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  <front>
    <journal-meta><journal-id journal-id-type="publisher">NHESS</journal-id><journal-title-group>
    <journal-title>Natural Hazards and Earth System Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">NHESS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Nat. Hazards Earth Syst. Sci.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1684-9981</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/nhess-18-1567-2018</article-id><title-group><article-title>Using kites for 3-D mapping of gullies at decimetre-resolution <?xmltex \hack{\break}?>over several
square kilometres: a case study on the <?xmltex \hack{\break}?>Kamech catchment, Tunisia</article-title><alt-title>3-D mapping of gullies by kites on square kilometres</alt-title>
      </title-group><?xmltex \runningtitle{3-D mapping of gullies by kites on square kilometres}?><?xmltex \runningauthor{D.~Feurer et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Feurer</surname><given-names>Denis</given-names></name>
          <email>denis.feurer@ird.fr</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Planchon</surname><given-names>Olivier</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>El Maaoui</surname><given-names>Mohamed Amine</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Ben Slimane</surname><given-names>Abir</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Boussema</surname><given-names>Mohamed Rached</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Pierrot-Deseilligny</surname><given-names>Marc</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Raclot</surname><given-names>Damien</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>LISAH, Univ Montpellier, INRA, IRD, Montpellier SupAgro, Montpellier, France</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>El Manar University, National Engineering School of Tunis, LTSIRS, B.P 37,
1002 Tunis-Belvédère, Tunis, Tunisia</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Rural Engineering Laboratory, National Research Institute of Rural Engineering,
Water and Forests, <?xmltex \hack{\break}?>INRGREF, Rue Hédi Karray El Menzah IV – B.P 10, Ariana 2080, Tunisia</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Université Paris-Est, IGN/SR, LOEMI, 73 avenue de Paris, 94165 Saint-Mandé,
France</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Denis Feurer (denis.feurer@ird.fr)</corresp></author-notes><pub-date><day>7</day><month>June</month><year>2018</year></pub-date>
      
      <volume>18</volume>
      <issue>6</issue>
      <fpage>1567</fpage><lpage>1582</lpage>
      <history>
        <date date-type="received"><day>3</day><month>February</month><year>2017</year></date>
           <date date-type="rev-request"><day>8</day><month>February</month><year>2017</year></date>
           <date date-type="rev-recd"><day>27</day><month>April</month><year>2018</year></date>
           <date date-type="accepted"><day>8</day><month>May</month><year>2018</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2018 Denis Feurer et al.</copyright-statement>
        <copyright-year>2018</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018.html">This article is available from https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018.html</self-uri><self-uri xlink:href="https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018.pdf">The full text article is available as a PDF file from https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018.pdf</self-uri>
      <abstract>
    <p id="d1e161">Monitoring agricultural areas threatened by soil erosion often requires
decimetre topographic information over areas of several square kilometres.
Airborne lidar and remotely piloted aircraft system (RPAS) imagery have the
ability to provide repeated decimetre-resolution and -accuracy digital
elevation models (DEMs) covering these extents, which is unrealistic with
ground surveys. However, various factors hamper the dissemination of these
technologies in a wide range of situations, including local regulations for
RPAS and the cost for airborne laser systems and medium-format RPAS imagery.
The goal of this study is to investigate the ability of low-tech kite aerial
photography to obtain DEMs with decimetre resolution and accuracy that permit
3-D descriptions of active gullying in cultivated areas of several square
kilometres. To this end, we developed and assessed a two-step workflow.
First, we used both heuristic experimental approaches in field and
numerical simulations to determine the conditions that make a photogrammetric flight possible and
effective over several square kilometres with a kite
and a consumer-grade camera. Second, we mapped and characterised the entire
gully system of a test catchment in 3-D. We showed numerically and
experimentally that using a thin and light line for the kite is key for
a complete 3-D coverage over several square kilometres.
We thus obtained a decimetre-resolution DEM covering 3.18 km<inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> with a
mean error and standard deviation of the error of <inline-formula><mml:math id="M2" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>7 and
22 cm respectively, hence achieving decimetre accuracy. With this data set,
we showed that high-resolution topographic data permit both the detection and
characterisation of an entire gully system with a high level of detail and an
overall accuracy of 74 % compared to an independent field survey. Kite
aerial photography with simple but appropriate equipment is hence an
alternative tool that has been proven to be valuable for surveying gullies
with sub-metric details in a square-kilometre-scale catchment. This case
study suggests that access to high-resolution topographic data on these
scales can be given to the community, which may help facilitate a better
understanding of gullying processes within a broader spectrum of conditions.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e187">Soil losses caused by erosion are a major hazard in agricultural areas.
