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  <front>
    <journal-meta><journal-id journal-id-type="publisher">NHESS</journal-id><journal-title-group>
    <journal-title>Natural Hazards and Earth System Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">NHESS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Nat. Hazards Earth Syst. Sci.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1684-9981</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/nhess-21-723-2021</article-id><title-group><article-title>Typhoon rainstorm simulations with radar data assimilation <?xmltex \hack{\break}?>on the  southeast coast of China</article-title><alt-title>Typhoon rainstorm simulations with radar data assimilation on the southeast coast of China</alt-title>
      </title-group><?xmltex \runningtitle{Typhoon rainstorm simulations with radar data assimilation on the southeast coast of China}?><?xmltex \runningauthor{J. Tian et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Tian</surname><given-names>Jiyang</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Liu</surname><given-names>Ronghua</given-names></name>
          <email>liurh@iwhr.com</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Ding</surname><given-names>Liuqian</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Guo</surname><given-names>Liang</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Zhang</surname><given-names>Bingyu</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>China Institute of Water Resources and Hydropower Research, Beijing, 100038, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Research Center on Flood &amp; Drought Disaster Reduction, the Ministry of Water Resources of China, <?xmltex \hack{\break}?>Beijing, 100038, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Ronghua Liu (liurh@iwhr.com)</corresp></author-notes><pub-date><day>23</day><month>February</month><year>2021</year></pub-date>
      
      <volume>21</volume>
      <issue>2</issue>
      <fpage>723</fpage><lpage>742</lpage>
      <history>
        <date date-type="received"><day>29</day><month>April</month><year>2020</year></date>
           <date date-type="accepted"><day>16</day><month>January</month><year>2021</year></date>
           <date date-type="rev-recd"><day>1</day><month>January</month><year>2021</year></date>
           <date date-type="rev-request"><day>6</day><month>July</month><year>2020</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2021 </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://nhess.copernicus.org/articles/.html">This article is available from https://nhess.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://nhess.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://nhess.copernicus.org/articles/.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e127">As an effective technique to improve the rainfall forecast, data assimilation plays an important role in meteorology and hydrology. The aim of this study is to explore the reasonable use of Doppler radar data assimilation to correct the initial and lateral boundary conditions of the numerical weather prediction (NWP) systems. The Weather Research and Forecasting (WRF) model is applied to simulate three typhoon storm events on the southeast coast of China. Radar data from a Doppler radar station in Changle, China, are assimilated with three-dimensional variational data assimilation (3-DVar) model. Nine assimilation modes are designed by three kinds of radar data and at three assimilation time intervals. The rainfall simulations in a medium-scale catchment, Meixi, are evaluated by three indices, including relative error (RE), critical success index (CSI), and root mean square error (RMSE). Assimilating radial velocity at a time interval of 1 h can significantly improve the rainfall simulations, and it outperforms the other modes for all the three storm events. Shortening the assimilation time interval can improve the rainfall simulations in most cases, while assimilating radar reflectivity always leads to worse simulations as the time interval shortens. The rainfall simulations can be improved by data assimilation as a whole, especially for the heavy rainfall with strong convection. The findings provide references for improving the typhoon rainfall forecasts at catchment scale and have great significance on typhoon rainstorm warning.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

      <?xmltex \hack{\newpage}?>
<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e141">Although the resolution of numerical weather prediction (NWP) systems is increasing with the improvement of computational efficiency and abundance of observation data, rainfall is still one of the most difficult meteorological factors to forecast (Lu et al., 2017; Avolio and Federico, 2018). A typhoon always comes with heavy rainfall which leads to great loss. However, due to the uncertainty of the rainfall and the imperfect generation of NWP systems, rainfall forecast with severe convection is unsatisfactory in medium and small catchment scales (Tian et al., 2017a). Data assimilation plays an important role in NWP and is always applied to correct the initial and lateral boundary condition of NWP systems, which can effectively improve the rainfall forecast (Mohan et al., 2015; Liu et al., 2018).</p>
      <p id="d1e144">Various kinds of observation data have been tested and assimilated by different assimilation methods. Wan and Xu (2011) simulated a heavy rainstorm using the Weather Research and Forecasting (WRF) model with the Gridpoint Statistical Interpolation (GSI) data assimilation (DA) system in the central Guangdong Province of southeast China. The rainfall simulation error was reduced at 4 <inline-formula><mml:math id="M1" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> grid scale by assimilating satellite radiance data, which helped to analyze rainfall causes accurately. Giannaros et al. (2016) evaluated a lightning data assimilation (LTNGDA) technique over eight rainfall events occurring in Greece. The verification scores of the rainfall simulations were significantly improved by the employment of the WRF-LTNGDA scheme, especially for heavy rainfall. Zhang et al. (2013) presented a regional ensemble data assimilation system that assimilated microwave radiances into the WRF model for hydrological applications.<?pagebreak page724?> The rainfall simulations were improved in terms of the accumulated rainfall and spatial rainfall distribution in the southeastern United States. Yucel et al. (2015) assimilated conventional meteorological data by a three-dimensional variational data assimilation (3-DVar) model into the coupled atmospheric–hydrological system. The rainfall simulations, as well as the runoff simulations, improve significantly in large basins in the western Black Sea region of Turkey.</p>
      <p id="d1e155">Due to their high spatiotemporal resolution, radar data are assimilated to correct the NWP system for mesoscale and microscale weather prediction (Milan et al., 2008; Zhao and Jin, 2008). Wang et al. (2013) tested the four-dimensional variational data assimilation (4-DVar) system by simulating a midlatitude squall-line case in the US Great Plains, and the results indicated that radar data assimilation was able to improve rainfall forecasts from the WRF model at the convective scale. Liu et al. (2013) selected four storm events in a small catchment (135.2 <inline-formula><mml:math id="M2" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) located in southwest England to explore the effect of data assimilation for rainfall forecasts based on the WRF model, and assimilating radar reflectivity by the 3-DVar model can significantly improve the forecasting accuracy for the events with one-dimensional evenness in either space or time. By using the WRF model and Advanced Regional Prediction System (ARPS) 3-Dvar, Hou et al. (2015) improved the short-term forecast skill by up to 9 h by assimilating radar data in southern China.</p>
      <p id="d1e169">Most studies focus on the assimilation algorithm and data selection.  However, consistent conclusions have not been obtained for the option of radar reflectivity and radial velocity, and few studies pay attention to the time interval setting of data assimilation. Based on the WRF and 3-DVar models, Tian et al. (2017b) found that radar reflectivity assimilation led to better rainfall simulations than radial velocity assimilation at the time interval of 6 h. Maiello et al. (2014) assimilated both radar reflectivity and radial velocity by the 3-DVar model with a 3 h assimilation cycle to improve the WRF high-resolution initial conditions, and the rainfall forecast became more accurate for several experiments in the urban area of Rome. Bauer et al. (2015) used the WRF model in combination with the 3-DVar scheme to estimate the rainfall simulations, and the results showed that radar data assimilation significantly improved the rainfall simulations by a 1 h Rapid Update Cycle at the high resolution of 3 <inline-formula><mml:math id="M3" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> in Germany.</p>
      <p id="d1e181">In reality, the operational forecasts from meteorological departments are guidance forecasts with a large forecasting area. It is impossible to focus on the accuracy of the rainfall in small and medium catchment scales. Limited computing power means that the number of restarting times for the forecasting system is only 2–4 times per day (Xie et al., 2016). The forecasting accuracy descends gradually as the run time goes on because the data assimilation is not in real time. Due to the poor accuracy at small scales and low resolutions, the rainfall forecasting from the meteorological department cannot be used directly as the input for hydrological forecasting in small and medium catchments (Tian et al., 2019). The local meteorological observations are necessary to be assimilated to improve the high-resolution rainfall forecast. The NWP model may not be corrected in a timely manner at a long time interval of data assimilation, while shortening the time interval needs a lot of computational resources, and the observation errors in local meteorological observations may also be amplified with high assimilation frequency in the NWP model.</p>
      <p id="d1e184">China suffers approximately nine tropical cyclones (TCs) each year on average (Shen et al., 2017). Most TCs develop into typhoons which always bring huge economic losses and a great number of casualties. Fujian is one of the most regularly affected provinces on the coastline of southeast China, and heavy rainfall caused by the interaction of typhoons and complex terrain leads to severe flood disasters. Accurate rainfall forecasting is of great significance to flood control and disaster mitigation. However, typhoon rainstorms are still difficult to predict (Li et al., 2019). There are eight Doppler radar stations to obtain full coverage for meteorological monitoring in Fujian Province. The plentiful radar data provide convenience and a basis for the exploration of radar data assimilation at catchment scale.</p>
      <p id="d1e187">In this study, Meixi catchment located in Fujian Province is chosen as the study area. Due to the frequent heavy rainfall, flood disasters are up more than 20 times since 1949. On 9 July 2016, heavy rainfall caused by typhoon Nepartak led to severe flooding and attracted strong interest from the public, academics, and government. Accurate rainfall simulations have a great practical significance in the study area. In order to explore the reasonable use of Doppler radar data assimilation to correct the initial and lateral boundary conditions of the NWP systems, the WRF model is applied to simulate three typhoon storm events affecting the Meixi catchment, and the 3-DVar model is used to assimilate the radar data to improve the typhoon rainstorm simulations. Nine assimilation modes are designed by three kinds of radar data (radar reflectivity, radial velocity, and radar reflectivity and radial velocity) and at three assimilation time intervals (1, 3, and 6 h). The rainfall simulations are evaluated by three indices, including relative error (RE), critical success index (CSI), and root mean square error (RMSE).</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Study area and case studies</title>
      <p id="d1e198">The Meixi catchment lies in central-eastern Fujian Province with a subtropical monsoon climate (Fig. 1). The drainage area is 956 <inline-formula><mml:math id="M4" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, and the average annual rainfall is approximately 1560 <inline-formula><mml:math id="M5" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula>. There are eight rain gauges and one hydrologic station (Fig. 2). In order to investigate the radar data assimilation effects on rainfall simulations, different kinds of rainfall processes caused by different stages of the typhoons are chosen in Meixi catchment. Three rainfall storms are shown in Table 1. Saola formed on 28 July 2012 and<?pagebreak page725?> landed at Fuding, Fujian, by 3 August. Then Saola weakened into a tropical storm at Jiangxi. With the movement of Saola, Meixi catchment was not directly affected, and the accumulated 24 h rainfall was only 84 <inline-formula><mml:math id="M6" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula>.  Hagibis landed at Shantou, Guangdong, on 15 June 2014 and then moved toward the north at a fast-moving speed. Fortunately, Hagibis weakened into a tropical depression quickly while moving to northeastern Fujian on 17 June.  Event II occurred after the typhoon passed Meixi catchment, and the accumulated 24 h rainfall was only 66 <inline-formula><mml:math id="M7" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula>. Nepartak reached Fujian on 9 July 2016 and strengthened at Putian. Then Nepartak moved towards the northwest at a fast-moving speed, and event III occurred when Nepartak was close to Meixi catchment. During the period, Nepartak reached its peak intensity. The 24 h accumulated rainfall was 242 <inline-formula><mml:math id="M8" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula>, which led to a high peak flow of 4710 <inline-formula><mml:math id="M9" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> in Meixi catchment. The most destructive flood caused water and power outages in 11 villages and towns. Official figures stand at 74 dead and 15 missing from the flood, which also caused a direct economic loss of CNY 5.234 billion. Accurate rainfall forecasts appeared to be particularly important for Meixi catchment.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e267">The location of the Meixi catchment and three nested domains.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f01.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e278">Radar scan area and Meixi basin.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f02.png"/>

      </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Table}?><label>Table 1</label><caption><p id="d1e291">Three storm events occurring in Meixi catchment.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Event ID</oasis:entry>
         <oasis:entry colname="col2">Typhoon</oasis:entry>
         <oasis:entry colname="col3">Storm start time (<inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mtext>UTC</mml:mtext><mml:mo>+</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4">Storm end time (<inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:mtext>UTC</mml:mtext><mml:mo>+</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">24 h accumulated</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">rainfall (mm)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">I</oasis:entry>
         <oasis:entry colname="col2">Saola</oasis:entry>
         <oasis:entry colname="col3">3 August 2012 00:00</oasis:entry>
         <oasis:entry colname="col4">4 August 2012 00:00</oasis:entry>
         <oasis:entry colname="col5">84</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">II</oasis:entry>
         <oasis:entry colname="col2">Hagibis</oasis:entry>
         <oasis:entry colname="col3">17 June 2014 21:00</oasis:entry>
         <oasis:entry colname="col4">18 June 2014 21:00</oasis:entry>
         <oasis:entry colname="col5">66</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">III</oasis:entry>
         <oasis:entry colname="col2">Nepartak</oasis:entry>
         <oasis:entry colname="col3">8 July 2016 18:00</oasis:entry>
         <oasis:entry colname="col4">9 July 2016 18:00</oasis:entry>
         <oasis:entry colname="col5">242</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Model description and numerical experiments</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Model description</title>
<sec id="Ch1.S3.SS1.SSS1">
  <label>3.1.1</label><title>WRF model and configurations</title>
      <p id="d1e448">As the latest-generation mesoscale NWP system, the WRF model in version 4.0 is used to simulate the three typhoon storm events. Three nested domains (Dom 1, Dom 2, and Dom 3) with two-way nesting are designed and centered over Meixi catchment. The grid spacings are set at 4, 12, and 36 <inline-formula><mml:math id="M12" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> for the three nested domains from inside to outside (Chen et al., 2017). The grid numbers for the nested domain sizes are <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mn mathvariant="normal">100</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> for Dom 1, <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:mn mathvariant="normal">210</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">210</mml:mn></mml:mrow></mml:math></inline-formula> for Dom 2, and <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:mn mathvariant="normal">300</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">300</mml:mn></mml:mrow></mml:math></inline-formula> for Dom 3 (Fig. 1). Meixi catchment is completely covered by the innermost domain. All domains are comprised of 40 vertical pressure levels with the top level set at 50 <inline-formula><mml:math id="M16" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">hPa</mml:mi></mml:mrow></mml:math></inline-formula> (Maiello et al., 2014). The NCEP Final (FNL) Operational Global Analysis data with <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> grids are used to drive the WRF model and provide the initial and lateral boundary conditions. The time step is set to be 1 h for the WRF model output. The spin-up period of 12 h is applied to obtain a more accurate rainfall simulation. The option of physical parameterizations has a significant effect on the rainfall simulations, especially for microphysics, planetary boundary layer (PBL), radiation, land surface model (LSM), and cumulus physics (Otieno et al., 2019). According to the previous studies on physics options selection, WRF Single-Moment 6 (WSM 6) for microphysics, Yonsei University (YSU) for PBL, the Rapid Radiative Transfer Model for application to GCMs (RRTMG) for longwave and shortwave radiation, Noah for LSM, and Kain–Fritsch (KF) for cumulus physics are adopted in this study (Srivastava et al., 2015; Hazra et al., 2017; Cai et al., 2018; Tian et al., 2021).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Table}?><label>Table 2</label><caption><p id="d1e527">Physical parameterizations used in the WRF model.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Physical parameterization</oasis:entry>
         <oasis:entry colname="col2">Scheme</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Microphysics</oasis:entry>
         <oasis:entry colname="col2">WRF Single-Moment 6 (WSM 6)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Planetary boundary layer (PBL)</oasis:entry>
         <oasis:entry colname="col2">Yonsei University (YSU)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Longwave and shortwave radiation</oasis:entry>
         <oasis:entry colname="col2">Rapid Radiative Transfer Model for application to GCMs (RRTMG)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Land surface model (LSM)</oasis:entry>
         <oasis:entry colname="col2">Noah</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Cumulus</oasis:entry>
         <oasis:entry colname="col2">Kain–Fritsch (KF)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S3.SS1.SSS2">
  <label>3.1.2</label><title>The 3-DVar data assimilation and observation operator</title>
      <p id="d1e607">The fundamental aim of the 3-DVar data assimilation is to produce an optimal estimate of the true atmospheric state by the iterative solution of a prescribed cost function (Ide et al., 1997):

