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  <front>
    <journal-meta><journal-id journal-id-type="publisher">AMT</journal-id><journal-title-group>
    <journal-title>Atmospheric Measurement Techniques</journal-title>
    <abbrev-journal-title abbrev-type="publisher">AMT</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Atmos. Meas. Tech.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1867-8548</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/amt-14-785-2021</article-id><title-group><article-title>Smartphone pressure data: quality control and impact on atmospheric analysis</article-title><alt-title>Smartphone pressure data</alt-title>
      </title-group><?xmltex \runningtitle{Smartphone pressure data}?><?xmltex \runningauthor{R. Li et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Li</surname><given-names>Rumeng</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Zhang</surname><given-names>Qinghong</given-names></name>
          <email>qzhang@pku.edu.cn</email>
        <ext-link>https://orcid.org/0000-0002-9697-8622</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Sun</surname><given-names>Juanzhen</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Chen</surname><given-names>Yun</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4 aff5">
          <name><surname>Ding</surname><given-names>Lili</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1817-6421</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Wang</surname><given-names>Tian</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Department of Atmospheric and Oceanic Sciences, School of Physics,
Peking University, Beijing 100871, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>National Center for Atmospheric Science, Boulder, Colorado, United
States</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>National Meteorological Center, Chinese Meteorological
Administration, Beijing 100080, China</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Moji Co., Ltd, Beijing, 100015, China</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Theme Tech Inc, Beijing, 100020, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Qinghong Zhang (qzhang@pku.edu.cn)</corresp></author-notes><pub-date><day>2</day><month>February</month><year>2021</year></pub-date>
      
      <volume>14</volume>
      <issue>2</issue>
      <fpage>785</fpage><lpage>801</lpage>
      <history>
        <date date-type="received"><day>14</day><month>May</month><year>2020</year></date>
           <date date-type="rev-request"><day>27</day><month>July</month><year>2020</year></date>
           <date date-type="rev-recd"><day>23</day><month>November</month><year>2020</year></date>
           <date date-type="accepted"><day>10</day><month>December</month><year>2020</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2021 Rumeng Li et al.</copyright-statement>
        <copyright-year>2021</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021.html">This article is available from https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021.html</self-uri><self-uri xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021.pdf">The full text article is available as a PDF file from https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e153">Smartphones are increasingly being equipped with
atmospheric measurement sensors providing huge auxiliary resources for
global observations. Although China has the highest number of cell phone
users, there is little research on whether these measurements provide useful
information for atmospheric research. Here, for the first time, we present
the global spatial and temporal variation in smartphone pressure
measurements collected in 2016 from the Moji Weather app. The data have an
irregular spatiotemporal distribution with a high density in urban areas, a
maximum in summer and two daily peaks corresponding to rush hours. With the
dense dataset, we have developed a new bias-correction method based on a
machine-learning approach without requiring users' personal information,
which is shown to reduce the bias of pressure observation substantially. The
potential application of the high-density smartphone data in cities is
illustrated by a case study of a hailstorm that occurred in Beijing in which
high-resolution gridded pressure analysis is produced. It is shown that the
dense smartphone pressure analysis during the storm can provide detailed
information about fine-scale convective structure and decrease errors from
an analysis based on surface meteorological-station measurements. This study
demonstrates the potential value of smartphone data and suggests some future
research needs for their use in atmospheric science.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e165">A lack of high-resolution observational data is one of the obstacles that
limits the advance of numerical weather prediction (Bauer et
al., 2015). This limitation can be extended to all areas in atmospheric
research. In recent years, many new observational technologies have emerged,
including built-in smartphone sensors, such as those for pressure,
temperature, humidity and aerosols (Overeem et al., 2013; Snik et al.,
2014; Muller et al., 2015; Droste et al., 2017; Meier et al., 2017; Zheng et
al., 2018). With over 2.7 billion people in possession of smartphones
(Bankmycell, 2019) and an increasing trend in equipping smartphones
with atmospheric measurement sensors, smartphone data can potentially be an
auxiliary resource for global, high-density observations capable of
resolving convective-scale features with a resolution lower than 2 km
(Mass and Madaus, 2014).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e170">The workflow for smartphone pressure data quality control
and preprocessing. See text for details.</p></caption>
        <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f01.png"/>