Management of this risk requires a good understanding of various erosion
forms and the quantification of eroded volumes over areas of several square
kilometres, which is the scale of the elementary watershed as defined by
<xref ref-type="bibr" rid="bib1.bibx20" id="normal.1"/>. As noted by <xref ref-type="bibr" rid="bib1.bibx46" id="normal.2"/>, topography is one of the
major factors in most hazard analyses and the generation of DEMs plays a
central role in their analysis. This is all the more true for gully erosion,
considering that differencing DEMs theoretically allow for a<?pagebreak page1568?> direct
estimation of eroded volumes. It is therefore appropriate to develop methods
for generating detailed descriptions of landforms threatened by gully erosion
at a limited cost. Cost-effective approaches are of great interest for
monitoring on several spatial and temporal scales.</p>
      <p id="d1e196">Before the advent of remotely piloted aircraft systems (RPASs), developments in
remote sensing technology had already brought very high-resolution
topographic data to the earth sciences community. Among these data, airborne
lidar constituted a breakthrough, allowing for the characterisation of
terrain surfaces with metre-size details. Such dense topographic data are of
major importance for the description of hydrological-oriented
geomorphological features <xref ref-type="bibr" rid="bib1.bibx48" id="paren.3"/>. These even allowed for the
development of the first algorithms for automatic gully detection.
<xref ref-type="bibr" rid="bib1.bibx15" id="normal.4"/> used a 2 m lidar DEM to detect gullies as zones with high
curvature and low altitude relative to the average surrounding elevation
computed within a moving window. With a lidar data set with a point density of
4 points m<inline-formula><mml:math id="M3" 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>, <xref ref-type="bibr" rid="bib1.bibx2" id="normal.5"/> performed curvature analyses
to detect gully candidates in segments and then connect them to a complete
network. Another example of curvature analysis is the work of
<xref ref-type="bibr" rid="bib1.bibx39" id="normal.6"/>, who identified gully headcuts from a 1 m lidar DEM as
zones showing negative profile curvature below a given threshold and having a
drainage area greater than 5000 m<inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>. <xref ref-type="bibr" rid="bib1.bibx17" id="normal.7"/>
proposed a method adapted to gullies of cushion peatlands using terrestrial
lidar. In their work, gullies were delineated as polygons by detecting
breaklines in the lidar DEM, and then artificial dams were manually
positioned on the DEM, and finally, the formed sinks were filled. Occlusion
effects due to the steep slopes of gully banks and the low-altitude point of
view were noted by the authors. Most recently, <xref ref-type="bibr" rid="bib1.bibx31" id="normal.8"/> used fuzzy
logic on several topographic indices computed on a 1 m lidar DEM and combined
it with image information and morphological operators to map gullies.</p>
      <p id="d1e239">Although lidar technology has been developed for use aboard RPASs and has
proven its potential in gully detection over large areas, this technology
remains costly, which compromises its widespread use as an everyday
monitoring tool. Structure from motion (SfM) and multi-view stereo (MVS)
algorithms, which are recent developments in photogrammetry, represent new means of
computing very high-resolution topographic data with a limited cost and have
high potential in the geosciences as noted by <xref ref-type="bibr" rid="bib1.bibx53" id="normal.9"/> and
<xref ref-type="bibr" rid="bib1.bibx16" id="normal.10"/>. In the specific field of gully erosion mapping and in
line with lidar-based gully mapping approaches, <xref ref-type="bibr" rid="bib1.bibx8" id="normal.11"/> proposed
an automated algorithm tested on three DEMs of different types and scales –
SfM <inline-formula><mml:math id="M5" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> MVS DEMs computed from ground and aerial images and a coarser and more
classical DEM provided by the Spanish geographic institute – and demonstrated
the potential of SfM <inline-formula><mml:math id="M6" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> MVS DEMs for gully erosion studies. For interested
readers, in-depth details on SfM and MVS algorithms and their use in the
geosciences can be found in the reviews of <xref ref-type="bibr" rid="bib1.bibx41" id="normal.12"/>,
<xref ref-type="bibr" rid="bib1.bibx14" id="normal.13"/>, <xref ref-type="bibr" rid="bib1.bibx27" id="normal.14"/> and <xref ref-type="bibr" rid="bib1.bibx7" id="normal.15"/>.</p>
      <p id="d1e278">The advent of SfM and MVS in the geosciences has made it possible to
implement cost-effective solutions that can take advantage of developments
previously achieved with lidar data for landform mapping applications.
Indeed, SfM-based methods can be deployed with consumer-grade cameras and
even smartphones (e.g. Micheletti 2015). As image data acquisition is now
possible with fewer constraints, the field of 3-D modelling has opened to a
wide range of applications from worldwide modelling of cities and landscapes
<xref ref-type="bibr" rid="bib1.bibx42 bib1.bibx43" id="paren.16"/> to the geosciences (<xref ref-type="bibr" rid="bib1.bibx16" id="altparen.17"/>;
<xref ref-type="bibr" rid="bib1.bibx53" id="altparen.18"/>). In combination with small-format RPASs, the potential of
SFM and MVS algorithms for 3-D mapping is huge, as reviewed by
<xref ref-type="bibr" rid="bib1.bibx30" id="normal.19"/>. However, covering several square kilometres with RPASs still
requires costly fixed-wing or medium-format multi-rotor unmanned aircraft.
