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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-18-2049-2018</article-id><title-group><article-title>High-resolution sampling and analysis of ambient particulate matter in the
Pearl River Delta region of southern China: <?xmltex \hack{\break}?>source apportionment and health
risk implications</article-title><alt-title>High-resolution sampling and analysis of ambient particulate matter</alt-title>
      </title-group><?xmltex \runningtitle{High-resolution sampling and analysis of ambient particulate matter}?><?xmltex \runningauthor{S. Zhou et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Zhou</surname><given-names>Shengzhen</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Davy</surname><given-names>Perry K.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Huang</surname><given-names>Minjuan</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Duan</surname><given-names>Jingbo</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff5">
          <name><surname>Wang</surname><given-names>Xuemei</given-names></name>
          <email>eeswxm@mail.sysu.edu.cn</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Fan</surname><given-names>Qi</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Chang</surname><given-names>Ming</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Liu</surname><given-names>Yiming</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Chen</surname><given-names>Weihua</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Xie</surname><given-names>Shanju</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Ancelet</surname><given-names>Travis</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Trompetter</surname><given-names>William J.</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>School of Atmospheric Sciences, Sun Yat-sen University, Guangzhou, 510275, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Guangdong Province Key Laboratory for Climate Change and Natural Disaster Studies,<?xmltex \hack{\break}?> Sun Yat-sen University, Guangzhou 510275, China</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>National Isotope Centre, Institute of Geological and Nuclear Sciences, 30 Gracefield Road,<?xmltex \hack{\break}?> P.O. Box 31312, Lower Hutt, New Zealand</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Key Laboratory of Environmental Optics and Technology, Anhui Institute of Optics and Fine Mechanics,<?xmltex \hack{\break}?> Chinese Academy of Sciences, 350 Shu Shan Hu Road, Hefei, Anhui 230031, China</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Institute for Environment and Climate Research, Jinan University, Guangzhou, China</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Auckland Council, Auckland, New Zealand</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Xuemei Wang (eeswxm@mail.sysu.edu.cn)</corresp></author-notes><pub-date><day>13</day><month>February</month><year>2018</year></pub-date>
      
      <volume>18</volume>
      <issue>3</issue>
      <fpage>2049</fpage><lpage>2064</lpage>
      <history>
        <date date-type="received"><day>30</day><month>August</month><year>2017</year></date>
           <date date-type="rev-request"><day>6</day><month>November</month><year>2017</year></date>
           <date date-type="rev-recd"><day>2</day><month>January</month><year>2018</year></date>
           <date date-type="accepted"><day>6</day><month>January</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/18/2049/2018/acp-18-2049-2018.html">This article is available from https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018.html</self-uri><self-uri xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018.pdf</self-uri>
      <abstract>
    <p id="d1e223">Hazardous air pollutants, such as trace elements in
particulate matter (PM), are known or highly suspected to cause detrimental
effects on human health. To understand the sources and associated risks of PM
to human health, hourly time-integrated major trace elements in
size-segregated coarse (PM<inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:mtext>–</mml:mtext><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and fine (PM<inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> particulate
matter were collected at the industrial city of Foshan in the Pearl River
Delta region, China. Receptor modeling of the data set by positive matrix
factorization (PMF) was used to identify six sources contributing to
PM<inline-formula><mml:math id="M3" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M4" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> concentrations at the site. Dominant sources
included industrial coal combustion, secondary inorganic aerosol, motor
vehicles and construction dust along with two intermittent sources (biomass
combustion and marine aerosol). The biomass combustion source was found to be
a significant contributor to peak PM<inline-formula><mml:math id="M5" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> episodes along with motor
vehicles and industrial coal combustion. Conditional probability function
(CPF) analysis was applied to estimate the source locations using the
PMF-resolved source contribution coupled with the surface wind direction
data. Health exposure risk of hazardous trace elements (Pb, As, Si, Cr, Mn
and Ni) and source-specific values were estimated. The total hazard quotient
(HQ) of PM<inline-formula><mml:math id="M6" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> was 2.09, higher than the acceptable limit (HQ <inline-formula><mml:math id="M7" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1). The
total carcinogenic risk (CR) was 3.37 <inline-formula><mml:math id="M8" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for PM<inline-formula><mml:math id="M10" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, which
was 3 times higher than the least stringent limit (1.0 <inline-formula><mml:math id="M11" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>.
Among the selected trace elements, As and Pb posed the highest
non-carcinogenic and carcinogenic risks to human health, respectively. In
addition, our results show that the industrial coal combustion source is the
dominant non-carcinogenic and carcinogenic risk contributor, highlighting the
need for stringent control of this source. This study provides new insight
for policy makers to prioritize sources in air quality management and health
risk reduction.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e357">Ambient particulate matter (PM) is ubiquitously suspended in the atmosphere,
which profoundly affects human health, visibility and global climate. A
number of epidemiologic studies have suggested that short- or long-term
exposure to PM is associated with a growing risk of the respiratory and
cardiac illness, and even premature mortality (Pope et al., 2009;
Dockery et al., 1993). PM mass concentration is considered a standard
metric used for examining human health<?pagebreak page2050?> risks. More recently, the size and chemical
component of PM have been recognized as the important factors for their
toxicity. For instance, Kan et al. (2007) found significant associations of
daily mortality with PM<inline-formula><mml:math id="M13" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> (fine mode), but not with PM<inline-formula><mml:math id="M14" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:mtext>–</mml:mtext><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> (coarse mode) in Shanghai. Reche et al. (2012) reported higher toxicity
for PM<inline-formula><mml:math id="M15" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">1.0</mml:mn><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> than PM<inline-formula><mml:math id="M16" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:mtext>–</mml:mtext><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> to human cells. From the
epidemiological and experimental findings, it is convincing that trace
elements in the PM components such as Ni, V, Pb and Zn appear to be important causes of both
pulmonary and cardiovascular diseases (Chen and
Lippmann, 2009; Heal et al., 2012). Moreover, airborne particles and
associated trace elements originate from various emission sources, such as
motor vehicles, metallurgical industry, coal burning and soil dust, and could
be emitted in a broad size range. Studies suggest that some particle sources
are more harmful than others and recommend that controlling some of the
specific sources of PM could be a more effective way for protecting public
health (Bell et al., 2014; Khan et al., 2016). Airborne particle health risk
assessment is increasingly dependent on the source apportionment of PM using
chemical component data. In particular, elemental components are often
applied for PM source identification because of their atmospheric stability
and source specificity (Taiwo et al., 2014; Visser et al., 2015b).</p>
      <p id="d1e411">To identify the sources contributing to measured PM concentrations,
multivariate receptor models were used. Positive matrix factorization (PMF)
is a powerful and commonly used multivariate receptor technique that is
capable of resolving factors, or PM sources, without prior source knowledge.
It is, however, important to note that source-specific profiles
(fingerprints) must be known to properly assign the PMF model outputs. PMF
has a number of advantages over traditional factor analysis techniques
including non-negativity constraints and the ability to accommodate data that
are missing or below the detection limit. The results of the analysis are
directly interpretable as mass contributions to PM from each source factor
(Paatero and Tapper, 1994; Paatero, 1997; Song et al., 2001). A majority of
PM source apportionment studies in the literature are documented at a lower
temporal resolution, typically in 12–24 h integrated filter samples (Pant
and Harrison, 2012; Belis et al., 2013). Only limited studies have applied
PMF to determine the trace element emission sources at a high time (hourly)
resolution (Gao et al., 2016; Dall'Osto et al., 2013; Pancras et al., 2013;
Moreno et al., 2011; Crilley et al., 2017; Visser et al., 2015a; Ancelet et
al., 2012, 2014). Increasing the time resolution of measurements can capture
the impact of PM concentration and personal exposure from many intermittent
sources such as biomass combustion or industry emission plumes.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><caption><p id="d1e416">Location of sampling site at Foshan City in the PRD region of
southern China.</p></caption>
        <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018-f01.png"/>