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M18" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E1"><mml:mtd><mml:mtext>1</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>J</mml:mi><mml:mfenced open="(" close=")"><mml:mi mathvariant="bold-italic">x</mml:mi></mml:mfenced><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>-</mml:mo><mml:msup><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:mrow></mml:mfenced><mml:mi>T</mml:mi></mml:msup><mml:msup><mml:mi mathvariant="bold">B</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>-</mml:mo><mml:msup><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mtr><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo>-</mml:mo><mml:msup><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:mfenced><mml:mi>T</mml:mi></mml:msup><mml:msup><mml:mi mathvariant="bold">R</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo>-</mml:mo><mml:msup><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>

              where <inline-formula><mml:math id="M19" display="inline"><mml:mi mathvariant="bold-italic">x</mml:mi></mml:math></inline-formula> is the vector of the analysis, <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> is the vector of first guess or background, <inline-formula><mml:math id="M21" display="inline"><mml:mi mathvariant="bold-italic">y</mml:mi></mml:math></inline-formula> is the vector of the model-derived observation that is transformed from <inline-formula><mml:math id="M22" display="inline"><mml:mi mathvariant="bold-italic">x</mml:mi></mml:math></inline-formula> by the observation operator <inline-formula><mml:math id="M23" display="inline"><mml:mi mathvariant="bold">H</mml:mi></mml:math></inline-formula>, i.e., <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="bold">H</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> is the vector of the observation. <inline-formula><mml:math id="M26" display="inline"><mml:mi mathvariant="bold">B</mml:mi></mml:math></inline-formula> is the background error covariance matrix, and <inline-formula><mml:math id="M27" display="inline"><mml:mi mathvariant="bold">R</mml:mi></mml:math></inline-formula> is the observational and representative error covariance matrix. Equation (<xref ref-type="disp-formula" rid="Ch1.E1"/>) shows that the 3-DVar is based on a multivariate incremental formulation. Velocity potential, total water mixing ratio, unbalanced pressure, and stream function are all preconditioned control variables. Radial velocity has already been derived into component winds that are the same as the analysis variables; hence, radial velocity can be assimilated directly by Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>). However, radar reflectivity assimilation needs an additional forward operator that associates the model hydrometeors with the radar reflectivity. Due to the wide applicability, the matrix of CV3 is adopted in this<?pagebreak page726?> study to simplify the data assimilation procedure (Meng and Zhang, 2008).</p>
      <p id="d1e811">The observation operator <inline-formula><mml:math id="M28" display="inline"><mml:mi mathvariant="bold">H</mml:mi></mml:math></inline-formula> in Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>) links the model variables to the observation variables. For radar reflectivity, the observation operator is shown as follows (Sun and Crook, 1997):
              <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M29" display="block"><mml:mrow><mml:mi>Z</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">43.1</mml:mn><mml:mo>+</mml:mo><mml:mn mathvariant="normal">17.5</mml:mn><mml:mi>log⁡</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M30" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> is the radar reflectivity (in dBZ), <inline-formula><mml:math id="M31" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula> is the density of air (in <inline-formula><mml:math id="M32" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kg</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), and <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is rainwater mixing ratio (in <inline-formula><mml:math id="M34" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">kg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>). Equation (<xref ref-type="disp-formula" rid="Ch1.E2"/>) is derived by assuming a Marshall–Palmer raindrop size distribution and that the ice phases have no effect on reflectivity.</p>
      <p id="d1e914">For radial velocity, the model-derived radial velocity <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can be calculated as follows (Tian et al., 2017b):
              <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M36" display="block"><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi>u</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi>v</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>y</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mfenced close=")" open="("><mml:mrow><mml:mi>w</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>v</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>z</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M37" display="inline"><mml:mi>u</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M38" display="inline"><mml:mi>v</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M39" display="inline"><mml:mi>w</mml:mi></mml:math></inline-formula> are the three-dimensional wind field, <inline-formula><mml:math id="M40" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M41" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M42" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula> represent the location of the observation point, and <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> represent the location of the radar station; <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the distance between the location of a data point and the radar station, and <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the hydrometeor fall speed or terminal velocity. According to Sun and Crook (1998), <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can be given by

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M49" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E4"><mml:mtd><mml:mtext>4</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>v</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5.40</mml:mn><mml:mi>a</mml:mi><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">0.125</mml:mn></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E5"><mml:mtd><mml:mtext>5</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi>a</mml:mi><mml:mo>=</mml:mo><mml:msup><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow><mml:mover accent="true"><mml:mi>p</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">0.4</mml:mn></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where <inline-formula><mml:math id="M50" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> is the correction factor, <inline-formula><mml:math id="M51" display="inline"><mml:mover accent="true"><mml:mi>p</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> is the base-state pressure, and <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the pressure at the ground.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Numerical experiments</title>
<sec id="Ch1.S3.SS2.SSS1">
  <label>3.2.1</label><title>Assimilation modes</title>
      <p id="d1e1243">An S-band Doppler weather radar located at Changle can completely cover Meixi catchment. The observation radius of Changle radar reaches 250 <inline-formula><mml:math id="M53" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula>, and the distance between Meixi catchment and the radar station is less than 100 <inline-formula><mml:math id="M54" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km<?pagebreak page727?></mml:mi></mml:mrow></mml:math></inline-formula> (Fig. 2), which makes the quality of radar data credible. The assimilated data – radar reflectivity and radial velocity – can be obtained once every 6 min continuously. All the radar data with quality control are provided by the newest generation weather radar network of China (CINRAD/SC). The observation error standard deviations of radar reflectivity and radial velocity are set 2 <inline-formula><mml:math id="M55" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">dBZ</mml:mi></mml:mrow></mml:math></inline-formula> and 1 <inline-formula><mml:math id="M56" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> in the 3-DVar model, respectively (Caya et al., 2005). The radar data assimilation modes are designed by three kinds of radar data (radar reflectivity, radial velocity, and radar reflectivity and radial velocity) and at three assimilation time intervals (1, 3, and 6 h).  The rainfall simulation without data assimilation is used as the control mode.  Nine modes are shown in Table 3.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Table}?><label>Table 3</label><caption><p id="d1e1290">Radar data assimilation modes designed with data types and time intervals.</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="justify" colwidth="18mm"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="30mm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Modes</oasis:entry>
         <oasis:entry colname="col2">Time intervals of data assimilation</oasis:entry>
         <oasis:entry colname="col3">Assimilated radar<?xmltex \hack{\hfill\break}?>data</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">1</oasis:entry>
         <oasis:entry colname="col2">6 h</oasis:entry>
         <oasis:entry colname="col3">Radar reflectivity</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">2</oasis:entry>
         <oasis:entry colname="col2">6 h</oasis:entry>
         <oasis:entry colname="col3">Radial velocity</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">3</oasis:entry>
         <oasis:entry colname="col2">6 h</oasis:entry>
         <oasis:entry colname="col3">Radar reflectivity<?xmltex \hack{\hfill\break}?>and radial velocity</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">4</oasis:entry>
         <oasis:entry colname="col2">3 h</oasis:entry>
         <oasis:entry colname="col3">Radar reflectivity</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">5</oasis:entry>
         <oasis:entry colname="col2">3 h</oasis:entry>
         <oasis:entry colname="col3">Radial velocity</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">6</oasis:entry>
         <oasis:entry colname="col2">3 h</oasis:entry>
         <oasis:entry colname="col3">Radar reflectivity<?xmltex \hack{\hfill\break}?>and radial velocity</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">7</oasis:entry>
         <oasis:entry colname="col2">1 h</oasis:entry>
         <oasis:entry colname="col3">Radar reflectivity</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">8</oasis:entry>
         <oasis:entry colname="col2">1 h</oasis:entry>
         <oasis:entry colname="col3">Radial velocity</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">9</oasis:entry>
         <oasis:entry colname="col2">1 h</oasis:entry>
         <oasis:entry colname="col3">Radar reflectivity<?xmltex \hack{\hfill\break}?>and radial velocity</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <label>3.2.2</label><title>WRF cycling runs for data assimilation</title>
      <p id="d1e1447">In order to obtain the whole process of the rainfall simulations, the running time is set at 3, 42, and 36 h for storm events I, II, and III, respectively. As shown in Fig 3, the cycling runs are set according to the time interval of data assimilation, and run 1 can be regarded as the WRF run without data assimilation. The dashed line segment represents the model spin-up. The first guess generated by run 1 is applied to drive run 2. As time progresses, the first guess file generated in the previous run is used to provide the initial conditions for the following run. For storm event I, data assimilation starts on 3 August 2012 at 00:00 (all times are <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:mtext>UTC</mml:mtext><mml:mo>+</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula>) and occurs at intervals of 6, 3, and 1 h. The start time of data assimilation is 18:00 on 17 June 2014, and the end time is 00:00 on 18 June 2014 for storm event II. Data assimilation takes place on 8 July at 18:00 and ends on 9 July at 18:00 at intervals of 6, 3, and 1 h for storm event III.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e1464">The time bars of the assimilation cycling runs for <bold>(a)</bold> storm event I, <bold>(b)</bold> storm event II, and <bold>(c)</bold> storm event III.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f03.png"/>

          </fig>

</sec>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Rainfall evaluation statistics</title>
      <p id="d1e1493">In this study, the observation of areal rainfall in Meixi catchment is averaged by the eight stations with the Thiessen polygon method (Sivapalan and Blöschl, 1998), while the simulation of areal rainfall is averaged from all grids of the WRF model inside the Meixi catchment. The relative error (RE) is used to evaluate the total rainfall amount simulation:
          <disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M58" display="block"><mml:mrow><mml:mtext>RE</mml:mtext><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msup><mml:mi>P</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>-</mml:mo><mml:mi>P</mml:mi></mml:mrow><mml:mi>P</mml:mi></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
        where <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msup><mml:mi>P</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> is the simulation of 24 h accumulated areal rainfall, and <inline-formula><mml:math id="M60" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> is the observation of 24 h accumulated areal rainfall.</p>
      <p id="d1e1547">The spatiotemporal patterns of the rainfall simulations are evaluated by the critical success index (CSI) and modified root mean square error (m-RMSE), which is defined as the ratio of root mean square error (RMSE) to the mean values of the corresponding observations (Liu et al., 2012; Prakash et al., 2014; Agnihotri and Dimri, 2015):
          <disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M61" display="block"><mml:mrow><mml:mtext>CSI</mml:mtext><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>N</mml:mi></mml:mfrac></mml:mstyle><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:munderover><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mtext>NA</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mtext>NA</mml:mtext><mml:mi>i</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mtext>NB</mml:mtext><mml:mi>i</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mtext>NC</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

          <disp-formula id="Ch1.E8" content-type="numbered"><label>8</label><mml:math id="M62" display="block"><mml:mrow><mml:mtext>m-RMSE</mml:mtext><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:msqrt><mml:mrow><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>M</mml:mi></mml:mfrac></mml:mstyle><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>M</mml:mi></mml:munderover><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:msubsup><mml:mi>P</mml:mi><mml:mi>j</mml:mi><mml:mo>′</mml:mo></mml:msubsup><mml:mo>-</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt><mml:mrow><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>M</mml:mi></mml:mfrac></mml:mstyle><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>M</mml:mi></mml:munderover><mml:msub><mml:mi>P</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
        The CSI is calculated based on the rain or no rain contingency table (Dai et al., 2019). Table 4 shows that <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:mtext>rainfall</mml:mtext><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M64" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">h</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> as the threshold is regarded as no rain. In order<?pagebreak page728?> to evaluate the simulation of spatial rainfall distribution by CSI, <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:msub><mml:mtext>NA</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mtext>NB</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:msub><mml:mtext>NC</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> at each time step <inline-formula><mml:math id="M68" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> h) are calculated by comparing the rainfall observation with the simulation extracted at eight rain gauge locations, and then the values of <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:msub><mml:mtext>NA</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:msub><mml:mtext>NB</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:msub><mml:mtext>NC</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> at all time steps are averaged to produce the final verification results.  Therefore, <inline-formula><mml:math id="M73" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> refers to the total time steps (<inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">24</mml:mn></mml:mrow></mml:math></inline-formula>). For temporal dimension evaluation, <inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:msub><mml:mtext>NA</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mtext>NB</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:msub><mml:mtext>NC</mml:mtext><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are first calculated using the time series data of simulations and observations at each rain gauge <inline-formula><mml:math id="M78" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>), then the averaged index values of all rain gauges are regarded as the final verification results. Thus instead of the simulation time steps, <inline-formula><mml:math id="M80" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> represents the total number of the rainfall gauges (<inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula>) for temporal dimension evaluation. The perfect score of CSI is 1.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Table}?><label>Table 4</label><caption><p id="d1e1895">Rain/no rain contingency table for the WRF simulation against observation.</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="justify" colwidth="25mm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Simulation/observation</oasis:entry>
         <oasis:entry colname="col2">Rain</oasis:entry>
         <oasis:entry colname="col3">No rain <?xmltex \hack{\newline}?>(<inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M83" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">h</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Rain</oasis:entry>
         <oasis:entry colname="col2">NA (hit)</oasis:entry>
         <oasis:entry colname="col3">NB (false alarm)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">No rain (<inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M85" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">h</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">NC (failure)</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e2008">The m-RMSE is calculated using Eq. (<xref ref-type="disp-formula" rid="Ch1.E8"/>). For spatial dimension evaluation, <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msubsup><mml:mi>P</mml:mi><mml:mi>j</mml:mi><mml:mo>′</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> refer to the simulation and observation of 24 h accumulated rainfall at rain gauge <inline-formula><mml:math id="M88" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>, respectively. <inline-formula><mml:math id="M89" display="inline"><mml:mi>M</mml:mi></mml:math></inline-formula> is the total number of rain gauges (<inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:mi>M</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula>). For temporal dimension evaluation, <inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:msubsup><mml:mi>P</mml:mi><mml:mi>j</mml:mi><mml:mo>′</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the simulation and observation of areal rainfall at each time <inline-formula><mml:math id="M93" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>, respectively. <inline-formula><mml:math id="M94" display="inline"><mml:mi>M</mml:mi></mml:math></inline-formula> represents the total amount of time (<inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:mi>M</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">24</mml:mn></mml:mrow></mml:math></inline-formula>). The perfect score of RMSE is 0.</p>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Results</title>
<sec id="Ch1.S5.SS1">
  <label>5.1</label><title>Accumulated rainfall simulations of the nine data assimilation modes</title>
      <p id="d1e2129">Nine data assimilation modes for three storm events are evaluated by RE for 24 h accumulated areal rainfall. The average values of the RE (ARE) of the three storm events for each mode are also calculated. As shown in Table 5, data assimilation modes make the rainfall simulations worse according to the REs of event I. Only mode 8 has the closest rainfall simulation to the observation in the nine data assimilation modes, and the RE is below 1 %. For event II, all data assimilation modes can improve the accumulated rainfall simulations, while for event III, most modes make the accumulated rainfall simulations better except for modes 2 and 3. Mode 8, i.e., assimilating radial velocity at a time interval of 1 h, always has the lowest RE and performs the best. The improvement of the rainfall simulations is the most obvious for event III, and the rainfall magnitude is quite close to the observation, which has important significance in torrential<?pagebreak page729?> rainfall forecasts and catastrophic flood forecasts in medium and small basins.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Table}?><label>Table 5</label><caption><p id="d1e2135">Accumulated rainfall simulation values (mm) and RE values (%) of the nine data assimilation modes for three storm events.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="8">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right" colsep="1"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right" colsep="1"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:thead>
       <oasis:row>