Furthermore, the use of more affordable small-format rotary wing RPASs, which
have shorter flight times, is limited in strong wind conditions. Finally,
local regulations may hamper or even prohibit the use of autonomous aircraft
in many places around the world. According to <xref ref-type="bibr" rid="bib1.bibx9" id="normal.20"/>, this is
the main restriction on the widespread use of these powerful and versatile
technologies.</p>
      <p id="d1e297">For all these reasons, kites, which were used for more than a century
for aerial image acquisition, have been enjoying renewed interest
<xref ref-type="bibr" rid="bib1.bibx12" id="paren.21"/> for several years. In combination with most recent 3-D
image processing algorithms, kites can hence be at the root of dependable and
low-tech solutions, relying on the principles of so-called “frugal
innovation”, which can simply be defined as “doing more with less”
<xref ref-type="bibr" rid="bib1.bibx38" id="paren.22"/>. In various fields in the geosciences, kites have indeed
already been used with photogrammetric techniques for applications requiring
3-D mapping. <xref ref-type="bibr" rid="bib1.bibx32" id="normal.23"/> used kite imagery to compute a 3-D model of an
urban area. <xref ref-type="bibr" rid="bib1.bibx55" id="normal.24"/> compared a DEM computed from kite
aerial imagery to a ground survey and classified vegetation in mountainous
areas with favourable results. <xref ref-type="bibr" rid="bib1.bibx40" id="normal.25"/> also demonstrated the
potential of kite aerial photography for DEM production over small areas
(i.e. less than 1 ha) using off-the-shelf cameras and professional
photogrammetry software. More recently, 3-D modelling from kite imagery was
carried out by a small number of authors with SfM <inline-formula><mml:math id="M7" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> MVS software.
<xref ref-type="bibr" rid="bib1.bibx11" id="normal.26"/> have compared this technique (called “Ecosynth” by
the authors) to lidar data for deriving elevation data and canopy-height
models. <xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx4" id="normal.27"/> performed centimetre 3-D mapping of
vegetation in coastal areas and mapped coastal changes. <xref ref-type="bibr" rid="bib1.bibx54" id="normal.28"/>
assessed the accuracy of SfM <inline-formula><mml:math id="M8" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> MVS DEMs acquired with kites in comparison to
lidar data in mountainous areas, where conditions limit the use of RPASs. More
specifically, in the field of gully<?pagebreak page1569?> erosion, the potential of small-format
cameras aboard kites and other platforms has been established by
<xref ref-type="bibr" rid="bib1.bibx23" id="normal.29"/> and <xref ref-type="bibr" rid="bib1.bibx24" id="normal.30"/>, who realised the 3-D monitoring
of several individual gullies in southern Spain.</p>
      <p id="d1e346">Yet there are no studies at the headwater catchment scale – i.e. over areas
of several square kilometres – showing the use of kites for 3-D topography
acquisition and gully erosion mapping. Indeed, kites suffer from several
limitations, of which flight control is the most challenging, as noted by
<xref ref-type="bibr" rid="bib1.bibx50" id="normal.31"/>. Some authors have given instructions for ensuring proper
data acquisition with kites: <xref ref-type="bibr" rid="bib1.bibx5" id="normal.32"/> used graduated lines to
control flight altitude, and <xref ref-type="bibr" rid="bib1.bibx1" id="normal.33"/> dedicated a chapter section to
the principles and methods of kite aerial photography. However, the kite's
ability to follow a predefined flight plan that enables 3-D coverage of
several square kilometres has not yet been proven.</p>
      <p id="d1e358">Thus, the aim of this study is to test the ability of low-tech kite aerial
photography to obtain high-resolution DEMs that permit 3-D descriptions of
active gullying in cultivated areas of several square kilometres. This goal
jointly requires (i) the determination and assessment of the conditions that allow the
use of a simple kite to acquire a suitable photogrammetric data set on a
relatively large area and (ii) a 3-D map of gullies and assessment of
the relevance of this map for erosion studies. To achieve this goal, we first
expose and verify the conditions required to allow the use of a kite for
photogrammetric acquisition over several square kilometres with numerical and
field experiments. We then present a case study of image acquisition and
processing on the Kamech catchment, located in northern Tunisia. Next, we
propose a semi-automatic method for mapping gullies from the kite DEM.