      </fig>

      <p id="d1e425">The subtropical Pearl River Delta (PRD) region is one of the most urbanized
and industrialized areas in China. In recent years, the PRD region has been
facing severe particulate matter pollution and photochemical smog events
(Zhang et al., 2008; R. J. Huang et al., 2014), threatening the health of
over 57 million residents
(<uri>http://www.gdstats.gov.cn/tjnj/2016/directory.html</uri>). We have collected
hourly samples of fine (PM<inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and coarse (PM<inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:mtext>–</mml:mtext><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>
particulate matter at an important industrial city, Foshan, in the PRD
region. Trace elements were measured by the particle-induced X-ray emission
(PIXE) technique, providing hourly elemental concentration in the fine and
coarse PM. The average concentration, temporal and diurnal variations and
effects of meteorology on the trace element concentrations have been reported
in Zhou et al. (2016). In this study, we applied a PMF receptor model (EPA
PMF 5.0) to characterize the PM sources in Foshan city utilizing the
size-resolved hourly elemental data and other gas-phase pollutants. In
addition, we assessed the human health risk exposure to selected trace
elements in PM released from specific sources, as identified by the PMF
model. Our results provide valuable information for optimizing the
corresponding management and control strategies of PM pollution in the PRD
region and cities in other regions.</p>
</sec>
<sec id="Ch1.S2">
  <title>Sampling and analysis</title>
<sec id="Ch1.S2.SS1">
  <title>Description of the sampling site</title>
      <p id="d1e471">The monitoring station was located in Foshan, Guangdong Province, China
(Fig. 1), on top of the Foshan Environmental Monitoring Center (Foshan
EMC; 23.0025<inline-formula><mml:math id="M19" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 113.1035<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; approximately 35 m above ground level). Foshan
is one of the most important manufacturing hubs in China, characterized by
the ceramics industry and household appliance industry, and produces
<inline-formula><mml:math id="M21" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 15 % of China's home appliances and <inline-formula><mml:math id="M22" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 30 %
of the world's ceramics (Guo et al., 2011). Adjacent to the monitoring site
is a continuous sampling system measuring NO<inline-formula><mml:math id="M23" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> (Advanced Pollution
Instrumentation, API, model 200E), CO (API, model 300E), SO<inline-formula><mml:math id="M24" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> (API,
model 100E), O<inline-formula><mml:math id="M25" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> (API, model 300E) and PM<inline-formula><mml:math id="M26" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M27" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> (Thermo
Scientific, model FH62C14), operated by the Foshan Environmental Monitoring
Center. The station is surrounded by residential buildings and business
offices on flat terrain. Meteorological parameters, including wind speed
(WS), wind direction (WD), temperature (<inline-formula><mml:math id="M28" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula>), relative humidity (RH) and rainfall
were obtained from Foshan Meteorological Bureau. The meteorological station
is situated in the Foshan No. 1 Middle School, about 5 km north of Foshan
EMC. The time resolution for the meteorological data is 10 min.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>Sampling of aerosol</title>
      <p id="d1e565">Hourly time-integrated samples of size-segregated coarse
(PM<inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:mtext>–</mml:mtext><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and fine (PM<inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> PM samples were collected using
a modified Streaker sampler (PIXE International Corporation, USA ). The
Streaker sampler has previously been described in detail (Annegarn et al.,
1988), and used in a number of studies (Annegarn et al., 1992, 1996; Filippi
et al., 1999; D'Alessandro et al., 2004). The Streaker sampler system used in
this study is described in Zhou et al. (2016).<?pagebreak page2051?> Briefly, the Streaker sampler
consists of a pre-impactor that removes particles larger than PM<inline-formula><mml:math id="M31" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> from
the incoming air flow, a thin Kapton foil that collects coarse particles
through impaction and a Nucleopore filter (0.4 <inline-formula><mml:math id="M32" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m pore size) that
collects fine particles. An electronic control system regulates the Streaker
sampler pneumatics mass flow (1 L min<inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) and stepper motor rotation of
the filter between each user-defined sampling period. The hourly samples were
collected with discrete spacing between each deposit to ensure that each
deposit only consisted of particulate matter collected during the intended
hour. A total of 60 samples or 60 h can be collected on each filter.</p>
      <p id="d1e625">The high-resolution particulate matter sampling system was installed on the
roof of Foshan Environmental Monitoring Center. The sampler was set to
collect hourly samples beginning at 12:00 UTC<inline-formula><mml:math id="M34" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>8 on 24 October 2014 and
ending at 10:00 on 14 December 2014. A total of 47 samples or 2 days were
collected per filter (coarse and fine) with the sampling ending at 11:00
(47 h later), allowing an hour to change over filters before the sampling
was restarted again at 12:00. In all, 1127 samples each of PM<inline-formula><mml:math id="M35" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and
PM<inline-formula><mml:math id="M36" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:mtext>–</mml:mtext><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> were collected, representing 1127 h or 7 weeks of
sampling.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Sample analysis</title>
      <p id="d1e664">Ion beam analysis (IBA) was used to measure the concentrations of elements
with atomic numbers above neon in the PM samples. The IBA was performed using
a 3 MeV accelerator proton beam with standards (SrF<inline-formula><mml:math id="M37" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, NaCl, Cr, Ni,
SiO, KCl, Al) run before and after each analytical cycle. Spectral X-ray peak
deconvolution was performed using Gupix software (Maxwell et al., 1995). The
number of pulses (counts) in each peak for a given element is used by the
Gupix software to calculate the concentration of that element. The background
and neighboring elements determine the statistical error and the limit of
detection. Note that Gupix provides a specific statistical error and limit of
detection (LOD) for each element in each PM sample and these have been used
to provide the uncertainty matrix using in the PMF analysis. IBA measurements
were carried out at the New Zealand National Isotope Centre operated by the
Institute of Geological and Nuclear Sciences (GNS) in Gracefield, Lower Hutt,
New Zealand (Trompetter et al., 2005). Further details on the IBA techniques
used, analytical uncertainties and limits of detection have been reported
previously (Ancelet et al., 2012). Black carbon was measured using a M43D
digital smoke stain reflectometer (Ancelet et al., 2011).</p>
</sec>
<sec id="Ch1.S2.SS4">
  <title>Receptor modeling using PMF</title>
      <p id="d1e682">Receptor modeling and apportionment of PM mass by PMF was performed using the
EPAPMF version 5.0.14 program in accordance with the user's guide
(<ext-link xlink:href="https://www.epa.gov/air-research/epa-positive-matrix-factorization-50-fundamentals-and-user-guide">https://www.epa.gov/air-research/epa-positive-matrix-factorization-50-fundamentals-and-user-guide</ext-link>).
With PMF, sources are constrained to have non-negative species
concentrations; no sample can have a negative source contribution and error
estimates for each observed point are used as point-by-point weights. This is
a distinct advantage of PMF, since it can accommodate missing or below
detection limit data that is a common feature of environmental monitoring
(Song et al., 2001). Another advantage of PMF is that PM mass concentrations
can be included in the model as another variable and the results are directly
interpretable as the covariant PM mass contributions associated with each
factor (source). Prior to the PMF analyses, data and uncertainty matrices
were prepared in the same manner as previous studies (Polissar et al., 1998;
Song et al., 2001). Data screening and the source apportionment were
performed in accordance with the protocols and recommendations set out by
Paatero et al. (2014) and Brown et al. (2015). Due to the effect that random
analytical noise can have on the receptor modeling process, variables with
low signal-to-noise ratios were examined by alternate inclusion and exclusion
in a modeling run and only those variables that could be explained in
