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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">
  <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-22-3725-2022</article-id><title-group><article-title>Multi-hazard analysis of flood and tsunamis on the western Mediterranean coast of Turkey</article-title><alt-title>Multi-hazard analysis of flood and tsunamis</alt-title>
      </title-group><?xmltex \runningtitle{Multi-hazard analysis of flood and tsunamis}?><?xmltex \runningauthor{C. Yavuz et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Yavuz</surname><given-names>Cuneyt</given-names></name>
          <email>cuneyt.yavuz@dpu.edu.tr</email>
        <ext-link>https://orcid.org/0000-0001-9767-7234</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Yilmaz</surname><given-names>Kutay</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Onder</surname><given-names>Gorkem</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Department of Construction Technologies, Technical Sciences Vocational
School, Dumlupinar University, <?xmltex \hack{\break}?>43000, Kutahya, Turkey</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>ALTER International Engineering Inc. Co., 06800, Ankara, Turkey</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Sumodel Engineering Inc. Co., 06800, Ankara, Turkey</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Cuneyt Yavuz (cuneyt.yavuz@dpu.edu.tr)</corresp></author-notes><pub-date><day>21</day><month>November</month><year>2022</year></pub-date>
      
      <volume>22</volume>
      <issue>11</issue>
      <fpage>3725</fpage><lpage>3736</lpage>
      <history>
        <date date-type="received"><day>12</day><month>April</month><year>2022</year></date>
           <date date-type="rev-request"><day>9</day><month>June</month><year>2022</year></date>
           <date date-type="rev-recd"><day>20</day><month>October</month><year>2022</year></date>
           <date date-type="accepted"><day>3</day><month>November</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Cuneyt Yavuz et al.</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/22/3725/2022/nhess-22-3725-2022.html">This article is available from https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022.html</self-uri><self-uri xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022.pdf">The full text article is available as a PDF file from https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e114">Flooding has always been a devastating hazard for social and
economic assets and activities. Especially, lowland areas such as coastal
regions can be more vulnerable to inundations. The combination of different
natural hazards observed at the same time is definitely worsening the
situation in the affected regions. The goal of this study is to conduct a
distinctive multi-hazard analysis considering flood hazards with the
contribution of potential earthquake-triggered tsunamis that might be
observed throughout the Fethiye coastline and city center. For this purpose,
tsunami hazard curves are generated based on Monte Carlo simulations.
Comprehensive stochastic hazard analyses are performed considering the
aleatory variability of earthquake-triggered tsunamis and epistemic
uncertainty of floods having 10-, 50-, and 100-year return periods. Numerical
simulations are conducted to combine the potential tsunamis and flood events
that are able to adversely affect the selected region. The results of this
study show that the blockage of stream outlets due to tsunami waves
drastically increases the inundated areas and worsens the condition for the
selected region.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

      <?xmltex \hack{\allowdisplaybreaks}?>
<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e128">Flood hazards have been one of the most destructive and frequent global-wide
natural hazards resulting in loss of lives, livestock, and economic assets
(Slater and Villarini, 2016; Alfieri et al., 2017; Kreibich et al., 2017;
Qiang, 2019; Zhai et al., 2020). Even though lowland and plain areas where
80 % of the world population live can create an easy way for urbanization,
they also vulnerable to flood risk, and the hazardous effects of floods will
increase in the future due to the changing hydrological cycle in recent
years (Lamond et al., 2011). As the number of flood hazards increases, the
amount of flood losses are going to follow a parallel trend, accordingly.
Hemmati et al. (2020) stated that both the number of floods and destructive
economic results have been drastically increased since the 1990s. Munich RE (2020) has compiled a natural catastrophe loss database on natural disasters
since 1980s for analyzing and assessing losses resulting from natural
disasters. The database reveals that number of floods and their destructive
economic results have an upward trend at a global scale.</p>
      <p id="d1e131">Independently of flood hazard, the tsunami, which can be a long- or short-term
event, is rare but can cause catastrophic damage to economic and social
assets and activities (Wolfgang, 2005; Kundzewicz et al., 2017; Subyani et
al., 2017; Fukao, 1979). Devastating economic losses and loss of lives have
been recorded for the countries that experienced tsunami events, especially
for the last 2 decades (Nadim and Glade, 2006; Carreño et al., 2007;
Cardona et al., 2010; Sørensen et al., 2012; Lane et al., 2013; Horspool
et al., 2014; Goda and Abilova, 2016). Scientists have revealed significant
and reliable hazard evaluation methods for tsunami hazard assessment
according to adverse consequences of the experienced tsunamis (Jelínek
et al., 2012).</p>
      <p id="d1e134">Multi-hazard assessment of floods with different natural hazards can be
found in the literature. For instance, climate-change-related flood hazard
assessment has been widely investigated (Blöschl et al., 2017; Skougaard Kaspersen
et al., 2017; Szewrański et al., 2018; Carter et al., 2018; Barkey et
al., 2019; Yavuz et. al., 2020b). However, the investigations covering simultaneous assessment of
flood and tsunami events have been limited. Even if the coincidence of flood
and tsunami hazards may be experienced once in a blue moon, it should also
be investigated due to the uncertainty in the time of occurrence of these
natural hazards. The objective of this study is to reveal a statistical
methodology to evaluate the aggregate potential hazard levels due to flood
hazards with the presence of earthquake-triggered tsunamis.</p>
      <p id="d1e137">As commonly used issues in stochastic hazard analysis of any kind of hazard
in the literature (Bommer, 2003; Helton et al., 2010), aleatory and
epistemic uncertainties are considered to generate multi-hazard analysis in
this study. The exceedance of flood hazard is strongly likely depending on
geological and meteorological circumstances; the hazard is included in the
stochastic analyses conducted in this study as epistemic uncertainty. Since
the occurrence of the tsunami is generally rare compared with flood hazards,
tsunami events are inspected by considering aleatory variability in this
study. Additionally, hypothetical earthquake magnitudes <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are
generated using Monte Carlo simulations to obtain a required number of
random earthquake sources in the bathymetry.</p>
      <p id="d1e152">The proposed methodology is applied to Fethiye city center, which is one of
the most popular touristic destinations on the Western Mediterranean coast
of Turkey. The selection of this site is based on the documented seven tsunami
events throughout history and evidence of tsunami deposits found by researchers (Cita and Rimoldi, 1997; Papadopoulos, 2009; Altinok et al.,
2011) around Fethiye Bay. The Fethiye coastline was hit several times with
destructive tsunami waves reaching up to 1.8 m, and significant inundation
distances were recorded (Papadopoulos, 2009). The location of the study area for
the case study is shown in Fig. 1.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e157">Study area and its location on satellite image (sources:
Esri, Maxar, GeoEye, Earthstar Geographics, CNES/Airbus DS, USDA, USGS,
AeroGRID, IGN, and the GIS User Community).</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f01.jpg"/>