Finally we compared our results with independent ground surveys to assess the
quality of the 3-D mapping of gullies and to exhibit the potential of kite
DEMs with decimetre resolution and accuracy to study gully erosion.</p>
</sec>
<sec id="Ch1.S2">
  <title>Material and methods</title>
<sec id="Ch1.S2.SS1">
  <title>Study site</title>
      <p id="d1e372">The study site is the Kamech catchment, located in Cap Bon, a peninsula in
north-eastern Tunisia (Fig. <xref ref-type="fig" rid="Ch1.F1"/>a).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><caption><p id="d1e379">Location of the Kamech test site and ground-truth data used in the
SfM process. <bold>(a)</bold> Location of the Cap Bon peninsula, in north-eastern
Tunisia; Kamech is marked in red. <bold>(b)</bold> Close-up of the Kamech catchment, 2.63 km<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>,
delineated in red; its outlet is an artificial lake,
visible in the south-east of the catchment. <bold>(c)</bold> Close-up of the available
ground-truth data around the lake; scale is given by the external graduations
(projection UTM, EPSG : 32632); the dam is the linear feature visible on the
south-eastern side of the lake. The ground-truth data set is composed of ground
control points (GCPs, crosses), which are used to give spatial references to
the image data set, and validation points (black dots), which are used to
independently validate the DEM computed from the image data set.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018-f01.jpg"/>

        </fig>

      <p id="d1e406">Kamech is one of the two catchments of the OMERE long-term
hydro-meteorological research observatory (<uri>http://www.obs-omere.org</uri>, last access: 29 May 2018). A
detailed description of the Kamech catchment can be found in
<xref ref-type="bibr" rid="bib1.bibx25" id="normal.34"/>, <xref ref-type="bibr" rid="bib1.bibx26" id="normal.35"/> and <xref ref-type="bibr" rid="bib1.bibx37" id="normal.36"/>. More than 70 % of
the catchment area is ploughed and cultivated with rainfed crops. The climate
is semi-arid to sub-humid with a mean interannual rainfall of 650 mm and a
long dry summer season from May to October. The elevation ranges between 80
and 160 m. The slope can locally exceed 45<inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. The substratum is mainly
composed of marl and clay intercalated with sandstone layers. These layers
have an average south-eastern dip of approximately 30<inline-formula><mml:math id="M11" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> corresponding to
the global anticline of Cape Bon. The right bank of the catchment shows a
natural slope generally parallel to this dip and mainly presents marly
layers. Hence, most gullies of the area have developed on this side.
Sandstone outcrops are visible on the left bank of the catchment (Fig. <xref ref-type="fig" rid="Ch1.F1"/>b).
The soils have a sandy-loam texture with depths ranging
from zero to more than 2 m depending on the location within the
catchment and local topography. The drainage network is composed of several
kilometres of wadi and gully sections with decimetre to pluri-metre widths.
The network drains intermittent flow discharge into a reservoir of 140 000 m<inline-formula><mml:math id="M12" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula>
built in 1994 that silts up at an annual rate of 15 t ha<inline-formula><mml:math id="M13" 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> because of water erosion <xref ref-type="bibr" rid="bib1.bibx18" id="paren.37"/>. The
gullies are permanent, and the gully heads are located at the edge of the
agricultural fields. There is no significant ephemeral gully in the sense of
<xref ref-type="bibr" rid="bib1.bibx47" id="normal.38"/> or <xref ref-type="bibr" rid="bib1.bibx29" id="normal.39"/>.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>Conditions for the use of a kite as a photogrammetric platform</title>
      <p id="d1e479">To ensure photogrammetric image acquisition of several square kilometres, the
method is based on the following hypothesis: with a very stable kite as a
payload carrier, the position of the camera remains stationary relative to
the kite operator. With this hypothesis, the flight path (i.e. the kite
coordinates) is then a translation of the operator's course. Moreover, to use
the simplest and most reliable apparatus, image acquisition is automatically
triggered at a pre-set time interval. The flight plan can hence be prepared
prior to the survey itself and followed on the ground without any need for
remote control of the platform or a radio link between the camera and the
operator. Thus, this hypothesis and the conditions ensuring its validity have
to be carefully verified. This verification has been done with two
complementary approaches, namely field observations and numerical
simulations, which are described in the two following subsections.</p>
<sec id="Ch1.S2.SS2.SSS1">
  <title>Empirical kite flight characterisation</title>
      <p id="d1e487">In this study, two delta kites were used, one with an area of 4 m<inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>
and another with an area of 10 m<inline-formula><mml:math id="M15" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>. We used
framed delta kites chosen from a large variety of kites because of their
flight qualities (stability and high flight angles), easy assembly – with no
need for adjustment in the field – and a reasonable payload capacity. A
schematic representation and a close view of the equipment used for this
study are shown in Fig. <xref ref-type="fig" rid="Ch1.F2"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><caption><p id="d1e512">Left: schematic principle of kite image acquisition with a steady
flight angle. Right: payload close-up, which consists of a tripod with <bold>(a)</bold> an
automatic trigger <bold>(b)</bold> a camera and <bold>(c)</bold> a GPS logger. The yaw angle is the
angle of the camera around the <inline-formula><mml:math id="M16" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula> axis.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018-f02.png"/>

          </fig>

      <?pagebreak page1570?><p id="d1e537">As shown, the camera was mounted under a protective tripod hanging from a
long line forming a simple pendulum. This long pendulum smoothed out the
potentially erratic movements of the kite. Finally, acting as a
vane in the wind, the tripod allowed for natural aerodynamic stabilisation of the yaw
angle, which is the rotation angle around the vertical axis of the tripod
(Fig. <xref ref-type="fig" rid="Ch1.F2"/>c). The line used for all experimental
set-ups was Cousin-Trestec TopLine Ultimate 16175, which is made of
Dyneema<sup>®</sup>, a strong and light material. This line had a
strength of 87 daN, a diameter of 0.8 mm and a linear mass density of
0.39 g m<inline-formula><mml:math id="M17" 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>. The two delta kites performed a total of five
flights, with wind conditions ranging from Beaufort 3 to Beaufort 7 and with
line lengths ranging from 150 to 700 m. The use of the Beaufort scale was
preferred in the field because it can be estimated from direct observation of
land conditions (moving branches, raised dust, etc.) and does not require an
anemometer. Camera and operator positions were simultaneously logged with a
standalone QSTARZ BT1400S GPS data logger used with a 1 Hz acquisition rate
(Fig. <xref ref-type="fig" rid="Ch1.F2"/>c). This data logger had a given accuracy
