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  <front>
    <journal-meta><journal-id journal-id-type="publisher">ESurf</journal-id><journal-title-group>
    <journal-title>Earth Surface Dynamics</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ESurf</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Earth Surf. Dynam.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2196-632X</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/esurf-8-471-2020</article-id><title-group><article-title>Measuring river planform changes from remotely sensed data – a Monte Carlo approach to assessing
the impact of spatially variable error</article-title><alt-title>Significance assessment of historical surficial planform changes in mid-sized rivers</alt-title>
      </title-group><?xmltex \runningtitle{Significance assessment of historical surficial planform changes in mid-sized rivers}?><?xmltex \runningauthor{T.~Jautzy et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Jautzy</surname><given-names>Timothée</given-names></name>
          <email>timothee.jautzy2@etu.unistra.fr</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Herrault</surname><given-names>Pierre-Alexis</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Chardon</surname><given-names>Valentin</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Schmitt</surname><given-names>Laurent</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7203-6032</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Rixhon</surname><given-names>Gilles</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Laboratoire Image, Ville, Environnement (LIVE UMR 7362), Université de Strasbourg, CNRS, ENGEES, ZAEU LTER, 3 rue de l'Argonne, 67083 Strasbourg, France</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Ecole Nationale du Génie de l'Eau et de l'Environnement de Strasbourg (ENGEES), CNRS, <?xmltex \hack{\break}?> 1 quai Koch, 67000 Strasbourg, France</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Timothée Jautzy (timothee.jautzy2@etu.unistra.fr)</corresp></author-notes><pub-date><day>3</day><month>June</month><year>2020</year></pub-date>
      