association with source emissions were included in the final results (Paatero
and Hopke, 2003).</p><?xmltex \hack{\newpage}?>
</sec>
<?pagebreak page2052?><sec id="Ch1.S2.SS5">
  <title>Conditional probability function (CPF)</title>
      <p id="d1e696">In order to locate the local sources and estimate the wind direction impacts
on each source identified using PMF, the CPF method was applied. The CPF
calculates the probability that a source is located with a particular wind
direction sector (Pekney et al., 2006). The probability that a source
originates from a given wind direction is estimated by comparing the wind
direction distribution for the upper 25 % (or 75 percentile) of source
contributions relative to the total wind direction distribution in this
study:
            <disp-formula id="Ch1.Ex1"><mml:math id="M38" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CPF</mml:mi><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the number of occurrences from wind sector <inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:math></inline-formula> for the upper 25 % of concentrations and <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the total number of occurrences from the same wind sector.</p>
      <p id="d1e775">Using the high-temporal-resolution data, bivariate polar plots were generated
with the R statistical and Openair software packages (Carslaw and Ropkins,
2012). Using bivariate polar plots, source concentrations can be shown as a
function of both wind speed and direction, providing invaluable information
about the direction of potential sources and the influence of wind speed on
concentrations. In this study we produced bivariate polar plots using the
conditional probability function analysis (CPF) to identify the directions
from which high source concentrations are likely to originate. A full
description of CPF analysis can be found in Carslaw and Ropkins (2012).</p>
</sec>
<sec id="Ch1.S2.SS6">
  <title>Human health risk assessment</title>
      <p id="d1e784">Among the detected elements, As, Pb, Mn, Si and Cr were identified as
non-carcinogenic risks, while inorganic As, Pb and Ni were considered
carcinogenic (USEPA, 2017). The reference levels and cancer risk slopes for
Cr vary with its valences (e.g., Cr(VI) and Cr(III)) and exposure pathways
(e.g., oral intake, inhalation). However, neither reference
concentration (Rfc) nor cancer risk slope for inhalation of Cr(III) are
available in the Integrated Risk Information System (IRIS), so we assumed that
the total Cr in our study was Cr(VI), the Rfc and cancer risk slope of which
are provided in IRIS (USEPA, 2017).</p>
      <p id="d1e787">The adjusted air concentrations (<inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>air-adj</mml:mtext></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> for the toxic elements
contained in PM<inline-formula><mml:math id="M43" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> was calculated from Eq. (1), modified based on the
equations in the risk assessment guidance (USEPA, 2009).
            <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M44" display="block"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>air-adj</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">24</mml:mn></mml:munderover><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:msub><mml:mi mathvariant="normal">ET</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mo>×</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mtext>day</mml:mtext><mml:mo>/</mml:mo><mml:mn mathvariant="normal">24</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mtext>h</mml:mtext><mml:mo>)</mml:mo><mml:mo>×</mml:mo><mml:mi mathvariant="normal">ED</mml:mi><mml:mo>×</mml:mo><mml:mi mathvariant="normal">EF</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">AT</mml:mi><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1000</mml:mn></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>air</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is the hourly ambient trace elements concentration
detected in PM<inline-formula><mml:math id="M46" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> (<inline-formula><mml:math id="M47" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>; ET<inline-formula><mml:math id="M49" display="inline"><mml:msub><mml:mi/><mml:mi>i</mml:mi></mml:msub></mml:math></inline-formula> is the exposure time
(1 h day<inline-formula><mml:math id="M50" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>); ED is the exposure duration (6 years for children and
30 years for adults); EF is exposure frequency (350 days year<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in this
study); AT is the averaging time (30 years <inline-formula><mml:math id="M52" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 365 days year<inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>
for non-carcinogens; 75 years <inline-formula><mml:math id="M54" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 365 days year<inline-formula><mml:math id="M55" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for
carcinogens; M. Huang et al., 2014, 2016).</p>
      <p id="d1e1000">The obtained adjusted air concentrations of the toxic trace elements were
subsequently divided by their respiratory reference concentrations
(RfC<inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> to yield the respective hazard quotient (HQ; USEPA, 2017).
Hazard index (HI) was produced by summing up all the hazard quotients (HQs)
based on the hypothesis that the adverse effect is proportional to the sum
of hazard quotients (HQs). Hazard index of less than 1 indicated no significant adverse
non-carcinogenic effect.</p>
      <p id="d1e1015">For the carcinogenic risks assessment, the obtained adjusted air
concentrations of the toxic elements of cancer risks from Eq. (1) were
multiplied by their slope factors to calculate the carcinogenic risks (CRs; USEPA, 2017). The carcinogenic risk refers to a person's chance of
developing cancer from the exposure to any carcinogenic agent. CR equal to 1 <inline-formula><mml:math id="M57" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> is considered as the least stringent level, above which
indicating significant cancer risk.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Results and discussion</title>
<sec id="Ch1.S3.SS1">
  <?xmltex \opttitle{Concentrations of PM${}_{{2.5}}$ and PM${}_{{10}}$ and mass closure
analysis}?><title>Concentrations of PM<inline-formula><mml:math id="M59" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M60" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> and mass closure
analysis</title>
      <p id="d1e1068">The hourly variations of PM<inline-formula><mml:math id="M61" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M62" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> mass concentrations during
the observation are displayed in Fig. S1 in the Supplement. The PM<inline-formula><mml:math id="M63" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M64" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> concentrations varied from <inline-formula><mml:math id="M65" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 8
to <inline-formula><mml:math id="M66" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 270 and <inline-formula><mml:math id="M67" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 16 to 363 <inline-formula><mml:math id="M68" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M69" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, with an average
value of 62.5 <inline-formula><mml:math id="M70" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 33.5 and 91.6 <inline-formula><mml:math id="M71" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 47.2 <inline-formula><mml:math id="M72" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M73" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively. Around 25 % PM<inline-formula><mml:math id="M74" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass concentrations exceeded the second grade of new issued National Ambient
Air Quality Standard (NAAQS, GB 3095-2012) of China, with daily average
value of 75 <inline-formula><mml:math id="M75" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M76" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. In addition, the mean ratio of
PM<inline-formula><mml:math id="M77" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> / PM<inline-formula><mml:math id="M78" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> was estimated to be about 0.67, which is consistent
with the ratio reported by the previous studies in the Pearl River Delta
region, North China Plain and Yangtze River Delta region (Wang et al., 2006;
Sun et al., 2004; Hu et al., 2014). This result indicated that fine
particles, PM<inline-formula><mml:math id="M79" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, accounted for a majority of PM<inline-formula><mml:math id="M80" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p id="d1e1249">Elemental reconstructed mass versus PM mass measured using the beta
attenuation monitor (BAM) technique for
<bold>(a)</bold> PM<inline-formula><mml:math id="M81" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and <bold>(b)</bold> PM<inline-formula><mml:math id="M82" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> at the Foshan site.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018-f02.pdf"/>