of 3 m. These logs were used to compute effective kite flight angles
from the pairs of camera and operator positions. Analysis of these flight
angles was performed to verify the validity of our hypothesis and to
empirically estimate the actual average flight angles. This information also
made it possible to check the wind range in which the wing remained stable
with a steady flight angle and with neither shocks nor sudden movements
during the flight.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <title>Simulations of kite flights</title>
      <p id="d1e565">In addition to collecting the experimental data, numerical simulations
of line shape and kite position were performed for different wind conditions
(from 3 m s<inline-formula><mml:math id="M18" 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> to 11 m s<inline-formula><mml:math id="M19" 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> in increments
of 2 m s<inline-formula><mml:math id="M20" 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>) and for different line lengths (from 0 to 700 m).
The materials used for kite lines are of particular interest.
Highly resistant lines such as Dyneema<sup>®</sup>  can be used in much
smaller diameters than polyester of comparable strength, which results in
less weight and aerodynamic drag. Polyester, Dyneema<sup>®</sup>  and a
perfect theoretical material with negligible mass and diameter were
numerically compared to<?pagebreak page1571?> each other. For all the simulations, the rig load was
500 g, which is the actual mass of the rig we used (shown in Fig. <xref ref-type="fig" rid="Ch1.F2"/>). Simulations were performed with the physical
characteristics of the 10 m<inline-formula><mml:math id="M21" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> delta wing, which has a mass
of 2.7 kg.</p>
      <p id="d1e622">The model used was an ad hoc finite element model written in MATLAB. The line
was sampled in sections of 1 m. The aerodynamics of the line were taken
into account with the equation <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:mi>F</mml:mi><mml:mo>=</mml:mo><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:mi>A</mml:mi><mml:mi mathvariant="italic">ρ</mml:mi><mml:msup><mml:mi>V</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:msub><mml:mi>C</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, where
<inline-formula><mml:math id="M23" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> is the drag force in N, <inline-formula><mml:math id="M24" display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> is the projected surface area in m<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M26" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula> is the air bulk density in
kg m<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M28" display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula> is the wind speed in m s<inline-formula><mml:math id="M29" 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>,
and <inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the dimensionless drag coefficient. This equation was also
used to calculate the wind forces on the kite as a function of wind strength.
All the parameters used for the simulations are reported in Table <xref ref-type="table" rid="Ch1.T1"/>.
These numerical simulations aimed to assess the impact of the kite line characteristics on the aforementioned
hypothesis.</p>

<table-wrap id="Ch1.T1"><caption><p id="d1e732">Parameters used for the simulation of line shapes and flight angle</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="76.822441pt"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Parameter</oasis:entry>
         <oasis:entry colname="col2">Perfect line</oasis:entry>
         <oasis:entry colname="col3">Dyneema<sup>®</sup></oasis:entry>
         <oasis:entry colname="col4">Polyester</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Line diameter (mm)</oasis:entry>
         <oasis:entry colname="col2">0.01</oasis:entry>
         <oasis:entry colname="col3">0.8</oasis:entry>
         <oasis:entry colname="col4">2.5</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Line linear mass <?xmltex \hack{\hfill\break}?>density (g m<inline-formula><mml:math id="M31" 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="col2">0.01</oasis:entry>
         <oasis:entry colname="col3">0.39</oasis:entry>
         <oasis:entry colname="col4">3</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Resistance (daN)</oasis:entry>
         <oasis:entry colname="col2">n/a</oasis:entry>
         <oasis:entry colname="col3">87</oasis:entry>
         <oasis:entry colname="col4">59</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Pull angle (<inline-formula><mml:math id="M32" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry namest="col2" nameend="col4" align="center">60 </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Total mass (kg)</oasis:entry>
         <oasis:entry namest="col2" nameend="col4" align="center">2.7 (wing) <inline-formula><mml:math id="M33" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> 0.5 (payload)  </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Wing area (m<inline-formula><mml:math id="M34" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry namest="col2" nameend="col4" align="center">10 (<inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mi>A</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">8.7</mml:mn></mml:mrow></mml:math></inline-formula>) </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Wing drag</oasis:entry>
         <oasis:entry namest="col2" nameend="col4" align="center"><inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.15</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Line drag</oasis:entry>
         <oasis:entry namest="col2" nameend="col4" align="center"><inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> (used for cylinders) </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Air density (kg m<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry namest="col2" nameend="col4" align="center"><inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.18</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Line length (m)</oasis:entry>
         <oasis:entry namest="col2" nameend="col4" align="center">[0,700] </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Wind speed (m s<inline-formula><mml:math id="M40" 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 namest="col2" nameend="col4" align="center"><inline-formula><mml:math id="M41" display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M42" display="inline"><mml:mo>∈</mml:mo></mml:math></inline-formula> {3; 5; 7; 9; 11} </oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Photogrammetric acquisition </title>
      <p id="d1e1019">Image acquisition was performed in September 2013 after the dry season, when
vegetation cover was minimal. The equipment used for photogrammetric
acquisition is shown in Fig. <xref ref-type="fig" rid="Ch1.F2"/> above. The
Dyneema<sup>®</sup>  kite line was graduated every 10 m for the first 100 m
and then every 50 m with a simple colour/thickness coding system with a
comparable approach to that used by <xref ref-type="bibr" rid="bib1.bibx5" id="normal.40"/>. Image acquisition was
performed with the 10 m<inline-formula><mml:math id="M43" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> kite. A maximum flight altitude of
500 m was chosen to acquire images with decimetre ground sampling distance.