      <volume>8</volume>
      <issue>2</issue>
      <fpage>471</fpage><lpage>484</lpage>
      <history>
        <date date-type="received"><day>22</day><month>September</month><year>2019</year></date>
           <date date-type="rev-request"><day>5</day><month>November</month><year>2019</year></date>
           <date date-type="rev-recd"><day>22</day><month>April</month><year>2020</year></date>
           <date date-type="accepted"><day>29</day><month>April</month><year>2020</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2020 Timothée Jautzy et al.</copyright-statement>
        <copyright-year>2020</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://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020.html">This article is available from https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020.html</self-uri><self-uri xlink:href="https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020.pdf">The full text article is available as a PDF file from https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e125">Remotely sensed data from fluvial systems are extensively used to document historical planform changes.
However, geometric and delineation errors inherently associated with these data can result in poor or even misleading
interpretation of measured changes, especially rates of channel lateral migration. It is thus imperative to take into account a
spatially variable (SV) error affecting the remotely sensed data. In the wake of recent key studies using this SV error as
a level of detection, we introduce a new framework to evaluate the significance of measured channel migration. Going beyond
linear metrics (i.e. migration vectors between diachronic river centrelines), we assess significance through a channel polygon
method yielding a surficial metric (i.e. quantification of eroded, deposited, or eroded-then-deposited surfaces).</p>
    <p id="d1e128">Our study area is a mid-sized active wandering river: the lower Bruche, a <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> m wide tributary of the Rhine in eastern France.
Within our four test sub-reaches, the active channel is digitised using diachronic orthophotos (1950 and 1964), and the
SV error affecting the data is interpolated with an inverse-distance weighting (IDW) technique. The novelty of our approach arises from then
running Monte Carlo (MC) simulations to randomly translate active channels and propagate geometric and delineation errors
according to the SV error. This eventually leads to the computation of percentage of uncertainties associated with each of the
measured planform changes, which allows us to evaluate the
significance of the planform changes. In the lower Bruche, the uncertainty associated with the documented changes ranges from
15.8 % to 52.9 %.</p>
    <p id="d1e141">Our results show that (i) orthophotos are affected by a significant SV error; (ii) the latter strongly
affects the uncertainty of measured changes; and (iii) the significance of changes is dependent on both the magnitude and the
shape of the surficial changes.
Taking the SV error into account is strongly recommended even in orthorectified aerial photos,
especially in the case of mid-sized rivers (<inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> m width) and/or low-amplitude river planform changes (<inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M4" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>).
In addition to allowing detection of low-magnitude planform changes, our approach
is also transferable as we use well-established tools (IDW and MC): this opens new perspectives in the fluvial context
(e.g. multi-thread river channels) for robustly assessing surficial channel changes.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<?pagebreak page472?><sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e202">In a fluvial context, remotely sensed data provide spatial information on historical lateral dynamics of
river channels <xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx5 bib1.bibx6 bib1.bibx14 bib1.bibx15 bib1.bibx22" id="paren.1"/>. This is of crucial importance for creating a scientific framework
applicable to sustainable management
of hydrosystems, including river restoration <xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx42 bib1.bibx50" id="paren.2"/>. Aerial photographs
are thus commonly used to document and measure planform channel changes over a time period of at the most the last century in a wide variety of fluvial
settings. Requiring data co-registration and river bank digitisation, these planimetric studies often result in the
quantification of lateral migration rates <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx20 bib1.bibx30 bib1.bibx38" id="paren.3"><named-content content-type="pre">e.g.</named-content></xref>.</p>
      <p id="d1e216">However, two major sources of spatial uncertainty inherently compromise the robustness of these planimetric methods:
the delineation error due to digitisation of river banks <xref ref-type="bibr" rid="bib1.bibx10 bib1.bibx13 bib1.bibx14 bib1.bibx33 bib1.bibx53" id="paren.4"/>
and the geometric error due to data co-registration <xref ref-type="bibr" rid="bib1.bibx12 bib1.bibx18 bib1.bibx26 bib1.bibx41 bib1.bibx51" id="paren.5"/>.
Whatever the scope of the study and
the environmental context, these uncertainties must be assessed as accurately as possible <xref ref-type="bibr" rid="bib1.bibx7 bib1.bibx9 bib1.bibx36 bib1.bibx37" id="paren.6"/>.
Root mean square error (RMSE) has been
frequently used for this purpose over the past several decades to quantify the uniform geometric error affecting co-registered planimetric data (Table <xref ref-type="table" rid="Ch1.T1"/>).
<xref ref-type="bibr" rid="bib1.bibx24" id="text.7"/>, however, demonstrated that the RMSE approach was too simplistic because co-registered data are affected by
spatially variable (SV) geometric error. To test the impact of such error on the quantification of lateral migration, the SV error was used as a
SV level of detection (LoD): this approach allowed detecting 33 % of statistically significant changes (migrations) instead of only 24 % with the
RMSE/uniform-error approach <xref ref-type="bibr" rid="bib1.bibx24" id="paren.8"/>. The thorough review of <xref ref-type="bibr" rid="bib1.bibx9" id="text.9"/> reached the same conclusion: they
encouraged the generalisation of SV error assessment and also noted the potential need for testing SV-LoD on new metrics of
lateral migration, including areal metrics of surface change.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e243">Literature review of recent studies quantifying channel lateral migration using the channel polygon method (P) and/or the centreline trajectory method (T). x: error not assessed. U: use of a uniform error. SV: use of a spatially variable error.
The table is sorted by the mean width of the channel(s) studied. Bold font highlights the characteristics of this study.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="6">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Authors (year)</oasis:entry>
         <oasis:entry colname="col2">Lateral migration</oasis:entry>
         <oasis:entry colname="col3">Delineation</oasis:entry>
         <oasis:entry colname="col4">Geometric</oasis:entry>
         <oasis:entry colname="col5">Channel width</oasis:entry>
         <oasis:entry colname="col6">Erosion order of magnitude</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">metric</oasis:entry>
         <oasis:entry colname="col3">error  (m)</oasis:entry>
         <oasis:entry colname="col4">error  (m)</oasis:entry>
         <oasis:entry colname="col5">(m)</oasis:entry>
         <oasis:entry colname="col6">(<inline-formula><mml:math id="M5" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx8" id="text.10"/>
                </oasis:entry>
         <oasis:entry colname="col2">P/T</oasis:entry>
         <oasis:entry colname="col3">x</oasis:entry>
         <oasis:entry colname="col4">U: 1.0</oasis:entry>
         <oasis:entry colname="col5">1–12</oasis:entry>
         <oasis:entry colname="col6">/</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx17" id="text.11"/>
                </oasis:entry>
         <oasis:entry colname="col2">P</oasis:entry>
         <oasis:entry colname="col3">U: 1.0</oasis:entry>
         <oasis:entry colname="col4">x</oasis:entry>
         <oasis:entry colname="col5">15</oasis:entry>
         <oasis:entry colname="col6">4.4</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx25" id="text.12"/>
                </oasis:entry>
         <oasis:entry colname="col2">P/T</oasis:entry>
         <oasis:entry colname="col3">x</oasis:entry>
         <oasis:entry colname="col4">U: 0.8–1.8</oasis:entry>
         <oasis:entry colname="col5">10–20</oasis:entry>
         <oasis:entry colname="col6">/</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx24" id="text.13"/>
                </oasis:entry>
         <oasis:entry colname="col2">T</oasis:entry>
         <oasis:entry colname="col3">U: 2.0</oasis:entry>
         <oasis:entry colname="col4">SV: 0–5</oasis:entry>
         <oasis:entry colname="col5">15</oasis:entry>
         <oasis:entry colname="col6">/</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><bold>This study</bold></oasis:entry>
         <oasis:entry colname="col2"><bold>P</bold></oasis:entry>
         <oasis:entry colname="col3"><bold>U: 0.5</bold></oasis:entry>
         <oasis:entry colname="col4"><bold>SV: 0.3–1.9</bold></oasis:entry>
         <oasis:entry colname="col5"><bold>20</bold></oasis:entry>
         <oasis:entry colname="col6"><bold>0.6</bold></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx46" id="text.14"/>
                </oasis:entry>
         <oasis:entry colname="col2">P</oasis:entry>
         <oasis:entry colname="col3">x</oasis:entry>
         <oasis:entry colname="col4">U: 1.5</oasis:entry>
         <oasis:entry colname="col5">7–40</oasis:entry>
         <oasis:entry colname="col6">/</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx14" id="text.15"/>
                </oasis:entry>
         <oasis:entry colname="col2">P</oasis:entry>
         <oasis:entry colname="col3">U: 2.0</oasis:entry>
         <oasis:entry colname="col4">U: 1.4–4.5</oasis:entry>
         <oasis:entry colname="col5">30</oasis:entry>
         <oasis:entry colname="col6">0.03</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx44" id="text.16"/>
                </oasis:entry>
         <oasis:entry colname="col2">P</oasis:entry>
         <oasis:entry colname="col3">x</oasis:entry>
         <oasis:entry colname="col4">U: <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">30</oasis:entry>
         <oasis:entry colname="col6">0.03</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx20" id="text.17"/>
                </oasis:entry>
         <oasis:entry colname="col2">P</oasis:entry>
         <oasis:entry colname="col3">x</oasis:entry>
         <oasis:entry colname="col4">U: 3.5</oasis:entry>
         <oasis:entry colname="col5">35</oasis:entry>
         <oasis:entry colname="col6">/</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx9" id="text.18"/>
                </oasis:entry>
         <oasis:entry colname="col2">T</oasis:entry>
         <oasis:entry colname="col3">U: 1.4</oasis:entry>
         <oasis:entry colname="col4">SV: 0–10</oasis:entry>
         <oasis:entry colname="col5">45</oasis:entry>
         <oasis:entry colname="col6">/</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx48" id="text.19"/>
                </oasis:entry>
         <oasis:entry colname="col2">T</oasis:entry>
         <oasis:entry colname="col3">x</oasis:entry>
         <oasis:entry colname="col4">U: <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1.6</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">50</oasis:entry>
         <oasis:entry colname="col6">/</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx35" id="text.20"/>
                </oasis:entry>
         <oasis:entry colname="col2">P</oasis:entry>
         <oasis:entry colname="col3">x</oasis:entry>
         <oasis:entry colname="col4">U: 0.9–3.6</oasis:entry>
         <oasis:entry colname="col5">30–80</oasis:entry>
         <oasis:entry colname="col6">0.02</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx22" id="text.21"/>
                </oasis:entry>
         <oasis:entry colname="col2">T</oasis:entry>
         <oasis:entry colname="col3">x</oasis:entry>
         <oasis:entry colname="col4">U: 2.3</oasis:entry>
         <oasis:entry colname="col5">11.5–107.3</oasis:entry>
         <oasis:entry colname="col6">/</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx21" id="text.22"/>
                </oasis:entry>
         <oasis:entry colname="col2">T</oasis:entry>
         <oasis:entry colname="col3">x</oasis:entry>
         <oasis:entry colname="col4">U: 2.3–6.6</oasis:entry>
         <oasis:entry colname="col5">150; 50; 50; 15</oasis:entry>
         <oasis:entry colname="col6">/</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx28" id="text.23"/>
                </oasis:entry>
         <oasis:entry colname="col2">P</oasis:entry>
         <oasis:entry colname="col3">x</oasis:entry>
         <oasis:entry colname="col4">x</oasis:entry>
         <oasis:entry colname="col5">130</oasis:entry>
         <oasis:entry colname="col6">5.4</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                  <xref ref-type="bibr" rid="bib1.bibx38" id="text.24"/>
                </oasis:entry>
         <oasis:entry colname="col2">P/T</oasis:entry>
         <oasis:entry colname="col3">x</oasis:entry>
         <oasis:entry colname="col4">x</oasis:entry>
         <oasis:entry colname="col5">90–240</oasis:entry>
         <oasis:entry colname="col6">/</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e766">Both <xref ref-type="bibr" rid="bib1.bibx24" id="text.25"/> and <xref ref-type="bibr" rid="bib1.bibx9" id="text.26"/> developed a LoD for a linear metric (Fig. <xref ref-type="fig" rid="Ch1.F1"/>a) implemented in the Planform Statistics
Toolbox <xref ref-type="bibr" rid="bib1.bibx23" id="paren.27"/>, which reports fluvial planform changes as a linear adjustment. However, by conflating river banks onto a
unique centreline (Fig. <xref ref-type="fig" rid="Ch1.F1"/>a), a linear metric can oversimplify geomorphological changes. This approach can fail to detect observed lateral
adjustments when, for instance, channel widening or narrowing occurs without any significant lateral migration
of the centreline <xref ref-type="bibr" rid="bib1.bibx34 bib1.bibx45" id="paren.28"/>.
This is all the more relevant for mid-sized rivers (width <inline-formula><mml:math id="M8" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 30 m; <xref ref-type="bibr" rid="bib1.bibx11" id="author.29"/>, <xref ref-type="bibr" rid="bib1.bibx11" id="year.30"/>; Table <xref ref-type="table" rid="Ch1.T1"/>), which, along with their importance
in terms of river geomorphological management <xref ref-type="bibr" rid="bib1.bibx31" id="paren.31"/>, are particularly prone to be impacted by delineation and geometric errors <xref ref-type="bibr" rid="bib1.bibx22" id="paren.32"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><label>Figure 1</label><caption><p id="d1e810">Illustration of the lateral migration metric used <bold>(a)</bold> by <xref ref-type="bibr" rid="bib1.bibx24" id="text.33"/> and <xref ref-type="bibr" rid="bib1.bibx9" id="text.34"/> and
<bold>(b)</bold> in this study.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020-f01.png"/>