      </fig>

<?xmltex \floatpos{h!}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Table}?><label>Table 1</label><caption><p id="d1e182">Parameters used for machine learning.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Data type/source</oasis:entry>
         <oasis:entry colname="col2">Field</oasis:entry>
         <oasis:entry colname="col3">Description</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Smartphone</oasis:entry>
         <oasis:entry colname="col2">Gridded pressure at each smartphone site</oasis:entry>
         <oasis:entry colname="col3">Pressure to be corrected</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Longitude</oasis:entry>
         <oasis:entry colname="col3">Location information</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Latitude</oasis:entry>
         <oasis:entry colname="col3">Location information</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Time</oasis:entry>
         <oasis:entry colname="col3">Time information</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Land cover</oasis:entry>
         <oasis:entry colname="col3">Geographical information</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Number of pressure observations aggregated at each smartphone site</oasis:entry>
         <oasis:entry colname="col3">Data uncertainty</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Standard deviation of pressure observations at each smartphone site</oasis:entry>
         <oasis:entry colname="col3">Data uncertainty</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Distance from domain center</oasis:entry>
         <oasis:entry colname="col3">Additional location information</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Automatic weather station</oasis:entry>
         <oasis:entry colname="col2">Pressure observation interpolated to each smartphone site</oasis:entry>
         <oasis:entry colname="col3">“True” pressure</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e317">The smartphone sensors monitor atmospheric parameters and convert them into
electrical signals which can then be collected by different platforms, such
as mobile weather applications. Low-cost smartphone sensor data have been
used in several atmospheric research studies.
Overeem et al. (2013) and Droste et al. (2017) used smartphone battery data
to study air temperature and their application to urban heat islands.
Snik et al. (2014) mapped atmospheric aerosols using
smartphone spectropolarimeters. Surface pressure is one of the most useful
variables because it can reflect information about the whole atmospheric
column and is less sensitive to the observational background (e.g.,
indoors/outdoors<?pagebreak page786?> or the influence of the underlying surface versus other
variables like temperature and wind; Mass and Madaus,
2014; Hanson, 2016); therefore, smartphone pressure data have received
considerable attention from researchers. In addition to applications in
weather forecasting  (Mass and Madaus, 2014; Madaus and Mass,
2017; McNicholas and Mass, 2018b; Hintz et al., 2019), smartphone pressure
data can be used to monitor atmospheric tides  (Price et
al., 2018).</p>
      <p id="d1e320">While smartphone pressure data may have potential value, they require
validation and quality control before use.  Price et al. (2018) and Hintz et al. (2019) showed that, although the
variability between smartphone pressure data and meteorological-station
observations is highly correlated, there exists noticeable bias.
Price et al. (2018) calibrated the long-term stable bias
using a one-point calibration method, while  Hintz et al. (2019)
developed screening methods to reduce observational noise. Machine learning
has also been applied to correct atmospheric pressure data (Kim et al.,
2015, 2016; McNicholas and Mass, 2018a). Most previous
publications on smartphone data calibration adopted a user-based approach
which required the identification of each unique user and personal information.
However, this raises privacy and ethical issues that pose a concern to the
public. As highlighted by  Muller et al. (2015) and
Mooney et al. (2017), collecting as little personal information as
possible and keeping raw data private are guiding principles of privacy
preservation. Moreover, without a stable data collocation platform,
performing user-based calibration can be time and resource consuming,
especially for densely populated regions. It is therefore imperative to
develop a new method that can efficiently calibrate smartphone pressure
bias while protecting user privacy. It is worth noting that the need for
such an effort has been recognized by other researchers, and similar efforts
are being undertaken  (McNicholas, 2020).</p>

      <?xmltex \floatpos{t!}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e325">Locations of global pressure observations in 2016 from the
Moji Weather application.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f02.png"/>

      </fig>

      <?xmltex \floatpos{ht!}?><fig id="Ch1.F3"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e336">Hourly pressure observation counts (log10 transformed)
averaged over the year 2016. Data are binned into a 0.1<inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M2" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.1<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f03.png"/>

      </fig>

      <p id="d1e370">China has one of the world's most densely distributed smartphone user bases
(Bankmycell, 2019) which can potentially produce highly dense
observations. In this paper, we present, for the first time, a year-long
dense and extensive smartphone dataset collected by the Moji Weather<?pagebreak page787?> app,
which is developed and operated by the internet environmental meteorological
corporation Moji. The Moji Weather app is a popular smartphone weather app
used in many countries with a 53.90 % market share and more than 500 million users, as well as over 100 million weather queries made every day
(Moji, 2019a, b). In the present study, we use the Moji smartphone
pressure data for all of 2016 to show the spatial and temporal distribution
of the dataset. With this highly dense network, we demonstrate the
feasibility of a new machine-learning bias-correction method that does not
require users' private information, thereby ameliorating ethical issues. The
dense network also makes it possible to study the detailed structure of
atmospheric convection, which is demonstrated in this study by applying the
bias-corrected data to the fine-scale analysis of a hailstorm that occurred
in Beijing.</p>
      <p id="d1e374">This paper is organized as follows. Sect. 2 describes the data and methods
used in our research. The statistical characteristics of this dataset, bias-correction results and its application to a hailstorm case are presented in
Sects. 3, 4 and 5, respectively. Conclusions and discussion are given in the
final section.</p>

      <?xmltex \floatpos{h!}?><fig id="Ch1.F4"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e379"><bold>(a)</bold> Hourly pressure observation counts (log10 transformed)
averaged over the year 2016. <bold>(b)</bold> Same as <bold>(a)</bold> but for the Chinese Meteorological
Administration (CMA) surface stations. Data are binned into a 0.1<inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M5" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.1<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid in <bold>(a)</bold> and <bold>(b)</bold>. The location of the port of
Shanghai and the port of Tianjin are labeled as “SH” and “TJ” in <bold>(a)</bold>.
The red circles indicate the  urban agglomerations of (from north to
south) Beijing–Tianjin–Hebei region, Shanghai and nearby cities, and
Guangzhou and nearby cities.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f04.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e433"><bold>(a)</bold> Seasonal variation in global hourly counts of
smartphone data for each month. <bold>(b)</bold> Diurnal variation in global smartphone
data counts. <bold>(c)</bold> Annual mean hourly data count at different local standard
times (LSTs) and months.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f05.png"/>

      </fig>

</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data and methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Data description</title>
      <p id="d1e465">Three types of datasets were used to perform this research. (1) Pressure
data were collected by a smartphone mobile weather application every second in
2016. The application collects longitude, latitude, time and pressure data
for each user without an unencrypted or encrypted ID. (2) Pressure data were
collected every 5 min by CMA (Chinese Meteorological Administration)
in 2016. There are 68 909 stations (including automatic weather stations, AWSs, and conventional stations) collecting meteorological data across the
country, but only 13.32 % of the stations make pressure observations.
These weather station surface data are used as the authentication for the bias correction
of smartphone pressure data and for the verification of the surface analysis. (3) Land-use and land-cover data for China in 2015 at a resolution of 1 km were accessed via the Data Center for Resources and Environmental
Sciences, Chinese Academy of Sciences (RESDC; Xu et al., 2018). These
geographical data provide additional information necessary for our
machine-learning-based bias-correction method.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e470">Spatial distribution of the standardized value of the data
number at each site for each hour on 20 July 2016. The time is shown in Beijing standard time (BJT). The
standardized number is defined as the difference between the data number in
this grid at a specific hour and daily mean of the number divided by the
standard deviation of the number. The dark gray color fill stands for the
region in nighttime. Warm colors indicate a rise in data volume, while cool
colors indicate a decrease.</p></caption>
          <?xmltex \igopts{width=441.017717pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f06.png"/>