The corresponding line length was estimated with the worst case for the
flying angle (50<inline-formula><mml:math id="M44" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>) and resulted in a maximum line length of 600 m. The
targeted area was covered with parallel flight lines. These lines were
oriented north-east to south-west along the global orientation of the catchment.
The corresponding ground path was walked from the right bank towards the left
bank. To simplify the field work, the operator remained at first on the same
path near the right bank crest and unrolled different line lengths (150, 360
and then 600 m) so that the kite was positioned at the right downwind
distance from the operator. Then, the operator continued to walk the rest of
the ground path towards the right bank and covered the targeted area as
planned. Images were taken with a Sony NEX-5N camera (Fig. <xref ref-type="fig" rid="Ch1.F2"/>b),
which has a 16 Mpix 23.4 <inline-formula><mml:math id="M45" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 15.6 mm sensor. This
camera was used with a fixed 18 mm focal length, and the image stabiliser was
disabled, which are two important settings for the lens auto-calibration step
in SfM processing. This camera was chosen as the best compromise at the time
of the experiment between mass, suitability for photogrammetric analysis and
cost (see Table <xref ref-type="table" rid="App1.Ch1.T1"/> in the Appendix). Automatic
triggering was performed with a gentLED-Auto 05C intervalometer (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a).
A time interval of 5 s between each
image was chosen to ensure sufficient overlap.</p>
      <p id="d1e1062">Complete coverage of the targeted area in the Kamech catchment was achieved
within two flights of 3 h each. A total of 752 images were used to cover
an area of 3.18 km<inline-formula><mml:math id="M46" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>. The maximum flight altitude of 500 m
led to a maximum estimated ground pixel size of 0.13 m (see Table <xref ref-type="table" rid="Ch1.T2"/>
for a summary of all these data). The upstream part of the catchment being crossed by a power
line, we avoided having the kite line near it for safety reasons. As a
result, a small area of the catchment was not covered by multi-view imagery.
However, more of the area downstream and outside the catchment was reached. As a
result, the data set covered an area of 3.18 km<inline-formula><mml:math id="M47" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>, which
exceeded the area of the catchment itself (2.63 km<inline-formula><mml:math id="M48" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2"><caption><p id="d1e1097">Flight conditions and characteristics of the photogrammetric survey.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Estimated Beaufort</oasis:entry>
         <oasis:entry colname="col2">4–5</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kite used</oasis:entry>
         <oasis:entry colname="col2">10 m<inline-formula><mml:math id="M49" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Line lengths (m)</oasis:entry>
         <oasis:entry colname="col2">150, 360, 600</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Flying heights (m)</oasis:entry>
         <oasis:entry colname="col2">120, 300, 500</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GCPs</oasis:entry>
         <oasis:entry colname="col2">8</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Focal length (mm)</oasis:entry>
         <oasis:entry colname="col2">18</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Sensor size (mm)</oasis:entry>
         <oasis:entry colname="col2">23.4 <inline-formula><mml:math id="M50" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 15.6</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Images used</oasis:entry>
         <oasis:entry colname="col2">752</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Max pixel size (m)</oasis:entry>
         <oasis:entry colname="col2">0.13</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Total covered surface (km<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">3.18</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e1227">Finally, eight points (cross marks on Fig. <xref ref-type="fig" rid="Ch1.F1"/>c) that were clearly
visible in the kite images were used as GCPs. Their position was measured
with a Topcon GR-3 RTK DGPS with a theoretical altimetric and planimetric
accuracy of 1.5 cm. These GCPs were used as a spatial reference in the
photogrammetric processing.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <title>DEM computation</title>
      <p id="d1e1238">Kite images were processed with MicMac open-source software
<xref ref-type="bibr" rid="bib1.bibx36" id="paren.41"/>. This software implements both a bundle block adjustment
and a hierarchical, true multi-view dense matching algorithm that is<?pagebreak page1572?> also
used by the French Institut Géographique National to produce 3-D
cartography. MicMac hierarchically computes multi-view dense matching from
coarse grids to the full resolution by gradually refining the results at
successive scales. The full resolution of the DEM is the average ground
resolution of the images, which is estimated from the average flying height.
