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<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" xml:lang="en" dtd-version="3.0" article-type="research-article"><?xmltex \makeatother\@nolinetrue\makeatletter?>
  <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-22-345-2022</article-id><title-group><article-title>Development of damage curves for buildings near La Rochelle during storm Xynthia based on insurance claims and<?xmltex \hack{\break}?> hydrodynamic simulations</article-title><alt-title>Development of damage curves for buildings near La Rochelle</alt-title>
      </title-group><?xmltex \runningtitle{Development of damage curves for buildings near La Rochelle}?><?xmltex \runningauthor{M. A. Diaz~Loaiza et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff7">
          <name><surname>Diaz Loaiza</surname><given-names>Manuel Andres</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-0300-2653</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff6">
          <name><surname>Bricker</surname><given-names>Jeremy D.</given-names></name>
          <email>j.d.bricker@tudelft.nl</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Meynadier</surname><given-names>Remi</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3 aff4 aff5">
          <name><surname>Duong</surname><given-names>Trang Minh</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3 aff4 aff5">
          <name><surname>Ranasinghe</surname><given-names>Rosh</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Jonkman</surname><given-names>Sebastiaan N.</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Department of Hydraulic Engineering, Delft University of Technology, Delft, the Netherlands</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Group Risk Management, AXA GIE, Paris, France</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Coastal and Urban Risk and Resilience, IHE Delft
Institute for Water Education, <?xmltex \hack{\break}?>P.O. Box 3015, 2601 DA Delft, the Netherlands</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Department of Water Engineering and Management, University of Twente, P.O. Box 217, <?xmltex \hack{\break}?>7500 AE Enschede, the Netherlands</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Harbour, Coastal and Offshore Engineering, Deltares, P.O. Box 177,
2600 MH Delft, the Netherlands</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Department of Civil and Environmental Engineering, University of
Michigan, Ann Arbor, MI, USA</institution>
        </aff>
        <aff id="aff7"><label>7</label><institution>JBA Consulting, Dublin, Ireland</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Jeremy D. Bricker (j.d.bricker@tudelft.nl)</corresp></author-notes><pub-date><day>8</day><month>February</month><year>2022</year></pub-date>
      
      <volume>22</volume>
      <issue>2</issue>
      <fpage>345</fpage><lpage>360</lpage>
      <history>
        <date date-type="received"><day>4</day><month>June</month><year>2021</year></date>
           <date date-type="rev-request"><day>18</day><month>June</month><year>2021</year></date>
           <date date-type="rev-recd"><day>15</day><month>December</month><year>2021</year></date>
           <date date-type="accepted"><day>15</day><month>December</month><year>2021</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 </copyright-statement>
        <copyright-year>2022</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="d1e174">The Delft3D hydrodynamic and wave model is used to
hindcast the storm surge and waves that impacted La Rochelle, France, and the
surrounding area (Aytré, Châtelaillon-Plage, Yves, Fouras, and Île de Ré) during storm Xynthia. These models are validated against tide and
wave measurements. The models then estimate the footprint of flow depth,
speed, unit discharge, flow momentum flux, significant wave height, wave
energy flux, total water depth (flow depth plus wave height), and total
(flow plus wave) force at the locations of damaged buildings for which
insurance claims data are available. Correlation of the hydrodynamic and
wave results with the claims data generates building damage functions. These
damage functions are shown to be sensitive to the topography data used in
the simulation, as well as the hydrodynamic or wave forcing parameter chosen
for the correlation. The most robust damage functions result from highly
accurate topographic data and are correlated with water depth or total
(flow plus wave) force.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

      <?xmltex \hack{\allowdisplaybreaks}?><?xmltex \hack{\newpage}?>
<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e189">In February 2010 the Xynthia extratropical storm caused damage and
casualties along the Atlantic coast of Spain and France (Slomp et al., 2010;
Chauveau et al., 2011). The strong winds and low atmospheric pressure
together with the landfall of the storm at high spring tide generated
unprecedented water levels at La Rochelle and surroundings (Bertin et al.,
2014). The present paper develops damage curves for buildings in the area
where the storm surge and waves from the Xynthia storm caused the most
damage. We draw on methods used to quantify damage due to hurricanes and
tsunamis in the USA and Japan (Suppasri, 2013; Hatzikyriakou et al., 2018;
Tomiczek et al., 2017) but for the first time apply these to modern masonry
structures in Europe affected by storm surge and waves from an extratropical
cyclone. Therefore, the main objective of the present study is to develop
damage functions from insurance claims data supported by hydrodynamic
modelling. A total of 423 reported claims in the area of study were used
(Fig. 1). The damage ratio (DR) is defined as the
ratio of damages claimed by each property to the total insured value of
that property. More than 9 % of the structures had a damage ratio (DR)
higher<?pagebreak page346?> than 0.5 (considerable damages), 30 % had DR higher than 0.2
(medium damages), and 49 % had low damages. This is a typical distribution
for damage claims (see for example Fuchs  et al., 2019).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e194">Damage ratio histogram for insurance claims data in the region.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/345/2022/nhess-22-345-2022-f01.png"/>