         <oasis:entry colname="col1" morerows="1">Modes</oasis:entry>

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

         <oasis:entry rowsep="1" namest="col4" nameend="col5" align="center" colsep="1">Event II </oasis:entry>

         <oasis:entry rowsep="1" namest="col6" nameend="col7" align="center">Event III </oasis:entry>

         <oasis:entry colname="col8" morerows="1">ARE (%)</oasis:entry>

       </oasis:row>
       <oasis:row>

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

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

         <oasis:entry colname="col4">Rainfall</oasis:entry>

         <oasis:entry colname="col5">RE</oasis:entry>

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

         <oasis:entry colname="col7">RE</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1"/>

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

         <oasis:entry colname="col3">(%)</oasis:entry>

         <oasis:entry colname="col4">simulation</oasis:entry>

         <oasis:entry colname="col5">(%)</oasis:entry>

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

         <oasis:entry colname="col7">(%)</oasis:entry>

         <oasis:entry colname="col8"/>

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

         <oasis:entry colname="col1"/>

         <oasis:entry colname="col2">(mm)</oasis:entry>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4">(mm)</oasis:entry>

         <oasis:entry colname="col5"/>

         <oasis:entry colname="col6">(mm)</oasis:entry>

         <oasis:entry colname="col7"/>

         <oasis:entry colname="col8"/>

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

         <oasis:entry colname="col1">No radar</oasis:entry>

         <oasis:entry colname="col2"><?xmltex \hack{\hfill}?> 85.16</oasis:entry>

         <oasis:entry colname="col3"><?xmltex \hack{\hfill}?>  0.88</oasis:entry>

         <oasis:entry colname="col4"><?xmltex \hack{\hfill}?> 43.16</oasis:entry>

         <oasis:entry colname="col5"><?xmltex \hack{\hfill}?> 34.32</oasis:entry>

         <oasis:entry colname="col6"><?xmltex \hack{\hfill}?> 64.20</oasis:entry>

         <oasis:entry colname="col7"><?xmltex \hack{\hfill}?> 73.47</oasis:entry>

         <oasis:entry colname="col8"><?xmltex \hack{\hfill}?> 36.22</oasis:entry>

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

         <oasis:entry colname="col1">data assimilation</oasis:entry>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4"/>

         <oasis:entry colname="col5"/>

         <oasis:entry colname="col6"/>

         <oasis:entry colname="col7"/>

         <oasis:entry colname="col8"/>

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

         <oasis:entry colname="col1">1</oasis:entry>

         <oasis:entry colname="col2"><?xmltex \hack{\hfill}?> 61.74</oasis:entry>

         <oasis:entry colname="col3"><?xmltex \hack{\hfill}?> 26.86</oasis:entry>

         <oasis:entry colname="col4"><?xmltex \hack{\hfill}?> 70.37</oasis:entry>

         <oasis:entry colname="col5"><?xmltex \hack{\hfill}?> 7.09</oasis:entry>

         <oasis:entry colname="col6"><?xmltex \hack{\hfill}?> 66.79</oasis:entry>

         <oasis:entry colname="col7"><?xmltex \hack{\hfill}?> 72.40</oasis:entry>

         <oasis:entry colname="col8"><?xmltex \hack{\hfill}?> 35.45</oasis:entry>

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

         <oasis:entry colname="col1">2</oasis:entry>

         <oasis:entry colname="col2"><?xmltex \hack{\hfill}?> 60.97</oasis:entry>

         <oasis:entry colname="col3"><?xmltex \hack{\hfill}?> 27.77</oasis:entry>

         <oasis:entry colname="col4"><?xmltex \hack{\hfill}?> 80.88</oasis:entry>

         <oasis:entry colname="col5"><?xmltex \hack{\hfill}?> 23.09</oasis:entry>

         <oasis:entry colname="col6"><?xmltex \hack{\hfill}?> 58.59</oasis:entry>

         <oasis:entry colname="col7"><?xmltex \hack{\hfill}?> 75.79</oasis:entry>

         <oasis:entry colname="col8"><?xmltex \hack{\hfill}?> 42.22</oasis:entry>

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

         <oasis:entry colname="col1">3</oasis:entry>

         <oasis:entry colname="col2"><?xmltex \hack{\hfill}?> 35.44</oasis:entry>

         <oasis:entry colname="col3"><?xmltex \hack{\hfill}?> 58.02</oasis:entry>

         <oasis:entry colname="col4"><?xmltex \hack{\hfill}?> 70.85</oasis:entry>

         <oasis:entry colname="col5"><?xmltex \hack{\hfill}?> 7.83</oasis:entry>

         <oasis:entry colname="col6"><?xmltex \hack{\hfill}?> 61.11</oasis:entry>

         <oasis:entry colname="col7"><?xmltex \hack{\hfill}?> 74.75</oasis:entry>

         <oasis:entry colname="col8"><?xmltex \hack{\hfill}?> 46.87</oasis:entry>

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

         <oasis:entry colname="col1">4</oasis:entry>

         <oasis:entry colname="col2"><?xmltex \hack{\hfill}?> 41.49</oasis:entry>

         <oasis:entry colname="col3"><?xmltex \hack{\hfill}?> 50.86</oasis:entry>

         <oasis:entry colname="col4"><?xmltex \hack{\hfill}?> 79.69</oasis:entry>

         <oasis:entry colname="col5"><?xmltex \hack{\hfill}?> 21.29</oasis:entry>

         <oasis:entry colname="col6"><?xmltex \hack{\hfill}?> 71.75</oasis:entry>

         <oasis:entry colname="col7"><?xmltex \hack{\hfill}?> 70.35</oasis:entry>

         <oasis:entry colname="col8"><?xmltex \hack{\hfill}?> 47.50</oasis:entry>

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

         <oasis:entry colname="col1">5</oasis:entry>

         <oasis:entry colname="col2"><?xmltex \hack{\hfill}?> 66.16</oasis:entry>

         <oasis:entry colname="col3"><?xmltex \hack{\hfill}?> 21.63</oasis:entry>

         <oasis:entry colname="col4"><?xmltex \hack{\hfill}?> 72.19</oasis:entry>

         <oasis:entry colname="col5"><?xmltex \hack{\hfill}?> 9.86</oasis:entry>

         <oasis:entry colname="col6"><?xmltex \hack{\hfill}?> 101.23</oasis:entry>

         <oasis:entry colname="col7"><?xmltex \hack{\hfill}?> 58.17</oasis:entry>

         <oasis:entry colname="col8"><?xmltex \hack{\hfill}?> 29.89</oasis:entry>

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

         <oasis:entry colname="col1">6</oasis:entry>

         <oasis:entry colname="col2"><?xmltex \hack{\hfill}?> 37.10</oasis:entry>

         <oasis:entry colname="col3"><?xmltex \hack{\hfill}?> 56.05</oasis:entry>

         <oasis:entry colname="col4"><?xmltex \hack{\hfill}?> 77.49</oasis:entry>

         <oasis:entry colname="col5"><?xmltex \hack{\hfill}?> 17.94</oasis:entry>

         <oasis:entry colname="col6"><?xmltex \hack{\hfill}?> 151.64</oasis:entry>

         <oasis:entry colname="col7"><?xmltex \hack{\hfill}?> 37.34</oasis:entry>

         <oasis:entry colname="col8"><?xmltex \hack{\hfill}?> 37.11</oasis:entry>

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

         <oasis:entry colname="col1">7</oasis:entry>

         <oasis:entry colname="col2"><?xmltex \hack{\hfill}?> 61.12</oasis:entry>

         <oasis:entry colname="col3"><?xmltex \hack{\hfill}?> 27.60</oasis:entry>

         <oasis:entry colname="col4"><?xmltex \hack{\hfill}?> 80.64</oasis:entry>

         <oasis:entry colname="col5"><?xmltex \hack{\hfill}?> 22.72</oasis:entry>

         <oasis:entry colname="col6"><?xmltex \hack{\hfill}?> 104.28</oasis:entry>

         <oasis:entry colname="col7"><?xmltex \hack{\hfill}?> 56.91</oasis:entry>

         <oasis:entry colname="col8"><?xmltex \hack{\hfill}?> 35.74</oasis:entry>

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

         <oasis:entry colname="col1">8</oasis:entry>

         <oasis:entry colname="col2"><?xmltex \hack{\hfill}?> 83.65</oasis:entry>

         <oasis:entry colname="col3"><?xmltex \hack{\hfill}?> 0.91</oasis:entry>

         <oasis:entry colname="col4"><?xmltex \hack{\hfill}?> 70.67</oasis:entry>

         <oasis:entry colname="col5"><?xmltex \hack{\hfill}?> 7.55</oasis:entry>

         <oasis:entry colname="col6"><?xmltex \hack{\hfill}?> 227.96</oasis:entry>

         <oasis:entry colname="col7"><?xmltex \hack{\hfill}?> 5.80</oasis:entry>

         <oasis:entry colname="col8"><?xmltex \hack{\hfill}?> 4.75</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">9</oasis:entry>

         <oasis:entry colname="col2"><?xmltex \hack{\hfill}?> 82.50</oasis:entry>

         <oasis:entry colname="col3"><?xmltex \hack{\hfill}?> 2.28</oasis:entry>

         <oasis:entry colname="col4"><?xmltex \hack{\hfill}?> 71.31</oasis:entry>

         <oasis:entry colname="col5"><?xmltex \hack{\hfill}?> 8.53</oasis:entry>

         <oasis:entry colname="col6"><?xmltex \hack{\hfill}?> 188.01</oasis:entry>

         <oasis:entry colname="col7"><?xmltex \hack{\hfill}?> 22.31</oasis:entry>

         <oasis:entry colname="col8"><?xmltex \hack{\hfill}?> 11.04</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<sec id="Ch1.S5.SS1.SSS1">
  <label>5.1.1</label><title>Evaluation of assimilating effects for the different kinds of radar data</title>
      <p id="d1e2634">The assimilating effects for three kinds of radar data are compared at different assimilating time intervals. Based on the REs of modes 1, 2, and 3, assimilating radar reflectivity always leads to better simulations than assimilating the other two kinds of radar data at a time interval of 6 h. The worst mode for event I is assimilating both radar reflectivity and radial velocity, while for events II and III, it is assimilating radial velocity.  According to the REs of modes 4, 5, and 6, assimilating radial velocity becomes the best choice at a time interval of 3 h for the three storm events.  Assimilating radar reflectivity has the worst performance in the three modes for events II and III, whereas assimilating radar reflectivity and radial velocity together has the worst performance for event I. When the time interval of data assimilation becomes 1 h, the ranking of assimilation modes for accumulated rainfall simulations is <inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:mtext>assimilating radial velocity</mml:mtext><mml:mo>&gt;</mml:mo><mml:mtext>assimilating radar reflectivity</mml:mtext></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:mtext>radial velocity</mml:mtext><mml:mo>&gt;</mml:mo><mml:mtext>assimilating radar reflectivity</mml:mtext></mml:mrow></mml:math></inline-formula>.</p>
</sec>
<sec id="Ch1.S5.SS1.SSS2">
  <label>5.1.2</label><title>Evaluation of assimilation effects for the different assimilation time intervals</title>
      <p id="d1e2670">The influences of assimilating time intervals on rainfall simulations are analyzed in this section. Comparing the REs of modes 1, 4, and 7, shortening the time interval of radar reflectivity assimilation has no obvious improvement for rainfall simulations and even makes the rainfall simulations worse. For assimilating radial velocity, all the rainfall simulations of the three storm events become more accurate, and the assimilation effects are significantly improved as the time interval shortens from 6 to 1 h. The REs of the three storm events are all lower than 8 % for the radial velocity assimilation at a time interval of 1 h. According to modes 3, 6, and 9, shortening the assimilation time interval can improve the rainfall simulations in most cases for assimilating radar reflectivity and radial velocity at the same time, while only the RE of mode 6 is higher than the RE of mode 3.</p>
</sec>
</sec>
<sec id="Ch1.S5.SS2">
  <label>5.2</label><title>Spatiotemporal distribution of rainfall simulations based on the nine data assimilation modes</title>
      <p id="d1e2682">The spatiotemporal patterns of the rainfall have a significant effect on flood peak and peak time in medium and small catchments. The indices of CSI and RMSE are also applied to compare the nine radar data assimilation modes. The average CSI values and the average RMSE values for the three storm events are also calculated for different modes.</p>
<sec id="Ch1.S5.SS2.SSS1">
  <label>5.2.1</label><title>Evaluation in the spatial dimension</title>
      <p id="d1e2692">Table 6 indicates that although mode 8 with the highest CSI and lowest RMSE is the best choice in the nine data assimilation modes, rainfall simulations with data assimilation are always worse than without data assimilation for event I. Figure 4 shows that the observed rainfall center is located in the east of Meixi catchment, and it rains more in the upstream side than the downstream side. However, the spatial distribution of the accumulated 24 h rainfall with no data assimilation is even. Modes 1 and 2 simulate the rainfall on the east side of Meixi catchment accurately, while the simulated rainfall on the west side is much smaller than the observation. The rainfall simulations of modes 3, 4, 5, and 6 are all even in spatial dimension and lower than the observation. The simulation of mode 7 shows that the rainfall in the downstream side is less than the upstream side, whereas the different distribution in a east–west direction is not obvious, and the simulated rainfall is smaller than the observation. For mode 9, the spatial distribution of rainfall is also inconsistent with the observation. Only the simulation of mode 8 is close to the observed rainfall.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Table}?><label>Table 6</label><caption><p id="d1e2698">CSIs and RMSEs for the spatial distribution of rainfall simulations based on the nine data assimilation modes.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="9">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right" colsep="1"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right" colsep="1"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right" colsep="1"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:thead>
       <oasis:row>

         <oasis:entry colname="col1" morerows="1">Modes</oasis:entry>

         <oasis:entry namest="col2" nameend="col3" align="center" colsep="1">Event I </oasis:entry>

         <oasis:entry namest="col4" nameend="col5" align="center" colsep="1">Event II </oasis:entry>