      </fig>

<?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Materials and methods</title>
      <p id="d1e176">The probabilistic multi-hazard assessment approach is applied in this study. In doing so, the aim is to evaluate the two dynamic natural hazards one by one
and simultaneously. In total, 523 historical earthquakes recorded between 1900–2013
are retrieved from the European Union-funded “Tsunami risk and strategies for the
European region” (TRANSFER Project, 2022) project catalogue. The Gutenberg–Richter
relationship is used to determine the best-fitted distribution for the
historical earthquake magnitudes. The Gutenberg–Richter relationship is a
mathematical expression of the relationship between a number of earthquakes
and the Richter magnitudes (<inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) of these earthquakes that occurred in a
specific region (Gutenberg and Richter, 1954). They proposed a widely
accepted and commonly used empirical equation that explains the relationship
between the occurrence probability of an earthquake depending on two seismic
constants (i.e., <inline-formula><mml:math id="M3" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M4" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> values) which define the frequency-magnitude
distribution and the Richter magnitudes experienced in a particular region.
The equation is defined as follows:
          <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M5" display="block"><mml:mrow><mml:mi>log⁡</mml:mi><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mi>b</mml:mi><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mi>a</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
        where <inline-formula><mml:math id="M6" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> is the number of earthquakes experienced in the selected region, and <inline-formula><mml:math id="M7" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula>
and <inline-formula><mml:math id="M8" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> are the constants that are defined specifically for the selected region.</p>
      <p id="d1e253">Tsunami hazard curves are generated based on the hypothetical earthquake
magnitudes (<inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) produced from 100 000 Monte Carlo simulations. The NAMI DANCE software is used to simulate hypothetical earthquakes having <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">6.5</mml:mn></mml:mrow></mml:math></inline-formula> (USGS, 2022) and the resulting tsunami wave heights are
computed at the coast of Fethiye city center.</p>
      <p id="d1e282">Flood hazards having recurrence periods of 10, 50, and 100 years
(<inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">100</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) on the other hand is modeled by MIKE 11, MIKE
21 FM, and MIKE Flood considered with and without tsunami wave existence at
the coasts (DHI, 2016a, b). As a more frequent flood period, <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is
evaluated in detail and hazard maps are generated for the flood events
having return periods of 50 years (<inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and 100 years (<inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">100</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). Additionally, tsunami-drifted flood hazard levels are also
provided for all three flood events to satisfy the multi-hazard assessment
procedure presented in this study. Thus, hazard levels considering both
flood, earthquake-triggered tsunami, and tsunami-drifted flood hazards can
be compared for the selected region. The inundation levels presented in this
study have resulted from the numerical analysis of both hazards.
Potential hazard that can result from seismicity are not within the scope
of this study. The flowchart of the methodology used in this study is
illustrated in 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="d1e355">Multi-hazard assessment framework used in this study.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f02.png"/>

      </fig>

<?xmltex \hack{\newpage}?>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Generation of hypothetical earthquakes</title>
      <p id="d1e373">Random <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values are generated using Monte Carlo simulation; also known as
stochastic modeling, it is accepted as one of the most flexible and easiest
methods to implement probabilistic hazard analysis (Ferson, 1996).
Probability density function is defined for <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, which is defined as the
independent parameter of the earthquake. Normal distribution is assigned to
<inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> depending on the probability density function. A Kolmogorov–Smirnov
test is applied to the assigned distribution to test the goodness of fit via
<inline-formula><mml:math id="M20" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value. The feasibility of <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> data production is satisfied by conducting
100 000 Monte Carlo simulations. Sufficiency of the generated data and the
consistency of normal distribution are inspected using a Gutenberg–Richter
relationship. For Fethiye Bay, the <inline-formula><mml:math id="M22" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M23" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> values used in the
Gutenberg–Richter relationship are obtained from Pamukçu et al. (2021)
as 4.6624 and 0.8644, respectively. The <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:mi>Q</mml:mi><mml:mo>-</mml:mo><mml:mi>Q</mml:mi></mml:mrow></mml:math></inline-formula> plot obtained from the Gutenberg–Richter
relationship for the study area is illustrated in Fig. 3. For the moment
magnitudes greater than 6.0 illustrated in Fig. 3, the normal distribution
has a good coincidence with the Gutenberg–Richter relation.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F3"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e456"><inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:mi>Q</mml:mi><mml:mo>-</mml:mo><mml:mi>Q</mml:mi></mml:mrow></mml:math></inline-formula> plot of <inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for Gutenberg–Richter law and the
normal distribution.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f03.png"/>