      </fig>

      <p id="d1e203">The damage curve is an important tool in risk assessment science related to
the vulnerability of structures (Pistrika and Jonkman, 2010; Englhardt et al.,
2019). From the structural point of view, damage curves depend on the
construction materials that buildings are made of (Huizinga, et al., 2017;
Postacchini et al., 2019; Masoomi et al., 2019). Damage curves also depend
on construction methods, codes, and building layout, including the distance
between buildings (Suppasri et al., 2013; Jansen et al., 2020; Masoomi et
al., 2019). The current paper focuses on one–two-storey masonry buildings under
the effect of storm surge and wave forces produced by an extratropical storm
in northwest France. The Xynthia storm provided a rare dataset of empirical
measured damage from coastal flooding in a European country. Similar
analysis of damage from other storms with different return periods in the
same region would help to reduce uncertainty (Breilh et al., 2014; Bulteau
et al., 2015), but for now no other claims data are available.</p>
      <p id="d1e207">In flood risk assessment, the relation between damage and hazard is
quantified by fragility curves and damage curves. The difference between
these two is that fragility curves express the probability that a structure
is damaged to a specified structural state (Tsubaki  et al., 2016), while
damage curves instead assess the cost of damage incurred by flooding of a
given structure (Englhardt  et al., 2019; Huizinga   et al., 2017).
For both cases it is important to highlight the fact that these curves
usually rely on the flood depth alone to quantify the hazard (Pregnolato
et al., 2015), while there are fewer studies that attempt to represent the
hazard by other quantities like the flow velocity, significant wave height,
or wave force (Kreibich   et al., 2009; De Risi   et al., 2017). For
instance, Tomiczek  et al. (2017) related the flow velocity to the
structure damage state (DS) in New Jersey for Hurricane Sandy. In the
present study we relate eight different hydrodynamic variables to the damage
ratio coming from insurance claims following extratropical storm Xynthia.</p>
      <p id="d1e210">Damage curves are commonly developed by the correlation of field or
laboratory measurements of damage, with numerical simulations of hazard
level. Tsubaki et al. (2016) measured railway embankment and ballast scour
in the field and correlated this damage with flood overflow surcharge
calculated by a hydrodynamic flood simulation. Englhardt et al. (2019) and
Huizinga et al. (2017) used big-data analytics to correlate tabulated
damages with estimated flood levels over a large scale. Pregnolato et al. (2015) showed that most damage functions are based on flood depth alone,
though a few also consider flow speed (De Risi et al., 2017; Jansen et al.,
2020) or flood duration. The water depth is an important variable since it
accounts for the static forces that act on a structure. Nevertheless, in
storm events, structures close to the coast at a foreshore/backshore can be
subjected to dynamical forces like the action of flow and waves (Kreibich et
al., 2009; Tomiczek et al., 2017). For this reason, in order to consider
other possible forces the following hydrodynamic parameters are analysed:
water depth (<inline-formula><mml:math id="M1" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula>), flow speed (<inline-formula><mml:math id="M2" display="inline"><mml:mi>v</mml:mi></mml:math></inline-formula>), unit discharge (<inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula>), flow momentum
flux (<inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>), significant wave height (<inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), total water
depth (<inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), wave energy flux (<inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), and total force
<inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:mfenced open="(" close=")"><mml:mrow><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula>. The wave energy flux is defined via
Eq. (1) as in Bricker et al. (2017).
          <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M9" display="block"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">16</mml:mn></mml:mfrac></mml:mstyle><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>g</mml:mi><mml:msubsup><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
        where <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (m) is the significant wave height, <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (m s<inline-formula><mml:math id="M12" 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>) is the wave
group velocity, <inline-formula><mml:math id="M13" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula> (kg m<inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) is the water density, <inline-formula><mml:math id="M15" display="inline"><mml:mi>g</mml:mi></mml:math></inline-formula>
(m s<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) is the acceleration due to gravity, and <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:mi>g</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msqrt></mml:mrow></mml:math></inline-formula> over
land where waves impact buildings.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Methods</title>
      <p id="d1e460">Damage curves were developed by hindcasting the hazard with a meteorological
model, followed by a hydrodynamic (tides and storm surge) and wave model,
and then correlating the resulting flood conditions with claimed damages
(Fig. 2).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e465">Flow chart of the framework used in development of damage curves.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/345/2022/nhess-22-345-2022-f02.png"/>

      </fig>

<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Meteorological model setup and description of the Xynthia storm</title>
      <p id="d1e481">From 23 February 2010 Météo-France recorded a low-pressure front that
was forming in the North Atlantic and passed north of Spain on 27 February,
with a minimum pressure of 966 hPa (Fig. 3). Early in the morning of 28
February it made landfall on the French coast at the same time that a high
astronomical tide was developing, causing a total of 65 casualties in the
regions of Vendée and Charente-Maritime and approximately EUR 2.5 billion
in damage to agricultural<?pagebreak page347?> (oyster farms and mussels) infrastructure, the
tourist industry, and residential/commercial zones (Slomp et al., 2010). To
generate pressure and wind fields to drive the storm surge model,
dynamically downscaled surface meteorological data were generated for the
French Atlantic study region (Fig. 3). This
contains zonal and meridional winds 10 m above ground (<inline-formula><mml:math id="M18" display="inline"><mml:mi>u</mml:mi></mml:math></inline-formula>10, <inline-formula><mml:math id="M19" display="inline"><mml:mi>v</mml:mi></mml:math></inline-formula>10) and surface
pressures over sea and land, with 3.5 km spatial resolution and 3 h
temporal resolution. The dynamical downscaling was performed with the
regional climate model WRF (Skamarock and  Klemp, 2008), based on National Centers for Environmental Prediction (NCEP) Climate Forecast System Reanalysis (CFSR)
data (Saha et al., 2010). The regional non-hydrostatic WRF model
(version 3.4) simulated 15 February 2010 to 5 March 2010. The initial
and lateral boundary conditions are taken from the CFSR reanalysis at
0.5<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> resolution, updated every 6 h. The horizontal resolution is 7 km; we use a vertical resolution of 35 sigma levels with a top of atmosphere
at 50 hPa. The simulation domain was chosen to be wide enough in latitude and
longitude for WRF to fully simulate the large-scale atmospheric features of
the Xynthia extratropical cyclone. A spin-up time of 5 d was considered
in the study to remove spurious effects of the top layer soil moisture
adjustment even though most of the analyses here are performed over the
ocean. Land surface processes are resolved by using the NOAA land surface
model scheme with four soil layers. Numerical schemes used in the WRF
simulation to downscale Xynthia data are the multi-scale Kain–Fritsch scheme
for convection, the Yonsei University scheme for the planetary boundary
layer, the WRF single-moment six-class scheme for microphysics, and the RRTMG
scheme for shortwave and longwave radiation. WRF outputs are generated every
3 h.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Hydrodynamic model of the Xynthia storm</title>
      <p id="d1e516">In order to capture the hydrodynamic storm characteristics, a regional model
domain over the Atlantic Spanish and French coasts was built. As shown
schematically in Fig. 2, Delft3D calculates non-steady flow phenomena that
result from tidal and meteorological forcing on a rectilinear or a
curvilinear grid (Deltares, 2021). At the same time, and coupled with
Delft3D, a spectral wave model (SWAN) calculates significant wave height and
period fields. Delft3D and SWAN were used to hindcast the physical forcing
at the locations of all claims in the database. Afterwards, a probability
standardized normal distribution function as proposed by Suppasri et al. (2013) was used to develop damage curves by correlating claimed damage with
a variety of hydrodynamic forcing variables. To conserve computational
resources and reduce computation time, domain decomposition (two-way
hydrodynamic nesting) was implemented with grids of resolution of
<inline-formula><mml:math id="M21" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 2 km over the open ocean, <inline-formula><mml:math id="M22" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 400 m close to the
study area, and <inline-formula><mml:math id="M23" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 80 m over the area of claims data
(Fig. 3).</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="d1e542">Domain decomposition with three nested grids running in parallel.
The centre of the Xynthia storm is shown as a triangle at the time of
minimum atmospheric pressure of 966 hPa on 27 February 2010 at 21:00:00 (Extreme Wind Storm Catalogue). Topographic map inset covers the smallest
domain shown on the large map. Satellite image by OpenLayers – QGIS.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/345/2022/nhess-22-345-2022-f03.jpg"/>