      </fig>

      <p id="d1e831">This study aims to advance the generalisation of SV error assessment methods in fluvial settings by testing its impact on the
quantification of lateral migration using a surficial metric: the channel polygon method (Fig. <xref ref-type="fig" rid="Ch1.F1"/>b). This
consists in the extraction of eroded, deposited, and eroded-then-deposited surfaces from overlaid diachronic channels. SV error is assessed in two
diachronic orthophotos of the lower Bruche (i.e. a mid-sized tributary of the Rhine), by spatial interpolation <xref ref-type="bibr" rid="bib1.bibx24" id="paren.35"/>
based on an independent set of ground control points <xref ref-type="bibr" rid="bib1.bibx18" id="paren.36"/>. The main novelty of our approach is running Monte Carlo (MC)
simulations <xref ref-type="bibr" rid="bib1.bibx32" id="paren.37"/> to propagate the geometric error in measurements of eroded and/or deposited surfaces.
This eventually allows computing the uncertainty associated with surficial changes, to which a threshold is applied to detect
non-significant planform changes.</p>
      <p id="d1e845">More specifically, this study tests three hypotheses in the fluvial context:
(1) orthophotos are affected by a locally significant SV error;
(2) SV error greatly affects the variability of MC-simulated measurements of eroded and/or deposited surfaces; and
(3) the uncertainty of surficial changes depends on their magnitude.
This work also evaluates the effectiveness of MC simulations
in measuring fluvially eroded and/or deposited surfaces and assessing their significance.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Study area</title>
      <?pagebreak page473?><p id="d1e856">Located in easternmost France (Alsace), the Bruche is a mid-sized tributary of the Rhine with a drainage area of about
730 <inline-formula><mml:math id="M9" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>.
The 80 <inline-formula><mml:math id="M10" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> long river firstly drains the eastern flank of the Vosges Massif before debouching into the Upper Rhine Graben (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a).
Although highly impacted by human activities (levee/canal construction, channelisation, and artificial cut-offs), this alluvial river is known to have been laterally active over historical times <xref ref-type="bibr" rid="bib1.bibx29 bib1.bibx41 bib1.bibx47" id="paren.38"/>.
This is especially true in its lowermost reach where it flows through the Strasbourg urban area (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a), raising
important management issues <xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx49" id="paren.39"/>. Our test site is a 6 <inline-formula><mml:math id="M11" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> long wandering reach located a few kilometres upstream of
the Ill confluence: the river freely meanders within its Holocene floodplain and locally erodes Late Pleistocene terrace deposits
of the lower Bruche about 2 <inline-formula><mml:math id="M12" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> from its confluence as well (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a; <xref ref-type="bibr" rid="bib1.bibx29" id="altparen.40"/>). In this reach, the Bruche has a 20 <inline-formula><mml:math id="M13" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> wide
mean active channel and a mean slope of 1 ‰. The daily 2-year (<inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)
and 10-year (<inline-formula><mml:math id="M15" 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>) peak flow discharges amount to 71 and 126 <inline-formula><mml:math id="M16" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, respectively, for the period 1965–2018. The specific stream power at the <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> discharge roughly amounts to 27 <inline-formula><mml:math id="M18" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><label>Figure 2</label><caption><p id="d1e991"><bold>(a)</bold> Study area. Localisation of the four sub-reaches in the lowermost Bruche course. Red and yellow crosses
indicates the position of the independent set of GCPs used to assess the SV error over the study area. <bold>(b)</bold> Planimetric evolution
of each sub-reach from 1950 to 1964 based on the two orthophotos.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020-f02.png"/>