        </fig>

      <p id="d1e487"><?xmltex \hack{\newpage}?>Three different tsunami hazards curve samples that are derived from 100 000 Monte
Carlo simulations are used to determine the reliability of Monte Carlo
simulations by considering the aleatory variability of each hypothetical
earthquake magnitude by checking the consistency of the curves. The curve
samples are shown as Sample_1, Sample_2, and
Sample_3 in Fig. 4.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e494">Tsunami hazard curve samples derived from 100 000 Monte
Carlo simulations.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f04.png"/>

        </fig>

      <p id="d1e503">The coincidence between the randomly generated <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> shows that 100 000 Monte
Carlo simulations are sufficient up to 10<inline-formula><mml:math id="M28" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> per year annual exceedance of
the tsunamigenic earthquake. As clearly stated in the literature,
earthquakes having <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">6.5</mml:mn></mml:mrow></mml:math></inline-formula> can be considered tsunamigenic earthquakes
(USGS, 2022). Depending on this statement, 1561 out of 100 000 randomly
generated <inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values have a magnitude greater than 6.5 and are regarded as a tsunamigenic earthquake in this study. The generation steps of the
hypothetical earthquake sources are given in Fig. 5.</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="d1e557">Generation steps of the hypothetical earthquake sources.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f05.png"/>

        </fig>

      <p id="d1e566">The calculation procedure of the parameters of the hypothetical earthquake
is explained. The fault length (<inline-formula><mml:math id="M31" display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula>) of the hypothetical
earthquake is calculated using the following equation (Takemura, 1998):

                <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M32" 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 class="stylechange" displaystyle="true"/><mml:mi>log⁡</mml:mi><mml:mi>L</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.91</mml:mn><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mi mathvariant="normal">for</mml:mi><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">6.8</mml:mn><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 displaystyle="true" class="stylechange"/><mml:mi>log⁡</mml:mi><mml:mi>L</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.75</mml:mn><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3.77</mml:mn><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mi mathvariant="normal">for</mml:mi><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">6.8</mml:mn><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula></p>
      <p id="d1e661">The fault width (<inline-formula><mml:math id="M33" display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula>) can then be calculated using the simple equation given
for the rupture area (<inline-formula><mml:math id="M34" display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula>) as <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mi>W</mml:mi><mml:mo>=</mml:mo><mml:mi>S</mml:mi><mml:mo>/</mml:mo><mml:mi>L</mml:mi></mml:mrow></mml:math></inline-formula>. Displacement (<inline-formula><mml:math id="M36" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>) is also calculated using
the empirical equation provided by Hanks and Kanamori (1979):</p>
      <p id="d1e702"><disp-formula specific-use="gather" content-type="numbered"><mml:math id="M37" display="block"><mml:mtable displaystyle="true"><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>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">3</mml:mn><mml:mi>log⁡</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>-</mml:mo><mml:mn mathvariant="normal">10.7</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E5"><mml:mtd><mml:mtext>5</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>M</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>L</mml:mi><mml:mi>W</mml:mi><mml:mi>D</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where <inline-formula><mml:math id="M38" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> is the shear modulus of crust (<inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.43</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">10</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> N m<inline-formula><mml:math id="M40" 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>).</p>
      <p id="d1e803">In this study, the asperity position of the hypocenter is assumed to be at
the center of the fault, and hypocenter distances are directly obtained from
the historical earthquake dataset. In some circumstances, hypocenter
distances are smaller than the calculated <inline-formula><mml:math id="M41" display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula> values. This phenomenon causes
some problematic solutions. To prevent this kind of miscalculations, dip
angles are randomly assigned as 30, 60, and 90<inline-formula><mml:math id="M42" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> to the
grouped hypocenter distances considering the <inline-formula><mml:math id="M43" display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula> values as well. The rest of
the parameters are obtained directly from a sampled historical earthquake
from the catalogue. The locations of the historical earthquakes are randomly
assigned as the epicenters of the hypothetical earthquakes and are
illustrated in Fig. 6. Then, these earthquake sources are simulated and
tsunami wave heights along the coast of Fethiye, Turkey, are computed by the NAMI DANCE software (Zaytsev et al., 2019).</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F6"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e831">Historical earthquake locations that are used as the
epicenters of the hypothetical earthquakes (sources: Esri, Maxar, GeoEye,
Earthstar Geographics, CNES/Airbus DS, USDA, USGS, AeroGRID, IGN, and the
GIS User Community).</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f06.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Tsunami simulations</title>
      <p id="d1e848">Overall, 100 000 earthquake magnitudes are generated via Monte Carlo simulations and
1561 hypothetical earthquake sources having <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">6.5</mml:mn></mml:mrow></mml:math></inline-formula> are compiled to
evaluate the flood and tsunami hazards simultaneously for the selected
region based on the suggested framework by Yavuz et al. (2020a). The bathymetry
of the study area has a 407 m grid size, and is retrieved from the <italic>General bathymetric chart of the oceans</italic> (GEBCO, 2022). The NAMI DANCE software that runs
the continuity and momentum equations as shallow-water equations is used to
perform tsunami simulations to compute the tsunami wave height (<inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) at
the coast of Fethiye, Turkey. The shallow-water equations are expressed as
follows (Velioglu et al., 2016):