This average flying height itself is estimated from the mean flight altitude
and the average altitude of key points computed with the SIFT algorithm
<xref ref-type="bibr" rid="bib1.bibx22" id="paren.42"/>. All images covering the same point of interest are taken
into account in the same bundle adjustment for the calculation of each point
in the DEM. This procedure results in an altimetric precision of 1 pixel on
average. The MicMac process is typical of SfM <inline-formula><mml:math id="M52" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> MVS algorithms (see Appendix)
and is comparable with them (see for instance <xref ref-type="bibr" rid="bib1.bibx44" id="altparen.43"/> and
<xref ref-type="bibr" rid="bib1.bibx19" id="altparen.44"/>).</p>
      <p id="d1e1260">The SfM step (i.e. SIFT point recognition and matching plus bundle
calibration) is completely automatic and followed by two manual steps. First,
the area for dense image matching was selected. Second, the GCP positions
were manually digitised in the images to give the project a cartographic
reference. The automatic MVS dense image matching was finally run and
resulted in a 0.20 m DEM. All image processing was performed on a laptop
computer with an Intel Core i7-3840QM CPU at 2.80 GHz and 32 GB of RAM.</p>
</sec>
<sec id="Ch1.S2.SS5">
  <title>Gully detection</title>
      <p id="d1e1270">Similarly to <xref ref-type="bibr" rid="bib1.bibx8" id="normal.45"/>, a gully is considered in this study to be a
morphological object with a marked depression that is in the immediate
proximity of a channel, the latter being determined by another algorithm. To
delimit depressions, most recent studies use sliding windows. For example,
<xref ref-type="bibr" rid="bib1.bibx8" id="normal.46"/> use a sliding “normalised elevation” kernel. We chose
another approach: we convolved the DEM with a Gaussian kernel by computing
the inverse Fourier transform of the pointwise product of the Fourier
transforms of the DEM and the Gaussian kernel. This method has two
advantages. The first relates to computation time: with the Fourier
transforms, the algorithm has a computational complexity of <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:mi>O</mml:mi><mml:mo>(</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:math></inline-formula> log(<inline-formula><mml:math id="M54" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>)),
with <inline-formula><mml:math id="M55" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> being the total number of pixels of the DEM. Sliding window
algorithms have a computational complexity of <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mi>O</mml:mi><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>.</mml:mo><mml:mi>m</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, with <inline-formula><mml:math id="M57" display="inline"><mml:mi>m</mml:mi></mml:math></inline-formula> being the
window size in pixels. Hence, convolution with Fourier transforms is faster
than filtering with sliding windows, except for very small windows. Above
all, the processing time with convolution is independent of the kernel size.
The second advantage is as follows: convolution by a Gaussian kernel
simulates diffusive processes. Hence the DEM after convolution represents the
hypothetical future shape of the ground surface after the processes involved
in linear erosion have stopped and the processes leading to the healing of
the gullies have begun.</p>
      <p id="d1e1331">For the delimitation of the channel network, the fully automated algorithm
proposed by <xref ref-type="bibr" rid="bib1.bibx34" id="normal.47"/> was tested at first (results not reported
here). With this algorithm, the automated localisation of gully heads
detected by high positive plan curvatures presented flaws. We observed that
different threshold values – including the proposed default value – resulted
either in an excessive number of missing gully heads or in categorising many
anthropogenic depressions as gully heads, such as village streets or spaces between trees in
orchards. As noted by <xref ref-type="bibr" rid="bib1.bibx33" id="normal.48"/>, the automatic
detection of channel heads is indeed most problematic for small-scale
features such as some of those targeted by our work. Thus, gully heads
were digitised from a shaded view of the DEM with the same type of expertise
as one would use in the field. This approach was used by <xref ref-type="bibr" rid="bib1.bibx17" id="normal.49"/> to
produce their validation data set. The entire digitisation of the gully heads
on the DEM was achieved within less than 2 h. Once the gully heads were
digitised, the algorithm followed the flow chart in Fig. <xref ref-type="fig" rid="Ch1.F3"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p id="d1e1347">Flow chart of the method used to map gullies from the kite DEM. The
letters associated with each step are referenced in the text describing the
method in Sect. <xref ref-type="sec" rid="Ch1.S2.SS5"/></p></caption>
          <?xmltex \igopts{width=213.395669pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018-f03.png"/>

        </fig>

      <p id="d1e1357">The raw DEM (Fig. 3a) was convoluted with a Gaussian kernel (b) of a standard
deviation of 10 m, which resulted in the smoothed DEM (c). We chose this
value so that twice the standard deviation of the kernel was equal to the
width of the largest gullies to be detected (i.e. 20 m). The raw DEM (a) was
subtracted from the smoothed DEM (c) to create a depth map (d), which was
therefore the estimated depth of the<?pagebreak page1573?> natural surface below the smoothed
surface. Step (e) consisted of applying a threshold to the depth map and cleaning
the result up. The threshold was chosen as slightly larger than the pixel
size considering that lower differences in elevation would probably be noise.