        </fig>

<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>Topography and bathymetry</title>
      <p id="d1e558">We use two types of topography datasets: a global dataset for the
bathymetry/topography (GEBCO, 2020, which is based on SRTM 15<inline-formula><mml:math id="M24" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> v2 over
land), and a higher-resolution bathymetry (MNT HOMONIM project) and
topography (IGN). Additionally, a survey of flood wall height was
performed during August 2020 in order to include flood walls as thin weirs
inside the Delft3D model and in this way overcome the fact that inside the
high-resolution 5 m topography, these structures are not represented, as
suggested by Bertin et al. (2014). Luppichini et al. (2019) and Ettritcha et
al. (2018) found that the quality of bathymetry and topography data has a
large effect on estimation of the hazard, and Brussee et al. (2021)
similarly found topography data quality affects resulting damage estimates.
In order to investigate the effect of the quality of topographic and
bathymetric data on the resulting damage functions, three scenarios are
considered in our work (Table 1).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e571">Case studies for investigating sensitivity of model result to digital elevation model (DEM) resolution.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <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:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Item</oasis:entry>
         <oasis:entry colname="col2">Low resolution (a)</oasis:entry>
         <oasis:entry colname="col3">High resolution (b)</oasis:entry>
         <oasis:entry colname="col4">High resolution <inline-formula><mml:math id="M25" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> structures (c)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Topography</oasis:entry>
         <oasis:entry colname="col2">GEBCO (500 m)</oasis:entry>
         <oasis:entry colname="col3">IGN (5 m)</oasis:entry>
         <oasis:entry colname="col4">IGN (5 m) <inline-formula><mml:math id="M26" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> flood walls surveyed</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">by the authors with an RTK-GPS</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Bathymetry</oasis:entry>
         <oasis:entry colname="col2">GEBCO (500 m)</oasis:entry>
         <oasis:entry colname="col3">GEBCO (500 m) in deep water</oasis:entry>
         <oasis:entry colname="col4">GEBCO (500 m) in deep water</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M27" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> MNT (100 m) near shore</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M28" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> MNT (100 m) near shore</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Hydrodynamic and wave model setup</title>
      <p id="d1e699">Delft3D was coupled together with SWAN in order to hindcast storm tide and
waves. Model boundary conditions consisted of astronomical tidal water
elevations from the Global Tide and Surge Model (GTSM) of Muis et al. (2016)
for the<?pagebreak page348?> period from 20 February until 1 March 2010. The hydrodynamic model
was run with a computational time step of 30 s and a uniform Manning <inline-formula><mml:math id="M29" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>
of 0.025. The air–sea drag coefficient of Smith and Banke (1975) was used.
Other model parameters retained their default settings.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Hydrodynamic and wave model validation</title>
<sec id="Ch1.S2.SS4.SSS1">
  <label>2.4.1</label><title>Storm tide validation</title>
      <?pagebreak page349?><p id="d1e724">The hydrodynamic model was run from 20 February until 1 March 2010, the
duration of the meteorological forcing data, with GTSM astronomical tide
boundary conditions. For validation, three accuracy indicators are assessed:
root mean square error (RMSE, Eq. 3), relative root square error (RRSE,
Eq. 4), and the Pearson correlation coefficient (<inline-formula><mml:math id="M30" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula>, Eq. 5).

                  <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M31" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E2"><mml:mtd><mml:mtext>2</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi mathvariant="normal">RMSE</mml:mi><mml:mo>=</mml:mo><mml:msqrt><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mi>T</mml:mi></mml:munderover><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:msup><mml:mi>y</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>-</mml:mo><mml:mi>y</mml:mi></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow><mml:mi>T</mml:mi></mml:mfrac></mml:mstyle></mml:msqrt><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E3"><mml:mtd><mml:mtext>3</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="normal">RRSE</mml:mi><mml:mo>=</mml:mo><mml:msqrt><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mo>∑</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mi>T</mml:mi></mml:msubsup><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:msup><mml:mi>y</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>-</mml:mo><mml:mi>y</mml:mi></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow><mml:mrow><mml:msubsup><mml:mo>∑</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mi>T</mml:mi></mml:msubsup><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:mi>y</mml:mi><mml:mo>-</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:msqrt><mml:mo>,</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mo>∑</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mi>T</mml:mi></mml:msubsup><mml:mi>y</mml:mi></mml:mrow><mml:mi>T</mml:mi></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E4"><mml:mtd><mml:mtext>4</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mrow><mml:mi>y</mml:mi><mml:mo>,</mml:mo><mml:msup><mml:mi>y</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">cov</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>y</mml:mi><mml:mo>,</mml:mo><mml:msup><mml:mi>y</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:msup><mml:mi>y</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              <?xmltex \hack{\newpage}?><?xmltex \hack{\noindent}?>where <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msup><mml:mi>y</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> is the predicted value, <inline-formula><mml:math id="M33" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> is the actual value and <inline-formula><mml:math id="M34" display="inline"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula>
is the average of the actual values to predict, <inline-formula><mml:math id="M35" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> is the number of values,
and <inline-formula><mml:math id="M36" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> indicates the standard deviation.</p>
      <p id="d1e962">After 2 d of model spin-up (the time required for the model to correct
the assigned initial condition), the comparison between the observed water
levels from the French Naval Hydrographic and Oceanographic Service (SHOM)-Coriolis tide gauges (<uri>http://www.coriolis.eu.org/</uri>, last access: 1 May 2021) and
modelled water levels from Delft3D during the whole simulation is
acceptable (Fig. 4) according to the results for the goodness-of-fit indices
in Table 2. If we compare these values with typical values in the literature
such as Matte et al. (2014) or Tranchant et al. (2021), we observe the
current modelled water levels fit the observations well. Note that the Les Sables-d'Olonne gauge failed at the peak of the storm (on 28 February 2010  at 03:00:00), so a
data point is missing in the observations at that time. At La Rochelle the
difference between the observed and modelled water level is only 36 cm at
peak storm tide.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e970">Observed and modelled tide at La Rochelle and Les Sables-d'Olonne. Note
that during the peak of the storm tide at Les Sables-d'Olonne, the tide measuring
gauge was out of operation, resulting in a missing data point in that data
series.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/345/2022/nhess-22-345-2022-f04.png"/>