                <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M46" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E6"><mml:mtd><mml:mtext>6</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi mathvariant="italic">η</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>M</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>y</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E7"><mml:mtd><mml:mtext>7</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mtable class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>M</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mo>∂</mml:mo><mml:mrow><mml:mo>∂</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msup><mml:mi>M</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow><mml:mi>D</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mo>∂</mml:mo><mml:mrow><mml:mo>∂</mml:mo><mml:mi>y</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>M</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mi>D</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>+</mml:mo><mml:mi>g</mml:mi><mml:mi>D</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi mathvariant="italic">η</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>g</mml:mi><mml:msup><mml:mi>n</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow><mml:mrow><mml:msup><mml:mi>D</mml:mi><mml:mrow><mml:mn mathvariant="normal">7</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>M</mml:mi><mml:msqrt><mml:mrow><mml:msup><mml:mi>M</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mi>N</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E8"><mml:mtd><mml:mtext>8</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mo>∂</mml:mo><mml:mrow><mml:mo>∂</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>M</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mi>D</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mo>∂</mml:mo><mml:mrow><mml:mo>∂</mml:mo><mml:mi>y</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msup><mml:mi>N</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow><mml:mi>D</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>+</mml:mo><mml:mi>g</mml:mi><mml:mi>D</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi mathvariant="italic">η</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>y</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>g</mml:mi><mml:msup><mml:mi>n</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow><mml:mrow><mml:msup><mml:mi>D</mml:mi><mml:mrow><mml:mn mathvariant="normal">7</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>N</mml:mi><mml:msqrt><mml:mrow><mml:msup><mml:mi>M</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mi>N</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E9"><mml:mtd><mml:mtext>9</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi>M</mml:mi><mml:mo>=</mml:mo><mml:mi>u</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:mi>h</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="italic">η</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mi>u</mml:mi><mml:mi>D</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E10"><mml:mtd><mml:mtext>10</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mi>v</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>h</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="italic">η</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mi>v</mml:mi><mml:mi>D</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where <inline-formula><mml:math id="M47" display="inline"><mml:mi mathvariant="italic">η</mml:mi></mml:math></inline-formula> is the disturbance at the sea surface due to fault
displacement, <inline-formula><mml:math id="M48" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> is time, <inline-formula><mml:math id="M49" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M50" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> are the horizontal axes on the sea
surface, <inline-formula><mml:math id="M51" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> is Manning's roughness coefficient, <inline-formula><mml:math id="M52" display="inline"><mml:mi>M</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M53" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> are the
discharge fluxes, <inline-formula><mml:math id="M54" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> is the total sea depth, <inline-formula><mml:math id="M55" display="inline"><mml:mi>g</mml:mi></mml:math></inline-formula> is the gravitational
acceleration, <inline-formula><mml:math id="M56" display="inline"><mml:mi>u</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M57" display="inline"><mml:mi>v</mml:mi></mml:math></inline-formula> are the water particle velocities, and <inline-formula><mml:math id="M58" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula> is the
undisturbed sea depth. The NAMI DANCE software has the capability to compute
generation, propagation, and amplification of tsunami waves using the
shallow-water equations given above (Velioglu et al., 2016).</p>
      <p id="d1e1352">In this study, tsunami wave amplification cannot be calculated due to the
coarse grid size of the bathymetry. Therefore, a commonly used empirical
equation proposed by Green (Synolakis, 1991; Løvholt et al., 2012, 2014;
Yavuz et al., 2020a) is used to calculate <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> at 1 m water depth at the
coast. To apply the equation, a gauge is digitized at 50 m water depth and
Green's law (Synolakis, 1991) is used to calculate <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> at 1 m depth at
the coast of the selected region.
            <disp-formula id="Ch1.E12" content-type="numbered"><label>12</label><mml:math id="M61" display="block"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mroot><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mn mathvariant="normal">4</mml:mn></mml:mroot><mml:msub><mml:mi>d</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are the undisturbed water
depths at 50  and 1 m, respectively. <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the tsunami wave height
recorded at the digitized gauge point in the simulation. <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is used to
determine the additional flooded lands resulting from the simultaneous
occurrence of the flood and tsunami hazards in the selected regions. The
hypothetical earthquakes having annual exceedance probabilities of 10<inline-formula><mml:math id="M66" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> to 10<inline-formula><mml:math id="M67" 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> per year are regarded as the earthquakes that can
generate a tsunami at the Fethiye coastline. It is known that a tsunami has
a wave period of a couple of minutes, while the river flood could be much
longer. However, it should be noted here that tsunami hazard is assumed to occur at the time of fully developed flood hazard condition in this
study. By doing so, <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is considered only as a water level at the
downstream boundary condition; it neither changes with time nor with the water
levels at the river mouths. Flood hazard analyses are conducted for the
discharge having a recurrence period of 10 years (<inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
flood discharge is selected due to its higher chance of coincidence with a
probable tsunami event than other commonly used flood periods in the
literature. Thus, there is a coincidence of the combination of these two hazards
changes from 10<inline-formula><mml:math id="M71" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> to 10<inline-formula><mml:math id="M72" 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> per year.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Hydrodynamic modeling and quantification of flood hazard</title>
      <p id="d1e1549">Fluvial hazards resulting from water level rise in the river and
overflow onto the neighboring lands are also evaluated considering three
different return periods with and without the presence of
earthquake-triggered tsunamis. We conducted 1D and 2D hydraulic modeling of the streams
within the Fethiye city center by implementing MIKE 11, MIKE
21 FM, and MIKE Flood, widely accepted and used software for simulating
hydraulic engineering problems (DHI, 2016a, b).</p>
      <p id="d1e1552">Firstly, 1D numerical modeling is conducted by MIKE 11, which solves Saint
Venant's equations (DHI, 2016b). For this purpose, the physical conditions of
each stream are determined by field trips. By using the Nivelman GPS device,
the layout of cross-sections is determined at every 100 m for each stream.
Moreover, the dimensions and locations of culverts or inline structures are
determined in the field. Therefore, obtained data from the field are
entered into MIKE 11 to represent the real physical conditions of the study
area. Finally, a 1D numerical model via MIKE 11 is conducted and areas prone
to flooding are determined by considering the bank elevations and water
levels within each cross-section.</p>
      <p id="d1e1555">After having implemented the 1D numerical model, it is able to conclude that
there is a possibility of flooding within Fethiye city center.
Therefore, the MIKE 21 FM model is implemented for the area of the city center.
MIKE 21 is widely used software for modeling free-surface flows (DHI, 2016b).
The software solves shallow-water equations which are incompressible
Reynolds-averaged Navier–Stokes equations (DHI, 2016b). Excess discharge
within the streambed (1D model) is released from the river banks and
released to the surface; thus a numerical solution of surface water flows is
implemented by MIKE 21. For this purpose, a digital elevation model (DEM) of
the area with a resolution of 1 m is obtained from Fethiye Municipality. The
DEM of the project area is illustrated in Fig. 7.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e1561">Demonstration of the DEM of study area (sources: Esri,
Maxar, GeoEye, Earthstar Geographics, CNES/Airbus DS, USDA, USGS, AeroGRID,
IGN, and the GIS User Community).</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f07.png"/>