      </fig>

</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Methodology</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Remotely sensed data</title>
      <p id="d1e1020">To measure eroded and/or deposited surfaces in our study area, two orthophotos from 1950 and 1964 were used. They were produced by
the French National Geographic Institute (IGN) and the Laboratoire Image, Ville, Environnement (LIVE) of the University of Strasbourg;
they have a spatial resolution of 50 and 20 cm, respectively. Both are projected in RGF93/CC48 CRS (EPSG: 3948), which is the most
accurate projection in this area. Despite the lack of hydrological data in the lower Bruche before 1965, we assume surveys were
conducted during moderate to low water, according to the period of the year during which the photos were taken (13 September 1950 and 17 April 1964) and
our inspection of the orthophotos.</p>
      <p id="d1e1023">Active channel is a widely used concept to objectively identify channel boundaries in aerial photographs, regardless of the river discharge.
It basically refers to the unvegetated area <xref ref-type="bibr" rid="bib1.bibx26 bib1.bibx27 bib1.bibx30 bib1.bibx50 bib1.bibx55" id="paren.41"/>.
Here, active channel boundaries have been digitised by a single user in QGIS at a <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">300</mml:mn></mml:mrow></mml:math></inline-formula> scale.
To reliably assess the SV error, we used a 2015 orthophoto as the base image; it was produced by the IGN with a resolution of 20 cm.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>SV error assessment</title>
      <p id="d1e1049">In both orthophotos (1950 and 1964) of our study area, spatial variations of geometric error are assessed by an approach similar to that
used by <xref ref-type="bibr" rid="bib1.bibx24" id="text.42"/>. However, because we use orthophotos (which are already co-registered), we must rely on an independent
set of ground control points (GCPs), as suggested by <xref ref-type="bibr" rid="bib1.bibx18" id="text.43"/>. We selected a total of 18 GCPs, including both hard (buildings and canal)
and soft (pathway intersections and trees) features (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a). After identification and manual plotting in the 2015 orthophoto, they are
identified in both older orthophotos on a <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">200</mml:mn></mml:mrow></mml:math></inline-formula> computer-screen scale. The spatial distribution of GCPs in the study area is rather
uniform, though hard edges are restricted to the northern sector (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a).</p>
      <?pagebreak page474?><p id="d1e1074">Local root square error (RSE) is then measured for each of the 18 GCPs, in both orthophotos. Error in <inline-formula><mml:math id="M21" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> or <inline-formula><mml:math id="M22" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> corresponds
to the Euclidean distance between the two points for <inline-formula><mml:math id="M23" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M24" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> coordinates, respectively. SV error is calculated by interpolating local RSE in our
whole study area with an inverse-distance weighting (IDW) technique at the original spatial resolution (Fig. <xref ref-type="fig" rid="Ch1.F4"/>). IDW uses
a linear combination of values at specific sampled points. It allocated weights proportional to the proximity of the sampled
points to estimate values at unknown locations <xref ref-type="bibr" rid="bib1.bibx19" id="paren.44"/>. We used the IDW interpolation method for two main reasons.
First, based on a comparison of five interpolation methods, <xref ref-type="bibr" rid="bib1.bibx24" id="text.45"/> showed that linear and nearest-neighbour methods reduce the areal extent of large co-registration errors. These methods are thus discarded as they can strongly limit
the influence of large co-registrations errors in the estimation of surficial changes.
Then, in a comparative study of spatial
interpolation methods for producing a digital elevation model from a small set of points that were not spatially uniform,
<xref ref-type="bibr" rid="bib1.bibx52" id="text.46"/> showed that
IDW provided better results than spline or kriging. Because of the difficulties of selecting a high number of independent control points
spatially uniform over time in archival remotely sensed data, we
argue that IDW is a reliable method for interpolating the registration error in our case.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Sub-reaches</title>
      <p id="d1e1125">To examine the implications of SV error in lateral migration measurements, we focus on four distinct sub-reaches
(Fig. <xref ref-type="fig" rid="Ch1.F2"/>). Their mean thalweg lengths amount to 530, 380, 700, and 890 <inline-formula><mml:math id="M25" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> long (upstream–downstream order).
They are (1) an extending and narrowing meander, (2) an almost straight (apparently inactive) sector, (3) two alternate
meanders (the first one slightly extending and the second one displaying a small cut-off), and (4) a long meander
extending at the downstream end of the curve.
We selected geomorphologically distinct sub-reaches to evaluate the effect of both different magnitude changes and types of geomorphic
processes.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><label>Figure 3</label><caption><p id="d1e1140">Workflow of the Monte Carlo translation process used in this study. <bold>(a)</bold> Measurements of channel changes after translation.
<bold>(b)</bold> Translation parameters (error values and directions). <bold>(c)</bold> Illustration of resulting boundary simulations with and without constraints
on the shifting direction.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020-f03.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>MC simulations</title>
<sec id="Ch1.S3.SS4.SSS1">
  <label>3.4.1</label><title>Channel boundary simulation method</title>
      <p id="d1e1173">MC simulations as statistical methods are generally used in cases where processes are random or when
assumptions in the theoretical mathematics are not well known <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx39" id="paren.47"/>. Applying
MC simulations in this research context is the main novelty of this study. This approach has two main advantages.
Firstly, MC simulations are particularly well suited to our problem because of the difficulty of distinguishing between
inherent and processing errors in the measured RSE over the whole area. Secondly, MC simulations assume a spatial
continuity and a relative spatial homogeneity of the error, which is consistent with resulting spatial patterns of
errors observed after the co-registration or digitising process. MC simulations are also relatively easy to perform
and applicable in very different cases. This approach could thus improve the generalisation of methods for calculating
planform changes and spatially variable uncertainty in a fluvial context, as suggested by <xref ref-type="bibr" rid="bib1.bibx9" id="text.48"/>.</p>
      <?pagebreak page475?><p id="d1e1182">The approach used in this study followed the rules of boundary simulations <xref ref-type="bibr" rid="bib1.bibx4" id="paren.49"/>.
Figure <xref ref-type="fig" rid="Ch1.F3"/> illustrates this part of our methodology. As described in the
previous section, SV error has been interpolated over the whole study area. For each channel node, all pixels in a 5 m buffer
were first selected. A check of the local distributions of error (Shapiro test) showed a normal distribution for a vast majority of them. The normal distribution of error was then calculated by averaging the mean local error and by calculating
the standard deviation for each node, in each sub-reach. Hence, for each run (1000 runs in total), a specific value of error
in <inline-formula><mml:math id="M26" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>[</mml:mo><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">1000</mml:mn><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>) and <inline-formula><mml:math id="M28" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>[</mml:mo><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">1000</mml:mn><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>) was randomly extracted from the respective normal distribution (Fig. <xref ref-type="fig" rid="Ch1.F3"/>b) in order to shift each node from its original position.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><?xmltex \currentcnt{4}?><label>Figure 4</label><caption><p id="d1e1267">SV error interpolation between GCPs from local RSEs, by the IDW method. Year 1950.
<bold>(a)</bold> Error in <inline-formula><mml:math id="M30" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>. <bold>(b)</bold> Error in <inline-formula><mml:math id="M31" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula>. <bold>(c)</bold> Total error.</p></caption>
            <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020-f04.png"/>

