<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing with OASIS Tables v3.0 20080202//EN" "journalpub-oasis3.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" dtd-version="3.0"><?xmltex \bartext{15th EMS Annual Meeting \& 12th European Conference on Applications of Meteorology (ECAM)}?>
  <front>
    <journal-meta>
<journal-id journal-id-type="publisher">ASR</journal-id>
<journal-title-group>
<journal-title>Advances in Science and Research</journal-title>
<abbrev-journal-title abbrev-type="publisher">ASR</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Adv. Sci. Res.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1992-0636</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/asr-13-27-2016</article-id><title-group><article-title>SATIN–Satellite driven nowcasting system</article-title>
      </title-group><?xmltex \runningtitle{SATIN--Satellite driven nowcasting system}?><?xmltex \runningauthor{I.~Meirold-Mautner et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Meirold-Mautner</surname><given-names>Ingo</given-names></name>
          <email>ingo.meirold-mautner@zamg.ac.at</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Kann</surname><given-names>Alexander</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Meier</surname><given-names>Florian</given-names></name>
          
        </contrib>
        <aff id="aff1"><institution>ZAMG – Zentralanstalt fü Meteorologie und Geodynamik, Department of forecasting models, Vienna, Austria</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Ingo Meirold-Mautner (ingo.meirold-mautner@zamg.ac.at)</corresp></author-notes><pub-date><day>16</day><month>March</month><year>2016</year></pub-date>
      
      <volume>13</volume>
      <fpage>27</fpage><lpage>35</lpage>
      <history>
        <date date-type="received"><day>17</day><month>December</month><year>2015</year></date>
           <date date-type="rev-recd"><day>1</day><month>March</month><year>2016</year></date>
           <date date-type="accepted"><day>10</day><month>March</month><year>2016</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under a Creative Commons Attribution 3.0 Unported License. To view a copy of this license, visit <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by/3.0/">http://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016.html">This article is available from https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016.html</self-uri>
<self-uri xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016.pdf">The full text article is available as a PDF file from https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016.pdf</self-uri>