        </fig>

      <p id="d1e1570">Both the 1D model and 2D model are coupled via the MIKE Flood software; thus,
excess discharge within the streambed is released from the banks of the
stream and the computational area is inundated. In order to solve the
surface flow, the computational domain is meshed with non-uniform
unstructured meshes. Moreover, the buildings and/or structures within the
computational area are digitized and implemented into the MIKE 21 model to
determine the area with fine meshes. The buildings within the computational
area are excluded from the meshing procedure by considering the building
elevations and possible inundation water levels. The result is provided by
solving 1D and 2D numerical models simultaneously. The stream network of the
selected region including Fethiye city center is presented in Fig. 8.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e1575">Stream network of the selected region (sources: Esri,
Maxar, GeoEye, Earthstar Geographics, CNES/Airbus DS, USDA, USGS, AeroGRID,
IGN, and the GIS User Community).</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f08.png"/>

        </fig>

      <p id="d1e1584">Throughout the simulations processes, input boundary conditions of each
stream are determined as the discharge of the 10-year recurrence interval
(<inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). The calculated <inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> discharges for each stream are tabulated
in Table 1 and are provided from the “Hydrology report” of the “Flood
management plan of Western Mediterranean Basin” which was prepared by the
General Directorate of Water Management of Turkey under the guidance of the “EU
flood directive 2007/60” and the “Water framework directive” (SYGM, 2022).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e1612">Peak discharges of the streams for
discharge of 10-year recurrence interval in the study area (SYGM, 2022).</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.99}[.99]?><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="left"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="center">Fethiye city center </oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Stream</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (m<inline-formula><mml:math id="M76" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M77" 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>)</oasis:entry>
         <oasis:entry colname="col3">Stream</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (m<inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M80" 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>)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Caybogazi</oasis:entry>
         <oasis:entry colname="col2">197.88</oasis:entry>
         <oasis:entry colname="col3">Kurtbeli_2</oasis:entry>
         <oasis:entry colname="col4">11.28</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kargi</oasis:entry>
         <oasis:entry colname="col2">32.93</oasis:entry>
         <oasis:entry colname="col3">Kurtbeli_3</oasis:entry>
         <oasis:entry colname="col4">4.56</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kurtbeli</oasis:entry>
         <oasis:entry colname="col2">24.44</oasis:entry>
         <oasis:entry colname="col3">Kurtbeli_4</oasis:entry>
         <oasis:entry colname="col4">10.16</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Kurtbeli_1</oasis:entry>
         <oasis:entry colname="col2">19.11</oasis:entry>
         <oasis:entry colname="col3">Susambeli</oasis:entry>
         <oasis:entry colname="col4">58.2</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Stream</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (m<inline-formula><mml:math id="M82" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M83" 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>)</oasis:entry>
         <oasis:entry colname="col3">Stream</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (m<inline-formula><mml:math id="M85" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M86" 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>)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Caybogazi</oasis:entry>
         <oasis:entry colname="col2">286.25</oasis:entry>
         <oasis:entry colname="col3">Kurtbeli_2</oasis:entry>
         <oasis:entry colname="col4">19.02</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kargi</oasis:entry>
         <oasis:entry colname="col2">50.95</oasis:entry>
         <oasis:entry colname="col3">Kurtbeli_3</oasis:entry>
         <oasis:entry colname="col4">5.56</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kurtbeli</oasis:entry>
         <oasis:entry colname="col2">45.15</oasis:entry>
         <oasis:entry colname="col3">Kurtbeli_4</oasis:entry>
         <oasis:entry colname="col4">20.32</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Kurtbeli_1</oasis:entry>
         <oasis:entry colname="col2">33.46</oasis:entry>
         <oasis:entry colname="col3">Susambeli</oasis:entry>
         <oasis:entry colname="col4">90.40</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Stream</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">100</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (m<inline-formula><mml:math id="M88" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M89" 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>)</oasis:entry>
         <oasis:entry colname="col3">Stream</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">100</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (m<inline-formula><mml:math id="M91" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M92" 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>)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Caybogazi</oasis:entry>
         <oasis:entry colname="col2">326.49</oasis:entry>
         <oasis:entry colname="col3">Kurtbeli_2</oasis:entry>
         <oasis:entry colname="col4">22.58</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kargi</oasis:entry>
         <oasis:entry colname="col2">59.38</oasis:entry>
         <oasis:entry colname="col3">Kurtbeli_3</oasis:entry>
         <oasis:entry colname="col4">10.39</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kurtbeli</oasis:entry>
         <oasis:entry colname="col2">55.60</oasis:entry>
         <oasis:entry colname="col3">Kurtbeli_4</oasis:entry>
         <oasis:entry colname="col4">25.80</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kurtbeli_1</oasis:entry>
         <oasis:entry colname="col2">40.53</oasis:entry>
         <oasis:entry colname="col3">Susambeli</oasis:entry>
         <oasis:entry colname="col4">105.20</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