          </fig>

</sec>
<sec id="Ch1.S2.SS4.SSS2">
  <label>2.4.2</label><title>Wave model validation</title>
      <p id="d1e987">The wave model was validated against data from the SHOM-Coriolis operational
oceanography centre (<uri>http://www.coriolis.eu.org/About-Coriolis</uri>, last access: 1 May 2021)
in Fig. 5. Important to mention is that the data
available at the buoys stations do not include the significant wave height;
therefore, the swell height was extracted to compare the results from
Delft3D–SWAN. The uncertainty produced by the meteorological downscaling by
means of the WRF model in the hindcast of the winds can add errors in the
results. Unfortunately, no more meteorological information is available. If
we again compare the indices from Table 2 to those found in the literature
such as Baron-Hyppolite et al. (2019), we find comparable goodness of fit
between modelled and measured waves.</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="d1e995">Deep water buoys of Yeu Nord <bold>(a)</bold> and Gascogne <bold>(b)</bold>. In the
first case the buoy is located close by an island of the same name. The
second is located in the open ocean almost in the middle of the Bay of
Biscay.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/345/2022/nhess-22-345-2022-f05.png"/>

          </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e1013">Goodness of fit for water level and wave measurements compared with
the results of Delft3D–SWAN.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <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:thead>
       <oasis:row>
         <oasis:entry colname="col1">Station</oasis:entry>
         <oasis:entry colname="col2">RMSE</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M37" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">RRSE</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">(m)</oasis:entry>
         <oasis:entry colname="col4"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Gascogne</oasis:entry>
         <oasis:entry colname="col2">1.5434</oasis:entry>
         <oasis:entry colname="col3">0.6228</oasis:entry>
         <oasis:entry colname="col4">0.10679</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Yeu Nord</oasis:entry>
         <oasis:entry colname="col2">0.8668</oasis:entry>
         <oasis:entry colname="col3">0.6985</oasis:entry>
         <oasis:entry colname="col4">0.1116</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Les Sables-d'Olonne</oasis:entry>
         <oasis:entry colname="col2">0.4959</oasis:entry>
         <oasis:entry colname="col3">0.9197</oasis:entry>
         <oasis:entry colname="col4">0.1381</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">La Rochelle</oasis:entry>
         <oasis:entry colname="col2">0.4991</oasis:entry>
         <oasis:entry colname="col3">0.9157</oasis:entry>
         <oasis:entry colname="col4">0.1374</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
</sec>
<sec id="Ch1.S2.SS5">
  <label>2.5</label><title>Damage curves</title>
      <p id="d1e1137">Damage curves express the amount of damage experienced by a structure,
relative to the structure's total insured value. The cumulative distribution
function, in terms of the standardized normal distribution function with the
damages (Suppasri et al., 2013; Thapa et al., 2020; Sihombing and Torbol,
2016), is shown in Eq. (2).
            <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M38" display="block"><mml:mrow><mml:mi>P</mml:mi><mml:mfenced open="(" close=")"><mml:mi>x</mml:mi></mml:mfenced><mml:mo>=</mml:mo><mml:mi mathvariant="normal">Φ</mml:mi><mml:mfenced open="[" close="]"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="italic">μ</mml:mi></mml:mrow><mml:mi mathvariant="italic">σ</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the cumulative probability of the damage ratio
with values between 0 and 1, and <inline-formula><mml:math id="M40" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> is the hydrodynamic variable,
<inline-formula><mml:math id="M41" display="inline"><mml:mi mathvariant="normal">Φ</mml:mi></mml:math></inline-formula> is the standardized normal distribution, <inline-formula><mml:math id="M42" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> is the
median, and <inline-formula><mml:math id="M43" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> is the standard deviation (Tsubaki et al., 2016). It is
also very common to express Eq. (1) as a logarithmic function in order
to easily obtain the parameters of the distribution with least squares
fitting as proposed by Suppasri et al. (2013). In the present paper, the
parameters are assessed using the Lmoments package within the open-source
program R. In this way, it is possible to relate different hydrodynamic
variables with the damage ratio. From the 423 claims data within our domain,
approximately 185 are from Île de Ré, and the remaining 238 are from the towns of
La Rochelle, Aytré, Yves, Châtelaillon-Plage, and Fouras. At each
claim location, the maximum of each hydrodynamic variable was extracted, and
from this the damage curves were compiled.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
      <p id="d1e1221">After determining the model hydrodynamic and wave results (Fig. 6) at the
location of each claim location, the data were subdivided into 10
categories according to damage ratio level, and box–whisker plots were built
to display the entire dataset and analyse the trend of the data (Appendix A). Among the flow-only variables, the unit discharge (<inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula>) appears to have
the clearest trend and least scatter. From the variables related to both
flow and waves, the total force <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:mfenced open="(" close=")"><mml:mrow><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula>
appears to have the clearest trend and correlation with the damage ratio.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e1269">Maximum water level and maximum significant wave height (Hsig) footprints
for the small model domain (case study area). Water depth and wave height
are in units of metres. The purple rectangle indicates the limits of the small
domain, outside of which data are not shown.</p></caption>
        <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/345/2022/nhess-22-345-2022-f06.png"/>