        </fig>

      <?pagebreak page2053?><p id="d1e1282">In order to compare the relationship between the range of analytes measured
in PM and the total PM mass, a mass closure approach was used. Ideally, when
elemental analysis and organic compound analysis have been undertaken on the
same sample one can reconstruct the mass using the following general
equation for ambient samples as a first approximation (Cahill et al., 1989;
Cohen, 1999; Malm et al., 1994):

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M83" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mtext>Reconstructed mass</mml:mtext><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>[</mml:mo><mml:mi mathvariant="normal">Soil</mml:mi><mml:mo>]</mml:mo><mml:mo>+</mml:mo><mml:mo>[</mml:mo><mml:mi mathvariant="normal">OM</mml:mi><mml:mo>]</mml:mo><mml:mo>+</mml:mo><mml:mo>[</mml:mo><mml:mi mathvariant="normal">BC</mml:mi><mml:mo>]</mml:mo><mml:mo>+</mml:mo><mml:mo>[</mml:mo><mml:mi mathvariant="normal">Smoke</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E2"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mo>+</mml:mo><mml:mo>[</mml:mo><mml:mi mathvariant="normal">Sulfate</mml:mi><mml:mo>]</mml:mo><mml:mo>+</mml:mo><mml:mo>[</mml:mo><mml:mi mathvariant="normal">Seasalt</mml:mi><mml:mo>]</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where [Soil] <inline-formula><mml:math id="M84" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 2.20[Al] <inline-formula><mml:math id="M85" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> 2.49[Si] <inline-formula><mml:math id="M86" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> 1.63[Ca] <inline-formula><mml:math id="M87" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> 2.42[Fe]
<inline-formula><mml:math id="M88" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> 1.94[Ti], [OM] <inline-formula><mml:math id="M89" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M90" display="inline"><mml:mi mathvariant="normal">Σ</mml:mi></mml:math></inline-formula>[Concentrations of organic compounds],
[BC] <inline-formula><mml:math id="M91" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Concentration of black carbon (soot),
[Smoke] <inline-formula><mml:math id="M92" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> [K] <inline-formula><mml:math id="M93" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula> 0.6[Fe], [Seasalt] <inline-formula><mml:math id="M94" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 2.54[Na],
[Sulfate] <inline-formula><mml:math id="M95" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 4.125[S].</p>
      <p id="d1e1446">The reconstructed mass (RCM) is based on the fact that the six composite
variables or “pseudo” sources given in Eq. (2) are generally the major
contributors to fine and coarse particle mass and are based on geochemical
principles and constraints. As a measure of [OM] was not available in this
study, it was assumed that it composed part of the “remaining mass” (the
difference between RCM and measured PM (BAM)) that includes water and nitrates as major components (Cahill et
al., 1989). As Na was below the LOD across most of the samples, the
reciprocal calculation of [Seasalt] <inline-formula><mml:math id="M96" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.65[Cl] was substituted, though
care was taken with the interpretation of this pseudo source due to the
potential for Cl loss by volatilization from aerosol (or from filters) in the
presence of acidic aerosol species, particularly in the fine fraction (Lee et
al., 1999; Chen et al., 2016). Most fine sulfate particles are the result of
oxidation of SO<inline-formula><mml:math id="M97" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> gas to sulfate particles in the atmosphere (Malm et
al., 1994). For RCM, it is assumed that sulfate is present in fully
neutralized form as ammonium sulfate. [Sulfate] therefore represents the
ammonium sulfate contribution to aerosol mass with the multiplicative factor
of 4.125[S] to account for ammonium ion and oxygen mass (i.e.,
(NH<inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>SO<inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> ((14 <inline-formula><mml:math id="M100" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> 4) <inline-formula><mml:math id="M101" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2 <inline-formula><mml:math id="M102" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> 32 <inline-formula><mml:math id="M103" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> (16 <inline-formula><mml:math id="M104" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 4) <inline-formula><mml:math id="M105" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> 32);
Cahill et al., 1989; Cohen, 1999; Malm et al., 1994).</p>
      <p id="d1e1535">The RCM and mass closure calculations using the pseudo-source and
pseudo-element approach are a useful way to examine initial relationships in
the data and how the measured mass of species in samples compares to total PM
mass, an important consideration for receptor modeling studies. Figure 2
indicates that the RCM of measured elements accounts for approximately
30 % of total mass for both PM<inline-formula><mml:math id="M106" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M107" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> and that there was
significant correlation (<inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M109" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.64 and 0.69 for PM<inline-formula><mml:math id="M110" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and
PM<inline-formula><mml:math id="M111" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>, respectively), which indicates that the unmeasured PM components
(OM, nitrate, bound H<inline-formula><mml:math id="M112" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O) are likely to be strongly associated with those
species that were measured. Analysis of the data showed that most of the
remaining mass (RM) for PM<inline-formula><mml:math id="M113" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> was in fact PM<inline-formula><mml:math id="M114" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, as would be
expected for such aerosol species as OM (including secondary organic aerosol)
and nitrate. Therefore, an extra variable was calculated,
RM<inline-formula><mml:math id="M115" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:msub></mml:math></inline-formula> (where
RM<inline-formula><mml:math id="M116" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M117" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> PM<inline-formula><mml:math id="M118" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M119" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula> RCM<inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mrow><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>,
to be included in the PMF analysis as a placeholder for the unmeasured
components, an approach that has been successfully applied in other studies
(Belis et al., 2013). The advantage of such an approach is that all PM mass
is accounted for in the PMF model. However, the limitation is that it still
does not define exactly what aerosol species the RMPM<inline-formula><mml:math id="M121" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> variable
includes, although some inferences can be made depending on the source
association.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p id="d1e1697">Factor profiles for sources at Foshan EMC showing the concentrations
of PM<inline-formula><mml:math id="M122" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>, PM<inline-formula><mml:math id="M123" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, SO<inline-formula><mml:math id="M124" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, NO<inline-formula><mml:math id="M125" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> (all in <inline-formula><mml:math id="M126" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>
and CO (in mg m<inline-formula><mml:math id="M128" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M129" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10; the error bars are the 5th and 95th
percentiles generated from EPAPMF diagnostics).</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018-f03.pdf"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS2">
  <?xmltex \opttitle{Sources identification and apportionment of PM${}_{{2.5}}$ and PM${}_{{10}}$
during the observation}?><title>Sources identification and apportionment of PM<inline-formula><mml:math id="M130" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M131" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>
during the observation</title>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p id="d1e1811">Source contributions to PM at Foshan showing the average
concentrations of PM<inline-formula><mml:math id="M132" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, PM<inline-formula><mml:math id="M133" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> (in <inline-formula><mml:math id="M134" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> during the
monitoring period.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018-f04.pdf"/>