      <abstract>
    <p>A precipitation nowcasting system (SATIN) is presented which relies entirely
on satellite based precipitation products and rain gauge measurements. Thus,
the proposed system is most suitable for areas where ground based radar
observations are not available, or potentially suffer from low quality. SATIN
delivers analyses on a 1 km grid every 15 min and nowcasts (obtained through
motion vectors) in 15 min time steps. Nowcasts are gradually merged with NWP
precipitation forecasts. An extensive validation including comparisons to
different NWP models yields superior performance for SATIN analyses as well
as nowcasts for lead times up to 1 h. Reducing the station density still
yields better performance than operationally available NWP's.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>Satellite based observations play an important role in many different
disciplines, such as meteorology, climatology, oceanography and many more.
Specifically, derived precipitation estimates from space already deliver
valuable information on a global scale. In regions with sparse ground based
observation networks (rain gauge stations and ground based radars – simply
referenced as “radar” in this paper), detailed knowledge about
precipitation patterns and climatologies is largely missing and satellite
observations are a key contributor for a better understanding of the regional
weather and climate. Furthermore, regions with complex topography, where
radar and station networks exist, may also profit from satellite
observations, as radars suffer, among others, from beam blocking and usually
only few station observations are available. Satellite based precipitation
measurements could deliver additional information to mitigate the mentioned
shortcomings.</p>
      <p>The obtained precision of satellite based precipitation products is
predominantly governed by the type of satellite orbit (polar orbiting,
geostationary), instrument types (frequency bands used) and integration times
(seasonal products to minutes). In this study we focus on nowcasting with
very high temporal and spatial resolution, thus, the most challenging
framework for satellite based precipitation products.</p>
      <p>A prototype of a nowcasting system based on satellite precipitation in
combination with rain gauge measurements (explicitly omitting radar
observations) is developed. Such a system is of interest for data sparse
regions where radar observations do not exist and rain gauge measurements are
also scarce. Nevertheless, our target area is Austria where a dense
observation network exists. This gives us the possibility of extensively
validating the developed nowcasting system and comparing it to operationally
available numerical weather prediction (NWP) models.</p>
      <p>This satellite driven nowcasting system is based on the concepts of the INCA
<xref ref-type="bibr" rid="bib1.bibx5" id="paren.1"><named-content content-type="pre">Integrated Nowcasting through Comprehensive Analysis,</named-content></xref>
precipitation nowcasting and can be summarized as follows:
<list list-type="bullet"><list-item><p>Analyses are computed as a combination of rain gauge measurements and satellite derived precipitation. For each grid point, an average distance to neighboring stations enters the algorithm.</p></list-item><list-item><p>Nowcasting is based on extrapolation by motion vectors computed from previous analyses.</p></list-item><list-item><p>Very short range forecasting sets in after pure extrapolation: nowcasts are merged with precipitation forecasts from NWP through a prescribed weighting function until the forecasts entirely consist of downscaled NWP.</p></list-item></list></p>
      <p>Results from long term validation and one case study are presented. Both
yield good results for the analyses compared to operationally available NWP
precipitation fields. Nowcastings deliver higher accuracy for lead times up
to around one hour compared to NWP forecasts. Additionally, sensitivity
studies are presented to show the influence of station density on the
results.</p>
</sec>
<sec id="Ch1.S2">
  <title>Data and methods</title>
<sec id="Ch1.S2.SS1">
  <title>Target grid and NWP models</title>
      <p>The target domain for the presented nowcasting system corresponds to the
operational INCA domain in Austria. The grid spacing is
1 km <inline-formula><mml:math display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1 km with 700 <inline-formula><mml:math display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 401 grid points. By choosing this
grid, validation of the results with INCA analyses becomes straightforward.
Additionally, the following NWP models are used for comparisons and are
interpolated onto the same grid: ALARO, AROME, AROME1km.</p>
      <p>The ALARO model <xref ref-type="bibr" rid="bib1.bibx4" id="paren.2"/> is a spectral limited area model (LAM)
running four times per day operationally at ZAMG up to <inline-formula><mml:math display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>72 h in
hydrostatic mode with 4.8 km horizontal grid spacing on a domain of
600 <inline-formula><mml:math display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 540 grid points covering Central Europe. It has 60 vertical
hybrid levels <xref ref-type="bibr" rid="bib1.bibx12" id="paren.3"/> and its physics package 3MT is especially
suitable for resolutions of few kilometers, where deep convection is only
partly resolved.</p>
      <p>Application of Research to Operations at Mesoscale (AROME) <xref ref-type="bibr" rid="bib1.bibx11" id="paren.4"/>
is the second operational LAM at ZAMG running 8 times per day up to <inline-formula><mml:math display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>48 h
with a horizontal grid space of 2.5 km, 600 <inline-formula><mml:math display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 432 grid points and
90 hybrid levels in non-hydrostatic mode. Different to ALARO, deep convection
is explicitly treated and the initial state of the atmosphere is generated by
its own 3-D-Var data assimilation system <xref ref-type="bibr" rid="bib1.bibx2" id="paren.5"/>. Both LAMs
are coupled with the global model Integrated Forecasting System (IFS) of the
European Centre for Medium-Range Weather Forecast (ECMWF) using Davies
relaxation <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx8" id="paren.6"/>. For several test cases
also a 1 km grid space version of AROME was run with a reduced time step
(30 s instead of 60 s for AROME 2.5 km) on a domain of 800 <inline-formula><mml:math display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 500
grid points covering Austria and its surroundings with the same vertical
resolution as AROME 2.5 km. It was coupled to and initialized by downscaled
data from either IFS or ALARO 4.8 km or AROME 2.5 km.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>Satellite data</title>
      <p>Requirements to satellite data for precipitation nowcasting are high spatial
and temporal resolution. To compete with radar based nowcastings, spatial
resolution of a few kilometers and temporal resolution of a few minutes are
necessary. Additionally, a low latency is required to ensure a rapid updating
frequency and temporal availability of products.</p>
      <p>Satellite products getting close to these requirements have been identified
to be EUMETSAT's Support to Operational Hydrology and Water Management
(H-SAF) and Support to Nowcasting and Very Short Range Forecasting (NWC SAF)
products as well as the HydroEstimator from NOAA. The products investigated
are summarized in Table <xref ref-type="table" rid="Ch1.T1"/>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p>Overview of satellite products evaluated.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="91.048819pt"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="108.120472pt"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="108.120472pt"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="85.358268pt"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">H03</oasis:entry>  
         <oasis:entry colname="col3">CRR</oasis:entry>  
         <oasis:entry colname="col4">HE</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Provider</oasis:entry>  
         <oasis:entry colname="col2">Hydrology SAF</oasis:entry>  
         <oasis:entry colname="col3">Nowcasting SAF</oasis:entry>  
         <oasis:entry colname="col4">NOAA STAR</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Spatial resolution</oasis:entry>  
         <oasis:entry colname="col2">8 km</oasis:entry>  
         <oasis:entry colname="col3">8 km</oasis:entry>  
         <oasis:entry colname="col4">5 km</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Temporal resolution</oasis:entry>  
         <oasis:entry colname="col2">15 min</oasis:entry>  
         <oasis:entry colname="col3">15 min</oasis:entry>  
         <oasis:entry colname="col4">1 h (Europe)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Satellite</oasis:entry>  
         <oasis:entry colname="col2">Meteosat (SEVIRI),<?xmltex \hack{\hfill\break}?>LEO MW instrument<?xmltex \hack{\hfill\break}?>(SSM/I, AMSU-A)</oasis:entry>  
         <oasis:entry colname="col3">Meteosat (SEVIRI)</oasis:entry>  
         <oasis:entry colname="col4">Meteosat (SEVIRI)<?xmltex \hack{\hfill\break}?>(or others, e.g. GOES)</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Characteristics</oasis:entry>  
         <oasis:entry colname="col2">10.8 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m LUT, calibrated with MW LEO data</oasis:entry>  
         <oasis:entry colname="col3">IR, VIS, WV channels, AUX data (NWP, etc.) for several correction algorithms</oasis:entry>  
         <oasis:entry colname="col4">Single channel: 11 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Reference</oasis:entry>  
         <oasis:entry colname="col2">
                      <xref ref-type="bibr" rid="bib1.bibx7" id="normal.7"/>
                    </oasis:entry>  
         <oasis:entry colname="col3">
                      <xref ref-type="bibr" rid="bib1.bibx9" id="normal.8"/>
                    </oasis:entry>  
         <oasis:entry colname="col4">Scofield and<?xmltex \hack{\hfill\break}?>Kuligowski (2003)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p>LEO: Low Earth Orbit; LUT: Look Up Table; MW: MicroWave;
SAF: EUMETSAT Satellite Application Facility</p></table-wrap-foot></table-wrap>