         <oasis:entry namest="col6" nameend="col7" align="center" colsep="1">Event III </oasis:entry>

         <oasis:entry namest="col8" nameend="col9" align="center">Average values for </oasis:entry>

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

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4"/>

         <oasis:entry colname="col5"/>

         <oasis:entry colname="col6"/>

         <oasis:entry colname="col7"/>

         <oasis:entry namest="col8" nameend="col9" align="center">the three events </oasis:entry>

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

         <oasis:entry colname="col1"/>

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

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

         <oasis:entry colname="col4">CSI</oasis:entry>

         <oasis:entry colname="col5">RMSE</oasis:entry>

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

         <oasis:entry colname="col7">RMSE</oasis:entry>

         <oasis:entry colname="col8">CSI</oasis:entry>

         <oasis:entry colname="col9">RMSE</oasis:entry>

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

         <oasis:entry colname="col1">No radar</oasis:entry>

         <oasis:entry colname="col2">0.7368</oasis:entry>

         <oasis:entry colname="col3">0.1535</oasis:entry>

         <oasis:entry colname="col4">0.4479</oasis:entry>

         <oasis:entry colname="col5">0.5635</oasis:entry>

         <oasis:entry colname="col6">0.6146</oasis:entry>

         <oasis:entry colname="col7">0.7482</oasis:entry>

         <oasis:entry colname="col8">0.5998</oasis:entry>

         <oasis:entry colname="col9">0.4884</oasis:entry>

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

         <oasis:entry colname="col1">data assimilation</oasis:entry>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4"/>

         <oasis:entry colname="col5"/>

         <oasis:entry colname="col6"/>

         <oasis:entry colname="col7"/>

         <oasis:entry colname="col8"/>

         <oasis:entry colname="col9"/>

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

         <oasis:entry colname="col1">1</oasis:entry>

         <oasis:entry colname="col2">0.7614</oasis:entry>

         <oasis:entry colname="col3">0.4524</oasis:entry>

         <oasis:entry colname="col4">0.3587</oasis:entry>

         <oasis:entry colname="col5">0.4070</oasis:entry>

         <oasis:entry colname="col6">0.6154</oasis:entry>

         <oasis:entry colname="col7">0.7841</oasis:entry>

         <oasis:entry colname="col8">0.5785</oasis:entry>

         <oasis:entry colname="col9">0.5478</oasis:entry>

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

         <oasis:entry colname="col1">2</oasis:entry>

         <oasis:entry colname="col2">0.6925</oasis:entry>

         <oasis:entry colname="col3">0.4967</oasis:entry>

         <oasis:entry colname="col4">0.2829</oasis:entry>

         <oasis:entry colname="col5">0.4771</oasis:entry>

         <oasis:entry colname="col6">0.6154</oasis:entry>

         <oasis:entry colname="col7">0.7844</oasis:entry>

         <oasis:entry colname="col8">0.5303</oasis:entry>

         <oasis:entry colname="col9">0.5861</oasis:entry>

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

         <oasis:entry colname="col1">3</oasis:entry>

         <oasis:entry colname="col2">0.6865</oasis:entry>

         <oasis:entry colname="col3">0.6907</oasis:entry>

         <oasis:entry colname="col4">0.3346</oasis:entry>

         <oasis:entry colname="col5">0.4618</oasis:entry>

         <oasis:entry colname="col6">0.6154</oasis:entry>

         <oasis:entry colname="col7">0.8147</oasis:entry>

         <oasis:entry colname="col8">0.5455</oasis:entry>

         <oasis:entry colname="col9">0.6557</oasis:entry>

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

         <oasis:entry colname="col1">4</oasis:entry>

         <oasis:entry colname="col2">0.7436</oasis:entry>

         <oasis:entry colname="col3">0.6261</oasis:entry>

         <oasis:entry colname="col4">0.3561</oasis:entry>

         <oasis:entry colname="col5">0.4359</oasis:entry>

         <oasis:entry colname="col6">0.6154</oasis:entry>

         <oasis:entry colname="col7">0.7905</oasis:entry>

         <oasis:entry colname="col8">0.5717</oasis:entry>

         <oasis:entry colname="col9">0.6175</oasis:entry>

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

         <oasis:entry colname="col1">5</oasis:entry>

         <oasis:entry colname="col2">0.7358</oasis:entry>

         <oasis:entry colname="col3">0.5341</oasis:entry>

         <oasis:entry colname="col4">0.3195</oasis:entry>

         <oasis:entry colname="col5">0.4170</oasis:entry>

         <oasis:entry colname="col6">0.6096</oasis:entry>

         <oasis:entry colname="col7">0.7123</oasis:entry>

         <oasis:entry colname="col8">0.5550</oasis:entry>

         <oasis:entry colname="col9">0.5545</oasis:entry>

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

         <oasis:entry colname="col1">6</oasis:entry>

         <oasis:entry colname="col2">0.7143</oasis:entry>

         <oasis:entry colname="col3">0.6614</oasis:entry>

         <oasis:entry colname="col4">0.2212</oasis:entry>

         <oasis:entry colname="col5">0.4783</oasis:entry>

         <oasis:entry colname="col6">0.5909</oasis:entry>

         <oasis:entry colname="col7">0.6285</oasis:entry>

         <oasis:entry colname="col8">0.5088</oasis:entry>

         <oasis:entry colname="col9">0.5894</oasis:entry>

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

         <oasis:entry colname="col1">7</oasis:entry>

         <oasis:entry colname="col2">0.5337</oasis:entry>

         <oasis:entry colname="col3">0.4275</oasis:entry>

         <oasis:entry colname="col4">0.3949</oasis:entry>

         <oasis:entry colname="col5">0.4896</oasis:entry>

         <oasis:entry colname="col6">0.5938</oasis:entry>

         <oasis:entry colname="col7">0.8004</oasis:entry>

         <oasis:entry colname="col8">0.5075</oasis:entry>

         <oasis:entry colname="col9">0.5725</oasis:entry>

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

         <oasis:entry colname="col1">8</oasis:entry>

         <oasis:entry colname="col2">0.7395</oasis:entry>

         <oasis:entry colname="col3">0.1505</oasis:entry>

         <oasis:entry colname="col4">0.4504</oasis:entry>

         <oasis:entry colname="col5">0.3589</oasis:entry>

         <oasis:entry colname="col6">0.6287</oasis:entry>

         <oasis:entry colname="col7">0.1643</oasis:entry>

         <oasis:entry colname="col8">0.6062</oasis:entry>

         <oasis:entry colname="col9">0.2246</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">9</oasis:entry>

         <oasis:entry colname="col2">0.7368</oasis:entry>

         <oasis:entry colname="col3">0.4211</oasis:entry>

         <oasis:entry colname="col4">0.3168</oasis:entry>

         <oasis:entry colname="col5">0.3152</oasis:entry>

         <oasis:entry colname="col6">0.6146</oasis:entry>

         <oasis:entry colname="col7">0.4519</oasis:entry>

         <oasis:entry colname="col8">0.5561</oasis:entry>

         <oasis:entry colname="col9">0.3961</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e3135">Spatial distribution of the simulated 24 h rainfall accumulations with nine data assimilation modes for event I.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f04.png"/>

          </fig>

      <p id="d1e3145">All RMSEs of the simulations with radar data assimilation are lower than without data assimilation, and only the CSI of mode 8 is higher than the simulation without data assimilation for event II. According to the rainfall distribution shown in Fig. 5, the falling areas of simulated rainfall without data assimilation are totally wrong. The observed rainfall center is located in the middle of the upstream and downstream catchment. However, the rainfall centers of modes 1, 4, and 7 are all located in the middle and lower region. The rainfall center is in the middle reaches for mode 2, while it is in the western catchment for mode 3. For modes 5 and 6, the spatial distributions of rainfall are also inconsistent with the observation. The simulated rainfall in the middle of the upstream catchment is close to the observation for modes 8 and 9 but in the downstream catchment is poor. Although the spatial rainfall distributions have deviations, nine modes get better than the simulations without data assimilation as a whole.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e3150">Spatial distribution of the simulated 24 h rainfall accumulations with nine data assimilation modes for event II.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f05.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e3161">Spatial distribution of the simulated 24 h rainfall accumulations with nine data assimilation modes for event III.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f06.png"/>

          </fig>

      <p id="d1e3170">Based on Table 6, not all data assimilation modes help improve the rainfall simulations for event III. Modes 4, 5, and 9 have just a little improvement on rainfall simulations in spatial distribution, and only the simulation of mode 8 is close to the observation. The simulations of modes 1, 2, 3, 4, and 5 are much lower than the observation in the whole catchment.  Most observed rainfall falls in the east of the catchment, while the simulated rainfall concentrates in the west for modes 6 and 9 and in the downstream catchment for mode 7.</p>
      <p id="d1e3173">Based on the CSIs and RMSEs of modes 1, 2, and 3, assimilating radar reflectivity performs better than assimilating the other two kinds of radar data at a time interval of 6 h. Assimilating radar reflectivity and radial velocity at the same time always leads to the worst simulations. Comparing the two indices of modes 4, 5, and 6,<?pagebreak page730?> assimilating radar reflectivity at a time interval of 3 h can obtain the highest CSI for the three storm events, while assimilating radial velocity has a better performance than the other two modes based on RMSE for events I and II. For the time interval of 1 h, the ranking of assimilation modes for the spatial distribution of rainfall simulations is <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:mtext>assimilating radial velocity</mml:mtext><mml:mo>&gt;</mml:mo><mml:mtext>assimilating radar reflectivity</mml:mtext></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mtext>radial velocity</mml:mtext><mml:mo>&gt;</mml:mo><mml:mtext>assimilating radar reflectivity</mml:mtext></mml:mrow></mml:math></inline-formula>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Table}?><label>Table 7</label><caption><p id="d1e3204">CSIs and RMSEs for the temporal distribution of rainfall simulations based on the nine data assimilation modes.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="9">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right" colsep="1"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right" colsep="1"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right" colsep="1"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:thead>
       <oasis:row>

         <oasis:entry colname="col1" morerows="1">Modes</oasis:entry>

         <oasis:entry namest="col2" nameend="col3" align="center" colsep="1">Event I </oasis:entry>

         <oasis:entry namest="col4" nameend="col5" align="center" colsep="1">Event II </oasis:entry>

         <oasis:entry namest="col6" nameend="col7" align="center" colsep="1">Event III </oasis:entry>

         <oasis:entry namest="col8" nameend="col9" align="center">Average values for </oasis:entry>

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

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4"/>

         <oasis:entry colname="col5"/>

         <oasis:entry colname="col6"/>

         <oasis:entry colname="col7"/>

         <oasis:entry namest="col8" nameend="col9" align="center">the three events </oasis:entry>

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

         <oasis:entry colname="col1"/>

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

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

         <oasis:entry colname="col4">CSI</oasis:entry>

         <oasis:entry colname="col5">RMSE</oasis:entry>

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

         <oasis:entry colname="col7">RMSE</oasis:entry>

         <oasis:entry colname="col8">CSI</oasis:entry>

         <oasis:entry colname="col9">RMSE</oasis:entry>

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

         <oasis:entry colname="col1">No radar</oasis:entry>

         <oasis:entry colname="col2">0.6875</oasis:entry>

         <oasis:entry colname="col3">0.6018</oasis:entry>

         <oasis:entry colname="col4">0.3718</oasis:entry>

         <oasis:entry colname="col5">1.3131</oasis:entry>

         <oasis:entry colname="col6">0.6146</oasis:entry>

         <oasis:entry colname="col7">1.9223</oasis:entry>

         <oasis:entry colname="col8">0.5580</oasis:entry>

         <oasis:entry colname="col9">1.2791</oasis:entry>

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

         <oasis:entry colname="col1">data assimilation</oasis:entry>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4"/>

         <oasis:entry colname="col5"/>

         <oasis:entry colname="col6"/>

         <oasis:entry colname="col7"/>

         <oasis:entry colname="col8"/>

         <oasis:entry colname="col9"/>

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

         <oasis:entry colname="col1">1</oasis:entry>

         <oasis:entry colname="col2">0.6830</oasis:entry>

         <oasis:entry colname="col3">1.0351</oasis:entry>

         <oasis:entry colname="col4">0.3069</oasis:entry>

         <oasis:entry colname="col5">1.3843</oasis:entry>

         <oasis:entry colname="col6">0.6034</oasis:entry>

         <oasis:entry colname="col7">1.8138</oasis:entry>

         <oasis:entry colname="col8">0.5311</oasis:entry>

         <oasis:entry colname="col9">1.4111</oasis:entry>

       </oasis:row>
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         <oasis:entry colname="col5">2.0950</oasis:entry>

         <oasis:entry colname="col6">0.6034</oasis:entry>

         <oasis:entry colname="col7">1.8232</oasis:entry>

         <oasis:entry colname="col8">0.4992</oasis:entry>

         <oasis:entry colname="col9">1.6990</oasis:entry>

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

         <oasis:entry colname="col1">3</oasis:entry>

         <oasis:entry colname="col2">0.6421</oasis:entry>

         <oasis:entry colname="col3">1.2414</oasis:entry>

         <oasis:entry colname="col4">0.2969</oasis:entry>

         <oasis:entry colname="col5">1.4631</oasis:entry>

         <oasis:entry colname="col6">0.6034</oasis:entry>

         <oasis:entry colname="col7">1.8318</oasis:entry>

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         <oasis:entry colname="col9">1.5121</oasis:entry>

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

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         <oasis:entry colname="col2">0.6674</oasis:entry>

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         <oasis:entry colname="col5">2.2037</oasis:entry>

         <oasis:entry colname="col6">0.6034</oasis:entry>

         <oasis:entry colname="col7">1.8153</oasis:entry>

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

         <oasis:entry colname="col1">5</oasis:entry>

         <oasis:entry colname="col2">0.6796</oasis:entry>

         <oasis:entry colname="col3">1.1115</oasis:entry>

         <oasis:entry colname="col4">0.2969</oasis:entry>

         <oasis:entry colname="col5">2.0414</oasis:entry>

         <oasis:entry colname="col6">0.6145</oasis:entry>

         <oasis:entry colname="col7">1.7793</oasis:entry>

         <oasis:entry colname="col8">0.5303</oasis:entry>

         <oasis:entry colname="col9">1.6441</oasis:entry>

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

         <oasis:entry colname="col1">6</oasis:entry>

         <oasis:entry colname="col2">0.6667</oasis:entry>

         <oasis:entry colname="col3">1.2878</oasis:entry>

         <oasis:entry colname="col4">0.2031</oasis:entry>

         <oasis:entry colname="col5">2.6387</oasis:entry>

         <oasis:entry colname="col6">0.5851</oasis:entry>

         <oasis:entry colname="col7">2.0122</oasis:entry>

         <oasis:entry colname="col8">0.4850</oasis:entry>

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

         <oasis:entry colname="col1">7</oasis:entry>

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         <oasis:entry colname="col4">0.3125</oasis:entry>