        </fig>

<?xmltex \hack{\newpage}?>
</sec>
<?pagebreak page788?><sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Quality control and preprocessing</title>
      <p id="d1e489">The quality-control and preprocessing procedure of the smartphone pressure
data is described as follows. A workflow diagram is shown in Fig. 1
summarizing the main processes of the procedure. First, a gross check is
conducted; pressure values lower than 890 hPa or higher than 1080 hPa are
considered outliers and discarded (Kim et al., 2015; Madaus and Mass,
2017). The gross-checked data are referred to as GC-data hereafter. Next, we perform temporal and spatial averaging. As described by
McNicholas and Mass (2018a) and Hintz et al. (2019), there is a spin-up time for each measurement, and location retrieval
for smartphones has an estimation error. To reduce such temporal and spatial
errors, the GC-data are averaged within a specified window of time and
space. The time window size is 5 min to match the temporal interval of
the weather station data or 6 min to match the radar update interval
whenever necessary. The spatial window size is 0.0001<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
latitude and longitude, i.e., the individual smartphone observation points are
binned into specific sites with fixed locations to eliminate the need for
user IDs. The bias correction is then conducted on the aggregated data in a
0.0001<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M9" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.0001<inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid box (<inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> m <inline-formula><mml:math id="M12" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10 m). In the rest of this paper, the aggregated data points will be
referred to as “smartphone sites” for convenience. The next step in the quality-control procedure
is a neighborhood check within each area of 0.01<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M14" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.01<inline-formula><mml:math id="M15" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> latitude and longitude. Data with values greater than 3 times the
standard deviation of the mean pressure in the area are removed. Finally, we
perform a statistical check. The boxplot approach is used to detect and
handle climatological outliers  (Iglewicz and Hoaglin, 1993). For each
boxplot, the upper quartile (<inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula>) is 75 % for the smartphone air-pressure
data, and the lower quartile (<inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>) is 25 %. Data that are 1.5 times the
interquartile range (<inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>) above <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> and below <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> are removed. The
quality-controlled data after all the above steps are referred to as QC-data
hereafter.</p>
      <?pagebreak page789?><p id="d1e630">It should be noted that the quality-control procedure above does not include
elevation correction of the pressure data not only because the Moji
smartphone data do not include the elevation information but also because
the elevation-based pressure correction may contain notable errors due to
the uncertainties in GPS elevation positioning  (Kaplan and Hegarty,
2006; Ye et al., 2018) and in assumed pressure–height relations. As an
alternative, we use a neighborhood-based bias-correction approach, as
described below, to correlate local pressure bias with the land-cover condition
using the machine-learning technique.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Bias correction</title>
      <p id="d1e641">Previous studies have demonstrated the importance of implementing
appropriate validation and bias-correction procedures before using
smartphone pressure data in meteorological analysis  (Muller et al.,
2015; Hanson, 2016; McNicholas and Mass, 2018a). In our study, three machine-learning techniques from the Waikato Environment for Knowledge Analysis
(WEKA) suite (Witten et al., 2011) are used to correct the smartphone
pressure data, and their effectiveness are compared. Unlike previous studies
in which an individual model was trained for each smartphone, in this study,
we developed a method, named the neighborhood-based bias-correction method,
that trains a single model in a specified area rather than for a single
phone. Properly choosing the area size is crucial for the method to work
effectively. It should be small enough to ensure some degree of homogeneity
in terms of geographical conditions, and on the other hand, it cannot be too
small because the machine learning requires a large enough data amount to
work properly. Since both users' behavior and synoptic weather background
differ among seasons, we conducted the training for each season. The data
were randomly separated into training and test sets
(Overeem et al., 2013). The parameters used as input
in the machine learning are listed in Table 1, including pressure from
QC-data, longitude, latitude, time, land cover, number and standard
deviation of raw data aggregated in a grid box, and distance of each
smartphone site from the domain center. The land cover is used to provide geographic
information, which is an important input parameter for the
neighborhood-based bias-correction approach. The number and standard
deviation of raw data aggregated in a grid box are used to provide data
uncertainty. The true pressure value used for the machine leaning is
provided by the 5 min pressure observations from AWS that are
interpolated to each smartphone site. To ensure some consistency in the two types of
pressure data, training data with a pressure bias (the difference of
pressure<?pagebreak page790?> values between smartphone and AWS) greater than 15 hPa are removed.</p>

      <?xmltex \floatpos{h!}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e646">Diurnal variation in the data volume for smartphone data
on the day of the hailstorm (red line) and the annual mean value (blue line)
for 39–41<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 115–118<inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E.
Panels <bold>(a)</bold>–<bold>(d)</bold> show a 3D view of data counts in a 0.05<inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M25" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.05<inline-formula><mml:math id="M26" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid over 6 min (colored columns) before each radar
volume and radar echo (gray columns). The color and height of each column
represent the value of the data count. BJ, Beijing; TJ, Tianjin.</p></caption>
          <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f07.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e707"><bold>(a, b)</bold> Pressure time series during the training period for
the AWS (black line) and smartphones (red dots); smartphone pressure was
interpolated into station location using the inverse distance weighting
method. <bold>(c)</bold> The domains of the machine-learning area. Shaded areas are regional land
use (PF, paddy field; RC, rainfed cropland; CFL, closed forest land; S,
shrubbery; SWL, sparse woodland; OWL, open woodlot; HCG, high-coverage
grassland; MCG, moderate coverage grassland; LCG, low-coverage grassland; G,
graff; L, lake; R, reservoir pond; PGS, permanent glacier snow; TF, tidal
flat; FL, flood land; UL, urban land; RSA, rural settlement area; OCL, other
construction land; S, sand; Go, Gobi; SAL, saline-alkali land; W, wetland;
BE, barren earth; BER, bare exposed rock). Automatic weather stations (AWSs)
with pressure observations are shown by black triangles (HD: Haidian; MTG: Mentougou; SJS: Shijingshan; FT: Fengtai; CY: Chaoyang; SY: Shunyi; FS: Fangshan; BJ: Beijing; TZ: Tongzhou; DX: Daxing; DC: Dachang; XH: Xianghe; LF: Langfang; GA: Guan; ZZ: Zhuozhou).</p></caption>
          <?xmltex \igopts{width=384.112205pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f08.png"/>