        </fig>

      <?pagebreak page2055?><p id="d1e1860">Using the combined fine and coarse PM elemental data sets along with the
gaseous data from the Foshan EMC, PMF was used to identify six factors or
sources contributing to PM concentrations during the monitoring period. PMF
modeling diagnostics and other parameters are detailed in the Supplement.
Multiple PMF model runs were performed choosing fewer and more factors to
examine the effect on modeling diagnostics and interpretability of the source
profiles coupled with the advantage of high-resolution data to examine the
diurnal concentration variations. The final six-factor solution adopted
included an Fpeak rotation (<inline-formula><mml:math id="M136" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>3, %dQ<inline-formula><mml:math id="M137" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Robust</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M138" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 2.91) that
provided good separation of the minor marine aerosol source as evidenced by
the Fpeak bootstrapping results. Note that the gaseous components (SO<inline-formula><mml:math id="M139" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>,
NO<inline-formula><mml:math id="M140" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and CO) have been included to aid with source identification and to
examine those PM emission sources or secondary aerosol sources they are
closely associated (covariant) with. This method has been also adopted in
previous studies, and proved to enhance the resolving power of source
apportionment studies (Zhou et al., 2005; Liu et al., 2006). The sources
identified were marine aerosol, biomass combustion, construction dust, motor
vehicles and road dust, secondary inorganic aerosol and industrial coal
combustion. These sources were found to explain 89 and 91 % of the
PM<inline-formula><mml:math id="M141" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M142" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> mass, respectively (Fig. S3). The factor profiles
are presented in Fig. 3, where elements in the coarse fraction are denoted as
<inline-formula><mml:math id="M143" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula>-C (e.g., Al-C). The first factor represents biomass combustion because of
the presence of BC, K and fine Cl as primary species along with Zn, which is
consistent with previous studies and represents the burning of wood or plant
material (Maenhaut, 2018; Ancelet et al., 2012). Motor vehicles and road dust
were identified as the source of the second factor based on the presence of
NO<inline-formula><mml:math id="M144" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, BC and crustal matter components Al, Si, Ca, Fe and Zn from the
coarse fraction as the significant elements in the profile. This profile
represents both exhaust (tailpipe) emissions and non-exhaust (road dust and
brake and tire wear) emissions, hence the combination of coarse and fine
elemental species and the higher contribution of the source to PM<inline-formula><mml:math id="M145" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>
concentrations relative to PM<inline-formula><mml:math id="M146" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>. Ambient source profiles derived for
motor vehicles generally include particulate matter from all engine types as
emissions tend to be co-mingled by turbulent air movement at street level due
to road traffic and are therefore temporally and spatially covariant (Amato
et al., 2009; Pant and Harrison, 2013). The third source contains most of the
black carbon, a substantial amount of CO, SO<inline-formula><mml:math id="M147" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, NO<inline-formula><mml:math id="M148" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, S and fine
fraction heavy metals (Cr, Mn, Cu, Zn, As, Pb) and has been attributed to
coal combustion which is likely to include coal-fired power station emissions
that are probably mixed with industrial process emissions (Song et al., 2007;
Tian et al., 2014). The fourth factor contains the majority of both coarse
and fine S, which dominates the elemental mass and is considered to represent
the secondary inorganic aerosol component from gas-to-particle transformation
in the atmosphere. Vanadium and nickel were also associated with this source
suggesting contributing source emissions from the combustion of
sulfur-containing fuels such as heavy fuel oil or oil refinery emissions
(Querol et al., 2008; Maenhaut, 2018). Secondary aerosols are primarily fine
particles from the gas-to-particle conversion process, but some of the
particle size range does extend into the coarse fraction (Anlauf et al.,
2006), particularly where heterogeneous atmospheric chemistry takes place on
the surface of particles or in aerosol droplets during the reaction of sulfur
gaseous species to form secondary sulfate particle species (George and
Abbatt, 2010). The fifth factor, construction dust, with a high Ca loading in
the profile along with crustal matter components (Al, Si, Fe) in both the
fine and coarse fractions, has been attributed to activities that generate
cementitious (hence the high Ca content) and crustal matter dusts in the area
such as construction/demolition of buildings and other structures (i.e.,
cement mixing, concrete pouring, concrete cutting or drilling and soil
excavation), which significantly distinguishes the source from that which
might be associated with motor vehicles/road dust emissions (Owega et al.,
2004; Chueinta et al., 2000; Maenhaut, 2018). The sixth source was
characterized as marine aerosol due to the predominance of Cl-C.
Interestingly, as indicated in Fig. 3 most of the calculated variable,
RMPM<inline-formula><mml:math id="M149" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> (derived in Sect. 3.1), was associated with the motor vehicle
and biomass combustion sources (45 and 17 %), respectively (Fig. S4),
most likely indicating the association of OC with these sources (Querol et
al., 2013; Pósfai et al., 2004), and the remainder of RMPM<inline-formula><mml:math id="M150" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>
(36 %) was associated with the secondary aerosol source and is probably
indicative of secondary nitrate and secondary organic aerosol concentrations
(Huang et al., 2011; Freney et al., 2014).</p>
      <p id="d1e1999">Average source contributions to particulate mass concentrations are
presented in Fig. 4, which shows that industrial coal combustion (26 %,
16.0 <inline-formula><mml:math id="M151" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, secondary inorganic aerosol (24 %, 14.8 <inline-formula><mml:math id="M153" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and motor vehicle emissions (20 %, 12.5 <inline-formula><mml:math id="M155" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>
dominated PM<inline-formula><mml:math id="M157" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> concentrations during the monitoring period. Mass
contributions to PM<inline-formula><mml:math id="M158" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> from coal combustion and secondary inorganic
aerosol were essentially unchanged from the fine fraction (16.8 and 16.9 <inline-formula><mml:math id="M159" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M160" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively), while the contributions
from motor vehicles (30.2 <inline-formula><mml:math id="M161" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and construction dust (15.1 <inline-formula><mml:math id="M163" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> increased due to the significant coarse particle
component associated with these latter sources.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p id="d1e2154">Time series for source contributions to PM<inline-formula><mml:math id="M165" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> at Foshan EMC
during the monitoring period.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018-f05.pdf"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p id="d1e2174">Time series for source contributions to PM<inline-formula><mml:math id="M166" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> at Foshan EMC
during the monitoring period.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018-f06.pdf"/>