         <oasis:entry colname="col5">2.3337</oasis:entry>

         <oasis:entry colname="col6">0.5938</oasis:entry>

         <oasis:entry colname="col7">1.8452</oasis:entry>

         <oasis:entry colname="col8">0.4537</oasis:entry>

         <oasis:entry colname="col9">1.8974</oasis:entry>

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

         <oasis:entry colname="col1">8</oasis:entry>

         <oasis:entry colname="col2">0.6877</oasis:entry>

         <oasis:entry colname="col3">0.3822</oasis:entry>

         <oasis:entry colname="col4">0.3969</oasis:entry>

         <oasis:entry colname="col5">0.7015</oasis:entry>

         <oasis:entry colname="col6">0.6221</oasis:entry>

         <oasis:entry colname="col7">0.8459</oasis:entry>

         <oasis:entry colname="col8">0.5689</oasis:entry>

         <oasis:entry colname="col9">0.6432</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">9</oasis:entry>

         <oasis:entry colname="col2">0.6875</oasis:entry>

         <oasis:entry colname="col3">1.3862</oasis:entry>

         <oasis:entry colname="col4">0.2663</oasis:entry>

         <oasis:entry colname="col5">1.1180</oasis:entry>

         <oasis:entry colname="col6">0.6146</oasis:entry>

         <oasis:entry colname="col7">1.1699</oasis:entry>

         <oasis:entry colname="col8">0.5228</oasis:entry>

         <oasis:entry colname="col9">1.2247</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{p}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e3641">Time series bars of observed and simulated areal rainfall with nine data assimilation modes and the rainfall observation for event I.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f07.png"/>

          </fig>

      <p id="d1e3650">Comparing the two indices of modes 1, 4, and 7, rainfall simulations become even worse as the time interval of radar reflectivity assimilation shortens.  For the three modes of assimilating radial velocity, most simulations become more accurate, and the assimilation effects are significantly improved as the time interval shortens from 6 to 1 h. The same conclusion can be obtained for assimilating radar reflectivity and radial velocity at the same time, while the improvement is not as obvious as assimilating radial velocity.</p>
</sec>
<?pagebreak page731?><sec id="Ch1.S5.SS2.SSS2">
  <label>5.2.2</label><title>Evaluation in the temporal dimension</title>
      <p id="d1e3661">As shown in Table 7, similar results can be found that most data assimilation modes cannot help the simulations of the WRF model get better for event I. Only mode 8 is outstanding with the highest CSI and lowest RMSE. Figure 7 shows that the rainfall is concentrated at 10:00–16:00 for the observation.  However, the main rainfall processes occur at 03:00–05:00 for modes 3, 4, and 6, 03:00–05:00 and 14:00–15:00 for mode 1, 03:00–05:00 and 17:00–19:00 for mode 2, 03:00–05:00 and 09:00–10:00 for mode 7, and 03:00–05:00 and 20:00–24:00 for mode 9. The rainfall processes of modes 5 and 8 are similar with the observation, while the rainfall<?pagebreak page732?> simulations at 12:00–13:00 and 15:00 for mode 5 are worse than for mode 8.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e3666">Time series bars of observed and simulated areal rainfall with nine data assimilation modes and the rainfall observation for event II.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f08.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><?xmltex \def\figurename{Figure}?><label>Figure 9</label><caption><p id="d1e3677">Time series bars of observed and simulated areal rainfall with nine data assimilation modes and the rainfall observation for event III.</p></caption>
            <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f09.png"/>

          </fig>

      <p id="d1e3687">According to the values of CSI and RMSE, only modes 8 and 9 are useful for the improvement of rainfall simulations, and obvious improvement can be found in mode 8 for event II. The actual main rainfall process occurs at 15:00–18:00, while the time is advanced by 3 h for modes 1, 4, 5, 6, and 7. There is a delay of 3 h for the main rainfall process of mode 3. Although the times of heavy rainfall for modes 2 and 9 are consistent with the observation, the areal rainfall at 18:00 is much higher than the observation.</p>
      <?pagebreak page734?><p id="d1e3690">For event III, although most CSIs of the simulations with radar data assimilation are lower than the simulations without data assimilation, the RMSEs show the opposite conclusions. From Fig. 9, the observed rainfall is concentrated at 08:00–11:00. It can be easily found that modes 1, 2, 3, 4, 5, and 6 cannot reproduce the heavy rainfall process in temporal dimension. The simulated rainfall is concentrated at 15:00–16:00 for mode 7. Only the simulation of mode 8 is basically consistent with the observation, while the simulation of mode 9 is worse than mode 8 at 08:00 and 10:00.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><?xmltex \def\figurename{Figure}?><label>Figure 10</label><caption><p id="d1e3695">Typhoon path and simulations for <bold>(a)</bold> Saola, <bold>(b)</bold> Hagibis, and <bold>(c)</bold> Nepartak.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f10.png"/>

          </fig>

      <p id="d1e3713">According to the CSIs and RMSEs of modes 1, 2, and 3, assimilating radar reflectivity at a time interval of 6 h performs better than assimilating the other two kinds of radar data. Assimilating radial velocity performs the worst for event II, and assimilating radar reflectivity and radial velocity at the same time always leads to the worst simulations for events I and III. Based on the two indices of modes 4, 5, and 6, assimilating radial velocity at a time interval of 3 h can obtain the highest CSI and lowest RMSE for the three storm events, while assimilating radar reflectivity and radial velocity at the same time performs worse than the other two modes. For the time interval of 1 h, the ranking of assimilation modes for the temporal distribution of rainfall simulations is <inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:mtext>assimilating radial velocity</mml:mtext><mml:mo>&gt;</mml:mo><mml:mtext>assimilating radar reflectivity</mml:mtext></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:mtext>radial velocity</mml:mtext><mml:mo>&gt;</mml:mo><mml:mtext>assimilating radar reflectivity</mml:mtext></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e3740">Comparing the indices of modes 1, 4 and 7, rainfall simulations for temporal distribution become even worse as the time interval of radar reflectivity assimilation shortens from 6 to 1 h. For modes 2, 5, and 8, shortening the time interval can significantly improve the rainfall simulations by assimilating radial velocity. Modes 3, 6, and 9 indicate that rainfall simulations are improved by shortening the time interval as a whole, whereas assimilating radar reflectivity and radial velocity at the same time at a time interval of 3 h obtains the worst rainfall simulations for events II and III.</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="d1e3746">Water vapor transportation increment and wind field (850 <inline-formula><mml:math id="M102" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">hPa</mml:mi></mml:mrow></mml:math></inline-formula>) for event I at 12:00 on 3 August 2012.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f11.png"/>

          </fig>

</sec>
</sec>
</sec>
<sec id="Ch1.S6">
  <label>6</label><title>Discussion</title>
      <p id="d1e3773">In order to prove the accuracy of the assimilation results, typhoon paths for different assimilation modes are also simulated (Fig. 10). According to the simulations of Saola and Nepartak, the accurate typhoon path simulations  always lead to accurate rainfall simulations. However, for typhoon Hagibis, the actual typhoon center is far away from the Meixi catchment during the assimilation process. Hence, only the actual typhoon path for Hagibis is added in Fig. 10. Comparing the nine radar data assimilation modes, assimilating radial velocity at a time interval of 6 h always performs the worst in rainfall simulations, while the rainfall simulations can be significantly improved by shortening the time interval of data assimilation.  According to Eq. (<xref ref-type="disp-formula" rid="Ch1.E3"/>), although the physical process of the rainfall formation cannot be influenced by the radial velocity assimilation directly, the wind field and the water vapor transportation in initial and lateral boundary conditions can be changed with the wind information in radial velocity. However, the wind field is quite variable, especially for stormy weather. As the time interval becomes longer, the WRF model cannot be corrected by the radial velocity in time, whereas compared to the simulations without data assimilation, the inevitable observation errors caused by atmospheric refractivity in the radial velocity might lead to worse performance in the WRF model as the running time goes on<?pagebreak page735?> (Montmerle and Faccani, 2009). That is the main reason that assimilating radial velocity at a time interval of 6 h cannot obtain satisfactory simulations. Increasing the frequency of data assimilation, the effective information in radial velocity can correct the wind field and the water vapor transportation in the background field of the WRF model timely, which is helpful to improve the rainfall simulations  (Kawabata et al., 2014).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12" specific-use="star"><?xmltex \currentcnt{12}?><?xmltex \def\figurename{Figure}?><label>Figure 12</label><caption><p id="d1e3780">Wind field and water vapor transportation increment (850 <inline-formula><mml:math id="M103" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">hPa</mml:mi></mml:mrow></mml:math></inline-formula>) for event II at 18:00 on 18 June 2014.</p></caption>
        <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f12.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F13" specific-use="star"><?xmltex \currentcnt{13}?><?xmltex \def\figurename{Figure}?><label>Figure 13</label><caption><p id="d1e3799">Wind field and water vapor transportation increment (850 <inline-formula><mml:math id="M104" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">hPa</mml:mi></mml:mrow></mml:math></inline-formula>) for event III at 06:00 on 9 July 2016.</p></caption>
        <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/21/723/2021/nhess-21-723-2021-f13.png"/>

      </fig>

      <p id="d1e3817">The water vapor transportation increments and wind field for different modes at the rainfall concentrating time are used to show how assimilating radial velocity and radar reflectivity affects the WRF model's initial and boundary conditions (Figs. 11–13). The shadows in Figs. 11–13 mean that water vapor transportation in the analysis field is more than in the background field. The darker the shadow in the figures is, the more the water vapor transportation increment is, which is one of the most important factors that affects the amount of rainfall. For event I, counterclockwise wind field has contributed to the water vapor transportation from ocean to inland at 12:00 on 3 August 2012. Modes 1, 2, 5, 7, 8, and 9 all obtain the shadow area with the obvious water vapor transportation increment. However, according to the coverage area of the shadow, only modes 5 and 8 influence Meixi catchment directly, which is consistent with the result that rainfall simulations with modes 5 and 8 are higher than simulations with no data assimilation at 12:00, while the increment of simulated rainfall is quite obvious for mode 8. The differences of nine modes can be easily found in both the wind field and water vapor transportation increments for event II. The water vapor transportation increases significantly in modes 2, 3, 8, and 9 at 18:00 on 18 June 2014, which has a direct impact on the rainfall simulations in Meixi catchment. That is the main reason why simulated rainfalls with modes 2, 3, 8, and 9 are higher than the simulated rainfall with no data assimilation. However, the wind fields in these modes indicate a lack of warm and wet flow supply, and the rainfall weakening is almost inevitable after 18:00. Considering the wind field and the range of water vapor transportation increments, the rainfalls may continue for a period of time after 18:00 in modes 3, 8, and 9, which can also be reflected by hourly simulated rainfall shown in Fig. 8. For event III, the water vapor transportation increases significantly in modes 2, 3, 5, 6, 7, 8, and 9 at 06:00 on 9 July 2016, while only modes 8 and 9 affect Meixi catchment directly. The range of shadows in Fig. 13 is also consistent with the rainfall simulations. The wind field indicates that water<?pagebreak page738?> vapor transportation is sufficient for mode 8 at a later time, which leads to a significant increase in simulated rainfall.</p>
      <p id="d1e3820">Does further shortening the assimilation interval obtain better rainfall simulations? In terms of theory, the answer is yes because improving the assimilation frequency can correct the initial and lateral boundary conditions in a timely manner. However, the observation errors of radial velocity may be amplified with the high assimilation frequency in the WRF model. There may be an “inverted u” relationship between the accuracy of the rainfall simulations and the assimilation time interval (Myung et al., 2000). Further study should be carried out to investigate the optimal assimilation time interval.</p>
      <?pagebreak page739?><p id="d1e3823">On the contrary, assimilating radar reflectivity offers little help for improving rainfall simulations except for accumulated rainfall.  Furthermore, rainfall simulations become even worse as the time interval of radar reflectivity assimilation shortens from 6 to 1 h. The background field of the WRF model has large differences from the actual weather situation, which can be reflected in the rainfall simulations without data assimilation against the rainfall observations for the three storm events. As shown in Eq. (<xref ref-type="disp-formula" rid="Ch1.E2"/>), radar reflectivity is closely related to the humidity field and contains the information of rainfall hydrometeors (Wattrelot et al., 2014). That is to say the humidity information in radar reflectivity is quite different from the actual weather situation, which makes it difficult for the 3-DVar data assimilation to produce an optimal estimate of the true atmospheric state by the iterative solution of a prescribed cost function. It should also be mentioned that due to its unchangeability, the matrix of CV3 has wide applicability but is not practical for all cases (Kong et al., 2017). The inadaptability of CV3 in the typhoon synoptic system and the large differences between the humidity information in radar reflectivity and the actual weather situation might be the main reasons for the poor performance of radar reflectivity assimilation (Sun, 2005). The more frequent the radar reflectivity assimilation is, the greater the pressure on the 3-DVar data assimilation model is. Other data assimilation models with variable background error covariance, such as the hybrid ensemble transform Kalman filter–three-dimensional variational data assimilation (ETKF-3DVAR) (Wang et al., 2012; Shen et al., 2016), should be tested for radar reflectivity assimilation in future studies.</p>
      <p id="d1e3828">For the even rainfall events in space and time, such as storm event I, data assimilation should be used carefully. The WRF model has good performance in rainfall simulations, especially for accumulated rainfall. The errors in the assimilated data may have a negative effect on the rainfall simulations.  Additionally, assimilating other kinds of data and radar data together may help to improve the rainfall simulations. Though the conventional observations, such as upper-air and surface observations from meteorological stations and sounding balloons, have low spatiotemporal resolution, the kinds of data are various and have wide coverage, which can help to improve the atmospheric motion in the WRF model at large scales (Li et al., 2018).  Yesubabu et al. (2016) indicate that assimilating the satellite observation also has a positive effect on the rainfall simulations. Assimilating different data sources, together with the radar data, may further improve the rainfall simulations at catchment scale. In reality, ECMWF was also tested for the data assimilation before FNL was used in this study (Zhang et al., 2018; Zhao et al., 2012). Although the rainfall simulations show some differences based on the two kinds of boundary conditions, the patterns of improvements from different data assimilation modes are quite similar, and the same conclusions can be obtained.</p>
</sec>
<sec id="Ch1.S7" sec-type="conclusions">
  <label>7</label><title>Conclusions</title>
      <p id="d1e3839">Data assimilation is an efficient technique for improving rainfall simulations. In order to explore the reasonable use of Doppler radar data assimilation to correct the initial and lateral boundary conditions of the NWP systems, three typhoon storm events, including Saola, Hagibis, and Nepartak, are chosen to be simulated by the WRF model with nine modes in Meixi catchment located on the southeast coast of China. The FNL analysis data with <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> grids are used to drive the WRF model, and radar data from the Changle Doppler radar station are applied to correct the initial and lateral boundary conditions. Three evaluating indices, RE, CSI, and RMSE, are used to evaluate the nine radar data assimilation modes, which are designed by three kinds of radar data (radar reflectivity, radial velocity, and radar reflectivity and radial velocity) and at three assimilation time intervals (1, 3, and 6 h).</p>
      <p id="d1e3862">Contrastive analyses of the nine modes are carried out from three aspects: accumulated rainfall simulations, spatial rainfall distribution, and temporal rainfall distribution. Four main conclusions are obtained: (1) in the nine radar data assimilation modes, assimilating radial velocity at a time interval of 1 h can significantly improve the rainfall simulations and outperform the other modes for all the three storm events; (2) shortening the assimilation time interval can improve the rainfall simulations in most cases, while assimilating radar reflectivity always leads to worse simulations as the time interval shortens; (3) radar reflectivity is the best choice for the data assimilation at a time interval of 6 h, while radial velocity performs best for the data assimilation at a time interval of 1 h; and (4) data assimilation can improve the rainfall simulations as a whole, especially for the heavy rainfall with strong convection, whereas the improvement for evenly distributed rainfall in space and time is limited. More numerical simulation experiments should be tested in other catchments in different climate conditions. Further studies also should be carried out to investigate the data assimilation techniques to improve the ability of the simulations of heavy rainfall in the study areas.</p>
</sec>