      </fig>

<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Damage curves from each digital elevation model</title>
      <p id="d1e1285">In order to build damage curves with Eq. (2), the median values are
extracted from the boxplots of Appendix A (Figs. A1 to A3) for each
variable. In Fig. 7
the damage curves for each hydrodynamic parameter are displayed as
three lines, one for each digital elevation model of Table 1. Similar to Reese
and Ramsay (2010), we find that more than 90 % of the damage occurs in the
first 5 m of flood depth.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e1290">Damage curves for the surge and wave variables (<inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>,</mml:mo><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>h</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) and different bathymetry/topography
conditions (Table 1). Markers indicate the observed data and lines the
fitted statistical distributions.</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/345/2022/nhess-22-345-2022-f07.png"/>

        </fig>

      <p id="d1e1382">Table 3 shows that among the hydrodynamic parameters
related only to storm surge, the water depth best fits Eq. (2), with
the lowest errors (RMSE and RRSE) and the highest Pearson coefficient (<inline-formula><mml:math id="M47" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula>). Among the combined surge and wave parameters, the best correlation is
the total (flow plus wave) force, using the IGN <inline-formula><mml:math id="M48" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> structures topography and
bathymetry (Table 3). This is related to the fact that this digital elevation
model includes thin flood walls that contribute to protection, and which can
substantially modify the flow and wave fields over land.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><?xmltex \currentcnt{3}?><label>Table 3</label><caption><p id="d1e1403">Goodness of fit for the flow-only and flow-plus-wave parameters.
The best fits for flow-only parameters are indicated in bold, and the best
fits for flow-plus-wave parameters are indicated in bold italic.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.98}[.98]?><oasis:tgroup cols="10">
     <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" colsep="1"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <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:colspec colnum="10" colname="col10" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Variable</oasis:entry>
         <oasis:entry rowsep="1" namest="col2" nameend="col4" align="center" colsep="1">RMSE (m) </oasis:entry>
         <oasis:entry rowsep="1" namest="col5" nameend="col7" align="center" colsep="1"><inline-formula><mml:math id="M49" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry rowsep="1" namest="col8" nameend="col10" align="center">RRSE </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">GEBCO</oasis:entry>
         <oasis:entry colname="col3">IGN</oasis:entry>
         <oasis:entry colname="col4">IGN<inline-formula><mml:math id="M50" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">GEBCO</oasis:entry>
         <oasis:entry colname="col6">IGN</oasis:entry>
         <oasis:entry colname="col7">IGN<inline-formula><mml:math id="M51" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">GEBCO</oasis:entry>
         <oasis:entry colname="col9">IGN</oasis:entry>
         <oasis:entry colname="col10">IGN<inline-formula><mml:math id="M52" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">structures</oasis:entry>
         <oasis:entry colname="col5"/>
         <oasis:entry colname="col6"/>
         <oasis:entry colname="col7">structures</oasis:entry>
         <oasis:entry colname="col8"/>
         <oasis:entry colname="col9"/>
         <oasis:entry colname="col10">structures</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Water depth (<inline-formula><mml:math id="M53" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.1595</oasis:entry>
         <oasis:entry colname="col3">0.1898</oasis:entry>
         <oasis:entry colname="col4"><bold>0.1495</bold></oasis:entry>
         <oasis:entry colname="col5">0.8134</oasis:entry>
         <oasis:entry colname="col6">0.7344</oasis:entry>
         <oasis:entry colname="col7"><bold>0.8328</bold></oasis:entry>
         <oasis:entry colname="col8">0.1009</oasis:entry>
         <oasis:entry colname="col9">0.1145</oasis:entry>
         <oasis:entry colname="col10"><bold>0.0902</bold></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Flow speed (<inline-formula><mml:math id="M54" display="inline"><mml:mi mathvariant="normal">v</mml:mi></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.3586</oasis:entry>
         <oasis:entry colname="col3">0.2561</oasis:entry>
         <oasis:entry colname="col4">0.2234</oasis:entry>
         <oasis:entry colname="col5">0.1284</oasis:entry>
         <oasis:entry colname="col6">0.5387</oasis:entry>
         <oasis:entry colname="col7">0.6406</oasis:entry>
         <oasis:entry colname="col8">0.2268</oasis:entry>
         <oasis:entry colname="col9">0.1545</oasis:entry>
         <oasis:entry colname="col10">0.1347</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Unit discharge (<inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.3352</oasis:entry>
         <oasis:entry colname="col3">0.2272</oasis:entry>
         <oasis:entry colname="col4">0.2120</oasis:entry>
         <oasis:entry colname="col5">0.2421</oasis:entry>
         <oasis:entry colname="col6">0.6558</oasis:entry>
         <oasis:entry colname="col7">0.6744</oasis:entry>
         <oasis:entry colname="col8">0.2120</oasis:entry>
         <oasis:entry colname="col9">0.1370</oasis:entry>
         <oasis:entry colname="col10">0.1278</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Flow momentum flux (<inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.3542</oasis:entry>
         <oasis:entry colname="col3">0.2540</oasis:entry>
         <oasis:entry colname="col4">0.1822</oasis:entry>
         <oasis:entry colname="col5">0.1314</oasis:entry>
         <oasis:entry colname="col6">0.5759</oasis:entry>
         <oasis:entry colname="col7">0.7622</oasis:entry>
         <oasis:entry colname="col8">0.2136</oasis:entry>
         <oasis:entry colname="col9">0.1532</oasis:entry>
         <oasis:entry colname="col10">0.1099</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Significant wave height (<inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.2211</oasis:entry>
         <oasis:entry colname="col3">0.2030</oasis:entry>
         <oasis:entry colname="col4">0.1600</oasis:entry>
         <oasis:entry colname="col5">0.6432</oasis:entry>
         <oasis:entry colname="col6">0.6901</oasis:entry>
         <oasis:entry colname="col7">0.8066</oasis:entry>
         <oasis:entry colname="col8">0.1398</oasis:entry>
         <oasis:entry colname="col9">0.1224</oasis:entry>
         <oasis:entry colname="col10">0.0965</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Total water depth (<inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.1767</oasis:entry>
         <oasis:entry colname="col3">0.2217</oasis:entry>
         <oasis:entry colname="col4">0.1522</oasis:entry>
         <oasis:entry colname="col5">0.7575</oasis:entry>
         <oasis:entry colname="col6">0.6404</oasis:entry>
         <oasis:entry colname="col7">0.8265</oasis:entry>
         <oasis:entry colname="col8">0.1117</oasis:entry>
         <oasis:entry colname="col9">0.1337</oasis:entry>
         <oasis:entry colname="col10">0.0918</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Wave energy flux (<inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.2649</oasis:entry>
         <oasis:entry colname="col3">0.2391</oasis:entry>
         <oasis:entry colname="col4">0.2307</oasis:entry>
         <oasis:entry colname="col5">0.5519</oasis:entry>
         <oasis:entry colname="col6">0.5851</oasis:entry>
         <oasis:entry colname="col7">0.6510</oasis:entry>
         <oasis:entry colname="col8">0.1676</oasis:entry>
         <oasis:entry colname="col9">0.1442</oasis:entry>
         <oasis:entry colname="col10">0.1391</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Total force <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:mfenced close=")" open="("><mml:mrow><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">0.3307</oasis:entry>
         <oasis:entry colname="col3">0.2494</oasis:entry>
         <oasis:entry colname="col4"><bold><italic>0.1499</italic></bold></oasis:entry>
         <oasis:entry colname="col5">0.2396</oasis:entry>
         <oasis:entry colname="col6">0.5888</oasis:entry>
         <oasis:entry colname="col7"><bold><italic>0.8387</italic></bold></oasis:entry>
         <oasis:entry colname="col8">0.2092</oasis:entry>
         <oasis:entry colname="col9">0.1504</oasis:entry>
         <oasis:entry colname="col10"><bold><italic>0.0904</italic></bold></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