      <p>To determine the quality of the individual satellite products, a point
validation against measurement stations and spatial validation against INCA
analyses has been carried out (not shown in this study). While INCA analyses
can not be considered to represent the truth <xref ref-type="bibr" rid="bib1.bibx6" id="paren.9"><named-content content-type="pre">see</named-content><named-content content-type="post">for details on the
quality of INCA precipitation analyses</named-content></xref>, they are the best option
available for carrying out spatial comparisons. This validation included the
computation of standard statistical scores (Root Mean Square Error RMSE,
Bias) as well as objective verification measures (SAL, see
Table <xref ref-type="table" rid="Ch1.T2"/>). Both, point verification as well as spatial
verification, indicate a consistent underestimation of satellite based
precipitation, especially for the Convective Rainfall Rate (CRR) product (see
Table <xref ref-type="table" rid="Ch1.T1"/> for details). Hydro-Estimator (HE) and H03 (precipitation
product from HSAF) exhibit overall similar performance with lower biases for
H03 but better representation of precipitation structures for HE
<xref ref-type="bibr" rid="bib1.bibx13" id="paren.10"><named-content content-type="pre">results from SAL verification,</named-content></xref>. As a consequence
from these evaluations, the H03 product of HSAF was selected as input for
SATIN as it shows best overall agreements with the reference and furthermore
has the advantage of being available at 15 min temporal resolution (in
contrast to 1 h for the HE product in Europe).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><caption><p>Statistical scores used in this study. See <xref ref-type="bibr" rid="bib1.bibx14" id="text.11"/> and
<xref ref-type="bibr" rid="bib1.bibx13" id="text.12"/> for details.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.75}[.75]?><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="56.905512pt"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="85.358268pt"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="85.358268pt"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="85.358268pt"/>
     <oasis:colspec colnum="5" colname="col5" align="justify" colwidth="85.358268pt"/>
     <oasis:colspec colnum="6" colname="col6" align="justify" colwidth="85.358268pt"/>
     <oasis:colspec colnum="7" colname="col7" align="justify" colwidth="85.358268pt"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">FBI</oasis:entry>  
         <oasis:entry colname="col3">TSS</oasis:entry>  
         <oasis:entry colname="col4">ETS</oasis:entry>  
         <oasis:entry colname="col5"/>  
         <oasis:entry colname="col6">SAL</oasis:entry>  
         <oasis:entry colname="col7"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Name</oasis:entry>  
         <oasis:entry colname="col2">Frequency Bias Index</oasis:entry>  
         <oasis:entry colname="col3">True Skill Score</oasis:entry>  
         <oasis:entry colname="col4">Equitable Threat Score</oasis:entry>  
         <oasis:entry colname="col5">Structure</oasis:entry>  
         <oasis:entry colname="col6">Amplitude</oasis:entry>  
         <oasis:entry colname="col7">Location</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Range</oasis:entry>  
         <oasis:entry colname="col2">0–<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">∞</mml:mi></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1–1</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1/3–1</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2–2</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2–2</oasis:entry>  
         <oasis:entry colname="col7">0–2</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Perfect</oasis:entry>  
         <oasis:entry colname="col2">1</oasis:entry>  
         <oasis:entry colname="col3">1</oasis:entry>  
         <oasis:entry colname="col4">1</oasis:entry>  
         <oasis:entry colname="col5">0</oasis:entry>  
         <oasis:entry colname="col6">0</oasis:entry>  
         <oasis:entry colname="col7">0</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Characteristic</oasis:entry>  
         <oasis:entry colname="col2">How did the forecast frequency of “yes”<?xmltex \hack{\hfill\break}?>events compare to the observed frequency of “yes” events?</oasis:entry>  
         <oasis:entry colname="col3">How well did the<?xmltex \hack{\hfill\break}?>forecast separate the<?xmltex \hack{\hfill\break}?>“yes”events from the<?xmltex \hack{\hfill\break}?>“no” events?</oasis:entry>  
         <oasis:entry colname="col4">How well did the<?xmltex \hack{\hfill\break}?>forecast “yes” events<?xmltex \hack{\hfill\break}?>correspond to the<?xmltex \hack{\hfill\break}?>observed “yes” events?</oasis:entry>  
         <oasis:entry colname="col5">Positive if cells are too large and/or too flat</oasis:entry>  
         <oasis:entry colname="col6">Relative deviation of<?xmltex \hack{\hfill\break}?>domain averaged<?xmltex \hack{\hfill\break}?>precipitation</oasis:entry>  
         <oasis:entry colname="col7">Displacement of<?xmltex \hack{\hfill\break}?>precipitation cells</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2.SS3">
  <title>SATIN analysis</title>
      <p>The SATIN analysis model is designed to take advantage from both constituent
data sources: it combines the spatial characteristics of the precipitation
patterns derived from satellite measurements with the accurate point
measurements of the stations.</p>
      <p>For a selected date/time combination, the developed system retrieves the
corresponding satellite product from the HSAF data portal and interpolates
the data to the INCA 1 km grid. This allows running SATIN for an arbitrary
date/time combination (within the limits of availability of H03 data).</p>
      <p>The second constituent of SATIN is precipitation measurements at stations.
For the Austrian domain there are about 200 point observations from the
“TeilAutomatisches Wetter ErfassungsSystem” (TAWES), equipped with
tipping-bucket rain gauges, available. Processing of these station
measurements corresponds to the algorithms developed for the operational INCA
system. Besides aggregation to 15 min sums, station measurements are exposed
to extensive quality control routines <xref ref-type="bibr" rid="bib1.bibx1" id="paren.13"/> in order to minimize
the deterioration of nowcasting results through erroneous station
measurements. These station observations are input to SATIN.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p>This figure depicts the SATIN domain (same as INCA operational
domain). Black dots represent automatic weather stations entering the SATIN
algorithm. Average distance for three nearest neighbors is shown (with a
cutoff at distances larger than 30 km).</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f01.pdf"/>