      <p id="d1e2055">The downstream boundary condition for a discharge having 10-, 50-, and 100-
year return periods of each stream is determined as mean sea level.
Moreover, calibration of the hydraulic model cannot be accomplished due
to the lack of data. However, the most important parameter for calibrating
the hydraulic model is Manning's roughness coefficient. The surface
roughness coefficients are determined by considering CORINE 2018 Land Cover
data (Papaioannou et al., 2018). The computational area was classified
according to the land use classification of CORINE 2018 data as shown in
Fig. 9. Spatially varied roughness coefficients of the specific land cover
were implemented according to the study conducted by Papaioannou et al. (2018).</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><?xmltex \def\figurename{Figure}?><label>Figure 9</label><caption><p id="d1e2060">Land cover classification of computational domain
according to CORINE 2018 Data (sources: Esri, Maxar, GeoEye, Earthstar
Geographics, CNES/Airbus DS, USDA, USGS, AeroGRID, IGN, and the GIS User
Community).</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f09.png"/>

        </fig>

      <p id="d1e2069">Average Manning's surface roughness coefficients of each land cover of
CORINE 2018 data were presented by Papaioannou et al. (2018). The land cover
of the computational domain is constructed by examining the CORINE data, and
the roughness coefficients of each land cover are tabulated in Table 2.</p>

