedbacks in
long-term averages, so we consider this to be a reasonable simplification. The
RegCM-generated meteorological fields are translated into CAMx input using
the RegCM2CAMx preprocessor <xref ref-type="bibr" rid="bib1.bibx27" id="paren.54"/>. In RegCM2CAMx, we replaced
the <xref ref-type="bibr" rid="bib1.bibx54" id="text.55"/> method for calculating the vertical eddy diffusion
coefficients (required by CAMx) with the more advanced <xref ref-type="bibr" rid="bib1.bibx3" id="text.56"/>
scheme. This leads to a better match of model results with measurements
<xref ref-type="bibr" rid="bib1.bibx10" id="paren.57"/>. With this choice, an inconsistency is introduced to the
modeling setup as the methods calculating vertical diffusion coefficient
differ between the climate and chemistry models. To achieve the highest
degree of coupling between the driving climate model and a chemistry
transport model, the <xref ref-type="bibr" rid="bib1.bibx24" id="text.58"/> scheme produced vertical diffusion
(Kv) parameters that should have been used directly to drive the vertical
diffusion in CAMx. As RegCM4 does not support the output of these parameters (in
the versions and configurations used), it was technically much simpler to take
the vertical profiles of wind speed and temperature as well as the PBL height
from the driving model and apply a diagnostic method to calculate the Kv for
CAMx (provided by <xref ref-type="bibr" rid="bib1.bibx3" id="altparen.59"/>). Applying a “inconsistent” method in
calculating Kv for CTMs, however, does not implicate less accurate results than
directly coupling the PBL parameters, as shown by <xref ref-type="bibr" rid="bib1.bibx45" id="text.60"/>.</p>
<sec id="Ch1.S2.SS1.SSS1">
  <title>Data and simulations</title>
      <p id="d1e768">The models were applied for the same domain and configuration as in
<xref ref-type="bibr" rid="bib1.bibx31" id="text.61"/>; i.e., 10 km <inline-formula><mml:math id="M32" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10 km horizontal resolution
centered over Prague, Czech Republic, with <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:mn mathvariant="normal">160</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">120</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">23</mml:mn></mml:mrow></mml:math></inline-formula> grid boxes in <inline-formula><mml:math id="M34" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M35" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula>, and
<inline-formula><mml:math id="M36" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula>
directions. It is clear that with such a horizontal resolution, the fine-scale
structure of chemical transformation of emissions from cities cannot be resolved.
With this resolution, emissions from cities enter the atmosphere through a few
grid boxes while considering instant dilution on the model scale. It is clear
that due to the nonlinearity of chemical processes, this can lead to some
errors in the final species concentrations. This effect is considered,
however, to be small in the case of city emissions <xref ref-type="bibr" rid="bib1.bibx49" id="paren.62"/>. Many
previous studies also agreed that resolutions similar to ours are suitable to
model the regional impact of urban emissions <xref ref-type="bibr" rid="bib1.bibx77 bib1.bibx75" id="paren.63"/>
although some overestimation of secondary species is documented when using
a coarser model resolution <xref ref-type="bibr" rid="bib1.bibx35" id="paren.64"/>.</p>
      <p id="d1e828">The top model levels correspond to 50 hPa for the climate model. CAMx was only set
up on the lowermost 18 levels (up to approximately 10 km). Lateral
boundary conditions for the regional climate calculations were taken from a
50 km <inline-formula><mml:math id="M37" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 50 km resolution experiment carried out using the RegCM4 model within
the EURO-CORDEX initiative <xref ref-type="bibr" rid="bib1.bibx78" id="paren.65"/> driven by the ERA-Interim
reanalysis <xref ref-type="bibr" rid="bib1.bibx70" id="paren.66"/>.</p>
      <p id="d1e844">The TNO emissions prepared in the framework of the FP7 MEGAPOLI project were
used <xref ref-type="bibr" rid="bib1.bibx41" id="paren.67"/> as the anthropogenic emissions' source. They provide
high-resolution (<inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msup><mml:mn mathvariant="normal">8</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> longitude, <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msup><mml:mn mathvariant="normal">16</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> latitude, roughly
7 km <inline-formula><mml:math id="M40" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 7 km) European data of annual emission estimates for <inline-formula><mml:math id="M41" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>,
<inline-formula><mml:math id="M42" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, non-methane volatile organic compounds (NMVOCs), methane
(<inline-formula><mml:math id="M43" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), ammonia (<inline-formula><mml:math id="M44" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), carbon monoxide (<inline-formula><mml:math id="M45" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>) and
particulates (PM<inline-formula><mml:math id="M46" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> and <inline-formula><mml:math id="M47" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) in 10 activity sectors. For each
sector, specific temporal disaggregation factors and NMVOC speciation
profiles were applied to decompose the annual sums into hourly emissions
following <xref ref-type="bibr" rid="bib1.bibx82" id="text.68"/>. For chemical initial and boundary
conditions (ICBCs), a 30 km <inline-formula><mml:math id="M48" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 30 km domain run was performed covering the
whole of Europe. This large domain run was, in turn, driven by time–space-invariant
chemical ICBCs. This choice of chemical ICBCs resulted in some model biases
listed in <xref ref-type="bibr" rid="bib1.bibx29" id="text.69"/>, especially regarding ozone.
Meteorology-dependent biogenic emissions of isoprene and monoterpenes (BVOCs)
were considered in the study following <xref ref-type="bibr" rid="bib1.bibx22" id="text.70"/>.</p>
      <p id="d1e977">Land use was extracted from the USGS data, while the urban land unit percentage was
derived from the <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">0.05</mml:mn><mml:mo>∘</mml:mo></mml:msup><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mo>×</mml:mo><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msup><mml:mn mathvariant="normal">0.05</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> resolution LandScan2004
dataset based on census, nighttime light satellite observations and road
proximity <xref ref-type="bibr" rid="bib1.bibx32" id="paren.71"/>. They define 132 regional categories (the world
is divided into 33 regions with similarities in urban characteristics, and
each category is subdivided into 4 subcategories representing different urban
intensities – tall building district (TBD), high density (HD), medium density
(MD) and low density (LD)). For each bottom category, average building
heights (H), urban canyon height-to-width ratios (H : W), and fractions of
pervious surface (e.g., vegetation), roof area and impervious surfaces
(e.g., roads and sidewalks) are defined, among other parameters. The urban
land unit within CLM4.5 is represented as a fraction in percentages of three (of
the four in Jackson et al.) urban intensities (HD, MD and LD). This gives a
reasonable description of urban coverage at 10 km resolution, and even small
cities well below 10 km in diameter are accounted for. For chemical
simulations, the land use was kept the same for all experiments in order to
separate the effect of meteorological changes only.</p>
      <?pagebreak page14063?><p id="d1e1004">The experiments cover a period 2001–2005, with the year 2000 as a spin-up.
Summer months (JJA) are analyzed in our study when urban effects are the most
pronounced. With the regional climate model, one pair of experiments was
carried out: (i) a reference simulation (NOURBAN experiment), which does not
consider the urban land unit, meaning that urban grid boxes are replaced with the
one that is most typical for the surrounding grid boxes, most often crops;
(ii) and a simulation that considers urban surfaces and that is parameterized with
the urban canopy model CLMU (URBAN experiment).</p>
      <p id="d1e1007">Within the impact of the simulated meteorological changes on chemistry, the
following effects are considered: (1) modified temperature (<inline-formula><mml:math id="M50" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> impact);
(2) modified absolute humidity (<inline-formula><mml:math id="M51" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> impact); (3) modified wind field (<inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula> impact)
and (4) modified turbulence (via changes in the vertical eddy diffusion
coefficient; <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula> impact). A number of experiments with the chemistry model
CAMx were carried out depending on which effect is ex-/included. The
reference CAMx simulation is driven by the reference climate simulation and
is denoted in the same way: NOURBAN. Afterwards, a “full” experiment was carried
out whereby all the listed effects were considered (the URB_t+q+uv+Kv
experiment). To obtain a more detailed picture about the role each process
plays, additional experiments were carried out by turning on the individual
components of the overall meteorological effect one by one following the
methodology in <xref ref-type="bibr" rid="bib1.bibx31" id="text.72"/>. Accordingly, the URB_t experiment only considered the urban temperature effects. In the URB_t+q experiment,
both temperature and humidity effects were accounted for. The effect of modified
wind was added to the URB_t+q+uv experiment. Finally, in the full
experiment, the effect of modified eddy diffusion coefficients on chemistry
was considered. With such a “cascading” approach, one can analyze the separate
impact of individual meteorological parameters and their contribution to the
total impact. Although this experimental approach must lead to some
inconsistency in the meteorological driving fields, e.g., the vertical layer
structure (layer interface heights) defined in the CAMx input will be not
consistent with the increased temperature in the URB_t experiment, these
simulations serve only to explain how the chemical changes are built
up from summing up of the meteorological influences, and an assumption
is made according to which of the possible effects of these inconsistencies is
small when averaged over a long period. Further, the role of the ordering of
individual impacts was investigated. Short runs were carried out for summer
2001 (not shown here) for which the temperature, humidity, wind and turbulence
changes are considered in different orders and the results for individual
components were practically the same. The effect of temperature-driven BVOC
changes is not accounted for as it is rather negligible <xref ref-type="bibr" rid="bib1.bibx31" id="paren.73"/>.</p>
      <p id="d1e1051">In <xref ref-type="bibr" rid="bib1.bibx29" id="text.74"/>, an extensive validation is provided for the chemistry
simulated by the RegCM4–CAMx couple for the 2001–2010 period. Here, the same
configuration and input data are used except that the CLM4.5 surface model is
used instead of the older BATS scheme. We only expect a minor impact on the
simulated species concentrations, as lateral boundary conditions and emissions
were identified as the main sources of model bias, and these are the same in
this study. We only provide a spatial comparison of modeled <inline-formula><mml:math id="M54" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
concentrations with observations (see the following), mainly to examine possible
model improvement when urban canopy effects are considered in the driving
meteorology. Regarding the meteorology, we use the same pair of
(URBAN–NOURBAN) experiments to drive CAMx as in <xref ref-type="bibr" rid="bib1.bibx31" id="text.75"/>. They
compared temperature and precipitation fields with observational data and
found an underestimation of modeled temperatures by 2–3 K and both under- and
overestimation of precipitation by <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> % depending on the location. In
this study, we make the assumption that the simulated impact of the urban canopy
on climate is only influenced by these biases in a minor way, as the impact
is always calculated as a difference, and thus the biases are partly eliminated.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Results</title>
<sec id="Ch1.S3.SS1">
  <title>Impact on meteorological conditions</title>
      <p id="d1e1094"><xref ref-type="bibr" rid="bib1.bibx31" id="text.76"/> provided both the spatial impact of the urban canopy on
meteorological conditions and the diurnal cycle of the impact over selected
cities. Here we limit our presentation to the diurnal cycles extended with
the impact on the absolute humidity. If not specified otherwise, the diurnal
cycles are plotted in sundial time (approximately UTC<inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> h for almost the
entire domain). We analyzed a large number of cities; however the results
showed a high degree of similarity between them. Therefore, here we
present only two cities, Berlin and Prague. For the humidity, we also show
the spatial impact presented for day- and nighttime, considering
11:00–16:00 and 00:00–05:00, respectively. Shaded areas
mean a statistically significant difference at the 98 % level using the <inline-formula><mml:math id="M57" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> test.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><caption><p id="d1e1118">Diurnal cycle of the modeled near-surface temperature in <inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C,
absolute humidity in <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">kg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, 10 m wind speed in <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">ms</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>
and the eddy diffusion coefficient in the fifth model level (about 700–800 m)
in <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> in local time for two selected cities, Berlin and Prague:
blue – URBAN experiment, green – NOURBAN experiment, red – difference of
URBAN and NOURBAN simulations, solid line – city averaged values, dashed line
– city vicinity.</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/14059/2018/acp-18-14059-2018-f01.png"/>