          </fig>

      <?pagebreak page476?><p id="d1e1300">Furthermore, in accordance with the results from <xref ref-type="bibr" rid="bib1.bibx43" id="text.50"/>, the shape of a particular channel is assumed to remain coherent
after simulation. In this study, as the distance between nodes is significantly higher than the local registration error, it
is possible to move nodes of each sub-reach in any <inline-formula><mml:math id="M32" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M33" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> direction without significantly impacting the shape. However,
when the condition above is violated (in historical maps for instance; see <xref ref-type="bibr" rid="bib1.bibx16" id="altparen.51"/>), the operation can
potentially lead to strong geometrical errors such as “butterfly polygons” or excessive geometric distortions (Fig. <xref ref-type="fig" rid="Ch1.F3"/>c). These errors
might be partially corrected (e.g. via a moving average algorithm or Douglas–Peucker filtering) but can result in erroneous modifications
of the original channel shape. Thus, we proposed a hybrid solution to simulate the node shifting in space: (1) nodes from one sub-reach
can move in any <inline-formula><mml:math id="M34" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> direction (i.e. positive or negative) at each run, and (2) nodes from one sub-reach can move in only one
<inline-formula><mml:math id="M35" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> direction at each run (Fig. <xref ref-type="fig" rid="Ch1.F3"/>b). Considering the strong correlation of registration errors between two successive points, constraining the shifting direction for one of the two coordinates allows maintaining the directional sequence of several successive nodes and avoiding the butterfly polygon issue. From a wider perspective, the last operation allows (i) avoiding topological errors (Fig. <xref ref-type="fig" rid="Ch1.F3"/>c) while simulating the most probable displacements
of channel polygons and (ii) probably enhancing the transferability of our method to other fluvial settings.
The direction of errors in <inline-formula><mml:math id="M36" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M37" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> were randomly selected at each MC simulation with equal probability weights (i.e. 50 % each).</p>
      <p id="d1e1358">Last, as mentioned by <xref ref-type="bibr" rid="bib1.bibx9" id="text.52"/>, it is quite hard to distinguish between errors inherent to the co-registration
and digitising processes. For this reason, a digitising error (<inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) equal to 1 pixel was added as a reasonable constraint within
the simulation process, considering the resolution of the orthophotos. This digitising error is assumed to be uniform over the
entire area and does not fluctuate in different simulation runs (Eqs. 1 and 2). Only the direction in <inline-formula><mml:math id="M39" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M40" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> was randomly defined for each node of one sub-reach at each MC simulation. These directions may vary from one node to another for one given sub-reach.</p>
      <p id="d1e1389">The overall mathematical expression of the simulation process can be expressed as follows:

                  <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M41" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E1"><mml:mtd><mml:mtext>1</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">changed</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">original</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mo>|</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>|</mml:mo><mml:mo>×</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><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:msub><mml:mi>y</mml:mi><mml:mi mathvariant="normal">changed</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi mathvariant="normal">original</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mo>|</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>|</mml:mo><mml:mo>×</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>|</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>|</mml:mo></mml:mrow></mml:math></inline-formula> are the absolute registration error in <inline-formula><mml:math id="M44" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M45" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula>, respectively. The constant <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the digitising error equal to 1 pixel. <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> respectively are the coefficients of shifting direction (i.e. 1 or <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>) of the registration error (i.e. <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>|</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>|</mml:mo></mml:mrow></mml:math></inline-formula>) and the digitising error (<inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), randomly selected at each run. In our study, <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> was constant for each <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">changed</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of one sub-reach (i.e. constrained in only one direction).</p>
</sec>
<sec id="Ch1.S3.SS4.SSS2">
  <label>3.4.2</label><title>Lateral migration measurements</title>
      <p id="d1e1666">Lateral migration of the river channel between 1950 and 1964 is calculated through three standard surficial morphological metrics
(erosion, deposition, and erosion then deposition), illustrated in Fig. <xref ref-type="fig" rid="Ch1.F1"/>b. Note that the metric “erosion then deposition”
measured in the area located between the former channel (T1) and the new one (T2) does not always imply continuous lateral channel
migration followed by deposition. Sudden lateral shifts of meanders (e.g. through meander cut-off) or meander belts (e.g. through
channel avulsion) may be involved as well and require specific geomorphological attention.
Therefore, at each MC run, new values of metrics are derived for each sub-reach (Fig. <xref ref-type="fig" rid="Ch1.F3"/>a) in order to estimate fluctuations induced by
co-registration and digitising errors.</p>
</sec>
<sec id="Ch1.S3.SS4.SSS3">
  <label>3.4.3</label><title>Impact of SV error on uncertainty of lateral migration measurements</title>
      <p id="d1e1681">To evaluate the uncertainty associated with lateral migration measurements within each sub-reach and to allow comparison between the four
sub-reaches,
two types of relative uncertainty were calculated for each morphological metric (erosion, deposition, and erosion then deposition).
The first one (Eq. 3) corresponds to the total percentage of uncertainty and involves the total range of measured
values (max–min) through MC simulation. The second one (Eq. 4) corresponds to the 95 % uncertainty percentage and
involves the 95 %<?pagebreak page477?> confidence interval. Their mathematical expressions are, respectively,

                  <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M55" display="block"><mml:mtable displaystyle="true"><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:mtext>total uncertainty</mml:mtext><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mo>(</mml:mo><mml:mo>max⁡</mml:mo><mml:mo>-</mml:mo><mml:mo>min⁡</mml:mo><mml:mo>)</mml:mo></mml:mrow><mml:mtext>mean</mml:mtext></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mo>,</mml:mo></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 displaystyle="true" class="stylechange"/><mml:mtable class="split" columnspacing="1em" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mn mathvariant="normal">95</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi><mml:mspace width="0.33em" linebreak="nobreak"/><mml:mtext>uncertainty</mml:mtext><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mn mathvariant="normal">95</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi><mml:mspace width="0.33em" linebreak="nobreak"/><mml:mtext>confidence interval width</mml:mtext></mml:mrow><mml:mtext>mean</mml:mtext></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mo>×</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mn mathvariant="normal">100</mml:mn><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula></p>
      <p id="d1e1784">Relative percentages of uncertainty provide information about the variability of measurements induced by the SV error through
MC simulation, observed in each sub-reach and for each morphological metric. We thus use these relative percentages
of uncertainty
to set a threshold of 50 %, above which the uncertainty is considered too high to yield a reliable measurement, i.e. a significant change in channel migration.
It is proposed to apply the 50 % threshold to both percentages of uncertainty: the less conservative one (i.e. 95 % uncertainty <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> %) and the more conservative one (i.e. total uncertainty <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> %).
While the former does not include outliers, the latter, which corresponds to a measurement whose mean value is lower than the total range of measured values (max–min), does.
In other words, applying the proposed 50 % threshold to the total uncertainty amounts to assuming that outliers can be “real” (i.e. that they can represent plausible situations). By contrast, applying the proposed 50 % threshold to the 95 % uncertainty amounts to rejecting the outliers, assuming that they cannot be real (implausible situations).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><label>Figure 5</label><caption><p id="d1e1809">Mean total SV error for each sub-reach, on both dates.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020-f05.png"/>