        </fig>

      <p id="d1e2192">When considering the gases, SO<inline-formula><mml:math id="M167" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> was strongly associated with the
industrial coal combustion source. Meanwhile, the majority of NO<inline-formula><mml:math id="M168" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> was
split between motor vehicles and the industrial coal combustion source.
Interestingly CO was primarily associated with the industrial coal combustion
and secondary inorganic aerosol sources. CO, NO<inline-formula><mml:math id="M169" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> and SO<inline-formula><mml:math id="M170" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions
are associated with the light-duty motor vehicles (i.e., petrol vehicles),
which emit few particles directly. The petrol vehicles as well as coal
combustion-emitted NO<inline-formula><mml:math id="M171" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> and SO<inline-formula><mml:math id="M172" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> transform to nitrate and sulfate
particles through chemical reactions. The association of CO with secondary
inorganic aerosol is explained by co-emission of CO with the gaseous
combustion product precursors (e.g., SO<inline-formula><mml:math id="M173" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, NO<inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> of secondary
inorganic aerosol, and they are therefore present (covariant) in the same air
mass. Diesel-powered vehicles produce very little CO initially (Rhys-Tyler et
al., 2011). It is assumed that diesel vehicle tailpipe emissions are
primarily responsible for motor-vehicle-related PM<inline-formula><mml:math id="M175" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> concentrations in
the Foshan urban airshed, consistent with international research
(Kirchstetter et al., 2008; Kim et al., 2009; Wang et al., 2012; Targino et
al., 2016). Therefore, CO is not associated with motor-vehicle-emitted
particulate<?pagebreak page2056?> matters (primary aerosol). Also included in the source
contribution graphs (Fig. 4) is the remaining mass (i.e., measured PM mass minus predicted PM mass). The time series plots
presented in Figs. 5 and 6 for PM<inline-formula><mml:math id="M176" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M177" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>, respectively, show
that the biomass burning and marine aerosol sources were episodic and that
the concentrations of the motor vehicles and construction dust sources
increased in PM<inline-formula><mml:math id="M178" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> due to the coarse particle content.</p>
      <p id="d1e2308">Peak PM<inline-formula><mml:math id="M179" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M180" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> episodes were associated with motor vehicle and
coal combustion, particularly when PM from biomass combustion was also a
significant contributor. This suggests that biomass combustion sources were
additive over the other sources and forced the PM<inline-formula><mml:math id="M181" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> concentrations to
extreme highs. Analysis of satellite imagery (MODIS fire spot) indicates that
biomass combustion activities were outside of the region to the north and
northeast of Foshan and were advected over the city during the peak PM
pollution events (Fig. S2). High concentrations of potassium were also
detected during the biomass burning episodes (Zhou et al., 2016). It is most
likely that the biomass combustion source is associated with agricultural
burn-off around Foshan. The time averaged daily patterns in source
concentrations were examined and as shown in Fig. 7a, the industrial coal
combustion source concentrations were generally higher at night, perhaps due
to a stable nocturnal boundary layer/mixing height effect. The construction
dust concentrations (Fig. 7b) were significantly higher during the day
reflecting the pattern of daytime activities generating the dusts. The motor
vehicles and road dust sources (Fig. 7c) showed a bimodal pattern with peaks
in the morning and evening rush hours, which was ascribed to the morning and
evening commuter traffic and lower
boundary layer. We could see the distinguishing diurnal variations between
motor vehicle/road dust and construction dust sources.</p>
      <p id="d1e2338">The secondary inorganic aerosol source (Fig. 7d) demonstrated slightly
higher concentrations at night than at<?pagebreak page2057?> daytime. Precursor gaseous
emissions are oxidized via various gas or aqueous pathways and are then
converted to sulfate aerosol (Seinfeld and Pandis, 2006; Sun et al., 2014).
However, the impacts of changes in the boundary layer tend to
build up the air pollutants during the nighttime. This is also consistent
with the fact that there is a considerable amount of precursor gas
emissions from upwind regions and that processing has already occurred
there, or while the parcel has undergone dynamical transport. This implies
that there is a higher chance of being mixed throughout the boundary layer
and lower troposphere as well and therefore it is not as sensitive with respect
to a ground-based measurement as more local emissions. The marine aerosol
and biomass combustion sources are not shown in Fig. 7 due to their episodic
nature.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p id="d1e2344">Diurnal patterns in source contributions to PM at Foshan EMC during
the monitoring period (the shaded area is the 5th and 95th confidence
interval of the calculated mean).</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018-f07.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><caption><p id="d1e2355">CPF bivariate polar plots for source concentrations at Foshan.</p></caption>
          <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018-f08.png"/>