      <?pagebreak page350?><p id="d1e1927">In Appendix B a comparison to two other typical distribution functions is
carried out. It can be seen that the gamma and generalized
normal (GNO) distributions have
similar goodness-of-fit indicators, while the log-normal distribution
performs slightly worse overall. An analysis on the uncertainty due to the
statistical distribution selection or the inclusion of properties with no
damages can be found in Fuchs et al. (2019). Another source of uncertainty,
in addition of the selected statistical distribution, is the parameter
fitting method (Diaz-Loaiza, 2015). Typical methods for this purpose include
Lmoments, maximum spacing estimation, maximum likelihood, moment method,
and least squares method (Oosterbaan, 1994).</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Discussion</title>
      <p id="d1e1940">The present paper considered the influence of flow-only variables (<inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) and combined flow-wave parameters (<inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub><mml:mi>h</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>). Flow depth and total
(flow plus wave) force produce the best fits with analytical functions.
Goodness of fit to damage curves improves with quality of the topographic
data used (Table 1). However, when applying damage curves in practice, it is
important to base predictions off a similar model setup to that used when
calculating the damage curves in the first place (Brussee et al., 2021). For
example, if damage curves are built using coarse topography that neglects
the presence of thin seawalls (i.e. sheet pile/cantilever walls, or T or L
walls), then the buildings protected by these walls might experience more
intense hydrodynamic conditions in the simulation than if the walls had been
present in the simulation. Since the actual recorded damage does not depend
on the model used to calculate<?pagebreak page351?> the hydrodynamic forcing conditions, damage
curves developed using the coarse-resolution topography will be shifted to
the right relative to damage curves generated with the thin flood walls
present. If these damage curves generated using a coarse-resolution
simulation are then applied for damage prediction by an external user who
applies a high-resolution simulation that resolves flood walls, the reduced
forcing (due to the presence of these flood walls) will generate a
non-conservative result (too little damage), because the damage curves had
been generated using forcing data from a simulation where the flood walls had
not been present. Therefore, when damage curves are reported in the
literature, it is important to quantify how these vary with the topography
used in the simulations on which the damage curves are based. However, in
the current paper, Fig. 7 shows that damage curves do not vary consistently
leftward or rightward as topographic data are improved. This is because the
response of forcing to the presence of these walls is more complex than
simply reducing wave height. If not overflowed, walls reduce damage greatly.
However, water depth can be exacerbated in front of walls, and flow can be
channelled and intensified along walls, all increasing hydrodynamic forcing
in some locations, preventing a simple relation between topographic
resolution and damage curve robustness.</p>
      <p id="d1e2027">In addition to the general sensitivity of damage curves to topographic data
quality, the damage curves displayed in Fig. 7 do
not consider certain physical wave-driven phenomena such as wave overtopping
of structures (Lashley et al., 2020a; Ke et al., 2021) or infragravity waves
generated by waves breaking in shallow water (Roeber and Bricker, 2015). For
instance Lashley et al. (2019) discussed the importance of dike overtopping
due to infragravity waves on nearshore developments that can induce
wave-driven coastal inundation. The wave model used here, SWAN, does not
include infragravity waves, nor does the combined Delft3D–SWAN flow–wave
model simulate wave overtopping of dikes,<?pagebreak page352?> possibly leading to an
underestimation of the hydrodynamic forces on buildings, which would affect
the resulting damage functions. However, consideration of wave overtopping
and infragravity effects requires either phase-resolving wave simulations or
empirical relations specific to the local topography (Lashley et al.,
2020b), though this is beyond the scope of the current study and is
similarly neglected by most other large-scale inundation studies (i.e.,
Sebastian et al., 2014; Kress et al., 2016; Kowaleski et al., 2020).
Nonetheless, the effect of infragravity oscillations and wave overtopping on
resulting damage is an important item for future research.</p>
      <p id="d1e2030">Another important factor mentioned by Bertin et al. (2015) was the
particular track direction of the storm that for the Xynthia event induced a
young sea state, enhancing the<?pagebreak page353?> surface stress, and adding up to 40 cm to the
theoretical surge and tide of their model. The uncertainty and variability
within this methodology can be explained by two factors: (1) the hydrodynamic
modelling, and consequently uncertainty in the hydrodynamic variables, and
(2) uncertainty in the claims data. Regarding the first point, there is a
trend that indicates that better topography/bathymetry data give
hydrodynamic variables that correlate better with the damage ratio. This is
because higher-resolution data generally more accurately reproduce the
actual flood conditions (Luppichini et al., 2019; Ettritcha et al.,
2018). Damage curves developed with a better representation of the
topography (IGN <inline-formula><mml:math id="M63" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> structures) improve the accuracy indicators
(Table 3), though scatter in the data themselves
(Figs. A1, A2 or A3) is large for all topographies. This first point is
also related to the mesh resolution and the roughness coefficients used. The
second point deals with the quality of the damage ratio data. It is known
that insurance claims can sometimes be subject to fraud or information
distortion. In addition, variables related to the vulnerability of the
assets like the construction characteristics, the materials, the quality, and
the age of the structures (Paprotny et al., 2021) play important roles in
determining whether a particular hydrodynamic is related to damage. This
adds a degree of complexity to the analysis. Finally, it is worth mentioning
that if more detailed information from the claims data is available (like
structure type, number of floors, and damage stage), then a more detailed
fragility functions can be generated instead of the bulk damage functions
determined here.</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d1e2049">Insurance claims data facilitated generation of damage curves for structures
located in La Rochelle and surroundings. This provides valuable information
for predicting future damages that can be expected from an extratropical
storm strike on the French Atlantic coast. In the present study, the
hydrodynamic variables that correlated best with the damage ratio are the
flow depth and the total (flow plus wave) force for the flow-only and
flow-plus-wave-related variables respectively. In addition to the
sensitivity of results to resolution of the topographic and bathymetric
data, the inclusion of thin flood walls via a land survey carried out by the
authors also had a significant effect on the damage functions generated.
This is important to note, as thin steel or concrete structures like flood
walls are typically only a few decimetres thick and therefore do not appear
in digital elevation models. The effect of these thin structures on the
resulting damage functions shows the importance of locally sourcing
elevation data for the thin structures that are present when conducting risk
analyses for coastal regions. However it is imperative to keep in mind
agreement between the simulations used for developing the damage relations
in the first place and those where the damage relations are applied for
further risk analysis.</p><?xmltex \hack{\clearpage}?>
</sec>