        </fig>

      <p>Once, all necessary input data for SATIN is collected and preprocessed, the
combination algorithm with the following principal steps is launched:
<list list-type="bullet"><list-item><p>At each grid point of the domain, an average distance <inline-formula><mml:math display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> to the surrounding observation stations is computed. This is done by
searching for <inline-formula><mml:math display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> nearest neighbors and averaging the obtained distances. Tests have been made with different numbers of nearest neighbours
to include in the computation. Small numbers yield a larger variability in the average distance and thus lead to more granularity regarding
the influence of satellite data on the SATIN analysis. <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> (as depicted in Fig. <xref ref-type="fig" rid="Ch1.F1"/>) was chosen for this study as it gives
more weight to satellite data in areas with smaller station density and shows a pronounced granularity in the transition from station to
satellite derived precipitation, when compared to larger values of <inline-formula><mml:math display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula>. This step is redone for each time step because station density is varying.</p></list-item><list-item><p>Station observations are interpolated to the INCA grid by inverse distance weighting (IDW) of the 8 nearest neighbor stations to each grid
point. Weights are computed proportional to <inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msup><mml:mi>d</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, i.e. with decreasing
weights for increasing distance <inline-formula><mml:math display="inline"><mml:mi>d</mml:mi></mml:math></inline-formula>. This results in the station
precipitation field <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:msub><mml:mi>R</mml:mi><mml:mtext>STAT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>.</p></list-item><list-item><p>Weighting factors at each grid point for merging satellite data with station data are computed. This weighting factor is computed from a
logistic function which describes the transition from station to satellite
data: <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>w</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi>exp⁡</mml:mi><mml:mo>(</mml:mo><mml:mo>-</mml:mo><mml:mi>k</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>-</mml:mo><mml:mi>u</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>. The above computed average distance enters
the logistic function as <inline-formula><mml:math display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>. Equal weights to satellite and station are
attributed at an average distance of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mo>=</mml:mo><mml:mn>30</mml:mn></mml:mrow></mml:math></inline-formula> km. The parameter
<inline-formula><mml:math display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> (set to <inline-formula><mml:math display="inline"><mml:mn>0.2</mml:mn></mml:math></inline-formula>) determines the steepness of the function, i.e. the rate at which weights are changing with distance. Experiments with
different parameters of the logistic function have been performed, with the above described setting found to provide a good balance between
station measurements and satellite precipitation for the characteristics of the Austrian domain. The weighting factor as a function of distance is plotted in Fig. <xref ref-type="fig" rid="Ch1.F2"/>.</p></list-item><list-item><p>The final precipitation rate based on satellite and station at each grid point is then obtained by
<inline-formula><mml:math display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:msub><mml:mi>R</mml:mi><mml:mtext>SATIN</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mi>w</mml:mi><mml:mi>R</mml:mi><mml:msub><mml:mi>R</mml:mi><mml:mtext>SAT</mml:mtext></mml:msub><mml:mo>+</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi>w</mml:mi><mml:mo>)</mml:mo><mml:mo>×</mml:mo><mml:mi>R</mml:mi><mml:msub><mml:mi>R</mml:mi><mml:mtext>STAT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:msub><mml:mi>R</mml:mi><mml:mtext>SAT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> denotes the preprocessed satellite precipitation.</p></list-item></list></p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><caption><p>Weights <inline-formula><mml:math display="inline"><mml:mi>w</mml:mi></mml:math></inline-formula> computed as a logistic function and plotted against
distance <inline-formula><mml:math display="inline"><mml:mi>d</mml:mi></mml:math></inline-formula>. Parameters of the logistic function are described in the text.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f02.png"/>