        </fig>

      <p id="d1e2364">Figure 8 presents bivariate CPF polar plots for the source contributions to
PM. Fig. 8a shows that the highest 25 % of industrial coal combustion
source contributions originated from the west to northwest quadrants under
light winds (1–3 m s<inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e2382">A highly resolved spatial anthropogenic emission inventory for PRD was
conducted by South China University of Technology for the base year 2012
(Yin et al., 2017). The data shows that the highest density of PM<inline-formula><mml:math id="M183" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>
combustion sources (including power plants and industrial combustion) and
industrial processes emissions were concentrated within 30 km to the west
and northwest of the Foshan EMC as presented in Fig. S5. Three other large
coal fired power stations were also located approximately 20 km to the
west–southwest of the monitoring site.</p>
      <p id="d1e2394">Peak marine aerosol (Fig. 8b) arrived at the site from the southeast at
higher wind speeds (5–7 m s<inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> in the direction of the South China
Sea. Secondary inorganic aerosol (Fig. 8c) came from the north-northeast
direction at moderate wind speeds (3–5 m s<inline-formula><mml:math id="M185" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> with a smaller
component from the south-southeast. Construction dusts (Fig. 8d) were
highest during low to moderate wind speeds out of the northeast sector,
arriving from the direction of the Foshan city center, where the majority of
construction activities were occurring. The upper 25 % of biomass
combustion concentrations (Fig. 8e) were from the northwest sector. It is
likely that the biomass combustion emission sources were intermittent and
regional, related to agricultural activities or possibly wildfires. Peak
motor vehicle source concentrations (Fig. 8f) occurred during
south-southwest winds. The PM sampler was located 35 m above Fen Jiang Nan
Road, which is an arterial route with six lanes running north–south past the
monitoring site. The CPF result suggests that winds from the south-southwest
were most effective in transporting roadway emissions to the sampler.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <?xmltex \opttitle{Health exposure risk of PM${}_{{2.5}}$ elements}?><title>Health exposure risk of PM<inline-formula><mml:math id="M186" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> elements</title>
<sec id="Ch1.S3.SS3.SSS1">
  <?xmltex \opttitle{PM${}_{{2.5}}$ elements human health assessment}?><title>PM<inline-formula><mml:math id="M187" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> elements human health assessment</title>
      <p id="d1e2458">Although none of the individual HQ values (As: 0.88, Mn: 0.54, Si: 0.29, Pb:
0.27, Cr: 0.09) for the identified toxic elements exceed 1, the HI value
(sum of their HQs) was 2.09, much higher than the safe level (HQ <inline-formula><mml:math id="M188" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1). This
indicates significant non-carcinogenic risks. Arsenic was observed to have
the highest risk, followed by Mn, Pb, Si and Cr (Fig. 9a). The
non-carcinogenic HI did not show a distinct diurnal pattern (Fig. 10a).</p>
      <p id="d1e2468">On the other hand, the total CR of the carcinogenic elements was
3.37 <inline-formula><mml:math id="M189" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M190" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, higher than the least stringent level of
1.0 <inline-formula><mml:math id="M191" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M192" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for adults. Pb (3.30 <inline-formula><mml:math id="M193" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> was found
to be the most risky element (Fig. 9b). In addition, the CRs of Cr and As
were 4.51 <inline-formula><mml:math id="M195" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M196" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 2.27 <inline-formula><mml:math id="M197" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M198" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively,
exceeding the middle stringent cancer risk level (1.0 <inline-formula><mml:math id="M199" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>,
and the CR of Ni was 8.71 <inline-formula><mml:math id="M201" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M202" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, lower than the least stringent level (1.0 <inline-formula><mml:math id="M203" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M204" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>.
The predominant contribution of Pb to the cancer risk could exactly explain
why the diurnal variation of carcinogenic risk was in response to the pattern
of ambient-air-detected Pb concentrations (Fig. 10). From the source
apportionment results, lead was mainly emitted from industrial coal
combustion (91.5 %), and slightly from biomass burning (8.5 %).
Around 08:00 was found to be the most risky time period of the day (Fig. 10).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9"><caption><p id="d1e2636"><bold>(a)</bold> Average contribution percentage of selected trace
elements to HI and <bold>(b)</bold> average contribution
percentage of selected trace elements to total carcinogenic risk (CR).</p></caption>
            <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018-f09.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><caption><p id="d1e2653">Diurnal variations of HI and CR from selected trace elements in
PM<inline-formula><mml:math id="M205" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> in Foshan City. Shaded areas represent the 95 % confidence
intervals.</p></caption>
            <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018-f10.pdf"/>

          </fig>

<?xmltex \hack{\newpage}?>
</sec>
<?pagebreak page2058?><sec id="Ch1.S3.SS3.SSS2">
  <title>Health risk assessment of resolved PM sources</title>
      <p id="d1e2679">Based on PMF source apportionment results and the contribution of each toxic
element to the non-carcinogenic/carcinogenic risks, the industrial coal
combustion source was identified as the largest non-carcinogenic risk
contributor (Fig. 11). Construction dust and
secondary inorganic aerosol were also important sources (Fig. 11). For the
carcinogenic risks, industrial coal combustion was found to be the largest
contributor, followed by biomass burning sources. Similar findings were
reported by Khan et al. (2016) in the tropical environment in Malaysia.
Secondary inorganic aerosols contributed approximately 25 % of the
PM<inline-formula><mml:math id="M206" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass, but they posed little carcinogenic risk. The other three
sources (i.e., construction dust, motor vehicles and road dust and marine
aerosol) also contributed generally low to CR.</p>
      <p id="d1e2691">From the perspective of human health effects, industrial coal combustion has
been identified as the most important emission source. We also found that it
contributed the most to PM<inline-formula><mml:math id="M207" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass from the source apportionment
results (Sect. 3.2). Therefore, controlling industrial coal combustion
sources achieves the benefit of reducing both PM<inline-formula><mml:math id="M208" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass concentration
and human health risks.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F11"><caption><p id="d1e2714">Daily variation of average contribution of the identified sources to
health risks over the observation periods.</p></caption>
            <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018-f11.pdf"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12" specific-use="star"><caption><p id="d1e2726">CPF analysis polar plots of <bold>(a)</bold> HI and
<bold>(b)</bold> total carcinogenic risk at Foshan City. The center of each plot
represents a wind speed of zero with increasing radially outward. The HI and
CR probability is shown by the color scale.</p></caption>
            <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/2049/2018/acp-18-2049-2018-f12.png"/>