      
      </body>
    <back><app-group>

<?pagebreak page354?><app id="App1.Ch1.S1">
  <?xmltex \currentcnt{A}?><label>Appendix A</label><title/>
      <p id="d1e2063">Whisker plots from which damage curves are developed are shown in Figs. A1, A2, and A3. Digital elevation models are as described in Table 1. The
damage curves of Fig. 7 use the median values (red lines) from each of the
figures in this appendix.</p>

      <?xmltex \floatpos{h!}?><fig id="App1.Ch1.S1.F8"><?xmltex \currentcnt{A1}?><?xmltex \def\figurename{Figure}?><label>Figure A1</label><caption><p id="d1e2068">Box–whisker plots for the variables (<inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi>h</mml:mi><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>,</mml:mo><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>h</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>)  with the GEBCO DEM.</p></caption>
        <?xmltex \hack{\hsize\textwidth}?>
        <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/345/2022/nhess-22-345-2022-f08.png"/>

      </fig>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{h!}?><fig id="App1.Ch1.S1.F9"><?xmltex \currentcnt{A2}?><?xmltex \def\figurename{Figure}?><label>Figure A2</label><caption><p id="d1e2168">Box–whisker plots for the variables (<inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi>h</mml:mi><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>,</mml:mo><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>h</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) with the IGN DEM.</p></caption>
        <?xmltex \hack{\hsize\textwidth}?>
        <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/345/2022/nhess-22-345-2022-f09.png"/>

      </fig>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{h!}?><fig id="App1.Ch1.S1.F10"><?xmltex \currentcnt{A3}?><?xmltex \def\figurename{Figure}?><label>Figure A3</label><caption><p id="d1e2267">Box–whisker plots for the variables (<inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>,</mml:mo><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>h</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>)  with the IGN <inline-formula><mml:math id="M67" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> structures DEM.</p></caption>
        <?xmltex \hack{\hsize\textwidth}?>
        <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/345/2022/nhess-22-345-2022-f10.png"/>

      </fig>

<?xmltex \hack{\clearpage}?>
</app>

<?pagebreak page357?><app id="App1.Ch1.S2">
  <?xmltex \currentcnt{B}?><label>Appendix B</label><title/>
      <p id="d1e2377">Probability distribution comparison for the<?xmltex \hack{\newline}?> bathymetry/topography of
IGN <inline-formula><mml:math id="M68" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> structures.</p>

      <?xmltex \floatpos{h!}?><fig id="App1.Ch1.S2.F11"><?xmltex \currentcnt{B1}?><?xmltex \def\figurename{Figure}?><label>Figure B1</label><caption><p id="d1e2391">Comparison of three typical statistical distributions used for
damage function development. The points correspond to the observed data and
lines the different statistical distributions.</p></caption>
        <?xmltex \hack{\hsize\textwidth}?>
        <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/345/2022/nhess-22-345-2022-f10.png"/>