          </fig>

</sec>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>SV error</title>
      <p id="d1e1835">Figure <xref ref-type="fig" rid="Ch1.F4"/> shows the interpolated SV error in <inline-formula><mml:math id="M58" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M59" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula>, and the total SV error (<inline-formula><mml:math id="M60" display="inline"><mml:msqrt><mml:mrow><mml:msubsup><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>e</mml:mi><mml:mi>y</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:msqrt></mml:math></inline-formula>) for the year 1950.
The mean value of total SV error in each sub-reach for both years (Fig. <xref ref-type="fig" rid="Ch1.F5"/>) indicates that sub-reach 4 is
affected by the highest (1.32 m) and the lowest (0.61 m) error in 1950 and in 1964, respectively.
These values approximately correspond to the range of total SV error reached by the four sub-reaches.
Whereas the total SV error was reduced by a factor of 2 between 1950 and 1964 in sub-reach 4, it remained
fairly stable in the three other ones, ranging from 0.6 (sub-reach 3) to 1.2 m (sub-reach 1).</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>MC simulations</title>
      <p id="d1e1887">An example of variations in measurements of eroded surface through MC simulations is presented for sub-reach 1 in Fig. <xref ref-type="fig" rid="Ch1.F6"/>.
The entirety of MC results are available in Appendix A. A large majority of the measurements appear to be randomly varying around and
close to the mean value, inside the 95 % confidence interval. Note that having few outliers sometimes greatly extends the maximum range
compared to the 95 % confidence interval, especially when very low values occur. For instance,
MC simulations for deposited surfaces in sub-reach 1 include an outlier with a value (<inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M62" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) corresponding to 38 % of
the mean measured value (<inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:mn mathvariant="normal">6.8</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M64" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><?xmltex \currentcnt{6}?><label>Figure 6</label><caption><p id="d1e1946">Measurements of eroded surface in sub-reach 1, through 1000 MC simulations. Grey horizontal line corresponds to the mean value.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020-f06.png"/>

        </fig>

      <p id="d1e1955">Mean changes inferred from MC simulations between 1950 and 1964 are presented in Fig. <xref ref-type="fig" rid="Ch1.F7"/>a. Comparison
between sub-reaches is allowed by the normalisation of the surficial changes by the respective thalweg lengths of each sub-reach
(expressed thus in <inline-formula><mml:math id="M65" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>).
Whatever the sub-reach, changes<?pagebreak page478?> in eroded or deposited surfaces are much larger than those associated with erosion/deposition. The latter are
either negligible (sub-reaches 1 and 3) or not recorded (sub-reaches 2 and 4).
Sub-reach 1 shows the largest migration: eroded and deposited surfaces amount to <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:mn mathvariant="normal">9.1</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">4.9</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:mn mathvariant="normal">12.8</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mrow class="unit"><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">3.5</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="unit"><mml:mi mathvariant="normal">%</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>, respectively.
By contrast, sub-reach 2 shows the lowest migration: eroded and deposited surfaces amount to <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.1</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">24.7</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.8</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30.8</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="unit"><mml:mi mathvariant="normal">%</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>, respectively.
Intermediate measurements are reported in sub-reaches 3 and 4, where
they range between <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.4</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">25.3</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> (deposition; sub-reach 4) and  <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mn mathvariant="normal">4.5</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">8.5</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="unit"><mml:mi mathvariant="normal">%</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> (erosion; sub-reach 4).
Note that, in these two last sub-reaches, changes in eroded surfaces
are at least twice as high as those in deposited surfaces.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><?xmltex \currentcnt{7}?><label>Figure 7</label><caption><p id="d1e2174"><bold>(a)</bold> Mean surficial changes normalised by the length of each sub-reach. Error bars correspond to the 95 % confidence interval.
<bold>(b)</bold> 95 % uncertainty percentage (without outliers). <bold>(c)</bold> Total uncertainty percentage (with outliers).
The red dashed line corresponds to the 50 % proposed threshold.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020-f07.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>Uncertainty in lateral migration measurements</title>
      <p id="d1e2199">The relative percentage of measurement uncertainty in surficial changes is presented both in the 95 % confidence interval
(95 % uncertainty; Eq. (4); Fig. <xref ref-type="fig" rid="Ch1.F7"/>b)
and in the whole range of measured values (total uncertainty; Eq. (3); Fig. <xref ref-type="fig" rid="Ch1.F7"/>c).
As a reminder, the 95 % uncertainty does not take into account the presence of outliers, while the total uncertainty does.
The 95 % uncertainty varies from 3.5 % to 43.4 %. These extreme values both occur in sub-reach 1, for the deposited and the
eroded-then-deposited surfaces, respectively.
The total uncertainty varies from 15.8 % to 52.9 %. These extreme values both occur in sub-reach 4 and 1, for the eroded
and the eroded-then-deposited surfaces, respectively.
Sub-reaches 2 and 4 both display the same pattern between the 95 % and the total uncertainty, with the uncertainty related to the
deposited surface being higher than that related to the eroded one.
In contrast, sub-reaches 1 and 3 do not display the same pattern between the 95 % and the total uncertainty.
For sub-reach 1 and relative to the uncertainty of the eroded surface, the uncertainty of the deposited surface is higher than the latter
only
when taking into account the presence of outliers (total uncertainty). For sub-reach 3 and relative to the uncertainty of the
eroded/deposited surface, the uncertainty of the eroded surface is higher than the latter only when taking into account the presence
of outliers (total uncertainty).</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Discussion and research perspectives</title>
      <p id="d1e2216">In the light of these new results, we first discuss the three hypotheses underlying this study.
In the second step, we propose some methodological guidelines together with promising further implications of this study.</p>
<sec id="Ch1.S5.SS1">
  <label>5.1</label><title>SV error implications for uncertainty of surficial planform changes</title>
      <p id="d1e2226">Our results support the first hypothesis: they confirm that orthophotos are affected by a local significant SV error.
Within our relatively small (<inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M73" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) and flat study area, we interpolated a total SV error ranging from 0.26 to 1.89 m (Fig. <xref ref-type="fig" rid="Ch1.F4"/>),
while mean values of total SV error range from 0.61 to 1.32 m for the four sub-reaches (Fig. <xref ref-type="fig" rid="Ch1.F5"/>).
This emphasises the need to take the SV error into account and,
importantly, to assess its impact on the uncertainty of the measured changes <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx9" id="paren.53"/>, even if the characteristics of the
studied reach may appear unproblematic at first glance. Moreover, as orthophotos are used in this study, we draw particular
attention to the relevance of this statement in the case of studies using co-registered aerial photographs for similar purposes
<xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx17 bib1.bibx46" id="paren.54"><named-content content-type="pre">e.g.</named-content></xref>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><?xmltex \currentcnt{8}?><label>Figure 8</label><caption><p id="d1e2265">Example of translated channels for sub-reach 1, resulting from two different MC runs. Distinction between an <bold>(a)</bold> inlier and an <bold>(b)</bold> outlier
according to the simulated deposited surface. Background corresponds to the 1964 orthophoto.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020-f08.png"/>