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

      <p id="d1e3869">The rainfall data from gauges used in this study were provided by the Fujian Institute of Water Resources and Hydropower. The radar data were provided by the newest-generation weather radar network of China (CINRAD/SC). The NCEP Final (FNL) Operational Global Analysis data are available at <uri>https://rda.ucar.edu/datasets/ds083.2/</uri> (NCAR, 2020).</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e3878">All the authors contributed to the conception and the development of this paper. JT and RL contributed to radar data assimilation and paper writing. LD and LG assisted in the design and analyses of the data assimilation modes. BZ helped with the figure production.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e3884">The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e3891">We thank the NHESS editor and two reviewers for constructive comments which improved the study.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e3896">This research has been supported by the National Key R&amp;D Program (grant nos. 2019YFC1510605 and 2018YFC1508105), the National Natural Science Foundation of
China (grant nos. 51909274 and 51822906), and the IWHR Research &amp; Development Support Program (grant nos. JZ0145B032020 and WR0145B732017).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e3902">This paper was edited by Vassiliki Kotroni and reviewed by two anonymous referees.</p>
  </notes><ref-list>
    <title>References</title>

      <ref id="bib1.bib1"><label>1</label><?label 1?><mixed-citation>Agnihotri, G. and Dimri, A. P.: Simulation study of heavy rainfall episodes over the southern Indian peninsula, Meteorol. Appl., 22, 223–235, <ext-link xlink:href="https://doi.org/10.1002/met.1446" ext-link-type="DOI">10.1002/met.1446</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib2"><label>2</label><?label 2?><mixed-citation>Avolio, E. and Federico, S.: WRF simulations for a heavy rainfall event in southern Italy: Verification and sensitivity tests, Atmos. Res., 209, 14–35, <ext-link xlink:href="https://doi.org/10.1016/j.atmosres.2018.03.009" ext-link-type="DOI">10.1016/j.atmosres.2018.03.009</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib3"><label>3</label><?label 3?><mixed-citation>Bauer, H. S., Schwitalla, T., Wulfmeyer V., Bakhshaii, A., Ehret, U., Neuper, M., and Caumont, O: Quantitative precipitation estimation based on high-resolution numerical weather prediction and data assimilation with WRF – a performance test, Tellus A., 67, 25047, <ext-link xlink:href="https://doi.org/10.3402/tellusa.v67.25047" ext-link-type="DOI">10.3402/tellusa.v67.25047</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib4"><label>4</label><?label 4?><mixed-citation>Cai, Y., Lu, X., Chen, G., and Yang, S: Diurnal cycles of Mei-yu rainfall simulated over eastern China: Sensitivity to cumulus convective parameterization, Atmos. Res., 213, 236–251, <ext-link xlink:href="https://doi.org/10.1016/j.atmosres.2018.06.003" ext-link-type="DOI">10.1016/j.atmosres.2018.06.003</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib5"><label>5</label><?label 5?><mixed-citation>Caya, A., Sun, J., and Snyder, C.: A comparison between the 4DVAR and the Ensemble Kalman Filter techniques for radar data assimilation, Mon. Weather Rev., 133, 3081–3094, <ext-link xlink:href="https://doi.org/10.1175/MWR3021.1" ext-link-type="DOI">10.1175/MWR3021.1</ext-link>, 2005.</mixed-citation></ref>
      <ref id="bib1.bib6"><label>6</label><?label 6?><mixed-citation>Chen, X., Wang, Y., Zhao, K., and Wu, D: A numerical study on rapid intensification of typhoon Vicente (2012) in the South China Sea. Part I: verification of simulation, storm-scale evolution, and environmental contribution, Mon. Weather Rev., 145, 877–898, <ext-link xlink:href="https://doi.org/10.1175/MWR-D-16-0147.1" ext-link-type="DOI">10.1175/MWR-D-16-0147.1</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib7"><label>7</label><?label 7?><mixed-citation>Dai, Q., Yang, Q., Han, D., Rico-Ramirez, M. A., and Zhang, S: Adjustment of radar-gauge rainfall discrepancy due to raindrop drift and evaporation using the Weather Research and Forecasting model and dual-polarization radar, Water Resour. Res., 55, 9211–9233, <ext-link xlink:href="https://doi.org/10.1029/2019WR025517" ext-link-type="DOI">10.1029/2019WR025517</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib8"><label>8</label><?label 8?><mixed-citation>Giannaros, T. M., Kotroni, V., and Lagouvardos, K.: WRF-LTNGDA: A lightning data assimilation technique implemented in the WRF model for improving precipitation forecasts, Environ. Model. Softw., 76, 54–68, <ext-link xlink:href="https://doi.org/10.1016/j.envsoft.2015.11.017" ext-link-type="DOI">10.1016/j.envsoft.2015.11.017</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib9"><label>9</label><?label 9?><mixed-citation>Hazra, A., Chaudhari, H. S., Ranalkar, M., and Chen, J. P: Role of interactions between cloud microphysics, dynamics and aerosol in the heavy rainfall event of June 2013 over Uttarakhand, India, Q. J. Roy. Meteor. Soc., 143, 986–998, <ext-link xlink:href="https://doi.org/10.1002/qj.2983" ext-link-type="DOI">10.1002/qj.2983</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib10"><label>10</label><?label 10?><mixed-citation>Hou, T., Kong, F., Chen, X., Lei, H., and Hu, Z: Evaluation of radar and automatic weather station data assimilation for a heavy rainfall event in southern China, Adv. Atmos. Sci., 32, 967–978, <ext-link xlink:href="https://doi.org/10.1007/s00376-014-4155-7" ext-link-type="DOI">10.1007/s00376-014-4155-7</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib11"><label>11</label><?label 11?><mixed-citation>Ide, K., Courtier, P., Ghil, M., and Lorenc, A. C: Unified Notation for data assimilation: Operational, sequential and variational, J. Meteorol. Soc. Jpn., 75, 181–189, <ext-link xlink:href="https://doi.org/10.1175/1520-0469(1997)054&lt;0679:OTRBTS&gt;2.0.CO;2" ext-link-type="DOI">10.1175/1520-0469(1997)054&lt;0679:OTRBTS&gt;2.0.CO;2</ext-link>, 1997.</mixed-citation></ref>
      <ref id="bib1.bib12"><label>12</label><?label 12?><mixed-citation>Kawabata, T., Iwai, H., Seko, H., Shoji, Y., Saito, K., Ishii, S., and Mizutani, K: Cloud-resolving 4D-Var assimilation of Doppler wind lidar data on a Meso-Gamma-Scale convective system, Mon. Weather Rev., 142, 4484–4498, <ext-link xlink:href="https://doi.org/10.1175/MWR-D-13-00362.1" ext-link-type="DOI">10.1175/MWR-D-13-00362.1</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib13"><label>13</label><?label 13?><mixed-citation>Kong, R., Xue, M., and Liu, C. Development of a hybrid En3DVar data assimilation system and comparisons with 3DVar and EnKF for radar data assimilation with observing system simulation experiments, Mon. Weather Rev., 146, 175–198, <ext-link xlink:href="https://doi.org/10.1175/MWR-D-17-0164.1" ext-link-type="DOI">10.1175/MWR-D-17-0164.1</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib14"><label>14</label><?label 14?><mixed-citation>Li, X., Fan, K., and Yu, E.: Hindcast of extreme rainfall with high-resolution WRF: model ability and effect of physical schemes, Theor. Appl. Climatol., 139, 639–658, <ext-link xlink:href="https://doi.org/10.1007/s00704-019-02945-2" ext-link-type="DOI">10.1007/s00704-019-02945-2</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib15"><label>15</label><?label 15?><mixed-citation>Li, Z., Ballard, S. P., and Simonin, D.: Comparison of 3D-Var and 4D-Var data assimilation in an NWP-based system for precipitation nowcasting at the Met Office, Q. J. Roy. Meteor. Soc., 144, 404–413, <ext-link xlink:href="https://doi.org/10.1002/qj.3211" ext-link-type="DOI">10.1002/qj.3211</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib16"><label>16</label><?label 16?><mixed-citation>Liu, J., Bray M., and Han, D.: Sensitivity of the Weather Research and Forecasting (WRF) model to downscaling ratios and storm types in rainfall simulation, Hydrol. Process., 26, 3012–3031, <ext-link xlink:href="https://doi.org/10.1002/hyp.8247" ext-link-type="DOI">10.1002/hyp.8247</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib17"><label>17</label><?label 17?><mixed-citation>Liu, J., Bray, M., and Han D.: Exploring the effect of data assimilation by WRF-3DVar for numerical rainfall prediction with different types of storm events, Hydrol. Process., 27, 3627–3640, <ext-link xlink:href="https://doi.org/10.1002/hyp.9488" ext-link-type="DOI">10.1002/hyp.9488</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib18"><label>18</label><?label 18?><mixed-citation>Liu, J., Tian, J., Yan, D., Li, C., Yu, F., and Shen, F.: Evaluation of Doppler radar and GTS data assimilation for NWP rainfall prediction of an extreme summer storm in northern China: from the hydrological perspective, Hydrol. Earth Syst. Sci., 22, 4329–4348, <ext-link xlink:href="https://doi.org/10.5194/hess-22-4329-2018" ext-link-type="DOI">10.5194/hess-22-4329-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib19"><label>19</label><?label 19?><mixed-citation>Lu, X., Wang X., Li Y., Tong, M., and Ma, X: GSI-based ensemble-variational hybrid data assimilation for HWRF for hurricane initialization and prediction: impact of various error covariances for airborne radar observation assimilation, Q. J. Roy. Meteor. Soc., 143, 223–239, <ext-link xlink:href="https://doi.org/10.1002/qj.2914" ext-link-type="DOI">10.1002/qj.2914</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib20"><label>20</label><?label 20?><mixed-citation>Maiello, I., Ferretti, R., Gentile, S., Montopoli, M., Picciotti, E., Marzano, F. S., and Faccani, C.: Impact of radar data assimilation for the simulation of a heavy rainfall case in central Italy using WRF–3DVAR, Atmos. Meas. Tech., 7, 2919–2935, <ext-link xlink:href="https://doi.org/10.5194/amt-7-2919-2014" ext-link-type="DOI">10.5194/amt-7-2919-2014</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib21"><label>21</label><?label 21?><mixed-citation>Meng, Z. and Zhang, F.: Tests of an ensemble Kalman filter for mesoscale and regional-scale data assimilation. Part III: Comparison with 3DVAR in a real-data case study, Mon. Weather Rev., 136, 522–540, <ext-link xlink:href="https://doi.org/10.1175/mwr3352.1" ext-link-type="DOI">10.1175/mwr3352.1</ext-link>, 2008.</mixed-citation></ref>
      <ref id="bib1.bib22"><label>22</label><?label 22?><mixed-citation>Milan, M., Venema, V., Schüttemeyer, D., and Simmer, C: Assimilation of radar and satellite data in mesoscale model<?pagebreak page741?>s: A physical initialization scheme, Meteorol. Z., 17, 887–902, <ext-link xlink:href="https://doi.org/10.1127/0941-2948/2008/0340" ext-link-type="DOI">10.1127/0941-2948/2008/0340</ext-link>, 2008.</mixed-citation></ref>
      <ref id="bib1.bib23"><label>23</label><?label 23?><mixed-citation>Mohan, G. M., Srinivas, C. V., and Naidu, C. V.: Real-time numerical simulation of tropical cyclone Nilam with WRF: experiments with different initial conditions, 3D-Var and Ocean Mixed Layer Model, Nat. Hazards., 77, 597–624, <ext-link xlink:href="https://doi.org/10.1007/s11069-015-1611-3" ext-link-type="DOI">10.1007/s11069-015-1611-3</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib24"><label>24</label><?label 24?><mixed-citation>Montmerle, T. and Faccani, C.: Mesoscale assimilation of radial velocities from Doppler radars in a preoperational framework, Mon. Weather Rev., 137, 1939–1953, <ext-link xlink:href="https://doi.org/10.1175/2008MWR2725.1" ext-link-type="DOI">10.1175/2008MWR2725.1</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bib25"><label>25</label><?label 25?><mixed-citation>Myung, J. I.: The importance of complexity in model selection, J. Math. Psychol., 44, 190–204, <ext-link xlink:href="https://doi.org/10.1006/jmps.1999.1283" ext-link-type="DOI">10.1006/jmps.1999.1283</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bib26"><label>26</label><?label 1?><mixed-citation>NCAR: NCEP Final (FNL) Operational Global Analysis data, available at: <uri>https://rda.ucar.edu/datasets/ds083.2/</uri>, last access: 10 January 2020.</mixed-citation></ref>
      <ref id="bib1.bib27"><label>27</label><?label 26?><mixed-citation>Otieno, G., Mutemi, J. N., Opijah, F. J., Ogallo, L. A., and Omondi, M. H: The sensitivity of rainfall characteristics to cumulus parameterisation schemes from a WRF model. Part I: a case study over East Africa during wet years, Pure Appl. Geophys., 1, 1–16, <ext-link xlink:href="https://doi.org/10.1007/s00024-019-02293-2" ext-link-type="DOI">10.1007/s00024-019-02293-2</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib28"><label>28</label><?label 27?><mixed-citation>Prakash, S., Sathiyamoorthy, V., Mahesh, C., and Gairola, R. M: An evaluation of high-resolution multisatellite rainfall products over the Indian monsoon region, Int. J. Remote Sens., 35, 3018–3035, <ext-link xlink:href="https://doi.org/10.1080/01431161.2014.894661" ext-link-type="DOI">10.1080/01431161.2014.894661</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib29"><label>29</label><?label 28?><mixed-citation>Shen, F., Min, J., and Xu, D.: Assimilation of radar radial velocity data with the WRF Hybrid ETKF-3DVAR system for the prediction of Hurricane Ike (2008), Atmos. Res., 169, 127–138, <ext-link xlink:href="https://doi.org/10.1016/j.atmosres.2015.09.019" ext-link-type="DOI">10.1016/j.atmosres.2015.09.019</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib30"><label>30</label><?label 29?><mixed-citation>Shen, F., Xue, M., and Min, J.: A comparison of limited-area 3DVAR and ETKF-En3DVAR data assimilation using radar observations at convective scale for the prediction of Typhoon Saomai (2006), Meteorol. Appl., 24, 628–641, <ext-link xlink:href="https://doi.org/10.1002/met.1663" ext-link-type="DOI">10.1002/met.1663</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib31"><label>31</label><?label 30?><mixed-citation>Sivapalan, M. and Blöschl, G.: Transformation of point rainfall to areal rainfall: Intensity-duration-frequency curves, J. Hydrol., 204, 150–167, <ext-link xlink:href="https://doi.org/10.1016/S0022-1694(97)00117-0" ext-link-type="DOI">10.1016/S0022-1694(97)00117-0</ext-link>, 1998.</mixed-citation></ref>