      </fig>

<?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S2.T4"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{B1}?><label>Table B1</label><caption><p id="d1e2406">Goodness-of-fit indices for the gamma, log-normal, and generalized
normal statistical distributions. The best fits for flow-only parameters are
indicated in bold, and the best fits for flow-plus-wave parameters are
indicated in bold italic.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.97}[.97]?><oasis:tgroup cols="10">
     <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" colsep="1"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <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:colspec colnum="10" colname="col10" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Variable</oasis:entry>
         <oasis:entry rowsep="1" namest="col2" nameend="col4" align="center" colsep="1">RMSE (m) </oasis:entry>
         <oasis:entry rowsep="1" namest="col5" nameend="col7" align="center" colsep="1"><inline-formula><mml:math id="M69" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry rowsep="1" namest="col8" nameend="col10" align="center">RRSE </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Gamma</oasis:entry>
         <oasis:entry colname="col3">Log normal</oasis:entry>
         <oasis:entry colname="col4">GNO</oasis:entry>
         <oasis:entry colname="col5">Gamma</oasis:entry>
         <oasis:entry colname="col6">Log normal</oasis:entry>
         <oasis:entry colname="col7">GNO</oasis:entry>
         <oasis:entry colname="col8">Gamma</oasis:entry>
         <oasis:entry colname="col9">Log normal</oasis:entry>
         <oasis:entry colname="col10">GNO</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Water depth (<inline-formula><mml:math id="M70" display="inline"><mml:mi mathvariant="normal">h</mml:mi></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.1574</oasis:entry>
         <oasis:entry colname="col3">0.2290</oasis:entry>
         <oasis:entry colname="col4"><bold>0.1495</bold></oasis:entry>
         <oasis:entry colname="col5">0.8256</oasis:entry>
         <oasis:entry colname="col6">0.7722</oasis:entry>
         <oasis:entry colname="col7"><bold>0.8328</bold></oasis:entry>
         <oasis:entry colname="col8">0.0949</oasis:entry>
         <oasis:entry colname="col9">0.1381</oasis:entry>
         <oasis:entry colname="col10"><bold>0.0902</bold></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Flow speed (<inline-formula><mml:math id="M71" display="inline"><mml:mi mathvariant="normal">v</mml:mi></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.2306</oasis:entry>
         <oasis:entry colname="col3">0.2802</oasis:entry>
         <oasis:entry colname="col4"><bold>0.2234</bold></oasis:entry>
         <oasis:entry colname="col5">0.6180</oasis:entry>
         <oasis:entry colname="col6">0.6087</oasis:entry>
         <oasis:entry colname="col7"><bold>0.6406</bold></oasis:entry>
         <oasis:entry colname="col8">0.1390</oasis:entry>
         <oasis:entry colname="col9">0.1690</oasis:entry>
         <oasis:entry colname="col10"><bold>0.1347</bold></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Unit discharge (<inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.2150</oasis:entry>
         <oasis:entry colname="col3">0.2440</oasis:entry>
         <oasis:entry colname="col4"><bold>0.2120</bold></oasis:entry>
         <oasis:entry colname="col5">0.6704</oasis:entry>
         <oasis:entry colname="col6"><bold>0.7244</bold></oasis:entry>
         <oasis:entry colname="col7">0.6744</oasis:entry>
         <oasis:entry colname="col8">0.1296</oasis:entry>
         <oasis:entry colname="col9">0.1471</oasis:entry>
         <oasis:entry colname="col10"><bold>0.1278</bold></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Flow momentum flux (<inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2"><bold>0.1790</bold></oasis:entry>
         <oasis:entry colname="col3">0.2341</oasis:entry>
         <oasis:entry colname="col4">0.1822</oasis:entry>
         <oasis:entry colname="col5"><bold>0.7686</bold></oasis:entry>
         <oasis:entry colname="col6">0.7591</oasis:entry>
         <oasis:entry colname="col7">0.7622</oasis:entry>
         <oasis:entry colname="col8"><bold>0.1079</bold></oasis:entry>
         <oasis:entry colname="col9">0.1412</oasis:entry>
         <oasis:entry colname="col10">0.1099</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Significant wave height (<inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.1719</oasis:entry>
         <oasis:entry colname="col3">0.2888</oasis:entry>
         <oasis:entry colname="col4"><bold><italic>0.1600</italic></bold></oasis:entry>
         <oasis:entry colname="col5">0.7987</oasis:entry>
         <oasis:entry colname="col6">0.6065</oasis:entry>
         <oasis:entry colname="col7"><bold><italic>0.8066</italic></bold></oasis:entry>
         <oasis:entry colname="col8">0.1037</oasis:entry>
         <oasis:entry colname="col9">0.1742</oasis:entry>
         <oasis:entry colname="col10"><bold><italic>0.0965</italic></bold></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Total water depth (<inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sig</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.1604</oasis:entry>
         <oasis:entry colname="col3">0.2453</oasis:entry>
         <oasis:entry colname="col4"><bold><italic>0.1522</italic></bold></oasis:entry>
         <oasis:entry colname="col5">0.8195</oasis:entry>
         <oasis:entry colname="col6">0.7582</oasis:entry>
         <oasis:entry colname="col7"><bold><italic>0.8265</italic></bold></oasis:entry>
         <oasis:entry colname="col8">0.0967</oasis:entry>
         <oasis:entry colname="col9">0.1479</oasis:entry>
         <oasis:entry colname="col10"><bold><italic>0.0918</italic></bold></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Wave energy flux (<inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">0.2522</oasis:entry>
         <oasis:entry colname="col3">0.2601</oasis:entry>
         <oasis:entry colname="col4"><bold><italic>0.2307</italic></bold></oasis:entry>
         <oasis:entry colname="col5">0.5774</oasis:entry>
         <oasis:entry colname="col6"><bold><italic>0.7130</italic></bold></oasis:entry>
         <oasis:entry colname="col7">0.6510</oasis:entry>
         <oasis:entry colname="col8">0.1521</oasis:entry>
         <oasis:entry colname="col9">0.1568</oasis:entry>
         <oasis:entry colname="col10"><bold><italic>0.1391</italic></bold></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Total force <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:mfenced close=")" open="("><mml:mrow><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>h</mml:mi><mml:msup><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><bold><italic>0.1462</italic></bold></oasis:entry>
         <oasis:entry colname="col3">0.2318</oasis:entry>
         <oasis:entry colname="col4">0.1499</oasis:entry>
         <oasis:entry colname="col5"><bold><italic>0.8410</italic></bold></oasis:entry>
         <oasis:entry colname="col6">0.7713</oasis:entry>
         <oasis:entry colname="col7">0.8387</oasis:entry>
         <oasis:entry colname="col8"><bold><italic>0.0882</italic></bold></oasis:entry>
         <oasis:entry colname="col9">0.1398</oasis:entry>
         <oasis:entry colname="col10">0.0904</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

<?xmltex \hack{\clearpage}?>
</app>
  </app-group><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e2918">Data will be available after publication on the data repository of TU Delft
at <ext-link xlink:href="https://doi.org/10.4121/16713340" ext-link-type="DOI">10.4121/16713340</ext-link> (Diaz Loaiza, 2022) as the AXA Xynthia storm research
project.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e2927">The present paper is based on the postdoctoral research of MADL on the research project INFRA. MADL, JB, RM, TD, and RR
conceptualized the study and maintained meetings of progress for the
project. MADL made the calculations and wrote the manuscript. JB and SJ
provided repeated feedback on the manuscript.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e2933">The contact author has declared that neither they nor their co-authors have any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e2939">Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e2945">This work is funded by the AXA Joint Research Initiative (JRI) project
INFRA: Integrated Flood Risk Assessment. A special acknowledgement is due to Adri Mourits from Deltares for the help provided with the Delft3D debugging and to
Christopher Lashley for the help during the field trip in Île de Ré and
surroundings during August 2020.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e2950">This research has been supported by the AXA Research Fund (AXA Joint Research Initiative (JRI) project INFRA: Integrated Flood Risk Assessment).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e2957">This paper was edited by Sven Fuchs and reviewed by Bret Webb and two anonymous referees.</p>
  </notes><ref-list>
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