        </fig>

      <p>The described algorithm is thus taking the satellite derived precipitation
product and merges this with the interpolated station observations. Depending
on average station density, more weight is either given to the satellite
product or the station observations. In regions with very sparse station
density, the SATIN analysis will therefore resemble the raw satellite
precipitation product, whereas regions with high station density will benefit
from accurate point measurements. Figure <xref ref-type="fig" rid="Ch1.F1"/> shows the average
distance computed with three nearest neighbors. Including more nearest
neighbors in the computation results in a smoother spatial distribution of
the weight factor (not shown). Figure <xref ref-type="fig" rid="Ch1.F2"/> depicts the weight factor as
a function of average distance which indicates that grid points within an
average distance of around 20 km are mostly influenced by station
measurements. Beyond this distance, the influence of satellite precipitation
is rapidly increasing.</p>
      <p>The SATIN analysis and nowcasting model is coded in Python with a modular
approach. A pre-processing module is responsible for fetching necessary
satellite products and interpolating them to the target grid. Some
functionalities are taken directly from the operational INCA model, such as
the computationally demanding motion vector estimation, and the quality
filtering of station measurements.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <title>SATIN nowcasting</title>
      <p>Pure nowcasting is based on motion vectors computed from previous satellite
precipitation fields. The same cross correlation algorithm as the one in INCA
is applied <xref ref-type="bibr" rid="bib1.bibx5" id="paren.14"><named-content content-type="pre">see</named-content></xref> to obtain the motion vectors.
However, no cross-checking with upper air flow from NWP output is done (as
opposed to the INCA algorithm). This decision is made in order to stay
independent of NWP input. The resulting motion vectors are however less
stable and spurious correlations exist, which introduces errors in the
translational nowcasting. In order to minimize the deterioration of the
relatively good SATIN analyses, the translational motion is obtained from
averaging the motion vectors.</p>
      <p>Beyond the pure nowcasting, merging with NWP is applied. This is done to
benefit from the different strengths of each forecasting system, the
observation based nowcasting for very short time ranges and the physically
based NWP for longer time ranges. Finding the optimal transition from
nowcasting to NWP amounts to identifying when NWP yields superior results
than pure nowcasting. Varying results are expected, especially when looking
at rather convective weather types opposed to stratiform precipitation
events.</p>
      <p>To investigate the characteristics of NWP and nowcasting performances for
both types of precipitation (convective and stratiform), scores have been
computed for one winter month (January 2014) and one summer month (July 2014)
with INCA analyses serving as reference. Figure <xref ref-type="fig" rid="Ch1.F3"/> shows relative
RMSE, MAE (Mean Absolute Error) and Bias while Fig. <xref ref-type="fig" rid="Ch1.F4"/> shows the
skill scores FBI, TSS and ETS (for a threshold of 1 mm 15 min<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)
averaged for July <xref ref-type="bibr" rid="bib1.bibx14" id="paren.15"><named-content content-type="pre">cf. to Table <xref ref-type="table" rid="Ch1.T2"/> and e.g.</named-content><named-content content-type="post">regarding skill
scores</named-content></xref>. Rather than discussing in detail the individual scores
(which all suffer from weaknesses, such as double-counting penalty), it is
important to note the variation with lead time. Average RMSE, MAE and Bias
for the NWP's remain almost constant for lead times up to 6 h, with ALARO
exhibiting a better performance than AROME except for bias in the convective
season. SATIN performance is very good for very short lead times and
decreases rapidly with increasing lead times. RMSE and MAE of ALARO reach
similar values to SATIN for lead times between 30 min and 1 h (for July and
January, respectively). A similar picture arises for the skill scores in
Fig. <xref ref-type="fig" rid="Ch1.F4"/> where lead times of roughly 1h mark the time when NWP
outperforms the SATIN nowcasting. In this paper only results from July are
shown as the results from January reveal a similar behavior with better
performance of SATIN in the first hour of forecasts. In January the error
levels are generally smaller for all models (SATIN, ALARO, AROME), which
indicates a better performance in the non-convective season.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p>Comparison of pure (translational) nowcasting with NWP: relative
RMSE, MAE and Bias averaged over July for ALARO (5 km), AROME (2.5 km) and
SATIN.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f03.pdf"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p>Comparison of pure (translational) nowcasting with NWP: FBI, TSS and
ETS averaged over July for ALARO (5 km), AROME (2.5 km) and SATIN.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f04.pdf"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S3">
  <title>Validation of SATIN and comparison to NWP</title>
<sec id="Ch1.S3.SS1">
  <title>Validation of SATIN analysis</title>
      <p>The SATIN algorithm strives to obtain an optimal combination of satellite
data and station observations to provide precipitation analyses. In this
section the SATIN analyses are compared to the pure satellite product that
serves as input to SATIN as well as to the currently operational local area
NWP at ZAMG (ALARO5).</p>
      <p>For the comparison with SATIN analyses, NWP output is taken as it would be
available in an operational environment (i.e. at a given SATIN analysis time
an NWP analysis is not available, thus an NWP forecast valid for this time
has to be taken for comparison purposes.). Reference in these comparisons are
the INCA precipitation analyses. At 5 selected days with heavy precipitation,
standard verification measures RMSE, MAE, Bias as well as the objective SAL
verification has been carried out. Figure <xref ref-type="fig" rid="Ch1.F5"/> represents the SAL
result. It can be seen from this figure, that SATIN analyses significantly
reduce the spread in the data and have narrower distributions than the
satellite and NWP products. Structure and Location are very well represented
by SATIN in most cases. The results for Amplitude exhibit much lower spread
as e.g. in the NWP output, however the mean values of NWP sometimes yield
better results than those of SATIN.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><caption><p>Validation of SATIN analyses with INCA analyses and comparison to
ALARO and H03 (SAT) satellite precipitation product. Box plots of daily
Structure, Amplitude, Location values for 5 cases with heavy precipitation.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f05.pdf"/>

        </fig>

      <p>Additionally to the case studies of the previous comparisons, statistics have
been computed for two months, one in winter and one in summer. SATIN has been
computed with 9 TAWES stations not entering the algorithm (see
Fig. <xref ref-type="fig" rid="Ch1.F6"/>). By excluding these stations, a cross validation can be
carried out by computing statistics at these exact stations. For comparison,
SAT (H03) and NWP (ALARO5) are also investigated and compared to SATIN.
Relative RMSE, MAE and Bias are averaged over the summer and winter months
and the results for January and July 2014 are shown in Table <xref ref-type="table" rid="Ch1.T3"/>.</p>
      <p>SATIN clearly outperforms both, ALARO5 and H03 in all standard verification
parameters. Specifically, the bias during the convective season in July 2014
is much smaller in SATIN than in the NWP fields.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p>INCA domain and topography. Information on excluded TAWES stations
for cross validation of SATIN analyses is included.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f06.png"/>