        </fig>

      <p id="d1e2280">Our results also support the second hypothesis: the SV error greatly affects the variability of MC-simulated measurements of
eroded and/or deposited surfaces. Variability of the surficial measurements has been assessed by
calculating the relative percentages of uncertainty induced by the SV error through the MC simulations.
Whereas the more conservative percentage of uncertainty (total uncertainty) ranges from 15.8 % to 52.9 %, depending on the metric
and the sub-reach,<?pagebreak page479?> the less conservative percentage of uncertainty (95 % uncertainty) still ranges from 3.5 % to 43.4 %.
These results highlight the potentially high impact that SV error can have on variability of surficial measurements and consequently
on their uncertainty.</p>
      <p id="d1e2284">When applying the more conservative threshold of significance (50 % of total uncertainty; cf Sect. <xref ref-type="sec" rid="Ch1.S3.SS4.SSS3"/>), it appears that only one
surficial change has to be considered non-significant (eroded/deposited surface in sub-reach 1; Fig. <xref ref-type="fig" rid="Ch1.F7"/>c). However, it
can be considered significant when applying the less conservative threshold of significance (Fig. <xref ref-type="fig" rid="Ch1.F7"/>b), because its uncertainty
does not reach the 50 % threshold.
While this contrast may call into question whether or not the presence of outliers should be taken into account,
visual comparison of specific situations may help to unravel this issue. As illustrated in Fig. <xref ref-type="fig" rid="Ch1.F8"/>, only subtle areal
and shape differences may be observed between an inlier and an outlier, the latter likely representing a geomorphologically
plausible situation. When using MC simulations in this context, we thus strongly suggest inspecting outliers and
not systematically rejecting them. When the geomorphological plausibility of outliers is doubtful, we recommend using the total percentage of uncertainty.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><label>Figure 9</label><caption><p id="d1e2297">Detailed flow chart of the methodology applied in this study, allowing uncertainty of eroded and/or
deposited surfaces to be assessed using SV error.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020-f09.png"/>

        </fig>

      <p id="d1e2306">Our results partly validate the third hypothesis: the uncertainty of surficial changes depends not only on their magnitude but also
possibly on their respective shapes. A contrasted pattern of uncertainty is observed in sub-reaches 2 and 4 versus
sub-reaches 1 and 3. Whereas the former seemingly display uncertainties solely related to the magnitude of changes
(i.e. higher uncertainties for lower surficial changes), the latter do not (i.e. in some cases, higher uncertainties for
higher surficial changes; see Sect. <xref ref-type="sec" rid="Ch1.S4.SS3"/>). It is the case for instance in sub-reach 3, which displays a higher total uncertainty for the eroded
surface than for the eroded-then-deposited surface. Yet, as sub-reaches 1 and 3 display more complex geomorphological shapes and channel
evolution than sub-reaches 2 and 4 (Fig. <xref ref-type="fig" rid="Ch1.F2"/>b), we suggest that uncertainty of surficial measurements might also be
strongly influenced by channel morphology and its evolution through time.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <label>5.2</label><title>Methodological guidelines and potential applications</title>
      <p id="d1e2321">In order to improve the generalisation of tools documenting fluvial planform changes and facilitate the implementation of our new
methodological framework, we can summarise the complete workflow as follows (see Fig. <xref ref-type="fig" rid="Ch1.F9"/> for more details): (1) interpolate the SV error
in the study area (as recommended in <xref ref-type="bibr" rid="bib1.bibx24" id="altparen.55"/>), (2) calibrate a normal distribution around nodes to randomly
translate these (see Fig. 3 for more details), (3) choose a significance threshold, and visually check the outliers to eventually
(4) assess the significance of the measured surficial planform changes. The key step (2) is achieved via
MC simulation, which is well known for its simplicity, reliability, and transferability <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx39" id="paren.56"/>.
Simulation outputs allow assessing both the total and the 95 % uncertainties (Fig. <xref ref-type="fig" rid="Ch1.F9"/>).</p>
      <p id="d1e2334">We suggest a few practical recommendations when applying the proposed methodological framework. If orthophotos are employed, we
strongly advise using an independent set of GCPs for co-registration, bearing in mind that orthophotos are affected by a significant
SV error (see Sect. 5.1). As for GCPs, their amount must be high enough and their distribution over the entire study area as homogeneous
as possible. As pointed out by <xref ref-type="bibr" rid="bib1.bibx18" id="text.57"/>, a location of these GCPs close to the river system is highly beneficial.
As for the 50 % significance threshold, we recommend applying it in the total uncertainty, as outliers
might represent geomorphologically plausible situations (Fig. <xref ref-type="fig" rid="Ch1.F8"/>).
Nevertheless, the few outliers (Fig. <xref ref-type="fig" rid="Ch1.F6"/>) should still be treated in an empirical manner by visually determining if they
should be rejected or not. Further work is required in the near future to deal with this issue in a more automatic way.
More generally, when studying historical lateral migration of mid-sized rivers (active channel width <inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> m) and/or
low-magnitude changes (<inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M76" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) with the channel polygon method,
we emphasise the systematic need for assessing both SV error and uncertainty, as some of the measured changes might be non-significant (see Sect. 5.1).</p>
      <p id="d1e2394">This study, though focusing on short sub-reaches of a mid-sized (<inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> m) meandering (single-thread) channel using specific
remotely sensed data on a short timescale (archival orthophotos), has great potential for transferability. Firstly,<?pagebreak page480?> we assume that
our methodological framework could be applied to any fluvial system, regardless of its size. Secondly, we likewise argue that it could
be relatively easily extended onto an entire river reach by increasing the sub-reach database and/or onto a longer temporal scale by
increasing the historical river channel database (Fig. <xref ref-type="fig" rid="Ch1.F9"/>). As for the size/length of the sub-reaches, we recommend adapting
it according to the complexity of the planform changes and/or the channel pattern (e.g. anastomosing and anabranching channel patterns).
As for the river channel database, other remotely sensed data, such as co-registered aerial
photographs and satellite imagery, or traditional planimetric data (maps) can be easily integrated as well. Thirdly, transferring this
framework to other channel patterns represents a promising future
research topic. In contrast to the centreline approach <xref ref-type="bibr" rid="bib1.bibx24" id="paren.58"><named-content content-type="pre">e.g.</named-content></xref>, the channel polygon method would actually suit the
study of lateral mobility of multi-threaded channels (including anastomosing rivers, which usually are characterised by low lateral
mobility), with a robust assessment of the SV error. Unlike this present
study, where planimetric changes associated with erosion/deposition are negligible, we might expect a higher proportion of these changes
in this kind of fluvial setting. Overall, long-term landscape reconstruction studies could also greatly benefit from the methodology we
propose. In particular, works combining multiple diachronic spatial sources (e.g. old aerial photographs, historical and cadastre maps, and
satellite images) should draw particular attention because of the possible propagation of uncertainty in the assessment of
landscape changes.</p>
      <p id="d1e2414">We conclude by stating that this study offers promising research prospects. Firstly, a key outcome is the ability of MC
simulations to actually detect low-magnitude planform changes in mid-sized river channels. This positive achievement thus overcomes
the main difficulty related to the use of classic planimetric methods in such settings <xref ref-type="bibr" rid="bib1.bibx42" id="paren.59"/>, as recently highlighted
by <xref ref-type="bibr" rid="bib1.bibx22" id="text.60"/>, who failed to detect noticeable changes in mid-sized active channels (width <inline-formula><mml:math id="M78" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 25 m). Secondly, as for river
restoration, our methodological framework should help in constructing robust scenarios of future river management, especially those based on
past planform changes <xref ref-type="bibr" rid="bib1.bibx31" id="paren.61"><named-content content-type="pre">e.g.</named-content></xref>. Thirdly, significance assessment of planform changes can strengthen the studies using
surfaces of an active channel as input for sediment budgeting <xref ref-type="bibr" rid="bib1.bibx54" id="paren.62"/>. Finally, while this study, together
with <xref ref-type="bibr" rid="bib1.bibx24" id="text.63"/> and <xref ref-type="bibr" rid="bib1.bibx9" id="text.64"/>, focus specifically on the SV error and,
more globally, uncertainties in planimetric studies in a wide range of fluvial settings, the proposed propagation of geometric error
via MC simulations could be extended to other geomorphological contexts where surface extraction from remotely sensed data is involved.</p><?xmltex \hack{\clearpage}?>
</sec>
</sec>