        </fig>

      <p id="d1e1186">In Fig. <xref ref-type="fig" rid="Ch1.F1"/>, the JJA average
diurnal cycle of (panels a–e) the near-surface temperature, humidity,
10 m wind speed and vertical eddy diffusion coefficient over selected cities
(solid lines) and their vicinities (dashed lines) is plotted. The pattern
regarding the temperature impact is very similar for both cities. As
expected, the experiment with urban surfaces predicts higher temperatures
over urban areas, while the difference reaches almost zero during morning
hours. Maximum temperatures are enhanced by about 0.5 to 1 <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>
when urban land use type is considered. The largest impact occurs during the late
afternoon and evening, peaking around 20:00. The plots further reveal an almost
negligible impact over the city vicinities (increase up to 0.2 <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>). The diurnal temperature range is reduced by 1.5 to 2 <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p id="d1e1230">Impact of urban canopy on the near-surface absolute humidity for
2001–2005 JJA in <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">kg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for daytime <bold>(a)</bold> and nighttime <bold>(b)</bold>.
Shaded areas represent a statistically significant impact at the 98 % level
using the <inline-formula><mml:math id="M66" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> test.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/14059/2018/acp-18-14059-2018-f02.png"/>

        </fig>

      <p id="d1e1269"><?xmltex \hack{\newpage}?>The diurnal cycle of absolute humidity is plotted in
Fig. <xref ref-type="fig" rid="Ch1.F1"/>, second column. In absolute
values, maximum values are reached during late afternoon hours, when the
evaporation from the surface is highest, reaching 9–10 <inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">kg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. As
expected, humidity is decreased due to the presence of urban surfaces, caused
mainly by decreased evaporation and increased runoff. The decrease is
largest simultaneously with the largest absolute values occurring during 19:00–20:00. It can reach <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">kg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>.
The plot also reveals that
during nighttime, the urban impact on absolute humidity can be positive.
Similarly, the humidity values from the urban vicinity are slightly lower than
over the city (seen in the URBAN experiment). This is probably connected to
higher capacity of urban air to hold water vapor (due to higher nighttime
temperatures), or in other words, rural air cools more quickly during the night
and more vapor is removed by condensation on the surface. Higher humidity
during nighttime due to the urban surfaces is also seen on the spatial
distribution of the impact in Fig. <xref ref-type="fig" rid="Ch1.F2"/>, where it can reach
0.2 <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">kg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, especially for cities over the western part of the
d<?pagebreak page14065?>omain, probably due to the more humid maritime climate that they have. On the other
hand, during daytime, a clear decrease of absolute moisture is modeled, with
peaks over cities often exceeding <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">kg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (e.g., for Milan, or
Budapest).</p>
      <p id="d1e1376">In the case of the impact on wind, as expected, the wind speeds during the day
are higher compared to those during the night. The decreases can reach about
<inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>
to <inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">ms</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and their timings match the timing of the highest
absolute wind speeds during daytime. This is expected as the change is
proportional to the absolute values. The impact on wind is smallest around
19:00–20:00, when the evening PBL transition occurs <xref ref-type="bibr" rid="bib1.bibx31" id="paren.77"/>.</p>
      <p id="d1e1416">The last column of Fig. <xref ref-type="fig" rid="Ch1.F1"/> shows
the diurnal cycle of the vertical maximum of the turbulent diffusion
coefficient. A systematic increase by 10–20 <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> is
modeled due to urban surfaces throughout the day, with a maximum occurring
during morning hours. The minimum is modeled during afternoon to late evening
hours. The impact on the city vicinities is practically negligible.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Impact on aerosols</title>
      <p id="d1e1446">Regarding the impact of urban canopy meteorological forcing on aerosol
concentration, we will start with the impact on the <inline-formula><mml:math id="M78" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> surface
concentrations. Next, the impact on its components, i.e., primary and
secondary (in)organic aerosols, will be evaluated. For all aerosol types,
besides the total impact, results will also be provided for the individual
components (<inline-formula><mml:math id="M79" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M80" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula> impact). These aerosol components are
considered: sulfates (<inline-formula><mml:math id="M83" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), nitrates (<inline-formula><mml:math id="M84" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PNO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), ammonium (<inline-formula><mml:math id="M85" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PNH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), primary
organic aerosol (POA), primary elemental carbon (PEC), other fine particulate
matter (FPRM) and secondary organic aerosol (SOA). Further, for each
component, both the spatial distribution of the impact and also the diurnal
cycle over selected cities is presented. In the spatial distribution figures,
shaded areas represent statistically significant differences at the 98 %
level using the <inline-formula><mml:math id="M86" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> test.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p id="d1e1537">Absolute surface <inline-formula><mml:math id="M87" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations in <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> averaged over the 2001–2005 JJA period for the NOURBAN experiment
(i.e., without urban surface meteorological effects) and with the experiment
for which all urban meteorological effects are considered. Circles represent
measured values from the AirBase database.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/14059/2018/acp-18-14059-2018-f03.png"/>

        </fig>

<sec id="Ch1.S3.SS2.SSS1">
  <?xmltex \opttitle{PM${}_{{2.5}}$}?><title>PM<inline-formula><mml:math id="M89" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula></title>
      <p id="d1e1590">Figure <xref ref-type="fig" rid="Ch1.F3"/> shows the modeled 2001–2005 average
surface concentration of <inline-formula><mml:math id="M90" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> for the NOURBAN experiment (left)
and for the experiment with all meteorological effects included
(URB_t+q+uv+Kv; right). Colored dots denote measured averages extracted
from the European Environment Agency AirBase data background stations.
Largest <inline-formula><mml:math id="M91" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> values are modeled over highly populated large
agglomerations like the Ruhr area in Germany, the Po valley in northern Italy or
southern Poland, where summer average values can reach 30–50 <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. The comparison to measured data shows some model underestimation,
especially over central European countries and northern Italy, where model
values are lower by 5–10 <inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. On the other hand, over large
parts of Germany, model results agree with measurements or are slightly
positively biased. If considering the urban canopy meteorological effects,
<inline-formula><mml:math id="M94" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is clearly decreased by about 3 <inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> over urban
areas. This leads to better model results over parts of western Europe, but
over areas where <inline-formula><mml:math id="M96" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is underestimated, the model bias is
increasing.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p id="d1e1699">Impact of urban canopy meteorological forcing on <inline-formula><mml:math id="M97" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
surface concentrations in <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for the 2001–2005 JJA period for <bold>(a)</bold> temperature (<inline-formula><mml:math id="M99" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>), <bold>(b)</bold> humidity (<inline-formula><mml:math id="M100" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula>), <bold>(c)</bold> wind
(<inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula>), <bold>(d)</bold> turbulence (<inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula>) and <bold>(e)</bold> total impact. Shaded areas represent a statistically
significant impact at the 98 % level using the <inline-formula><mml:math id="M103" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> test.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/14059/2018/acp-18-14059-2018-f04.png"/>