        </fig>

      <p id="d1e722">In order to evaluate the performance of the neighborhood-based bias-correction method, three experiments with the following machine-learning
methods, multilayer perceptron (MP)  (Pal and Mitra, 1992), support vector
machine (SVM)  (Shevade et al., 2000; Smola and Schölkopf, 2004), and
random forest (RF) (Breiman, 2001), were conducted, and their
results will be compared later.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Objective analysis</title>
      <p id="d1e733">It is well known that an accurate 2D surface analysis is
extremely useful for nowcasting severe weather and studying convective
processes. Traditionally, this type of analysis is mainly obtained from
surface weather station observations. However, since most of the weather
stations do not have pressure measurements, the surface pressure analysis
from them can only depict gross features of large-scale flow. The dense
pressure observations from smartphones create an opportunity to improve the
surface pressure analysis. In this study, we use an objective analysis method
modified from  Barnes (1964) to conduct the analysis. The
modified Barnes analysis method, described below, interpolates randomly
distributed data into a uniformly spaced coordinate system using a two-pass
successive correction method.</p>
      <p id="d1e736">If a variable <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is observed at a location <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, then the
first pass analysis at a grid point <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>g</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>g</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is obtained by Eq. (1):
            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M30" display="block"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>g</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>g</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mo>∑</mml:mo><mml:mi>k</mml:mi></mml:msub><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:msub><mml:mi>f</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi>k</mml:mi></mml:munder><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where the weight <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for the observation point is given by Eq. (2):
            <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M32" display="block"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mfenced open="{" close=""><mml:mrow><mml:mtable class="array" columnalign="left left"><mml:mtr><mml:mtd><mml:mrow><mml:mi mathvariant="normal">exp</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msubsup><mml:mi>r</mml:mi><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow><mml:mrow><mml:mi mathvariant="italic">γ</mml:mi><mml:msup><mml:mi>L</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:mstyle></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mi>r</mml:mi><mml:mo>≤</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mi>e</mml:mi></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mi>r</mml:mi><mml:mo>&gt;</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mi>e</mml:mi></mml:msub></mml:mrow></mml:mtd></mml:mtr></mml:mtable><mml:mo>,</mml:mo></mml:mrow></mml:mfenced></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the distance from the grid point
<inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>g</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>g</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> to the <inline-formula><mml:math id="M35" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>th observation point;
<inline-formula><mml:math id="M36" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula> is the convergence factor which controls the refinement
between the two passes (Barnes, 1974) and lies between 0 and 1
<inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>&lt;</mml:mo><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M38" display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula> is the length scale that controls
the rate of falloff of the weighting function; and <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi>e</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the radius of
influence within which the observations have an impact on the grid point.
Different from the standard Barnes interpolation technique using a uniform
length scale over the analysis domain, an adaptive Barnes scheme is applied
in this paper in which the length scale automatically adapts to data
density, i.e., a spatially variable length scale is computed according to
the data density.</p>
      <p id="d1e1046"><?xmltex \hack{\newpage}?>The analysis in subsequent refinement pass is described by Eq. (3):
            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M40" display="block"><mml:mtable class="split" columnspacing="1em" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>g</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>g</mml:mi></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>g</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>g</mml:mi></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mo>∑</mml:mo><mml:mi>k</mml:mi></mml:msub><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>f</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mo>-</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:msub><mml:mo>∑</mml:mo><mml:mi>k</mml:mi></mml:msub><mml:msub><mml:mi>w</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
          where <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) is the estimate value of <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> at an
observation point which is given by bilinear interpolation.</p>
      <p id="d1e1216">The objective analysis method described above was applied to generate
analysis fields with a 1 km grid spacing for a hailstorm case. In Sect. 5,
we will show that the high-resolution analysis fields can be used to analyze
fine-scale pressure patterns for the hailstorm.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Statistical characteristics</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Spatial distribution</title>
      <p id="d1e1235">We used the GC-data to analyze the spatial and temporal distribution of the
smartphone data counts in 2016. The data location map in Fig. 2 shows that
smartphone data are distributed over nearly all continents, although most of
the data counts occur in China with much higher data density (Fig. 3). The
global mean density of the data is 40 per bin per hour, whereas in China, the
density is 176 per bin per hour. The hourly pressure observation counts for the
entire year of 2016 for China and its surroundings (black box in Fig. 2) are
binned using a 0.1<inline-formula><mml:math id="M43" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M44" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.1<inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid and shown in
Fig. 4a, which indicates that the data density is higher in megacities, such
as the densely populated urban agglomerations of the Yangtze River Delta
(Shanghai and nearby cities), Pearl River Delta (Guangzhou and nearby
cities), and Beijing–Tianjin–Hebei region (marked by red circles in Fig. 4a). Because people carry mobile phones while traveling internationally,
ship trajectories can be seen from two ports, the port of Shanghai (SH) and
the port of Tianjin (TJ) (Fig. 4a), but the amount of data at sea is much
lower than on land. However, in comparison with the surface observations of the Chinese Meteorological Administration (CMA) (Fig. 4b), the amount and
spatial coverage of the smartphone data are remarkable in nearly all
regions.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Temporal distribution</title>
      <p id="d1e1271">The seasonal and diurnal distributions of the GC-data are displayed in Fig. 5 The data volume peaks during the Northern Hemisphere summer and reaches a
minimum in winter (Fig. 5a, c). The annual mean data volume is 279 377 per hour, which far exceeds the value of 47 000 per day in Korean shown in Kim
et al. (2015), suggesting a large user base of the Moji Weather app. The
data seasonality indicates that people check the weather more frequently in
summer than in winter, owing to the fact that the app can only get the
pressure information when the network is available and when the<?pagebreak page791?> users open
the app either on the front end or back end. The diurnal variation in global
data volume (Fig. 5b, c) shows two peaks at 07:00 and 18:00 local
standard time (LST), corresponding to the rush hour in the morning and
evening, respectively. Additionally, there is a steep decrease in data volume
at night, which is consistent with a previous report that smartphone data are
inhomogeneously distributed throughout the day  (Hintz et al.,
2019). The diurnal distribution characteristic indicates that users tend to
check the weather before going to work in the morning and getting off work
in the evening. To demonstrate this more clearly, the spatial distribution
of the standardized value of the hourly data number at each site is computed for 2 d and displayed in Fig. 6. Interestingly, the data volume peak occurs
earlier in northeast China, which corresponds well with an earlier sunrise
(Fig. 6b).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9"><?xmltex \currentcnt{9}?><?xmltex \def\figurename{Figure}?><label>Figure 9</label><caption><p id="d1e1276"><bold>(a)</bold> Mean absolute error (MAE) distribution at different
training subdomains for different machine-learning methods (MP refers to
multilayer perception method; SMO refers to support vector machine method;
RF refers to random forest method). Panel <bold>(b)</bold> is the same as <bold>(a)</bold> but for
computation time.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f09.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><?xmltex \def\figurename{Figure}?><label>Figure 10</label><caption><p id="d1e1295">Distribution of domain-average mean absolute error (MAE;
<bold>a</bold>, <bold>c</bold>) of ensemble mean and standard deviation <bold>(b, d)</bold>
for different subdomains for the original dataset <bold>(a, b)</bold> and the
bias-corrected dataset <bold>(c, d)</bold>. The line marked by dots is the ensemble mean
value, and shading is the double standard deviation ensemble spread. The red line
is the result for stable sites, and the blue line is the result for additional
sites. See text for the definitions of stable sites and additional sites.</p></caption>
          <?xmltex \igopts{width=384.112205pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f10.png"/>