<?xmltex \floatpos{p}?><table-wrap id="Ch1.T2" specific-use="star"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e2075">Peak discharges of the streams for
discharge of 10-year recurrence interval in the study area (Papaioannou et
al., 2018).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Label 1</oasis:entry>
         <oasis:entry colname="col2">Label 2</oasis:entry>
         <oasis:entry colname="col3">Manning's <inline-formula><mml:math id="M93" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">1 Artificial surfaces</oasis:entry>
         <oasis:entry colname="col2">1.1 Urban fabric</oasis:entry>
         <oasis:entry colname="col3">0.013</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">1.2 Industrial, commercial, and transport units</oasis:entry>
         <oasis:entry colname="col3">0.013</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">1.3 Mine, dump, and construction sites</oasis:entry>
         <oasis:entry colname="col3">0.013</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">1.4 Artificial, non-agricultural vegetated areas</oasis:entry>
         <oasis:entry colname="col3">0.025</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">2 Agricultural areas</oasis:entry>
         <oasis:entry colname="col2">2.1 Arable land</oasis:entry>
         <oasis:entry colname="col3">0.030</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">2.2 Permanent crops</oasis:entry>
         <oasis:entry colname="col3">0.080</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">2.3 Pastures</oasis:entry>
         <oasis:entry colname="col3">0.035</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">2.4 Heterogenous agricultural areas</oasis:entry>
         <oasis:entry colname="col3">0.045</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">3 Forest and semi-natural areas</oasis:entry>
         <oasis:entry colname="col2">3.1 Forests</oasis:entry>
         <oasis:entry colname="col3">0.100</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">3.2 Scrub and/or herbaceous vegetation associations</oasis:entry>
         <oasis:entry colname="col3">0.040</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">3.3 Open spaces with little or no vegetation</oasis:entry>
         <oasis:entry colname="col3">0.025</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">4 Wetlands</oasis:entry>
         <oasis:entry colname="col2">4.1 Inland wetlands</oasis:entry>
         <oasis:entry colname="col3">0.040</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">4.2 Coastal wetlands</oasis:entry>
         <oasis:entry colname="col3">0.040</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">5 Waterbodies</oasis:entry>
         <oasis:entry colname="col2">5.1 Inland waters</oasis:entry>
         <oasis:entry colname="col3">0.050</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">5.2 Coastal waters</oasis:entry>
         <oasis:entry colname="col3">0.070</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e2285">After having carried out the hydraulic analysis, the result of the model is
also used for flood hazard quantification. Flood hazard quantification is
often conducted by considering water depth and velocity. Although there are
various methods for quantifying flood hazards, direct multiplication of
depth and velocity is suggested by Smith et al. (2014). The threshold values for each hazard class and vulnerability classification are tabulated
in Table 3 below (Smith et al., 2014).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><?xmltex \currentcnt{3}?><label>Table 3</label><caption><p id="d1e2292">Hazard classes and vulnerability
thresholds (Smith et al., 2014).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="3cm"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="6cm"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="2.5cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Hazard vulnerability<?xmltex \hack{\hfill\break}?>classification</oasis:entry>
         <oasis:entry colname="col2">Description</oasis:entry>
         <oasis:entry colname="col3">Classification limit    (m<inline-formula><mml:math id="M94" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M95" 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>)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">H1</oasis:entry>
         <oasis:entry colname="col2">Generally safe for vehicles, people, and building</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:mi>D</mml:mi><mml:mo>⋅</mml:mo><mml:mi>V</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">H2</oasis:entry>
         <oasis:entry colname="col2">Unsafe for small vehicles</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:mi>D</mml:mi><mml:mo>⋅</mml:mo><mml:mi>V</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">H3</oasis:entry>
         <oasis:entry colname="col2">Unsafe for vehicles, children, and the elderly</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:mi>D</mml:mi><mml:mo>⋅</mml:mo><mml:mi>V</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">H4</oasis:entry>
         <oasis:entry colname="col2">Unsafe for vehicles and people</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mi>D</mml:mi><mml:mo>⋅</mml:mo><mml:mi>V</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">H5</oasis:entry>
         <oasis:entry colname="col2">Unsafe for vehicles and people; all buildings vulnerable to structural damage</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:mi>D</mml:mi><mml:mo>⋅</mml:mo><mml:mi>V</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">4.0</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">H6</oasis:entry>
         <oasis:entry colname="col2">Unsafe for vehicles and people; all building vulnerable to failure</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:mi>D</mml:mi><mml:mo>⋅</mml:mo><mml:mi>V</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">4.0</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e2504">Water depth within the inundated area and flood propagation velocity are
both considered with and without the presence of an earthquake-triggered
tsunami. Therefore, spatially varied hazard maps are constructed
accordingly.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results and discussions</title>
      <p id="d1e2516">In this study, potential multi-hazard assessment because of the fluvial
flood hazard (<inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">100</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), with and without the presence of
earthquake-triggered tsunamis, is analyzed for Fethiye city center.
Inundated areas due to flood only, earthquake-triggered tsunami only, and
multi-hazard conditions (i.e., flood <inline-formula><mml:math id="M105" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> earthquake-triggered tsunami) are determined by
numerical computations, and corresponding inundation levels are revealed for
each hazard circumstance.</p>
      <p id="d1e2559">For all flood hazard events considered in this study, maximum water levels
are observed within the riverbed. The inundated area due to flood is limited
along the streamlines for inland sections. There are also small inundated
sections that can be observed due to flood in some parts of the coast of the
study area. A large portion of the coastal region is not affected by the
flood waves and the inundated area is limited in the coastal parts. A sample
inundation map of the study area is given in Fig. 10 for the flood of
<inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">100</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> obtained from the numerical computations.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F10"><?xmltex \currentcnt{10}?><?xmltex \def\figurename{Figure}?><label>Figure 10</label><caption><p id="d1e2597">Inundation due to flood hazards considered in the study
(sources: Esri, Maxar, GeoEye, Earthstar Geographics, CNES/Airbus DS, USDA,
USGS, AeroGRID, IGN, and the GIS User Community).</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f10.jpg"/>

      </fig>

      <p id="d1e2607">Although a water inundation level exceeding 6 m is observed on some parts of the Kurtbeli_1 stream, the effect of the <inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> flood is limited at
the coastline. Depending on the computation results, the other streams also
have small inundations around the riverbeds.</p>
      <p id="d1e2621">For the flood hazard having a 50-year return period, maximum water levels
are observed only within the riverbed again, but the inundated area is
slightly extended compared with the flood event having a return period of
10 years as expected. A large portion of the coastal region is not affected
by the flood waves, and the inundated area is limited in the coastal parts.</p>
      <p id="d1e2624">Depending on the simulation results, a flood hazard having a 100-year return
period generates maximum water levels within the riverbeds in the study
area. The inundated area due to flood is limited along the streamlines for
inland sections. There are also small inundated sections that can be
observed due to flood in some parts of the coast of the study area. A large
portion of the coastal region is not affected by the flood waves, and the
inundated area is limited in the coastal parts.</p>
      <p id="d1e2627">For the earthquake-triggered tsunami hazard conditions on the other hand, a significant portion of the coastline is estimated to be inundated with 3.5 m
tsunami wave heights (see Fig. 11). Compared to the flood hazard level,
earthquake-triggered tsunamis might have considerable inundation levels at
the coastline. Up to 1 km of land inwards from the coastline is estimated
to be inundated due to tsunami waves depending on the hypothetical
earthquake-triggered tsunami analysis.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11"><?xmltex \currentcnt{11}?><?xmltex \def\figurename{Figure}?><label>Figure 11</label><caption><p id="d1e2632">Inundation levels resulting from an earthquake-triggered
tsunami hazard (sources: Esri, Maxar, GeoEye, Earthstar Geographics,
CNES/Airbus DS, USDA, USGS, AeroGRID, IGN, and the GIS User Community).</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f11.png"/>