      <ref id="bib1.bib32"><label>32</label><?label 31?><mixed-citation> Srivastava, P. K., Han, D., Rico-Ramirez, M. A., O'Neill, P., Islam, T., Gupta, M., and Dai, Q: Performance evaluation of WRF-Noah Land surface model estimated soil moisture for hydrological application: Synergistic evaluation using SMOS retrieved soil moisture, J. Hydrol., 529, 200–212, 2015.</mixed-citation></ref>
      <ref id="bib1.bib33"><label>33</label><?label 32?><mixed-citation> Sun, J.: Convective-scale assimilation of radar data: progress and challenges, Q. J. Roy. Meteor. Soc., 131, 3439–3463, 2005.</mixed-citation></ref>
      <ref id="bib1.bib34"><label>34</label><?label 33?><mixed-citation>Sun, J. and Crook, N. A.: Dynamical and microphysical retrieval from Doppler radar observations using a cloud model and its adjoint, Part I: model development and simulated data experiments, J. Atmos. Sci., 54, 1642–1661, <ext-link xlink:href="https://doi.org/10.1175/1520-0469(1997)054&lt;1642:DAMRFD&gt;2.0.CO;2" ext-link-type="DOI">10.1175/1520-0469(1997)054&lt;1642:DAMRFD&gt;2.0.CO;2</ext-link>, 1997.</mixed-citation></ref>
      <ref id="bib1.bib35"><label>35</label><?label 34?><mixed-citation>Sun, J. and Crook, N. A.: Dynamical and microphysical retrieval from Doppler radar observations using a cloud model and its adjoint. Part II: retrieval experiments of an observed Florida convective storm, J. Atmos. Sci., 55, 835–852, <ext-link xlink:href="https://doi.org/10.1175/1520-0469(1998)0552.0.CO;2" ext-link-type="DOI">10.1175/1520-0469(1998)0552.0.CO;2</ext-link>, 1998.</mixed-citation></ref>
      <ref id="bib1.bib36"><label>36</label><?label 35?><mixed-citation>Tian, J., Liu, J., Wang, J., Li, C., Yu, F., and Chu, Z: A spatio-temporal evaluation of the WRF physical parameterisations for numerical rainfall simulation in semi-humid and semi-arid catchments of Northern China, Atmos. Res., 198, 132–144, <ext-link xlink:href="https://doi.org/10.1016/j.atmosres.2017.03.012" ext-link-type="DOI">10.1016/j.atmosres.2017.03.012</ext-link>, 2017a.</mixed-citation></ref>
      <ref id="bib1.bib37"><label>37</label><?label 36?><mixed-citation>Tian, J., Liu, J., Yan, D., Li, C., Chu, Z., and Yu, F: An assimilation test of Doppler radar reflectivity and radial velocity from different height layers in improving the WRF rainfall forecasts, Atmos. Res., 198, 132–144, <ext-link xlink:href="https://doi.org/10.1016/j.atmosres.2017.08.004" ext-link-type="DOI">10.1016/j.atmosres.2017.08.004</ext-link>, 2017b.</mixed-citation></ref>
      <ref id="bib1.bib38"><label>38</label><?label 1?><mixed-citation>Tian, J., Liu, J., Yan, D., Ding, L., and Li, C.: Ensemble flood forecasting based on a coupled atmospheric-hydrological modeling system with data assimilation, Atmos. Res., 224, 127–137, <ext-link xlink:href="https://doi.org/10.1016/j.atmosres.2019.03.029" ext-link-type="DOI">10.1016/j.atmosres.2019.03.029</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib39"><label>39</label><?label 1?><mixed-citation>Tian, J., Liu, R., Ding, L., Guo, L., and Liu, Q.: Evaluation of the WRF physical parameterisations for Typhoon rainstorm simulation in southeast coast of China, Atmos. Res., 247, 105130, <ext-link xlink:href="https://doi.org/10.1016/j.atmosres.2020.105130" ext-link-type="DOI">10.1016/j.atmosres.2020.105130</ext-link>, 2021.</mixed-citation></ref>
      <ref id="bib1.bib40"><label>40</label><?label 37?><mixed-citation>Wan, Q. and Xu, J.: A numerical study of the rainstorm characteristics of the June 2005 flash flood with WRF/GSI data assimilation system over south-east China, Hydrol. Process., 25, 1327–1341, <ext-link xlink:href="https://doi.org/10.1002/hyp.7882" ext-link-type="DOI">10.1002/hyp.7882</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bib41"><label>41</label><?label 38?><mixed-citation>Wang, H., Sun, J., Zhang, X., Huang, X. Y., and Auligné, T: Radar data assimilation with WRF 4D-Var. Part I: System development and preliminary testing, Mon. Weather Rev., 141, 2224–2244, <ext-link xlink:href="https://doi.org/10.1175/MWR-D-12-00168.1" ext-link-type="DOI">10.1175/MWR-D-12-00168.1</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib42"><label>42</label><?label 39?><mixed-citation>Wang, X., Barker, D. M., Snyder, C., and Hamill, T. M: A hybrid ETKF–3DVAR data assimilation scheme for the WRF model. Part II: real observation experiments, Mon. Weather Rev., 136, 5132–5147, <ext-link xlink:href="https://doi.org/10.1175/2008MWR2445.1" ext-link-type="DOI">10.1175/2008MWR2445.1</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib43"><label>43</label><?label 40?><mixed-citation>Wattrelot, E., Caumont, O., and Mahfouf, J. F.: Operational implementation of the 1D<inline-formula><mml:math id="M106" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>3D-Var assimilation method of radar reflectivity data in the AROME model, Mon. Weather Rev., 142, 1852–1873, <ext-link xlink:href="https://doi.org/10.1175/mwr-d-13-00230.1" ext-link-type="DOI">10.1175/mwr-d-13-00230.1</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib44"><label>44</label><?label 1?><mixed-citation>Xie, Y., Xing, J., Shi, J., Dou, Y., and Lei, Y.: Impacts of radiance data assimilation on the Beijing 7.21 heavy rainfall, Atmos. Res., 169, 318–330, <ext-link xlink:href="https://doi.org/10.1016/j.atmosres.2015.10.016" ext-link-type="DOI">10.1016/j.atmosres.2015.10.016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib45"><label>45</label><?label 1?><mixed-citation>Yesubabu, V., Srinivas, C. V., Langodan, S., and Hoteit, I.: Predicting extreme rainfall events over Jeddah, Saudi Arabia: impact of data assimilation with conventional and satellite observations, Q. J. Roy. Meteorol. Soc., 142, 327–348, <ext-link xlink:href="https://doi.org/10.1002/qj.2654" ext-link-type="DOI">10.1002/qj.2654</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib46"><label>46</label><?label 41?><mixed-citation>Yucel, I., Onen, A., Yilmaz, K. K., and Gochis, D. J: Calibration and evaluation of a flood forecasting system: Utility of numerical weather prediction model, data assimilation and satellite-based rainfall, J. Hydrol., 523, 49–66, <ext-link xlink:href="https://doi.org/10.1016/j.jhydrol.2015.01.042" ext-link-type="DOI">10.1016/j.jhydrol.2015.01.042</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib47"><label>47</label><?label 42?><mixed-citation>Zhang, S. Q., Zupanski, M., Hou, A. Y., Lin, X., and Cheung, S. H: Assimilation of precipitation-affected radiances in a cloud-resolving WRF ensemble data assimilation system, Mon. Weather Rev., 141, 754–772, <ext-link xlink:href="https://doi.org/10.1175/mwr-d-12-00055.1" ext-link-type="DOI">10.1175/mwr-d-12-00055.1</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib48"><label>48</label><?label 43?><mixed-citation>Zhang, X., Xiong, Z., Zheng, J., and Ge, Q: High-resolution precipitation data derived from dynamical downscaling using the WRF model for the Heihe River Basin, northwest China, Theor. Appl. Climatol., 131, 1249–1259, <ext-link xlink:href="https://doi.org/10.1007/s00704-017-2052-6" ext-link-type="DOI">10.1007/s00704-017-2052-6</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib49"><label>49</label><?label 44?><mixed-citation>Zhao, P. K., Wang, B., and Liu, J.: A DRP–4DVar data assimilation scheme for typhoon initialization using sea level pressure data, Mon. Weather Rev., 140, 1191–1203, <ext-link xlink:href="https://doi.org/10.1175/MWR-D-10-05030.1" ext-link-type="DOI">10.1175/MWR-D-10-05030.1</ext-link>, 2012.</mixed-citation></ref>
      <?pagebreak page742?><ref id="bib1.bib50"><label>50</label><?label 45?><mixed-citation>Zhao, Q. and Jin, Y.: High-resolution radar data assimilation for hurricane Isabel (2003) at landfall, Bull. Am. Meteorol. Soc., 89, 1355, <ext-link xlink:href="https://doi.org/10.1175/2008BAMS2562.1" ext-link-type="DOI">10.1175/2008BAMS2562.1</ext-link>, 2008.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>Typhoon rainstorm simulations with radar data assimilation on the  southeast coast of China</article-title-html>
<abstract-html><p>As an effective technique to improve the rainfall forecast, data assimilation plays an important role in meteorology and hydrology. The aim of this study is to explore the reasonable use of Doppler radar data assimilation to correct the initial and lateral boundary conditions of the numerical weather prediction (NWP) systems. The Weather Research and Forecasting (WRF) model is applied to simulate three typhoon storm events on the southeast coast of China. Radar data from a Doppler radar station in Changle, China, are assimilated with three-dimensional variational data assimilation (3-DVar) model. Nine assimilation modes are designed by three kinds of radar data and at three assimilation time intervals. The rainfall simulations in a medium-scale catchment, Meixi, are evaluated by three indices, including relative error (RE), critical success index (CSI), and root mean square error (RMSE). Assimilating radial velocity at a time interval of 1&thinsp;h can significantly improve the rainfall simulations, and it outperforms the other modes for all the three storm events. Shortening the assimilation time interval can improve the rainfall simulations in most cases, while assimilating radar reflectivity always leads to worse simulations as the time interval shortens. The rainfall simulations can be improved by data assimilation as a whole, especially for the heavy rainfall with strong convection. The findings provide references for improving the typhoon rainfall forecasts at catchment scale and have great significance on typhoon rainstorm warning.</p></abstract-html>
<ref-html id="bib1.bib1"><label>1</label><mixed-citation> Agnihotri, G. and Dimri, A. P.: Simulation study of heavy rainfall episodes over the southern Indian peninsula, Meteorol. Appl., 22, 223–235, <a href="https://doi.org/10.1002/met.1446" target="_blank">https://doi.org/10.1002/met.1446</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>2</label><mixed-citation> Avolio, E. and Federico, S.: WRF simulations for a heavy rainfall event in southern Italy: Verification and sensitivity tests, Atmos. Res., 209, 14–35, <a href="https://doi.org/10.1016/j.atmosres.2018.03.009" target="_blank">https://doi.org/10.1016/j.atmosres.2018.03.009</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>3</label><mixed-citation> Bauer, H. S., Schwitalla, T., Wulfmeyer V., Bakhshaii, A., Ehret, U., Neuper, M., and Caumont, O: Quantitative precipitation estimation based on high-resolution numerical weather prediction and data assimilation with WRF – a performance test, Tellus A., 67, 25047, <a href="https://doi.org/10.3402/tellusa.v67.25047" target="_blank">https://doi.org/10.3402/tellusa.v67.25047</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>4</label><mixed-citation> Cai, Y., Lu, X., Chen, G., and Yang, S: Diurnal cycles of Mei-yu rainfall simulated over eastern China: Sensitivity to cumulus convective parameterization, Atmos. Res., 213, 236–251, <a href="https://doi.org/10.1016/j.atmosres.2018.06.003" target="_blank">https://doi.org/10.1016/j.atmosres.2018.06.003</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>5</label><mixed-citation> Caya, A., Sun, J., and Snyder, C.: A comparison between the 4DVAR and the Ensemble Kalman Filter techniques for radar data assimilation, Mon. Weather Rev., 133, 3081–3094, <a href="https://doi.org/10.1175/MWR3021.1" target="_blank">https://doi.org/10.1175/MWR3021.1</a>, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>6</label><mixed-citation> Chen, X., Wang, Y., Zhao, K., and Wu, D: A numerical study on rapid intensification of typhoon Vicente (2012) in the South China Sea. Part I: verification of simulation, storm-scale evolution, and environmental contribution, Mon. Weather Rev., 145, 877–898, <a href="https://doi.org/10.1175/MWR-D-16-0147.1" target="_blank">https://doi.org/10.1175/MWR-D-16-0147.1</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>7</label><mixed-citation> Dai, Q., Yang, Q., Han, D., Rico-Ramirez, M. A., and Zhang, S: Adjustment of radar-gauge rainfall discrepancy due to raindrop drift and evaporation using the Weather Research and Forecasting model and dual-polarization radar, Water Resour. Res., 55, 9211–9233, <a href="https://doi.org/10.1029/2019WR025517" target="_blank">https://doi.org/10.1029/2019WR025517</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>8</label><mixed-citation> Giannaros, T. M., Kotroni, V., and Lagouvardos, K.: WRF-LTNGDA: A lightning data assimilation technique implemented in the WRF model for improving precipitation forecasts, Environ. Model. Softw., 76, 54–68, <a href="https://doi.org/10.1016/j.envsoft.2015.11.017" target="_blank">https://doi.org/10.1016/j.envsoft.2015.11.017</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>9</label><mixed-citation> Hazra, A., Chaudhari, H. S., Ranalkar, M., and Chen, J. P: Role of interactions between cloud microphysics, dynamics and aerosol in the heavy rainfall event of June 2013 over Uttarakhand, India, Q. J. Roy. Meteor. Soc., 143, 986–998, <a href="https://doi.org/10.1002/qj.2983" target="_blank">https://doi.org/10.1002/qj.2983</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>10</label><mixed-citation> Hou, T., Kong, F., Chen, X., Lei, H., and Hu, Z: Evaluation of radar and automatic weather station data assimilation for a heavy rainfall event in southern China, Adv. Atmos. Sci., 32, 967–978, <a href="https://doi.org/10.1007/s00376-014-4155-7" target="_blank">https://doi.org/10.1007/s00376-014-4155-7</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>11</label><mixed-citation> Ide, K., Courtier, P., Ghil, M., and Lorenc, A. C: Unified Notation for data assimilation: Operational, sequential and variational, J. Meteorol. Soc. Jpn., 75, 181–189, <a href="https://doi.org/10.1175/1520-0469(1997)054&lt;0679:OTRBTS&gt;2.0.CO;2" target="_blank">https://doi.org/10.1175/1520-0469(1997)054&lt;0679:OTRBTS&gt;2.0.CO;2</a>, 1997.