        </fig>

      <p id="d1e1320">Analysis during a hailstorm that occurred in Beijing further reveals that
people respond promptly to severe weather events. The hailstorm occurred on
10 June 2016 as a squall line passed through Beijing city from 14:00 to
17:00 LST. The hourly data volume on the day of the hailstorm and annual mean
hourly data within 39–41<inline-formula><mml:math id="M46" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N,
115–118<inline-formula><mml:math id="M47" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E are plotted in Fig. 7. The
diurnal cycle on the day of the hailstorm shows that, in addition to the two
peaks in the morning and evening, another peak appeared at 16:00 LST with a data
volume 3 times that of the annual mean. A 3D view of the data volume and
radar echo accumulated within 6 min (Fig. 7b–d) clearly shows a rise in
data volume (Fig. 7b, d) as the storm approaches Beijing and Tianjin and a
drop after the storm passes (Fig. 7c), which demonstrates the influence of
severe weather on human behavior.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><?xmltex \currentcnt{11}?><?xmltex \def\figurename{Figure}?><label>Figure 11</label><caption><p id="d1e1343"><bold>(a, b)</bold> Scatter plot of mean absolute error (MAE) versus the
data number of observation sites for <bold>(a)</bold> stable sites and <bold>(b)</bold> additional
sites. <bold>(c, d) </bold> Scatter plot of station pressure versus bias-corrected
pressure for <bold>(c)</bold> the neighborhood-based method and <bold>(b)</bold> single-site method
of one ensemble member. Averaged mean absolute errors (MAEs) of the two methods
are shown in the plot.</p></caption>
          <?xmltex \igopts{width=384.112205pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f11.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12" specific-use="star"><?xmltex \currentcnt{12}?><?xmltex \def\figurename{Figure}?><label>Figure 12</label><caption><p id="d1e1371">The 5 min pressure change from surface stations
(triangles) and the 6 min pressure change from smartphones (points),
temperature observations from surface station (green contour), wind field
(black arrow), and composite radar reflectivity (shaded) during a hailstorm
that occurred on 10 June 2016 in Beijing, China. The station pressure
change is shown at the time closest to that of the radar volume. The
“<inline-formula><mml:math id="M48" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula>” symbol marks the locations where the 6 min pressure
change perturbation is greater than 0.52 hPa. The dashed blue line is the
<inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula> K
isoline from the analysis of surface observations (<inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is defined as the difference between the equivalent
potential temperature at a point and the domain-averaged value).</p></caption>
          <?xmltex \igopts{width=412.564961pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f12.png"/>