          </fig>

      <p id="d1e1796">The perturbation of <inline-formula><mml:math id="M104" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> surface concentrations due to urban
canopy meteorological changes is plotted in Fig. <xref ref-type="fig" rid="Ch1.F4"/> for
the temperature, humidity, wind and turbulence impact as well as the combined
total impact (from left to right from top to bottom). Regarding the
temperature impact, there is a domain-wide decrease peaking over cities with
values from <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, especially over the western part of
the domain (e.g., over the Ruhr area in Germany). Smaller decreases are
modeled for central and eastern European cities (up to <inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> decrease). The impact is not only seen over urban areas but
propagates to rural ones as well, with statistically significant decreases
around <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.1</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. Changes in moisture content (decrease
on average) only cause a slight decrease of <inline-formula><mml:math id="M113" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> over most of the
western part of the domain up to <inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. Over other parts,
small increases are modeled. The urbanization-induced wind stilling causes
<inline-formula><mml:math id="M116" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to increase over most of the domain, with peaks, as expected,
over cities up to 2 <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. Statistically significant increases
are modeled even over rural areas, with less urban fraction often exceeding
0.5 <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. <inline-formula><mml:math id="M119" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> responds to the increased vertical
mixing due to urban surfaces with decreases over cities by up to <inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, again mainly over the western part of the region in focus. Above
some rural areas, statistically significant increases are modeled; however
these are very small, not exceeding 0.1 <inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and most often
below 0.05 <inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. The total impact of all the considered
components shows spatial similarities with the turbulence impact – it is
enhanced or suppressed depending on the competition between the temperature
(decreases) and wind impact (increases). However, over most of the cities,
the temperature impact is stronger in magnitude than the wind impact, causing
the total impact to be enhanced, often reaching <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>
decrease.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p id="d1e2121">Impact of urban canopy meteorological forcing on <inline-formula><mml:math id="M126" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
average diurnal cycle of surface concentrations for the 2001–2005 JJA period
for two selected cities (Berlin and Prague) in <inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. Bold lines
represent the absolute concentrations (left <inline-formula><mml:math id="M128" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis) for the NOURBAN run
(blue) and the total impact URB_t+q+uv+Kv run (purple). Dashed lines
(right <inline-formula><mml:math id="M129" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis) show the change due to changes of individual meteorological
components (temperature – orange, humidity – aquamarine, wind – green,
turbulence – olive and total impact – purple).</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/14059/2018/acp-18-14059-2018-f05.png"/>

          </fig>

      <?pagebreak page14067?><p id="d1e2174">As has already been pointed out, the urban meteorological phenomenon has a
well defined diurnal cycle. Thus, it can be expected that the above-presented
impacts on aerosol are not uniformly distributed across the day but will have
a specific diurnal cycle too. In Fig. <xref ref-type="fig" rid="Ch1.F5"/> the diurnal
variation of the <inline-formula><mml:math id="M130" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> absolute surface concentrations and their
change over two representative cities, Berlin and Prague, is presented. The
impact over other cities is qualitatively the same in shape, only with different
magnitudes. The absolute values (solid lines) are plotted for the NOURBAN
case and for the experiment with all urban meteorological effects considered
(URB_t+uv+q+Kv). The changes due to individual and combined urban
meteorological effects are plotted with dashed lines. Fine particulates'
concentrations for the selected cities have a clear diurnal cycle with maxima
(minima) around 18:00–22:00 (10:00–14:00) <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> occurring around
19:00–20:00 (13:00-14:00). Regarding the diurnal cycle of the effect of individual
meteorological components, there are, however, substantial differences.
Temperature (orange) causes decreases by up to 1.5–2 <inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, with
a maximum during nighttime, while the minimum occurs around noon (around <inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> change). As already seen in the spatial figure, the
changes due to modified humidity (aquamarine) are very low, not exceeding 0.05 <inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. A wind decrease causes an increase in urban <inline-formula><mml:math id="M136" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
concentrations (green) by around 0.5–1 <inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> throughout the day,
while changes are higher when the absolute values are higher too, i.e., during
the evening and nighttime. A very clear daily cycle is modeled for the
turbulence-induced concentration change (olive), with a profound maximum (of the absolute
change) occurring at 18:00–19:00, with values around <inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.6</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for Berlin and Prague, respectively. The daily cycle of the total
impact (purple) has a similar shape to the turbulence impact, with a maximum
occurring around 18:00–19:00, reaching <inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for Berlin and
Budapest, respectively. A smaller secondary peak occurs during nighttime,
when the temperature component is strong. In summary, the most emphasized
change is caused by increased turbulence; thus the total impact is dominated
by this component too.</p>
      <p id="d1e2386">It is clear that, in general, different components of the fine aerosol will
contribute differently to the absolute concentrations as well as to the
changes presented above. To see what the relative importance of each
aerosol type is, in Fig. <xref ref-type="fig" rid="Ch1.F6"/> we plotted the relative
composition of the average summer aerosol for six selected cities. The largest
contribution is made by sulfates and nitrates, being around 50 %, while
sulfates dominate, especially over eastern European cities. Ammonium
constitutes about 15 % of the total fine aerosol. In the emission
database used (TNO), emissions of <inline-formula><mml:math id="M144" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">SO</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> over eastern European countries are
much higher than over western Europe, while the opposite is true for the
<inline-formula><mml:math id="M145" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> emissions. As ammonium emissions are also slightly higher over
western Europe, it is clear that over eastern Europe, sulfate ions will
prefer to stabilize nitrate ions, resulting in ammonium sulfate formation,
while over western Europe, the emissions ratios will favor the formation of
ammonium nitrates <xref ref-type="bibr" rid="bib1.bibx68" id="paren.78"/>. Primary organic aerosol, primary
elemental carbon (black carbon) and other fine particulate matter constitutes
around 10 %, 5 % and 10 %, respectively. Secondary organic aerosol has the
lowest contribution of around a few percent. In the following, the impact of each
component of the urban meteorological forcing on the individual aerosol type
will be analyzed, starting with the primary aerosols. Note that we ignored
the humidity effect, as its contribution to the total <inline-formula><mml:math id="M146" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> change
turned out to be minor.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><caption><p id="d1e2430">Average percentual composition of urban 2001-2005 JJA average
<inline-formula><mml:math id="M147" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> aerosol for selected cities: <inline-formula><mml:math id="M148" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> – sulfates, <inline-formula><mml:math id="M149" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PNO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> –
nitrates, <inline-formula><mml:math id="M150" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PNH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> – ammonium, POA – primary organic carbon, PEC – black carbon,
FPRM – other fine particle matter, SOA – secondary organic aerosol</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/14059/2018/acp-18-14059-2018-f06.png"/>