        </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3"><caption><p>Mean relative RMSE, MAE and Bias obtained from cross validation at 9
stations for January and July 2014. NWP refers to ALARO 5 km while SAT
refers to the HSAF H03 product.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.92}[.92]?><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3">January</oasis:entry>  
         <oasis:entry colname="col4"/>  
         <oasis:entry colname="col5"/>  
         <oasis:entry colname="col6">July</oasis:entry>  
         <oasis:entry colname="col7"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">NWP</oasis:entry>  
         <oasis:entry colname="col3">SAT</oasis:entry>  
         <oasis:entry colname="col4">SATIN</oasis:entry>  
         <oasis:entry colname="col5">NWP</oasis:entry>  
         <oasis:entry colname="col6">SAT</oasis:entry>  
         <oasis:entry colname="col7">SATIN</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">RMSE</oasis:entry>  
         <oasis:entry colname="col2">0.86</oasis:entry>  
         <oasis:entry colname="col3">1.12</oasis:entry>  
         <oasis:entry colname="col4">0.71</oasis:entry>  
         <oasis:entry colname="col5">1.26</oasis:entry>  
         <oasis:entry colname="col6">1.58</oasis:entry>  
         <oasis:entry colname="col7">0.99</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">MAE</oasis:entry>  
         <oasis:entry colname="col2">0.72</oasis:entry>  
         <oasis:entry colname="col3">0.99</oasis:entry>  
         <oasis:entry colname="col4">0.60</oasis:entry>  
         <oasis:entry colname="col5">0.89</oasis:entry>  
         <oasis:entry colname="col6">1.19</oasis:entry>  
         <oasis:entry colname="col7">0.64</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Bias</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.52</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.87</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.45</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.76</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.39</oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.35</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S3.SS2">
  <title>Nowcasting compared to NWP</title>
      <p>At lead times beyond the pure nowcasting range, the SATIN system is blended
with an NWP model. This is done because pure nowcasting (shifting of cells
according to motion vectors) does not include any dynamical or physical
aspects (as in NWP's) and thus is not able to describe the future state of
the atmosphere for lead times larger than a couple of hours. The combination
of pure nowcasting and NWP provides the advantage of merging current
observations and derived nowcasts with physically based NWP models. It is
crucial to determine the optimal timing for switching from one system
(nowcasting) to the other (NWP) in order to optimally profit from the
advantages of both systems.</p>
      <p>A transition phase marks the lead times where the different models,
nowcasting and NWP, are combined. Before the transition phase, SATIN consists
of pure nowcasting, after the transition phase SATIN is governed by NWP
exclusively. Within the transition phase the weights of the NWP model are
gradually increased while the contributions from pure nowcasting are
decreased. Therefore, at lead times beyond the transition phase, the SATIN
system entirely relies on the NWP model output, delivering the forecasts
interpolated on the 1km INCA grid.</p>
      <p>Deciding which NWP model should be used for the blending with nowcasting is
not an easy task, as each of the available models has its strengths and
weaknesses. Rather than evaluating the NWP models (which is beyond the scope
of this study), we compare several models to pure nowcasting.</p>
      <p>The NWP models investigated are ALARO (5 km), AROME (2.5 km) and AROME
(1 km). For the same cases as in Fig. <xref ref-type="fig" rid="Ch1.F5"/>, daily average error
scores (RMSE, MAE, Bias, SAL, FBI, TSS, ETS) are computed and plotted as a
function of the lead time. The resulting scores are then averaged (over the
cases) to obtain
Figs. <xref ref-type="fig" rid="Ch1.F7"/>–<xref ref-type="fig" rid="Ch1.F9"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p>Comparison of pure (translational) nowcasting with NWP models:
relative RMSE, MAE and Bias versus lead time, averaged over five days with
heavy precipitation.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f07.pdf"/>

        </fig>

      <p>Relative RMSE, MAE and Bias in Fig. <xref ref-type="fig" rid="Ch1.F7"/> show for
pure nowcasting (SATIN) a clear increase of error with increasing lead time.
At analysis time, the error measures are all below the values obtained from
the different NWP models. Relative RMSE and MAE reach the level of ALARO
(best performing NWP for the selected cases) after about 1h lead time.
Relative Bias of SATIN becomes larger than the one of AROME (2.5 km) after
less than 30 min lead time.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p>Comparison of pure (translational) nowcasting with NWP models:
Structure, Amplitude, Location versus lead time, averaged over five days with
heavy precipitation.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f08.pdf"/>

        </fig>

      <p>Objective verification measures Structure, Amplitude and Location as shown in
Fig. <xref ref-type="fig" rid="Ch1.F8"/> exhibit much less dependency on lead times.
Only the Location measure shows an increase for SATIN with lead time and
reaches values as those from the NWP's at around 1.5 to 2 h lead time. This
suggests, that localisation of precipitation cells are very well captured in
the analysis but the translational motion in pure nowcasting rapidly
deteriorates the result. In contrast NWP Location values are almost constant
over lead time. As was already noted in Sect. <xref ref-type="sec" rid="Ch1.S2.SS4"/>, the
computation of motion vectors can lead to unrealistic translational movement
of cells and needs further optimisation and revision which is beyond the
possibilities of this project.</p>
      <p>Amplitude and Structure values of SATIN remain relatively constant with lead
time and show similar values as AROME (1 km) and AROME (2.5 km)
respectively. The results for Amplitude and relative Bias do not match
exactly, with positive Amplitude values for ALARO and AROME (2.5 km) and
negative relative Bias of the same models. Structure is best represented by
SATIN and the AROME model in 2.5 km resolution. ALARO (5 km) is
overestimating Structure while AROME (1 km) is underestimating this
parameter. Thus, ALARO tends to overestimate the extent of precipitation
fields and AROME (1km) tends to underestimate them – compared to INCA
analyses.</p>
      <p>Skill scores FBI, TSS and ETS, as depicted in
Fig. <xref ref-type="fig" rid="Ch1.F9"/>, show again a dependency on lead time for
SATIN. Results for the NWP models are relatively constant. The scores for
SATIN yield better results than NWP models for lead times below about 1.5 h.
The bias related index FBI for the NWP's shows best results for ALARO and
worst results for AROME (1 km). This again indicates the different
characteristics of the scores (Bias, Amplitude and FBI). Scores were computed
for a threshold of 1 mm 15 min<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.</p>
      <p>The presented results are based on a few heavy precipitation cases and may
not be representative for low impact situations. Nevertheless, they give an
impression of what can be expected from a satellite based nowcasting system.
Analyses tend to give excellent results, with a pronounced decrease in
performance for increasing lead times. According to these results, transition
from pure nowcasting to NWP's should take place somewhere between 30 min and
2 h. As the investigated scores show quite different behavior, it is not easy
to exactly determine the best transition time exactly, but rather depend on
the scale of interest, the weather type and the application.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9"><caption><p>Comparison of pure (translational) nowcasting with NWP models: FBI,
TSS, ETS versus lead time, averaged over five days with heavy precipitation.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f09.pdf"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS3">
  <title>Sensitivity to station density</title>
      <p>In Austria (and most European countries), the density of automatic weather
stations of different providers (e.g. national meteorological services,
hydrological services, etc.) for precipitation measurements is relatively
high, with a mean distance between neighbouring stations of about 12 km, or
roughly 700 stations. However, in many regions of the world, where a
satellite based precipitation nowcasting would be most beneficial (due to the
absence of radar), station density is much lower. Therefore, the influence of
station density on the skill of the analysis is quite important to estimate
the benefit of such a system in data sparse regions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10"><caption><p>Relative RMSE, MAE and Bias per lead time (LT) averaged over
July 2014. Several SATIN runs are shown with progressively less stations
entering the algorithm. ALARO and AROME are shown as reference.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f10.pdf"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11"><caption><p>Satellite image (MSG IR), surface pressure analysis and frontal
zones for 15 May 2014 at 12:00 UTC.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f11.jpg"/>