      </fig>

      <p id="d1e2642">On the other hand, the coastline of the study area is severely inundated due
to flood (<inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) which takes place slightly before tsunami peak waves
hit the coastal parts of the city. Although the maximum tsunami wave height
obtained from the simulations is around 3.50 m, the inundation level for the
multi-hazard conditions reaches up to 7.00 m for some parts of the low-lying
sections of the study area (see Fig. 12).</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F12"><?xmltex \currentcnt{12}?><?xmltex \def\figurename{Figure}?><label>Figure 12</label><caption><p id="d1e2658">Inundation levels obtained from the simultaneous
occurrence of fully developed flood <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and earthquake-triggered
tsunami hazards (sources: Esri, Maxar, GeoEye, Earthstar Geographics,
CNES/Airbus DS, USDA, USGS, AeroGRID, IGN, and the GIS User Community).</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f12.png"/>

      </fig>

      <p id="d1e2678">Even for the contribution of flood hazard having the shortest return period
(i.e., <inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> in the study, the multi-hazard inundation level reaches up
to 7.00 m. It will not be surprising that higher inundation levels are
definitely observed for multi-hazard assessment with <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">100</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
flood hazards.</p>
      <p id="d1e2716">Quantification of the flood hazard is also carried out for all three case
studies by considering the threshold values and classes given in Table 3
(Smith et al., 2014). The results of hazard quantification are presented for all
return periods in Fig. 13.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F13"><?xmltex \currentcnt{13}?><?xmltex \def\figurename{Figure}?><label>Figure 13</label><caption><p id="d1e2721">Spatially varied hazard mapping for <bold>(a)</bold> flood only for
<inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">100</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <bold>(b)</bold> multi-hazard condition (i.e., flood<inline-formula><mml:math id="M118" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>earthquake-triggered tsunami) (sources: Esri, Maxar, GeoEye,
Earthstar Geographics, CNES/Airbus DS, USDA, USGS, AeroGRID, IGN, and the
GIS User Community).</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/22/3725/2022/nhess-22-3725-2022-f13.jpg"/>

      </fig>

      <p id="d1e2778">According to the hazard vulnerability classification proposed by Smith et
al. (2014), all three flood events having different recurrence intervals
(i.e., 10, 50, and 100 years) fall into the H1 hazard class, which can generate
negligible adverse effects in some coastal parts of the city center. On the
other hand, the fully developed flood events for all three recurrence
intervals just after peak tsunami waves reach the coast resulted in
varying hazard classes of H1 to H6. It should be noted that the major
portion of the hazard is caused by the tsunami.</p>
      <p id="d1e2781">It can be seen from Fig. 13 that the inundated area is slightly enhanced
due to the rate of change in flood discharges coming from the rivers.
However, a huge portion of the hazard resulted from the effect of
earthquake-triggered tsunamis. It can also be estimated that the rate of
change in discharges coming from the rivers may also have some positive
effect on the reduction in the additional adverse effect of multi-hazard conditions,
due to encountered flows at the coastline.</p>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Conclusions</title>
      <p id="d1e2793">Fluvial flood hazards having different recurrence intervals and potential
earthquake-triggered tsunami hazards are simultaneously analyzed to evaluate
the height of inundation levels at the coastline of Fethiye Bay and Fethiye
city center. Results demonstrate that the majority of the increase in inundation
levels is due to tsunami hazard. However, it should be emphasized that
inundation levels are almost doubled in the presence of all flood hazard
events at the same time. In the analyses, it is assumed that a fully developed
fluvial flood takes place just after the peak tsunami waves hit the coastal
region. Therefore, sea levels are determined accordingly for the hydraulic
models.</p>
      <p id="d1e2796">Floods with 10-, 50-, and 100-year recurrence periods were taken into
consideration in the study and potential hazards are calculated. Although it
is more sophisticated to reduce the effects of tsunamis, the prevention of
floods as well as their consequences are a more common procedure. Thus,
combined risk analyses of multiple hazards should be taken into
consideration in order to reduce risks due to natural disasters.</p>
      <p id="d1e2799">In conclusion, the coincidence of flood and tsunami events might be very unlikely. But the combination of these two hazards definitely increases the inundation levels and corresponding disaster levels in the selected
region. Some other factors, such as seasonal changes in economic and social
aspects, the expansion of residential sites, proximity to the fault
zones, and climate change effects, should be taken into consideration in
combined risk analysis for future years.</p>
</sec>

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

      <p id="d1e2806">All raw data can be provided by the corresponding authors upon request.</p>
  </notes><?xmltex \hack{\newpage}?><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e2813">CY and KY planned the scope of the study. The methodology was prepared by CY. Numerical simulations were conducted by CY, KY, and GO. The paper draft was written by CY and KY. CY reviewed and edited the paper based on the reviewers' comments.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e2819">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e2825">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><notes notes-type="sistatement"><title>Special issue statement</title>

      <p id="d1e2831">This article is part of the special issue “Coastal hazards and hydro-meteorological extremes”. It is not associated with a conference.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e2837">The authors express their appreciation to Ahmet Cevdet Yalciner and
his colleagues for providing the NAMI DANCE software ver. 9.0 BETA for conducting tsunami simulations.</p></ack><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e2842">This paper was edited by Francisco Campuzano and reviewed by Lucy Bricheno and two anonymous referees.</p>
  </notes><ref-list>
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