          </fig>

<?xmltex \hack{\newpage}?>
</sec>
<?pagebreak page14068?><sec id="Ch1.S3.SS2.SSS2">
  <title>Primary aerosols</title>
      <p id="d1e2491">Figure <xref ref-type="fig" rid="Ch1.F7"/> shows the spatial distribution of urban
meteorological forcing on the surface concentration of primary aerosols, POA,
PEC and FPRM. In the chosen model configuration, these primary aerosols do no
interact with chemistry, and their emissions as well as their contribution to
the total fine aerosol over urban areas are comparable (see
Fig. <xref ref-type="fig" rid="Ch1.F6"/>). Therefore, their response to different
meteorological modifications is comparable. The impact of temperature changes
is minor, reaching only a few <inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> change over urban
areas. A more emphasized impact is modeled due to urban wind changes reaching
0.3–0.4 <inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> over many cities. Increased turbulence leads to
statistically significant changes almost over the entire domain, with
decreases up to <inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. The total impact reflects the
opposite sign of the wind and turbulence changes and is somewhat lower
reaching <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, but over some areas where the wind impact
dominates, it can be even positive up to 0.2 <inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. Due to lower
values, the statistically significant changes occupy smaller areas,
mainly limited around large cities.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><caption><p id="d1e2626">Impact of urban canopy meteorological forcing on <bold>(a–c)</bold> POA, PEC, FPRM average 2001–2005 JJA surface concentrations in
<inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. The columns from left to right correspond to temperature,
wind, turbulence and the total impact. Shaded areas represent a statistically
significant impact at the 98 % level using the <inline-formula><mml:math id="M160" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> test.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/14059/2018/acp-18-14059-2018-f07.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><caption><p id="d1e2666">Impact of urban canopy meteorological forcing on <bold>(a–c)</bold> POA, PEC and FPRM average diurnal cycle of surface concentrations for
the 2001–2005 JJA period for two selected cities (Berlin and Prague) in
<inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. Bold lines represent the absolute concentrations (left
<inline-formula><mml:math id="M162" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis) for the NOURBAN run (blue) and the total impact URB_t+q+uv+Kv
run (purple). Dashed lines (right <inline-formula><mml:math id="M163" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis) show the change due to changes of
individual meteorological components (temperature – orange, humidity –
aquamarine, wind – green, turbulence – olive and total impact – purple).</p></caption>
            <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/14059/2018/acp-18-14059-2018-f08.png"/>

          </fig>

      <p id="d1e2712">The diurnal cycle of the absolute urban primary aerosol concentration as well
as changes due to urban meteorological forcing is shown in
Fig. <xref ref-type="fig" rid="Ch1.F8"/>. The pattern is very similar for both
selected cities, with two maxima for the absolute values mainly caused by the
diurnal cycle of urban emissions (mainly morning and evening heavy traffic).
As seen in the spatial figures, the temperature impact is almost zero, with a
tiny negative peak during evening hours when the absolute values are highest.
The wind-induced changes are similar in magnitude throughout the day, with a
maximum again during evening hours reaching 0.1–0.2 <inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for
the selected cities. The strongest impact is modeled for the turbulence
effects, with a very well expressed peak occurring during evening hours
(around 18:00). The strong <inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula> impact determines the cycle of the total impact
as well, which is slightly smaller due to the positive impact of the wind
changes. These results are similar to the diurnal cycle of <inline-formula><mml:math id="M166" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
values except that the <inline-formula><mml:math id="M167" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> impact is much stronger in the case of <inline-formula><mml:math id="M168" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.
This gives us a hint that the reason for this difference will probably lie in the contribution of secondary aerosol. In the following, we will look at their
contribution to the overall final aerosol modifications.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS3">
  <title>Secondary aerosols</title>
      <p id="d1e2783">Figure <xref ref-type="fig" rid="Ch1.F9"/> plots the spatial distribution of the
urban meteorological forcing on the surface concentration of secondary
inorganic aerosols, <inline-formula><mml:math id="M169" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M170" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PNO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M171" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PNH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, as well as of secondary organic
aerosols. The urban temperature changes cause a decrease of each aerosol type,
while the strongest decrease is modeled for nitrates, up to <inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. Sulfates decrease over urban areas by up to 0.3 <inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>
and ammonium is decreased by up to 0.4–0.5 <inline-formula><mml:math id="M175" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. The smallest
decrease is modeled for the SOA. Consequently, from secondary aerosols,
nitrates contribute the most to the temperature-induced <inline-formula><mml:math id="M176" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
changes. In the case of the wind impact, there is an evident increase in
concentration due to suppressed dilution from sources for all the examined
aerosol components. Here again, the strongest increases are modeled for
nitrates, up to 0.6–0.8 <inline-formula><mml:math id="M177" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (especially over western Europe),
while for sulfates and ammonium, the change reaches 0.3–0.4 <inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. For SOA, being a relatively minor modeled aerosol component, the
wind-induced changes encompass very small increases up to 0.015 <inline-formula><mml:math id="M179" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. A more complicated response of surface aerosol concentrations is
modeled for changes in the vertical eddy diffusion. In the western part of the
domain and over large cities, an increase in the diffusion coefficient leads to
a decrease of surface aerosols up to <inline-formula><mml:math id="M180" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M181" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, especially for
sulfates and ammonium. Over eastern Europe, a slight increase in secondary
aerosol is modeled, reaching 0.05 <inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> over larger areas. The
SOA is an exception here, where concentrations are suppressed all over the
domain, peaking over urban areas up to <inline-formula><mml:math id="M183" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p id="d1e3037">Impact of urban canopy meteorological forcing on <bold>(a–d)</bold> <inline-formula><mml:math id="M185" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M186" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PNO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M187" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PNH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and SOA average 2001–2005 JJA surface concentrations
in <inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. The columns from left to right correspond to
temperature, wind, turbulence and the total impact. Shaded areas represent a statistically significant impact
at the 98 % level using the <inline-formula><mml:math id="M189" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> test.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/14059/2018/acp-18-14059-2018-f09.png"/>

          </fig>

      <p id="d1e3109">As it combines both decreases (temperature and turbulence impact) and
increases (wind and partly the turbulence impact), the total impact of all
meteorological effects often tends to be smaller and the areas of statistical
changes occupy a smaller fraction of the domain. This is clearly seen in the case of <inline-formula><mml:math id="M190" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, where due to the combined effects of the urban meteorological
forcing, statistically significant effects are only modeled for the Ruhr area
in northwestern Germany, controlled by the temperature- and turbulence-induced
decrease reaching <inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. For PNO3 the combined
meteorological impact manifests itself as a statistically significant
decrease of concentrations over large cities, while the highest values (up to
<inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) are modeled over the largest cities. A similar
picture is obtained for ammonium, for which statistically significant decreases
are modeled for the western part of the domain. In each case above,
statistically significant effects are controlled by the combined effect of
temperature and turbulence, while the wind-induced increase is too small to
counterbalance them. For SOA, the situation is similar: the total impact is
dominated by decreases due to temperature- and turbulence-induced decreases,
reaching a <inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> decrease over urban areas.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><caption><p id="d1e3214">Same as Fig. <xref ref-type="fig" rid="Ch1.F9"/> but for <inline-formula><mml:math id="M197" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <bold>(a)</bold> and <inline-formula><mml:math id="M198" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <bold>(b)</bold> in <inline-formula><mml:math id="M199" display="inline"><mml:mi mathvariant="normal">ppbv</mml:mi></mml:math></inline-formula>.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/14059/2018/acp-18-14059-2018-f10.png"/>