        </fig>

      <?xmltex \floatpos{p}?><fig id="Ch1.F13"><?xmltex \currentcnt{13}?><?xmltex \def\figurename{Figure}?><label>Figure 13</label><caption><p id="d1e1421">Objective analysis domain (blue box), terrain height
(shaded), the distribution of surface stations (black and red dots with the
red dots representing the surface stations with pressure measurements) and
Beijing radar station (star). The boundary of Beijing is shown with the blue
line.</p></caption>
          <?xmltex \igopts{width=221.931496pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f13.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Evaluation of the bias-correction method</title>
      <p id="d1e1439">Three neighborhood-based bias-correction experiments, each using one of the
aforementioned machine-learning methods, were conducted on a domain covering
Beijing and its surrounding area from May to August 2016. The machine-learning bias correction was performed in each of the subdomains in Fig. 8c
using surface observations as the truth and<?pagebreak page792?> the smartphone input parameters
listed in Table 1. The region was affected by the 10 June 2016 hailstorm
and had a high density of smartphone pressure observations (Fig. 7a–d).</p>
      <p id="d1e1442">Constrained by the requirements of adequate data samples and reasonable
computation cost, we chose 16 subdomains of 0.25<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
(longitude) <inline-formula><mml:math id="M52" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.20<inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (latitude) in size. The pressure
time series from two representative stations in Fig. 8a and b show that,
although the trend in the weather station and smartphone is consistent, bias
is clearly present, which is consistent with the results of Price
et al. (2018) and Hintz et al. (2019).</p>
      <p id="d1e1470">Figure 9 shows the mean absolute error (MAE) and computation time at different
training regions for the three methods; it is evident that the RF method is
more accurate and time saving. The computation times for subdomain 2 and
subdomain 6 using the SMO method are more than 9 h. From this comparison, we have
found that the RF algorithm is more suitable for the neighborhood-based
bias correction of smartphone observations without requiring users'<?pagebreak page793?> personal
information. Furthermore, we discovered that the random data separation into
training set and test set can cause random errors in the bias-corrected
data; hence, in order to eliminate these errors, the correction procedure was
repeated for 50 times to generate an ensemble result.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F14" specific-use="star"><?xmltex \currentcnt{14}?><?xmltex \def\figurename{Figure}?><label>Figure 14</label><caption><p id="d1e1476">Surface pressure perturbation analyses (shaded) from the
experiment SFC <bold>(a, c, e)</bold> and SFC <inline-formula><mml:math id="M54" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SP <bold>(b, d, f)</bold> overlaid by VDRAS
wind field at 150 m (thick black arrows) and column maximum radar
reflectivity (contours). The valid time is 15:00 LST for the top row, 15:06 LST for the middle row and 15:12 LST for the bottom row.</p></caption>
        <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f14.png"/>