        </fig>

      <p>Experiments have been run to investigate the effect of reduced station
density on the SATIN nowcasting performance and consequently on the optimal
transition time to NWP model output. For each of the experiments an
increasing amount of stations measuring non-zero precipitation has been
selected and excluded from the SATIN nowcasting computation. SATIN runs were
performed for 10, 30, 50, 70 and 90 % of stations missing. Results are
averaged over July 2014 and are shown in Fig. <xref ref-type="fig" rid="Ch1.F10"/>. Reducing
the station density by half (50 %) shows for RMSE and MAE around half of
the original (no stations excluded) lead time as optimal transition time. For
the analysis, a 10 % increase of the error measures can be observed when
comparing 90 % excluded stations with standard SATIN runs. These results
suggest, that in regions with very low station density, an analysis and
nowcasting system as proposed in this study, still yields better results than
NWP models for the analysis and lead times of up to 30 min. Low station
density will not only affect a poorer nowcasting quality but also poorer NWP
performance, thus the quality of NWP forecasts will also deteriorate.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12"><caption><p>24 h precipitation sum from different models for 15 May 2014.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f12.jpg"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS4">
  <title>Case study – 15 May 2014</title>
      <p>The synoptic situation is characterised as a high pressure system over the
British Isles and a low pressure system over Romania with a cold air flow
from the north reaching Austria. On the backside of this low pressure system,
intensive precipitation is observed which is accompanied by strong
north-westerly winds. The center of the low pressure system is gradually
moving westwards which leads to increasing precipitation rates across the
Alps. Heavy precipitation is mostly centred over the eastern parts of the
domain (Figs. <xref ref-type="fig" rid="Ch1.F11"/> and <xref ref-type="fig" rid="Ch1.F12"/>).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F13"><caption><p>Comparison of pure (translational) nowcasting with NWP models on
15 May 2014: relative RMSE, MAE and Bias of forecasts per LT.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f13.pdf"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F14"><caption><p>Comparison of pure (translational) nowcasting with NWP models on
15 May 2014: Structure, Amplitude and Location of forecasts per LT.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/13/27/2016/asr-13-27-2016-f14.pdf"/>

        </fig>

      <p>Average scores per lead time are computed for each forecast and plotted in
Figs. <xref ref-type="fig" rid="Ch1.F13"/> and <xref ref-type="fig" rid="Ch1.F14"/>. Results on this day
clearly show the superior performance of SATIN (in pure translation mode
without model merging) compared to the other models for lead times up to
1 h. At longer lead times the SATIN result deteriorates and gradually drops
below the worst NWP results (in this case AROME 1 km). For this case a
gradual merging of SATIN with ALARO gives best results. This is also the
principal configuration chosen in the SATIN system. The good performance of
SATIN for this case can certainly be attributed to the measurement stations,
as the H03 product almost completely misses the heavy precipitation (compare
Fig. <xref ref-type="fig" rid="Ch1.F12"/>).</p>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <title>Conclusions</title>
      <p>The satellite based nowcasting system SATIN yields more accurate analysis
fields compared to operationally available NWP forecasts. This finding also
holds when the rain gauge station density is artificially reduced
significantly.</p>
      <p>Pure translational nowcasting with SATIN yields better scores than NWP
forecasts for lead teams of around 1 h. Results indicate, that a
transition from pure nowcasting to NWP should take place between 1 and 2 h.</p>
      <p>A simple approach of merging station observations with satellite
precipitation has been applied. As satellite precipitation products
occasionally suffer from massive underestimation of precipitation and
generally exhibit quite varying performance, a more sophisticated merging
algorithm might improve the analysis (e.g. Kriging methods).</p>
      <p>The computation of motion vectors can lead to unrealistic results and needs
further improvement. Possibly, other methods of computing translational
motion should be investigated (e.g. use of atmospheric motion vectors from
nowcasting SAF, or implementing other concepts such as optical flow).</p>
      <p>Nevertheless, the presented system is a simple and robust method for
obtaining accurate analyses and nowcasts in the absence of radars. Besides
possible improvements to the current system with the mentioned techniques,
further studies could investigate on the combination with radar data, or the
implementation of the system in data sparse regions.</p>
</sec>

      
      </body>
    <back><ack><title>Acknowledgements</title><p>This work was supported by the Austrian Space Applications Programme of the
Austrian Research Promotion Agency (FFG) as “Satellite-based short range
weather prediction with special emphasize on high impact events” with the
project no. 840117. The authors thank two anonymous referees who provided
valuable comments which led to improvements of the paper. <?xmltex \hack{\newline}?><?xmltex \hack{\newline}?> Edited by: A. Cress<?xmltex \hack{\newline}?> Reviewed by: two anonymous
referees</p></ack><ref-list>
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  </ref-list><app-group content-type="float"><app><title/>