          </fig>

      <p id="d1e3261">In order to better understand the modeled response of secondary inorganic
aerosol to changed meteorological forcing, we plot the response of the
precursor species as well. In <xref ref-type="bibr" rid="bib1.bibx31" id="text.79"><named-content content-type="post">Fig. 6</named-content></xref>, the response of
<inline-formula><mml:math id="M200" display="inline"><mml:mrow class="chem"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> to urbanization-induced meteorological changes was presented and
increases of species surface concentrations were modeled due to decreased
wind up to 2 ppbv. Due to turbulence increase, <inline-formula><mml:math id="M201" display="inline"><mml:mrow class="chem"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> responded with
a decrease up to <inline-formula><mml:math id="M202" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> ppbv. Here, in Fig. <xref ref-type="fig" rid="Ch1.F10"/>, the
responses
of sulfur dioxide (<inline-formula><mml:math id="M203" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and ammonia (<inline-formula><mml:math id="M204" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) surface
concentrations are presented as precursors of sulfates and particulate
ammonium (ammonium sulfates and ammonium nitrates). For both aerosol types,
surface concentrations decrease due to increased urban temperatures, by up to
<inline-formula><mml:math id="M205" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> ppbv, and this is probably<?pagebreak page14069?> connected to increased dry
deposition. Lower urban winds cause reduced horizontal dilution, resulting in
higher concentrations: this is seen for both <inline-formula><mml:math id="M207" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M208" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> of which concentrations are usually enhanced around cities by up to 2–4 ppbv.
However, in the case of sulfur dioxide, some rural areas encounter decreases,
probably due to the fact that transport is suppressed to these areas due to
reduced wind speeds. The same holds for ammonia; however, the decrease here is
very small. Enhanced urban turbulence leads to a clear decrease of
<inline-formula><mml:math id="M209" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> surface concentrations over and near urban areas, by up to <inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> ppbv. In the case of <inline-formula><mml:math id="M211" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, this decrease reaches <inline-formula><mml:math id="M212" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn></mml:mrow></mml:math></inline-formula> ppbv. A more
diverse picture is obtained for the combined effect of urban meteorological
changes, and both decreases and increases are encountered over and around
cities between <inline-formula><mml:math id="M214" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> and 3 ppbv (somewhat smaller values for ammonia). This is
probably caused by the competing effect of wind-induced increase and decrease
due to increased vertical eddy transport. In summary, primary precursors
respond to increased urban temperatures, decreased urban winds and increased
turbulence by a slight decrease, larger decrease and increase, respectively.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F11" specific-use="star"><caption><p id="d1e3435">Impact of urban canopy meteorological forcing on <bold>(a–d)</bold> <inline-formula><mml:math id="M215" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M216" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PNO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M217" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PNH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and SOA average diurnal cycle of surface
concentrations for the 2001–2005 JJA period for two selected cities (Berlin
and Prague) in <inline-formula><mml:math id="M218" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. Bold lines represent the absolute
concentrations (left <inline-formula><mml:math id="M219" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis) for the NOURBAN run (blue) and the total impact
URB_t+q+uv+Kv run (purple). Dashed lines (right <inline-formula><mml:math id="M220" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis) show the change
due to changes of individual meteorological components (temperature –
orange, humidity – aquamarine, wind – green, turbulence – olive and total
impact – purple).</p></caption>
            <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/14059/2018/acp-18-14059-2018-f11.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12"><caption><p id="d1e3516">Impact of urban canopy meteorological forcing on the vertical
profile of <inline-formula><mml:math id="M221" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations for two selected cities, Berlin and
Prague, in <inline-formula><mml:math id="M222" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> averaged over the 2001–2005 JJA period (temperature impact – orange, humidity impact – aquamarine, wind impact –
green, turbulence – brown and total impact – purple). Vertical axis shows
the layer interface heights in meters for the 18 CTM layers.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/14059/2018/acp-18-14059-2018-f12.png"/>