      </fig>

      <p id="d1e1498">Collecting smartphone data through a weather app is convenient and common; however,
the approach relies on the loyalty of users. Calibrating smartphone pressure
individually can be only applied to data from long-term users, but it
cannot be used for recently added users. In contrast, performing data
correction for the aggregated data in a 0.0001<inline-formula><mml:math id="M55" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M56" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.0001<inline-formula><mml:math id="M57" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid box in a subdomain makes it possible to collect data from
both user groups. In order to evaluate the applicability of our method on
data from both types of users, we define the data sites appearing in both the
training set and test set as stable sites and those only appearing in the test
set as additional sites. To quantify the performance of bias correction, the
domain-average MAE and standard deviation of ensemble mean for the 16
subdomains are displayed in Fig. 10 for the raw and bias-corrected data from
both the stable sites and the additional sites. The MAE was calculated using
data from the smartphone sites for each subdomain. Comparing the MAEs between the raw (Fig. 10a) and bias-corrected data (Fig. 10c), it is evident that the
neighborhood-based bias-correction method is capable of substantially
reducing the MAE not only for the stable sites but also for the additional
sites with slightly more reduction for the stable sites (from 5.95  to
0.53 hPa) than for the additional sites (from 5.90  to 0.99 hPa). It is
also shown that the method reduces the MAE spread by 78 % for the stable
sites and by 16 % for the additional sites (Fig. 10b, d). A lower MAE and
spread reduction for the additional sites is not surprising because they are
newly added data with shorter data history and hence have fewer data samples
(Fig. 11a, b). Encouragingly, our results suggest that the
neighborhood-based method can partially mitigate the difficulty related to
recently added data with shorter data history. In comparison with the bias-correction method based on a single site, the neighborhood-based method
resulted in a substantially smaller MAE (see Fig. 11c, d).</p>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Impact of smartphone data on hailstorm analysis</title>
      <p id="d1e1535">High-density pressure observations can potentially help identify small-scale
surface pressure patterns beneath a thunderstorm  (Johnson and
Hamilton, 1988). Although the quality-controlled gridded smartphone pressure
data reduce the number of data points, they are still adequate to represent
the fine-scale pressure patterns. In this section, we first show what
small-scale information the quality-controlled high-density pressure data at
the smartphone sites (with a spatial resolution of 0.0001<inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> or approximately 10 m) can provide and then demonstrate the impact of the smartphone data on
the gridded 1 km pressure analysis that is obtained using the objective
analysis method described in Sect. 2.4.</p>
      <p id="d1e1547">Figure 12 shows a composite plot of radar reflectivity, pressure changes
calculated from surface weather station observations and from smartphone
data, and wind and equivalent potential temperature from the station
observations. To be consistent with the time interval of the radar volume scan,
the smartphone QC-data averaged every 6 min were used to generate the
6 min pressure tendency. Further, because the weather station data are at
a 5 min interval, the pressure change and temperature from these data are
shown at times closest to those of the radar volume scan. Since there are only
15 weather stations providing pressure observations in this region, they are
unable to locate the leading edge of the cold pool. In contrast, the
smartphone pressure observations are much denser and hence are able<?pagebreak page794?> to
capture the fine-scale pressure change associated with the cold pool, as
depicted in Fig. 12 by the “<inline-formula><mml:math id="M59" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula>” symbol representing the 6 min
change in perturbation pressure (i.e., domain mean subtracted) greater than
0.52 mb. Compared with the cold pool leading edge identified by <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, following Schlemmer and Hohenegger (2014), from the
analysis of surface observations, the leading edge of the cold pool based on
the smartphone pressure change is about 10 km ahead at 15:06 LST (Fig. 12b)
and quite close at 15:24 LST (Fig. 12c). At 14:54 LST (Fig. 12a), the pressure
change is largely negative ahead of the cold pool, whereas Fig. 12d mainly
shows negative pressure changes after the leading edge has passed the area;
both are consistent with the surface station observations but are more detailed.</p>
      <p id="d1e1568">We conducted three objective analysis experiments using the method described
in Sect. 2.4 to demonstrate the potential benefit of using smartphone
observations along with surface weather station observations to improve
surface pressure analyses, i.e., the station observation
experiment (SFC) using only weather
station pressure observations, smartphone experiment (SP) using only smartphone data, and SFC <inline-formula><mml:math id="M61" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SP
using both the station and smartphone data. The analysis grid spacing is 1 km. Figure 13 shows the domain for surface analysis and the locations of the Beijing radar and surface stations.</p>
      <p id="d1e1578">The analyses of perturbation pressure (i.e., relative to domain mean) from
the experiments SFC (Fig. 14a, c, e) and SFC <inline-formula><mml:math id="M62" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SP (Fig. 14b, d, f) are
compared at 15:00, 15:06 and 15:12 LST in Fig. 14. To illustrate the coupling
between pressure and wind in the storm region, the wind field at 150 m from
VDRAS (Variational Doppler Radar Analysis System) and the composite
reflectivity observation are overlaid. VDRAS is a rapid update analysis
system based on the variational technique that blends radar radial velocity
and surface wind observations to produce 3D wind analyses (Sun
and Crook, 1997, 1998). We first note that the perturbation pressure
analysis from SFC <inline-formula><mml:math id="M63" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SP (right column) displays small-scale features in and
around the storm that are absent in SFC (left column). The high center of
pressure perturbation is nearly collocated with the center of the outflow
near the northwest flank of the main body of the storm system (Fig. 14b, d,
f). The vertical cross sections<?pagebreak page795?> shown in Fig. 15 through the line A–B (see
Fig. 14) indicate that the high-pressure perturbation corresponds to the
rear-flank downdraft aloft behind the intense radar echoes of the
southeastward moving convective system. Although the relatively low-pressure
regions are seen in front of the convective system in both experiments, only the SFC <inline-formula><mml:math id="M64" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SP experiment captures the relatively low-pressure region
northwest of the system. The overall distribution pattern of pressure
perturbation in SFC <inline-formula><mml:math id="M65" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SP is consistent with the conceptual model of
Markowski and Richardson (2010), but the current analysis reveals that
the surface high-pressure region and low-level divergence center slightly
lag behind the center of the intense reflectivity echoes rather than right
beneath it, as in their conceptual model. We believe the difference
results from the higher resolution of the smartphone data applied in this
study, but further studies are needed to draw a definite conclusion.
Furthermore, the pressure analysis from SFC <inline-formula><mml:math id="M66" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SP provides more detailed
information about storm evolution than what is shown in SFC. As the storm
moves southeastward, the cell in the southwest, denoted as cell 2 in Fig. 14,
separates into two (Fig. 14b), and the northern one merges into cell 1 (Fig. 14d, f). During the merging process, the high-pressure region behind cell 1
becomes stronger and wider, which may indicate the enhancement of cell 1 in
correspondence with the increased downdraft and updraft, as shown in Fig. 15c.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F15"><?xmltex \currentcnt{15}?><?xmltex \def\figurename{Figure}?><label>Figure 15</label><caption><p id="d1e1619">Vertical cross section of the radar reflectivity
(shaded), VDRAS wind field (thin black arrows) and vertical velocity field
(brown contours with dash lines for downward motion and solid lines for
upward motion) along the line A–B in Fig. 10. The solid blue line and
dashed red line are the surface pressure perturbation along the A–B line from
SFC and SFC <inline-formula><mml:math id="M67" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SP, respectively.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f15.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F16" specific-use="star"><?xmltex \currentcnt{16}?><?xmltex \def\figurename{Figure}?><label>Figure 16</label><caption><p id="d1e1637"><bold>(a)</bold>–<bold>(o)</bold> Temporal distribution of mean absolute error
(MAE) between model analyses and observations at different surface stations
for the smartphone experiment (SP; red line), the station observation
experiment (SFC; blue line) and the station observation plus smartphone
experiment (SFC <inline-formula><mml:math id="M68" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SP; black dash line), respectively. The
temporally averaged MAE is also shown within each plot, and the average MAEs
over all stations for the three experiments are shown below the plots. The
underlined and bold station names indicate that the MAE difference between SFC
and SP at those stations is significant with the confidence level of
90 %. The stations are as follows: HD: Haidian; MTG: Mentougou; SJS: Shijingshan; FT: Fengtai; CY: Chaoyang; SY: Shunyi; FS: Fangshan; BJ: Beijing; TZ: Tongzhou; DX: Daxing; DC: Dachang; XH: Xianghe; LF: Langfang; GA: Guan; ZZ: Zhuozhou.</p></caption>
        <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f16.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F17"><?xmltex \currentcnt{17}?><?xmltex \def\figurename{Figure}?><label>Figure 17</label><caption><p id="d1e1660">Scatter plot of mean absolute error (MAE) versus
observation number within 10 km and 5 min of the verifying
weather station. The blue dots stand for the station observation experiment
(SFC), red dots represent the smartphone experiment (SP), and the station
observation plus smartphone experiment (SFC <inline-formula><mml:math id="M69" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SP) is shown as black
crosses.</p></caption>
        <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://amt.copernicus.org/articles/14/785/2021/amt-14-785-2021-f17.png"/>