    </app></app-group></back>
    <!--<article-title-html>SATIN–Satellite driven nowcasting system</article-title-html>
<abstract-html><p class="p">A precipitation nowcasting system (SATIN) is presented which relies entirely
on satellite based precipitation products and rain gauge measurements. Thus,
the proposed system is most suitable for areas where ground based radar
observations are not available, or potentially suffer from low quality. SATIN
delivers analyses on a 1 km grid every 15 min and nowcasts (obtained through
motion vectors) in 15 min time steps. Nowcasts are gradually merged with NWP
precipitation forecasts. An extensive validation including comparisons to
different NWP models yields superior performance for SATIN analyses as well
as nowcasts for lead times up to 1 h. Reducing the station density still
yields better performance than operationally available NWP's.</p></abstract-html>
<ref-html id="bib1.bib1"><label>Bica(2012)</label><mixed-citation>
Bica, B.: Filter algorithms in the INCA precipitation analysis, Technical Report,
ZAMG, 1–2, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>Brousseau et al.(2008)Brousseau, Bouttier, Hello, Seity, Fischer,
Berre, Montmerle, Auger, and Malardel</label><mixed-citation>
Brousseau, P., Bouttier, F., Hello, G., Seity, Y., Fischer, C., Berre, L.,
Montmerle, T., Auger, L., and Malardel, S.: A prototype convective-scale data
assimilation system for operation: the Arome-RUC, HIRLAM Techn. Report, 68,
23–30, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>Davies(1976)</label><mixed-citation>
Davies, H.: A lateral boundary formulation for multi-level prediction models,
Q. J. Roy. Meteor. Soc., 102, 405–418, 1976.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>Gerard and Geleyn(2005)</label><mixed-citation>
Gerard, L. and Geleyn, J.-F.: Evolution of a subgrid deep convection
parametrization in a limited-area model with increasing resolution, Q.
J. Roy. Meteor. Soc., 131, 2293–2312, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>Haiden et al.(2011)Haiden, Kann, Wittmann, Pistotnik, Bica, and
Gruber</label><mixed-citation>
Haiden, T., Kann, A., Wittmann, C., Pistotnik, G., Bica, B., and Gruber, C.:
The Integrated Nowcasting through Comprehensive Analysis (INCA) system and
its validation over the Eastern Alpine region, Weather  Forecast., 26,
166–183, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>Kann et al.(2015)Kann, Meirold-Mautner, Schmid, Kirchengast,
Fuchsberger, Meyer, Tüchler, and Bica</label><mixed-citation>
Kann, A., Meirold-Mautner, I., Schmid, F., Kirchengast, G., Fuchsberger, J.,
Meyer, V., Tüchler, L., and Bica, B.: Evaluation of high-resolution
precipitation analyses using a dense station network, Hydrol. Earth Syst.
Sci., 19, 1547–1559, <a href="http://dx.doi.org/10.5194/hess-19-1547-2015" target="_blank">doi:10.5194/hess-19-1547-2015</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>Mugnai et al.(2013)Mugnai, Casella, Cattani, Dietrich, Laviola,
Levizzani, Panegrossi, Petracca, Sanò, Di Paola, Biron, De Leonibus, Melfi,
Rosci, Vocino, Zauli, Pagliara, Puca, Rinollo, Milani, Porcù, and
Gattari</label><mixed-citation>
Mugnai, A., Casella, D., Cattani, E., Dietrich, S., Laviola, S., Levizzani,
V.,
Panegrossi, G., Petracca, M., Sanò, P., Di Paola, F., Biron, D.,
De Leonibus, L., Melfi, D., Rosci, P., Vocino, A., Zauli, F., Pagliara, P.,
Puca, S., Rinollo, A., Milani, L., Porcù, F., and Gattari, F.:
Precipitation products from the hydrology SAF, Nat. Hazards Earth Syst. Sci., 13, 1959–1981, <a href="http://dx.doi.org/10.5194/nhess-13-1959-2013" target="_blank">doi:10.5194/nhess-13-1959-2013</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>Radnóti(1995)</label><mixed-citation>
Radnóti, G.: Comments on “A spectral limited-area formulation with
time-dependent boundary conditions applied to the shallow-water equations”,
Mon. Weather Rev., 123, 3122–3123, 1995.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>Rodríguez and Marcos(2014)</label><mixed-citation>
Rodríguez, A. and Marcos, C.: Product User Manual for the “Convective
Rainfall Rate”  (CRR – PGE05 v4.0), Techn. Rep., NWCSAF,
<a href="http://www.nwcsaf.org/" target="_blank">http://www.nwcsaf.org/</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>Scofield and Kuligowski(2003)</label><mixed-citation>
Scofield, R. A. and Kuligowski, R. J.: Status and outlook of operational
satellite precipitation algorithms for extreme-precipitation events, Weather
Forecast., 18, 1037–1051, 2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>Seity et al.(2011)Seity, Brousseau, Malardel, Hello, Bénard,
Bouttier, Lac, and Masson</label><mixed-citation>
Seity, Y., Brousseau, P., Malardel, S., Hello, G., Bénard, P., Bouttier,
F., Lac, C., and Masson, V.: The AROME-France convective-scale operational
model, Mon. Weather Rev., 139, 976–991, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>Simmons and Burridge(1981)</label><mixed-citation>
Simmons, A. J. and Burridge, D. M.: An energy and angular-momentum conserving
vertical finite-difference scheme and hybrid vertical coordinates, Mon.
Weather Rev., 109, 758–766, 1981.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>Wernli et al.(2008)Wernli, Paulat, Hagen, and Frei</label><mixed-citation>
Wernli, H., Paulat, M., Hagen, M., and Frei, C.: SAL–A novel quality
measure for the verification of quantitative precipitation forecasts, Mon.
Weather Rev., 136, 4470–4487, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>Wilks(2011)</label><mixed-citation>
Wilks, D. S.: Statistical methods in the atmospheric sciences, vol. 100,
Academic press, 2011.
</mixed-citation></ref-html>--></article>