          </fig>

      <p id="d1e3555">The diurnal cycle of the impact of urban meteorological forcing on secondary
(in)organic aerosol is shown in Fig. <xref ref-type="fig" rid="Ch1.F11"/> for two
selected cities, Berlin and Prague. As the formation of these, beginning with
uptake in the water phase and nucleation, is highly temperature-dependent and
lower temperatures favor gas–particle partitioning, the absolute values
(taken from the NOURBAN and URB_t+q+uv+Kv runs) are lower during
daytime, as expected. This behavior is evident from the <inline-formula><mml:math id="M223" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> impact (orange): it
follows the cycle of the urban impact on temperature, being largest during
nighttime hours when the UHI is the strongest. It is clearly seen that the
temperature impact is the dominant impact for nitrates and ammonium (note the
total impact curve in purple). The changes of aerosol concentrations due to
modified moisture content are negligible, as already seen for <inline-formula><mml:math id="M224" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.
The impact of wind changes follows the spatial result seen in
Fig. <xref ref-type="fig" rid="Ch1.F9"/> and is characterized by increases: it is
usually lower during daytime, when absolute values are also low compared to
nighttime values.</p>
      <p id="d1e3581">The impact of increased turbulence is evident in the case of SOA, which seems
to be the main contributor to the total impact for both cities. It
only causes small changes for nitrates and ammonium. In the case of <inline-formula><mml:math id="M225" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, however, the
two cities differ: while in Berlin, increased vertical mixing removes some
sulfates from the surface layer, reducing its concentrations, for Prague, the
behavior is more complicated, and concentrations can even increase due to
higher vertical mixing. The change is relatively small, however, in the case<?pagebreak page14070?> of
Prague, and the concentrations can vary as a function of some secondary
nonlinear effects like transport from higher model levels to lower ones due
to residual turbulence during nighttime.</p>
      <p id="d1e3595">In order to obtain an idea of the vertical extent of these effects that take place, in Fig. <xref ref-type="fig" rid="Ch1.F12"/> we plotted the vertical profile of
individual impacts on <inline-formula><mml:math id="M226" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations for Berlin and Prague.
As expected, the temperature, turbulence and the total impact reduce surface
concentrations while the wind increases them. At around 900–1200 m the changes
quickly become very small, and for the temperature effect, almost negligible. At
higher levels, the turbulence impact changes sign and shows a strong maximum
around 2700 m. The same secondary maximum occurs for the wind impact.
Consequently, the combined impact also has this large positive maximum,
reaching 0.2–0.3 <inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>.</p>
</sec>
</sec>
</sec>
<?pagebreak page14071?><sec id="Ch1.S4" sec-type="conclusions">
  <title>Discussion and conclusions</title>
      <p id="d1e3638">The modeled meteorological response due to introduction of urban canopy shows
expected features. The impact on temperature and its daily cycle has a very
similar magnitude as well as shape to those in numerous previous studies examining
European cities <xref ref-type="bibr" rid="bib1.bibx60 bib1.bibx19 bib1.bibx72 bib1.bibx67" id="paren.80"/>
but similar diurnal variations of the UHI (which is close to the impact of urban
land surface on temperature) were obtained for cities over other continents
<xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx65" id="paren.81"/>. Due to a notable increase in nighttime temperature
and only a slight enhancement of the daytime ones, a strong decrease of
diurnal temperature range is modeled, with values comparable to previous
works <xref ref-type="bibr" rid="bib1.bibx76" id="paren.82"><named-content content-type="pre">e.g.</named-content></xref>. The simulated wind speed changes are also
consistent with previous model experiments performed over Europe
<xref ref-type="bibr" rid="bib1.bibx72 bib1.bibx78" id="paren.83"/> or over Chinese urban areas
<xref ref-type="bibr" rid="bib1.bibx25 bib1.bibx90" id="paren.84"/>. The sudden drop of wind impact to almost zero during
evening hours is caused by relatively high downward momentum flux due
to enhanced turbulence <xref ref-type="bibr" rid="bib1.bibx31" id="paren.85"/> during the evening transition period
<xref ref-type="bibr" rid="bib1.bibx43" id="paren.86"/>. Concerning the urban impact on the turbulence, our
simulated eddy diffusion coefficient and their changes are in line with what
was previously modeled over urban areas <xref ref-type="bibr" rid="bib1.bibx40" id="paren.87"/> or in general over
complex terrain <xref ref-type="bibr" rid="bib1.bibx11" id="paren.88"/>, although they are slightly smaller. This
is probably<?pagebreak page14072?> caused by the inconsistencies introduced by the diagnostic
calculation of vertical diffusivity values rather than directly taking them
from the PBL scheme of the driving model used.</p>
      <p id="d1e3671">Due to the urban canopy, humidity decreased on average in our simulations, which
is in line with expectations. Urban areas are covered with materials that
have a low evapotranspiration and are covered with minimal vegetation.
Further, due to high runoff, the precipitated water is transported by sewer
system away from urban areas. In summary, sources of moisture over urban
areas are limited compared to rural surfaces with a much higher fraction of
vegetation <xref ref-type="bibr" rid="bib1.bibx61" id="paren.89"/>. However, during nighttime a slight increase in
the absolute humidity is observed in the model. In general, this can be a result
of both the increased source of moisture and the decreased sink. The first possible
reason can be dismissed. Regarding the reduced sinks of moisture, this is a
straight consequence of high urban temperatures. Compared to rural
environments, urban areas can hold a larger quantity of moisture as a
consequence of the Clausius–Clapeyron equation. In rural areas during the night,
the temperature often drops below the dew point, resulting in condensation, which
acts as a sink. This does not occur, however, to such an extent in urban areas, where a
reduced dew deposition has been observed in correspondence with expectations <xref ref-type="bibr" rid="bib1.bibx62" id="paren.90"/>. Hence, urban nighttime absolute humidity can
be slightly higher than the rural one, at least near the surface.</p>
      <p id="d1e3680">It has been shown that the urban canopy meteorological forcing decreases
fine aerosol concentrations, and this decrease is strongest during late
afternoon hours. The component analysis of the response revealed that the
most important contributor to this change is the enhanced turbulence over
cities, which facilitates the removal of both the aerosol itself and also its precursors (as seen for <inline-formula><mml:math id="M228" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M229" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and noted for