      </fig>

      <p id="d1e1676">Analysis accuracy for the two experiments was verified against the 15
weather station pressure measurements in the domain. In order to avoid
dependence between the analysis<?pagebreak page796?> and verification, both experiments were
repeated 15 times; each alternately excludes the measurement from the
specific station to be verified against. The temporal distributions of MAE
between model analysis and observation at different surface stations are
shown in Fig. 16. The results confirm that the experiment SFC <inline-formula><mml:math id="M70" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SP reduces
the analysis error at most stations, even at those around which there are
relatively fewer smartphone observations, such as the stations Xianghe (XH) and Langfang (LF).
Although at the stations where there are much fewer smartphone observations,
such as Guan (GA) and Zhuozhou (ZZ), the analysis with smartphone pressure data alone in the
experiment SP results in a larger error than in the experiment SFC; adding the
station observations in SFC <inline-formula><mml:math id="M71" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> SP results in reduced analysis error (Fig. 16n, o). The correlation between the smartphone data density and the
analysis accuracy is more clearly illustrated by Fig. 17, which shows that
the MAE is less than 0.20 hPa as long as there are more than three
smartphone sites around the verifying weather station measurement.</p>
      <?pagebreak page797?><p id="d1e1693">In summary, our quantitative verification results demonstrate that the
high-resolution smartphone data generally improve surface pressure analysis
in comparison with the weather station data; combining these two datasets
results in a further improvement, especially at the locations where the
smartphone data are sparse.</p>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusions and discussion</title>
      <p id="d1e1704">This study focused on smartphone pressure data acquired from the Moji
Weather app in 2016 and showed their characteristics for the first time. A
neighborhood-based bias-correction method applying machine-learning
techniques was developed without any privacy information needed. The
bias-corrected data were employed to explore the potential value of these
data for improving atmospheric analysis through the case of a hailstorm in
Beijing, China.</p>
      <p id="d1e1707">Since these data are produced by citizens at large, their spatial and
temporal distributions are affected by human behavior. It was shown that
the data are mostly distributed around urban areas, and data volume peaks
during summer. There is also a diurnal cycle in which the data volume is
higher during the day than at night, with two peaks appearing at 07:00
and 18:00 LST. Our case study showed an anomalous increase in data volume
when the hailstorm occurred, suggesting that public concern increases in
anticipation of<?pagebreak page798?> high-impact weather situations, which means the data can be
useful for disaster prevention.</p>
      <p id="d1e1710">We proposed and demonstrated a neighborhood-based bias-correction method
that can address user privacy issues. Despite growing concern from the
public regarding personal privacy, few studies have addressed how to
circumvent the problem. Since Moji protects data privacy during the
collection and processing stages, no private information was included in the
raw data that we received, and the bias-correction method proposed in this
study does not require such information. Our results showed that the MAE and
MAE spread can be successfully reduced not only for long-term stable sites
but also for recently added sites that present a challenge using the
traditional user-based bias-correction method.</p>
      <p id="d1e1713">With this feasible and effective bias-correction method, the potential
utility of the high-resolution smartphone data (approximately 10 m
horizontal resolution) is shown using a hailstorm case. We have found that
the 6 min pressure change can provide convective-scale information such as
cold pool leading edge, especially in megacities where the data are most
dense. Using a modified Barnes objective analysis method on a 1 km grid, we
also showed that the data can be used in conjunction with weather station
data to improve surface pressure analysis. The analysis is capable of
depicting the high pressure associated with the rear-flank downdraft of the
hailstorm and temporal variation in pressure perturbation related to the
splitting and merging process within the convective system.</p>
      <p id="d1e1717">Through the current study, we have gained an understanding of the smartphone
pressure data characteristics, developed a practical and effective
quality-control and bias-correction method, and demonstrated the value of
the data in surface objective analysis; our next step is to explore whether
the data can be useful in improving convective weather forecasting through
data assimilation. Previous data assimilation research with smartphone
pressure data mainly focused on assessing whether the data have a positive
impact on regions where weather stations are not available (McNicholas
and Mass, 2018b; Hintz et al., 2019). However, it may present a greater
challenge to demonstrate that the smartphone data can yield additional
benefits to the existing weather station network mainly because of the uneven
distribution of the smartphone data across the globe. Efforts are needed to
develop data assimilation approaches that can make best use of the
smartphone data in numerical weather prediction models by taking into
account the characteristics of these data. The current study also points to
the need of an improved smartphone data collection mechanism. The data
volume collected by a weather app relies heavily on the popularity of the
application that serves as the data-collection platform  (Kim et al.,
2015; Hintz et al., 2019). As such, the data distribution relies heavily on
the severity of local weather. Thus, a more stable and widely used platform
is needed to provide useful high-resolution global observations without a
correlation to local weather. Additionally, the smartphone information
included in our research is limited; additional auxiliary information, such
as smartphone models, sensor types and the altitude at which smartphone
data were measured, would be conducive to the bias-correction procedure and
subsequent analysis.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e1724">The land-use and land-cover data are available on the website <ext-link xlink:href="https://doi.org/10.12078/2018070201" ext-link-type="DOI">10.12078/2018070201</ext-link> (Xu et al., 2018). Smartphone data, surface observation data and radar data
are provided by Moji Corporation and the Chinese Meteorological
Administration and are available on demand.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e1733">The analysis and figures were produced by RL, and QZ and JS contributed to the
data analysis and supervised the writing and revision of the paper. YC,
LD and TW provided the data quality-control method used in the paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e1739">The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e1745">This study was supported by the National Natural Science Foundation of China grant no. 42030607.  We thank Moji Corporation for providing the smartphone pressure data.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e1750">This research has been supported by the National Natural Science Foundation of China (grant no. 42030607).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e1756">This paper was edited by Laura Bianco and reviewed by Colin Price and two anonymous referees.</p>
  </notes><ref-list>
    <title>References</title>

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<abstract-html><p>Smartphones are increasingly being equipped with
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global observations. Although China has the highest number of cell phone
users, there is little research on whether these measurements provide useful
information for atmospheric research. Here, for the first time, we present
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irregular spatiotemporal distribution with a high density in urban areas, a
maximum in summer and two daily peaks corresponding to rush hours. With the
dense dataset, we have developed a new bias-correction method based on a
machine-learning approach without requiring users' personal information,
which is shown to reduce the bias of pressure observation substantially. The
potential application of the high-density smartphone data in cities is
illustrated by a case study of a hailstorm that occurred in Beijing in which
high-resolution gridded pressure analysis is produced. It is shown that the
dense smartphone pressure analysis during the storm can provide detailed
information about fine-scale convective structure and decrease errors from
an analysis based on surface meteorological-station measurements. This study
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