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

<?pagebreak page481?><app id="App1.Ch1.S1">
  <?xmltex \currentcnt{A}?><label>Appendix A</label><title/>

      <?xmltex \floatpos{h!}?><fig id="App1.Ch1.S1.F10"><?xmltex \currentcnt{A1}?><label>Figure A1</label><caption><p id="d1e2459">Monte Carlo simulation results for every sub-reach.</p></caption>
        <?xmltex \hack{\hsize\textwidth}?>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/8/471/2020/esurf-8-471-2020-f10.png"/>

      </fig>

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

      <p id="d1e2476">Datasets and code are available upon request from Timothée Jautzy (timothee.jautzy2@etu.unistra.fr).</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e2482">All authors contributed to the conception of this study and manuscript writing.
TJ wrote most of the manuscript and produced the initial data and figures; TJ and PAH
conceptualised the global processing chain and performed Monte Carlo simulations;
VC contributed to result interpretation;
LS and GR provided a complete review of the manuscript; and GR supervised the text harmonisation.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e2488">The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e2494">We warmly thank Grégoire Skupinski (LIVE) for providing orthophotos.
We are grateful to Josué Jautzy (Geological Survey of Canada) for his valuable review of the first draft.
We also thank two anonymous reviewers, who helped to significantly improve this paper.
This work has been entirely produced with free and open-source programs (QGIS, R, GDAL, Inkscape, LibreOffice, and LaTeX).</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e2499">This research has been supported by the Scientific Council of the National School for Water and Environmental Engineering of Strasbourg (ENGEES, France; grant no. 6803MOBI).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e2505">This paper was edited by Francois Metivier and reviewed by two anonymous referees.</p>
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    <!--<article-title-html>Measuring river planform changes from remotely sensed data – a Monte Carlo approach to assessing the impact of spatially variable error</article-title-html>
<abstract-html><p>Remotely sensed data from fluvial systems are extensively used to document historical planform changes.
However, geometric and delineation errors inherently associated with these data can result in poor or even misleading
interpretation of measured changes, especially rates of channel lateral migration. It is thus imperative to take into account a
spatially variable (SV) error affecting the remotely sensed data. In the wake of recent key studies using this SV error as
a level of detection, we introduce a new framework to evaluate the significance of measured channel migration. Going beyond
linear metrics (i.e. migration vectors between diachronic river centrelines), we assess significance through a channel polygon
method yielding a surficial metric (i.e. quantification of eroded, deposited, or eroded-then-deposited surfaces).</p><p>Our study area is a mid-sized active wandering river: the lower Bruche, a  ∼ 20&thinsp;m wide tributary of the Rhine in eastern France.
Within our four test sub-reaches, the active channel is digitised using diachronic orthophotos (1950 and 1964), and the
SV error affecting the data is interpolated with an inverse-distance weighting (IDW) technique. The novelty of our approach arises from then
running Monte Carlo (MC) simulations to randomly translate active channels and propagate geometric and delineation errors
according to the SV error. This eventually leads to the computation of percentage of uncertainties associated with each of the
measured planform changes, which allows us to evaluate the
significance of the planform changes. In the lower Bruche, the uncertainty associated with the documented changes ranges from
15.8&thinsp;% to 52.9&thinsp;%.</p><p>Our results show that (i) orthophotos are affected by a significant SV error; (ii) the latter strongly
affects the uncertainty of measured changes; and (iii) the significance of changes is dependent on both the magnitude and the
shape of the surficial changes.
Taking the SV error into account is strongly recommended even in orthorectified aerial photos,
especially in the case of mid-sized rivers ( &lt; 30&thinsp;m width) and/or low-amplitude river planform changes ( &lt; 1&thinsp;m<sup>2</sup> m<sup>−1</sup> yr<sup>−1</sup>).
In addition to allowing detection of low-magnitude planform changes, our approach
is also transferable as we use well-established tools (IDW and MC): this opens new perspectives in the fluvial context
(e.g. multi-thread river channels) for robustly assessing surficial channel changes.</p></abstract-html>
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