          </fig>

      <p id="d1e2741">The CPF analysis indicated that the highest health risks of PM<inline-formula><mml:math id="M209" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> came
from north and northwest directions (Fig. 12). As stated in Sect. 3.2, there
are a large number of industrial activities in the north and northwest
directions including ceramic industry and coal combustion. Foshan is an
industrial city famous for its ceramic and manufacturing industries (Wan et
al., 2011; Tan et al., 2014). The emissions of large quantities of air
pollutants from the above-mentioned industries resulted in deteriorating air
quality in Foshan, a city which has always ranked among cities with the
heaviest air pollution in the PRD region. Since 2007, the Foshan government
has launched a series of policy measures to improve the local air quality.
The policies are effective in the reduction of PM concentrations, especially
in the anthropogenic elements and water soluble ions (Tan et al., 2016).
However, our results showed that more efforts are needed to further protect
human health.</p>
</sec>
</sec>
</sec>
<?pagebreak page2059?><sec id="Ch1.S4" sec-type="conclusions">
  <title>Conclusions</title>
      <p id="d1e2761">In this study, hourly time-resolved major trace elemental composition in
coarse (PM<inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:mtext>–</mml:mtext><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and fine (PM<inline-formula><mml:math id="M211" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> particulate matter were
measured during autumn 2014 at an industrial city Foshan, in the Pearl River
Delta region. PM<inline-formula><mml:math id="M212" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M213" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> mass concentration and some of
the gas-phase pollutants were concurrently recorded using commercial
continuous PM and gases monitors. The results showed that PM<inline-formula><mml:math id="M214" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and
PM<inline-formula><mml:math id="M215" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> displayed drastic variations with the highest hourly averaged
concentration over 250 and 350 <inline-formula><mml:math id="M216" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g m<inline-formula><mml:math id="M217" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>,
respectively, suggesting the severe PM pollution in autumn/winter seasons at
Foshan city. Source apportionment of PM using positive matrix factorization
on the hourly data revealed six PM<inline-formula><mml:math id="M218" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M219" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> sources:
industrial coal combustion, secondary inorganic aerosol, motor vehicles and
road dust, construction dust, biomass combustion and marine aerosol. Using
the hourly resolution elemental data, we improved the source apportionment
of PM, especially for the sources with notably temporal variation, such as
biomass burning. We found that the industrial coal combustion sources were
the largest contributor to PM<inline-formula><mml:math id="M220" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, while motor vehicles and road dust
sources had the highest contribution to PM<inline-formula><mml:math id="M221" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>. Additionally, biomass
combustion was observed to additively contribute to PM<inline-formula><mml:math id="M222" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> levels
resulting in the highest PM<inline-formula><mml:math id="M223" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> concentrations measured during the
monitoring period. Control<?pagebreak page2060?> of regional biomass combustion activities may be
one option for preventing extreme PM<inline-formula><mml:math id="M224" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> events and the associated
health burden.</p>
      <p id="d1e2913">Based on the PMF-resolved sources, the health risks posed by selected trace
elements (Pb, As, Si, Cr, Mn and Ni) in PM<inline-formula><mml:math id="M225" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> via inhalation exposure
were assessed. The results indicated that As and Pb posed the highest
non-carcinogenic and carcinogenic risks to human health, respectively.
Industrial coal combustion was the dominant source responsible for human
health impacts, constituting 66.8 % of the hazard index and 92 % of the
cancer risks. CPF results indicated high health risks in the north and
northwest directions, which was assigned to the intensive industrial
activities such as coal burning and manufacturing industry. Therefore,
controlling industrial coal combustion sources will result in reducing both
PM<inline-formula><mml:math id="M226" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass concentration and health risk. This study utilized the
hourly measured elemental components combined with PM<inline-formula><mml:math id="M227" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, PM<inline-formula><mml:math id="M228" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> and
gas pollutants, and provided valuable information on PM sources
identification and control. The source–risk apportionment method helps
decision makers to manage air quality more effectively.</p>
</sec>

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

      <p id="d1e2957">The data used in this study are available from the authors
upon request (eeswxm@mail.sysu.edu.cn).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e2960">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/acp-18-2049-2018-supplement" xlink:title="pdf">https://doi.org/10.5194/acp-18-2049-2018-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="competinginterests">

      <p id="d1e2969">The authors declare that they have no conflict of
interest.</p>
  </notes><?xmltex \hack{\newpage}?><notes notes-type="sistatement">

      <p id="d1e2976">This article is part of the special issue “Regional transport
and transformation of air pollution in eastern China”. It does not belong to
a conference.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e2982">Funding for the program collaboration was provided by the Natural Science
Foundation of Guangdong Province (2014A030310497), National Natural Science
Foundation of China (41505106), Guangdong Provincial Scientific Planning
Project (2016B050502005), National Science Fund for Distinguished Young
Scholars (41425020), High-end Foreign Experts Recruitment Program of
Guangdong Province (02090-52920003) and the Science and Technology Planning
Project of Guangdong Province (2014B020216003). The New Zealand Ministry of
Business, Innovation and Employment, the New Zealand Institute of Geological
and Nuclear Sciences, and Foshan Environmental Monitoring Center are also
acknowledged.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Jianmin Chen<?xmltex \hack{\newline}?>
Reviewed by: three anonymous referees</p></ack><ref-list>
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    <!--<article-title-html>High-resolution sampling and analysis of ambient particulate matter in the Pearl River Delta region of southern China: source apportionment and health risk implications</article-title-html>
<abstract-html><p>Hazardous air pollutants, such as trace elements in
particulate matter (PM), are known or highly suspected to cause detrimental
effects on human health. To understand the sources and associated risks of PM
to human health, hourly time-integrated major trace elements in
size-segregated coarse (PM<sub>2.5–10</sub>) and fine (PM<sub>2.5</sub>) particulate
matter were collected at the industrial city of Foshan in the Pearl River
Delta region, China. Receptor modeling of the data set by positive matrix
factorization (PMF) was used to identify six sources contributing to
PM<sub>2.5</sub> and PM<sub>10</sub> concentrations at the site. Dominant sources
included industrial coal combustion, secondary inorganic aerosol, motor
vehicles and construction dust along with two intermittent sources (biomass
combustion and marine aerosol). The biomass combustion source was found to be
a significant contributor to peak PM<sub>2.5</sub> episodes along with motor
vehicles and industrial coal combustion. Conditional probability function
(CPF) analysis was applied to estimate the source locations using the
PMF-resolved source contribution coupled with the surface wind direction
data. Health exposure risk of hazardous trace elements (Pb, As, Si, Cr, Mn
and Ni) and source-specific values were estimated. The total hazard quotient
(HQ) of PM<sub>2.5</sub> was 2.09, higher than the acceptable limit (HQ&thinsp; = &thinsp;1). The
total carcinogenic risk (CR) was 3.37&thinsp; × &thinsp;10<sup>−3</sup> for PM<sub>2.5</sub>, which
was 3 times higher than the least stringent limit (1.0&thinsp; × &thinsp;10<sup>−4</sup>).
Among the selected trace elements, As and Pb posed the highest
non-carcinogenic and carcinogenic risks to human health, respectively. In
addition, our results show that the industrial coal combustion source is the
dominant non-carcinogenic and carcinogenic risk contributor, highlighting the
need for stringent control of this source. This study provides new insight
for policy makers to prioritize sources in air quality management and health
risk reduction.</p></abstract-html>
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