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>12</label><mixed-citation> Kawabata, T., Iwai, H., Seko, H., Shoji, Y., Saito, K., Ishii, S., and Mizutani, K: Cloud-resolving 4D-Var assimilation of Doppler wind lidar data on a Meso-Gamma-Scale convective system, Mon. Weather Rev., 142, 4484–4498, <a href="https://doi.org/10.1175/MWR-D-13-00362.1" target="_blank">https://doi.org/10.1175/MWR-D-13-00362.1</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>13</label><mixed-citation> Kong, R., Xue, M., and Liu, C. Development of a hybrid En3DVar data assimilation system and comparisons with 3DVar and EnKF for radar data assimilation with observing system simulation experiments, Mon. Weather Rev., 146, 175–198, <a href="https://doi.org/10.1175/MWR-D-17-0164.1" target="_blank">https://doi.org/10.1175/MWR-D-17-0164.1</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>14</label><mixed-citation> Li, X., Fan, K., and Yu, E.: Hindcast of extreme rainfall with high-resolution WRF: model ability and effect of physical schemes, Theor. Appl. Climatol., 139, 639–658, <a href="https://doi.org/10.1007/s00704-019-02945-2" target="_blank">https://doi.org/10.1007/s00704-019-02945-2</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>15</label><mixed-citation> Li, Z., Ballard, S. P., and Simonin, D.: Comparison of 3D-Var and 4D-Var data assimilation in an NWP-based system for precipitation nowcasting at the Met Office, Q. J. Roy. Meteor. Soc., 144, 404–413, <a href="https://doi.org/10.1002/qj.3211" target="_blank">https://doi.org/10.1002/qj.3211</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>16</label><mixed-citation> Liu, J., Bray M., and Han, D.: Sensitivity of the Weather Research and Forecasting (WRF) model to downscaling ratios and storm types in rainfall simulation, Hydrol. Process., 26, 3012–3031, <a href="https://doi.org/10.1002/hyp.8247" target="_blank">https://doi.org/10.1002/hyp.8247</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>17</label><mixed-citation> Liu, J., Bray, M., and Han D.: Exploring the effect of data assimilation by WRF-3DVar for numerical rainfall prediction with different types of storm events, Hydrol. Process., 27, 3627–3640, <a href="https://doi.org/10.1002/hyp.9488" target="_blank">https://doi.org/10.1002/hyp.9488</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>18</label><mixed-citation> Liu, J., Tian, J., Yan, D., Li, C., Yu, F., and Shen, F.: Evaluation of Doppler radar and GTS data assimilation for NWP rainfall prediction of an extreme summer storm in northern China: from the hydrological perspective, Hydrol. Earth Syst. Sci., 22, 4329–4348, <a href="https://doi.org/10.5194/hess-22-4329-2018" target="_blank">https://doi.org/10.5194/hess-22-4329-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>19</label><mixed-citation> Lu, X., Wang X., Li Y., Tong, M., and Ma, X: GSI-based ensemble-variational hybrid data assimilation for HWRF for hurricane initialization and prediction: impact of various error covariances for airborne radar observation assimilation, Q. J. Roy. Meteor. Soc., 143, 223–239, <a href="https://doi.org/10.1002/qj.2914" target="_blank">https://doi.org/10.1002/qj.2914</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>20</label><mixed-citation> Maiello, I., Ferretti, R., Gentile, S., Montopoli, M., Picciotti, E., Marzano, F. S., and Faccani, C.: Impact of radar data assimilation for the simulation of a heavy rainfall case in central Italy using WRF–3DVAR, Atmos. Meas. Tech., 7, 2919–2935, <a href="https://doi.org/10.5194/amt-7-2919-2014" target="_blank">https://doi.org/10.5194/amt-7-2919-2014</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>21</label><mixed-citation> Meng, Z. and Zhang, F.: Tests of an ensemble Kalman filter for mesoscale and regional-scale data assimilation. Part III: Comparison with 3DVAR in a real-data case study, Mon. Weather Rev., 136, 522–540, <a href="https://doi.org/10.1175/mwr3352.1" target="_blank">https://doi.org/10.1175/mwr3352.1</a>, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>22</label><mixed-citation> Milan, M., Venema, V., Schüttemeyer, D., and Simmer, C: Assimilation of radar and satellite data in mesoscale models: A physical initialization scheme, Meteorol. Z., 17, 887–902, <a href="https://doi.org/10.1127/0941-2948/2008/0340" target="_blank">https://doi.org/10.1127/0941-2948/2008/0340</a>, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>23</label><mixed-citation> Mohan, G. M., Srinivas, C. V., and Naidu, C. V.: Real-time numerical simulation of tropical cyclone Nilam with WRF: experiments with different initial conditions, 3D-Var and Ocean Mixed Layer Model, Nat. Hazards., 77, 597–624, <a href="https://doi.org/10.1007/s11069-015-1611-3" target="_blank">https://doi.org/10.1007/s11069-015-1611-3</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>24</label><mixed-citation> Montmerle, T. and Faccani, C.: Mesoscale assimilation of radial velocities from Doppler radars in a preoperational framework, Mon. Weather Rev., 137, 1939–1953, <a href="https://doi.org/10.1175/2008MWR2725.1" target="_blank">https://doi.org/10.1175/2008MWR2725.1</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>25</label><mixed-citation> Myung, J. I.: The importance of complexity in model selection, J. Math. Psychol., 44, 190–204, <a href="https://doi.org/10.1006/jmps.1999.1283" target="_blank">https://doi.org/10.1006/jmps.1999.1283</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>26</label><mixed-citation>
NCAR: NCEP Final (FNL) Operational Global Analysis data, available at: <a href="https://rda.ucar.edu/datasets/ds083.2/" target="_blank"/>, last access: 10 January 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>27</label><mixed-citation> Otieno, G., Mutemi, J. N., Opijah, F. J., Ogallo, L. A., and Omondi, M. H: The sensitivity of rainfall characteristics to cumulus parameterisation schemes from a WRF model. Part I: a case study over East Africa during wet years, Pure Appl. Geophys., 1, 1–16, <a href="https://doi.org/10.1007/s00024-019-02293-2" target="_blank">https://doi.org/10.1007/s00024-019-02293-2</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>28</label><mixed-citation> Prakash, S., Sathiyamoorthy, V., Mahesh, C., and Gairola, R. M: An evaluation of high-resolution multisatellite rainfall products over the Indian monsoon region, Int. J. Remote Sens., 35, 3018–3035, <a href="https://doi.org/10.1080/01431161.2014.894661" target="_blank">https://doi.org/10.1080/01431161.2014.894661</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>29</label><mixed-citation> Shen, F., Min, J., and Xu, D.: Assimilation of radar radial velocity data with the WRF Hybrid ETKF-3DVAR system for the prediction of Hurricane Ike (2008), Atmos. Res., 169, 127–138, <a href="https://doi.org/10.1016/j.atmosres.2015.09.019" target="_blank">https://doi.org/10.1016/j.atmosres.2015.09.019</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>30</label><mixed-citation> Shen, F., Xue, M., and Min, J.: A comparison of limited-area 3DVAR and ETKF-En3DVAR data assimilation using radar observations at convective scale for the prediction of Typhoon Saomai (2006), Meteorol. Appl., 24, 628–641, <a href="https://doi.org/10.1002/met.1663" target="_blank">https://doi.org/10.1002/met.1663</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>31</label><mixed-citation> Sivapalan, M. and Blöschl, G.: Transformation of point rainfall to areal rainfall: Intensity-duration-frequency curves, J. Hydrol., 204, 150–167, <a href="https://doi.org/10.1016/S0022-1694(97)00117-0" target="_blank">https://doi.org/10.1016/S0022-1694(97)00117-0</a>, 1998.
</mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>32</label><mixed-citation> Srivastava, P. K., Han, D., Rico-Ramirez, M. A., O'Neill, P., Islam, T., Gupta, M., and Dai, Q: Performance evaluation of WRF-Noah Land surface model estimated soil moisture for hydrological application: Synergistic evaluation using SMOS retrieved soil moisture, J. Hydrol., 529, 200–212, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>33</label><mixed-citation> Sun, J.: Convective-scale assimilation of radar data: progress and challenges, Q. J. Roy. Meteor. Soc., 131, 3439–3463, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>34</label><mixed-citation> Sun, J. and Crook, N. A.: Dynamical and microphysical retrieval from Doppler radar observations using a cloud model and its adjoint, Part I: model development and simulated data experiments, J. Atmos. Sci., 54, 1642–1661, <a href="https://doi.org/10.1175/1520-0469(1997)054&lt;1642:DAMRFD&gt;2.0.CO;2" target="_blank">https://doi.org/10.1175/1520-0469(1997)054&lt;1642:DAMRFD&gt;2.0.CO;2</a>, 1997.
</mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>35</label><mixed-citation> Sun, J. and Crook, N. A.: Dynamical and microphysical retrieval from Doppler radar observations using a cloud model and its adjoint. Part II: retrieval experiments of an observed Florida convective storm, J. Atmos. Sci., 55, 835–852, <a href="https://doi.org/10.1175/1520-0469(1998)0552.0.CO;2" target="_blank">https://doi.org/10.1175/1520-0469(1998)0552.0.CO;2</a>, 1998.
</mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>36</label><mixed-citation> Tian, J., Liu, J., Wang, J., Li, C., Yu, F., and Chu, Z: A spatio-temporal evaluation of the WRF physical parameterisations for numerical rainfall simulation in semi-humid and semi-arid catchments of Northern China, Atmos. Res., 198, 132–144, <a href="https://doi.org/10.1016/j.atmosres.2017.03.012" target="_blank">https://doi.org/10.1016/j.atmosres.2017.03.012</a>, 2017a.
</mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>37</label><mixed-citation> Tian, J., Liu, J., Yan, D., Li, C., Chu, Z., and Yu, F: An assimilation test of Doppler radar reflectivity and radial velocity from different height layers in improving the WRF rainfall forecasts, Atmos. Res., 198, 132–144, <a href="https://doi.org/10.1016/j.atmosres.2017.08.004" target="_blank">https://doi.org/10.1016/j.atmosres.2017.08.004</a>, 2017b.
</mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>38</label><mixed-citation>
Tian, J., Liu, J., Yan, D., Ding, L., and Li, C.: Ensemble flood forecasting based on a coupled atmospheric-hydrological modeling system with data assimilation, Atmos. Res., 224, 127–137, <a href="https://doi.org/10.1016/j.atmosres.2019.03.029" target="_blank">https://doi.org/10.1016/j.atmosres.2019.03.029</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>39</label><mixed-citation>
Tian, J., Liu, R., Ding, L., Guo, L., and Liu, Q.: Evaluation of the WRF physical parameterisations for Typhoon rainstorm simulation in southeast coast of China, Atmos. Res., 247, 105130, <a href="https://doi.org/10.1016/j.atmosres.2020.105130" target="_blank">https://doi.org/10.1016/j.atmosres.2020.105130</a>, 2021.
</mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>40</label><mixed-citation> Wan, Q. and Xu, J.: A numerical study of the rainstorm characteristics of the June 2005 flash flood with WRF/GSI data assimilation system over south-east China, Hydrol. Process., 25, 1327–1341, <a href="https://doi.org/10.1002/hyp.7882" target="_blank">https://doi.org/10.1002/hyp.7882</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>41</label><mixed-citation> Wang, H., Sun, J., Zhang, X., Huang, X. Y., and Auligné, T: Radar data assimilation with WRF 4D-Var. Part I: System development and preliminary testing, Mon. Weather Rev., 141, 2224–2244, <a href="https://doi.org/10.1175/MWR-D-12-00168.1" target="_blank">https://doi.org/10.1175/MWR-D-12-00168.1</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>42</label><mixed-citation> Wang, X., Barker, D. M., Snyder, C., and Hamill, T. M: A hybrid ETKF–3DVAR data assimilation scheme for the WRF model. Part II: real observation experiments, Mon. Weather Rev., 136, 5132–5147, <a href="https://doi.org/10.1175/2008MWR2445.1" target="_blank">https://doi.org/10.1175/2008MWR2445.1</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>43</label><mixed-citation> Wattrelot, E., Caumont, O., and Mahfouf, J. F.: Operational implementation of the 1D+3D-Var assimilation method of radar reflectivity data in the AROME model, Mon. Weather Rev., 142, 1852–1873, <a href="https://doi.org/10.1175/mwr-d-13-00230.1" target="_blank">https://doi.org/10.1175/mwr-d-13-00230.1</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>44</label><mixed-citation>
Xie, Y., Xing, J., Shi, J., Dou, Y., and Lei, Y.: Impacts of radiance data assimilation on the Beijing 7.21 heavy rainfall, Atmos. Res., 169, 318–330, <a href="https://doi.org/10.1016/j.atmosres.2015.10.016" target="_blank">https://doi.org/10.1016/j.atmosres.2015.10.016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>45</label><mixed-citation>
Yesubabu, V., Srinivas, C. V., Langodan, S., and Hoteit, I.: Predicting extreme rainfall events over Jeddah, Saudi Arabia: impact of data assimilation with conventional and satellite observations, Q. J. Roy. Meteorol. Soc., 142, 327–348, <a href="https://doi.org/10.1002/qj.2654" target="_blank">https://doi.org/10.1002/qj.2654</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>46</label><mixed-citation> Yucel, I., Onen, A., Yilmaz, K. K., and Gochis, D. J: Calibration and evaluation of a flood forecasting system: Utility of numerical weather prediction model, data assimilation and satellite-based rainfall, J. Hydrol., 523, 49–66, <a href="https://doi.org/10.1016/j.jhydrol.2015.01.042" target="_blank">https://doi.org/10.1016/j.jhydrol.2015.01.042</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>47</label><mixed-citation> Zhang, S. Q., Zupanski, M., Hou, A. Y., Lin, X., and Cheung, S. H: Assimilation of precipitation-affected radiances in a cloud-resolving WRF ensemble data assimilation system, Mon. Weather Rev., 141, 754–772, <a href="https://doi.org/10.1175/mwr-d-12-00055.1" target="_blank">https://doi.org/10.1175/mwr-d-12-00055.1</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>48</label><mixed-citation> Zhang, X., Xiong, Z., Zheng, J., and Ge, Q: High-resolution precipitation data derived from dynamical downscaling using the WRF model for the Heihe River Basin, northwest China, Theor. Appl. Climatol., 131, 1249–1259, <a href="https://doi.org/10.1007/s00704-017-2052-6" target="_blank">https://doi.org/10.1007/s00704-017-2052-6</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib49"><label>49</label><mixed-citation> Zhao, P. K., Wang, B., and Liu, J.: A DRP–4DVar data assimilation scheme for typhoon initialization using sea level pressure data, Mon. Weather Rev., 140, 1191–1203, <a href="https://doi.org/10.1175/MWR-D-10-05030.1" target="_blank">https://doi.org/10.1175/MWR-D-10-05030.1</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib50"><label>50</label><mixed-citation> Zhao, Q. and Jin, Y.: High-resolution radar data assimilation for hurricane Isabel (2003) at landfall, Bull. Am. Meteorol. Soc., 89, 1355, <a href="https://doi.org/10.1175/2008BAMS2562.1" target="_blank">https://doi.org/10.1175/2008BAMS2562.1</a>, 2008.
</mixed-citation></ref-html>--></article>