<inline-formula><mml:math id="M230" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). The diurnal change caused by all the considered meteorological
changes has an almost identical shape to the change caused purely by the
turbulence enhancement, especially at high absolute values. Our results
confirm the strong connection between aerosol concentration and vertical
turbulent transport that has been confirmed already by many authors
<xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx90" id="paren.91"><named-content content-type="pre">e.g.</named-content></xref>. These authors revealed, in line with
our results, that urbanization-triggered enhanced turbulence reduces the
modeled aerosol concentrations. It is mainly the primary aerosol (organics,
black carbon and other fine particulate matter) which has the most pronounced
responses to the turbulence changes.</p>
      <p id="d1e3721">Regarding the wind impact, our expectation has been confirmed – there is a
clear relationship between urban wind speeds and air pollution: reduced wind
causes reduction in pollutant dispersion, leading to increased concentration
near the sources or vice versa. This is in line with the recent findings of
<xref ref-type="bibr" rid="bib1.bibx33" id="text.92"/>, who showed that albedo-induced increases in urban
wind speeds result in a decrease of <inline-formula><mml:math id="M231" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations. The wind-induced aerosol increase has a clear diurnal cycle that reflects the cycle of
the absolute values: an approximately 2 times higher increase is modeled for nighttime
(from early evening to early morning) than for daytime.</p>
      <?pagebreak page14074?><p id="d1e3739">The simulated changes due to urban temperature increase are only evident in the case of secondary aerosols. This is expected as temperature strongly controls
the gas–particle partitioning and nucleation of aerosols with high
temperatures, reducing the tendency to form particles. In this regard, it is
not surprising that temperature-induced changes are strong in the case of
secondary aerosols and are negligible for primary ones. To support our
finding about the temperature-driven decrease of secondary aerosol
concentrations, <xref ref-type="bibr" rid="bib1.bibx34" id="text.93"/> and <xref ref-type="bibr" rid="bib1.bibx7" id="text.94"/> earlier reached the conclusion that secondary inorganic aerosol and SOA included in PM
decrease as they shift from the particle to the gas phase with increasing
temperature. In our simulations, this is most evident for nitrates, in line
with <xref ref-type="bibr" rid="bib1.bibx52" id="text.95"/> and <xref ref-type="bibr" rid="bib1.bibx7" id="text.96"/>.</p>
      <p id="d1e3754">An almost negligible impact on <inline-formula><mml:math id="M232" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is modeled due to changes in
moisture content. It has a slight effect on dry deposition velocities of
gases via increasing stomatal and cuticle resistance due to higher relative
humidity <xref ref-type="bibr" rid="bib1.bibx87" id="paren.97"/>. Further, reduced moisture negatively affects the
hydroxyl radical concentrations, reducing the oxidative capacity of the air
above urban areas. However, both processes are probably of minor importance
as the moisture variations are small.</p>
      <p id="d1e3771">The simulated impacts on secondary organic aerosol are in line with
expectations, although they are very small in magnitude. Higher urban
temperatures negatively affect the nucleation rates of organic vapors, leading
to the reduced SOA concentrations. Decreased urban winds reduce the dispersion
of SOA, leading to a slight increase in condensation. Thirdly, enhanced urban
turbulence favors the removal of both SOA and its precursors (semi-volatile
hydrocarbons), resulting in lower concentrations, which seems to dominate the
overall urban impact. This stands in contrast with inorganic aerosols, for
which the urbanization-induced turbulence increase resulted in both a concentration decrease
and increase. This can be explained by the different emission ratios of the
primary precursor species across the domain. Thus, turbulence impacts them
with different magnitudes, and the competition between sulfates, nitrates and
ammonium ions leads to different inorganic aerosol responses.</p>
      <p id="d1e3774">Our results showed that the effects of urban canopy meteorological forcing
are getting weaker with increasing height, which is not surprising, as the
meteorological changes are often limited to the first few model layers
<xref ref-type="bibr" rid="bib1.bibx28" id="paren.98"/>. The turbulence here is a different case, and
<xref ref-type="bibr" rid="bib1.bibx31" id="text.99"/> showed that it can be significantly perturbed over cities
at higher model layers as well (up to 2200 m). This can explain the vertical
secondary maximum occurring for the turbulence impact: it transports
pollutants from the surface to higher model layers; however, at certain
heights the turbulence is no longer affected by the urban areas and aerosol
can thus accumulate, increasing the upper level concentrations. For the wind
impact, the situation can be similar. Higher surface concentrations result
in more PM transported to higher model layers.</p>
      <p id="d1e3783">An important question is whether the inclusion of urban canopy effects in the
driving meteorological fields reduces the simulated aerosol bias. This is not
clear from the results. In areas where fine aerosol was overestimated by the
model, especially over western Europe, a decrease of <inline-formula><mml:math id="M233" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> reduced
the model bias. On the other hand, over eastern Europe, the model error is
enhanced as aerosol was underpredicted in our model here. In general, the
effort of more realistic representation of different processes in models does
not always imply better model performance. However, this should not
discourage the improvement of models, and in our case, it is evident that accounting
for the urbanization-induced meteorological changes in air quality simulations leads
to modified concentrations that cannot be disregarded in future urban air
quality oriented studies. Especially the temperature, wind and eddy diffusion
fields must be correct and reflect urban conditions.</p>
      <p id="d1e3797">There are some further documented effects of the urban canopy on meteorology, for
example, the urban breeze circulation <xref ref-type="bibr" rid="bib1.bibx23" id="paren.100"/>, which affects
pollutant transport over city scales <xref ref-type="bibr" rid="bib1.bibx65" id="paren.101"/>. Another meteorological
phenomenon occurring over urban areas is the impact on convection: the UHI-triggered convergence zone over urban areas favors the development of
convection and increases the frequency of extreme precipitation
<xref ref-type="bibr" rid="bib1.bibx88" id="paren.102"/>, directly influencing the air quality by decreased solar
radiation (due to cloud cover) and increased wet removal of pollutants.<?pagebreak page14075?> These
effects, however, act over scales that were not resolved in our modeling
setup;
thus applying higher resolutions for investigating the
urbanization–meteorology–air quality interactions is essential in future research.</p>
</sec>

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

      <p id="d1e3814">All data modeled and analyzed in this study are available
upon request. Please contact peter.huszar@mff.cuni.cz.</p>
  </notes><notes notes-type="authorcontribution">

      <p id="d1e3820">PH and TH designed the basic idea and organized the project team. PH and JK performed
the model simulations. MB configured the models and maintained the hardware the experiments were run on. TB and PP prepared the input and
validation data. PH wrote the paper with contributions from all other authors.</p>
  </notes><notes notes-type="competinginterests">

      <p id="d1e3826">The authors declare that they have no competing interests.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e3832">This work has been funded by the OP-PPR project (Operation Programme Prague
– Growth Pole)  CZ.07.1.02/0.0/0.0/16_040/0000383 “URBI PRAGENSI – Urbanization of weather forecast, air quality prediction and climate
scenarios for Prague”, by the PROGRESS Q47/Q16 – Programmes of Charles
University project, by the SVV 2018 project of Charles University and by the UNCE 2040202013
project. We further acknowledge the TNO MEGAPOLI emissions
dataset from the EU-FP7 project MEGAPOLI (<uri>http://megapoli.dmi.dk/</uri>, last access: 31 August 2018) and the
providers of the AirBase European Air Quality data
(<uri>https://www.eea.europa.eu/data-and-maps/data/aqereporting-8</uri>, last access: 31 August 2018).
<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Alex B. Guenther<?xmltex \hack{\newline}?>
Reviewed by: three anonymous referees</p></ack><ref-list>
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<abstract-html><p>The regional climate model RegCM4 extended with the land surface model CLM4.5
was coupled to the chemistry transport model CAMx to analyze the impact of
urban meteorological forcing on surface fine aerosol (PM<sub>2.5</sub>)
concentrations for summer conditions over the 2001–2005 period, focusing on
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modifications caused by urban canopy forcing, we found a significant increase
in urban surface temperatures (up to 2–3&thinsp;K), a decrease of specific humidity (by
up to 0.4–0.6&thinsp;gkg<sup>−1</sup>), a reduction of wind speed (up to −1&thinsp;ms<sup>−1</sup>) and an enhancement of vertical turbulent diffusion coefficient
(up to 60–70&thinsp;m<sup>2</sup>s<sup>−1</sup>).</p><p>These modifications translated into significant changes in surface aerosol
concentrations that were calculated by a <q>cascading</q> experimental approach.
First, none of the urban meteorological effects were considered. Then, the
temperature effect was added, then the humidity and the wind, and finally, the
enhanced turbulence was considered in the chemical runs. This facilitated the
understanding of the underlying processes acting to modify urban aerosol
concentrations. Moreover, we looked at the impact of the individual aerosol
components as well. The urbanization-induced temperature changes resulted in
a decrease of PM<sub>2.5</sub> by −1.5 to −2&thinsp;µg m<sup>−3</sup>, while decreased
urban winds resulted in increases by 1–2&thinsp;µg m<sup>−3</sup>. The enhanced
turbulence over urban areas resulted in decreases of PM<sub>2.5</sub> by −2&thinsp;µg m<sup>−3</sup>. The combined effect of all individual impact depends on
the competition between the partial impacts and can reach up to −3&thinsp;µg m<sup>−3</sup> for some cities, especially when the temperature impact was stronger
in magnitude than the wind impact. The effect of changed humidity was found
to be minor. The main contributor to the temperature impact is the
modification of secondary inorganic aerosols, mainly nitrates, while the wind
and turbulence impact is most pronounced in the case of primary aerosol (primary
black and organic carbon and other fine particle matter). The overall as well
as individual impacts on secondary organic aerosol are very small, with the
increased turbulence acting as the main driver. The analysis of the vertical
extent of the aerosol changes showed that the perturbations caused by urban
canopy forcing, besides being large near the surface, have a secondary
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the urban canopy meteorological effects in our chemistry simulations.</p></abstract-html>
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