Features that did not show depths greater than 25 cm were hence discarded. The
cleaning consisted of pruning out patches with volumes less than 1 m<inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula>. This value allowed us to eliminate small-scale noise while keeping
each detail of the gullies, even when they were made of discontinuous
patches. Step (e) resulted in the (f) map. Steps (a) to (f) are
illustrated with a section view in Fig. <xref ref-type="fig" rid="Ch1.F4"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p id="d1e1374">Principle of gully detection: (1) a Gaussian kernel with a 10 m
standard deviation; (2) original (blue) and smoothed (red) topography; (3) raw
negative differences between the original and smoothed topography; (4)
detection of the potential gullies, then pruning out elements of less than
1 m<inline-formula><mml:math id="M59" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula>; and (5) profiles of the detected gullies.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018-f04.png"/>

        </fig>

      <p id="d1e1392">Steps (g) to (k) correspond to the extraction of the hydrological network. To
map the hydrological network downstream of the previously digitised gully
heads (g), a depression-free DEM (i) was generated from the raw DEM by
filling gaps (h). The hydrological network (j) was generated by a steepest
descent algorithm in (i) from gully heads (g). Considering the typical width
of the gullies at the test site, a binary map (k) of the areas located less
than 15 m from the network was computed. Intersecting the binary maps
(f) and (k) resulted in the final gully map (m).</p>
</sec>
<sec id="Ch1.S2.SS6">
  <title>Validation</title>
<sec id="Ch1.S2.SS6.SSS1">
  <title>DEM quality</title>
      <p id="d1e1406">The kite DEM quality was evaluated on an independent validation data set
composed of 469 points (see Fig. <xref ref-type="fig" rid="Ch1.F1"/>c for their localisation)
and the median error, mean error and standard deviation of error were used as
evaluation criteria. This control data set was surveyed with the same Topcon
GR-3 RTK DGPS used for GCPs. These data came from a recurrent operation of
bathymetry and topography of the reservoir performed a few weeks before image
acquisition and from which points covered by vegetation were excluded. A
qualitative assessment was also performed with a visual inspection of the
kite DEM at full resolution.</p>
</sec>
<sec id="Ch1.S2.SS6.SSS2">
  <title>Gully map</title>
      <p id="d1e1417">The quality of the gully map derived from the kite DEM was also assessed with
independent data. The gully map was compared to a gully network derived from
a field survey and completed by the interpretation of a QuickBird image. The
field survey was carried out between 2009 and 2012 on nearly 70 % of the
total gully and wadi network length of the Kamech catchment
<xref ref-type="bibr" rid="bib1.bibx3" id="paren.50"/>. Each gully and wadi was divided into sections
whenever a branching (confluence) or significant change in the
cross-section size was identified. For each gully upstream, middle and
downstream positions were recorded with a handheld Garmin eTrex GPS. The
precise delineation of each section was photo-interpreted on the
orthorectified pan-sharpened QuickBird image using the upstream, middle and
downstream GPS positions of the surveyed sections. Gully sections that were
not described during the field survey were delineated on the orthorectified
pan-sharpened QuickBird image only.</p>
      <p id="d1e1423">As in <xref ref-type="bibr" rid="bib1.bibx45" id="normal.51"/>, the field-mapped network was considered as a
reference and two parameters were computed from the match: “the
false negative (underdetection), which is the length of the reference
not included in the extracted network domain, and the false positive
(overdetection), which is the length of the extracted network not
included in the reference domain.” We also added a parameter that aimed to
represent the overall accuracy and that was computed as the ratio of the
total length of correctly mapped gullies to the total length of surveyed
gullies.</p>
</sec>
<sec id="Ch1.S2.SS6.SSS3">
  <title>Gully 3-D morphology</title>
      <p id="d1e1435">Finally, we tested the ability of the DEM to derive 3-D information that
allows for gully morphology monitoring. This evaluation was based on a
profile comparison of the kite DEM with a reference DEM derived from an
intensive field topographic survey of a mid-size gully. This reference DEM
was calculated on a 0.05 by 0.05 m grid from a very dense point data set
acquired in 2009 using a total station that had an (<inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:mi>X</mml:mi><mml:mo>,</mml:mo><mml:mi>Y</mml:mi><mml:mo>,</mml:mo><mml:mi>Z</mml:mi></mml:mrow></mml:math></inline-formula>) accuracy better
than 0.01 m <xref ref-type="bibr" rid="bib1.bibx21" id="paren.52"/>. Standard statistics on the deviation
between the kite DEM and the reference DEM were derived on an elevation
profile of a path composed of a series of line segments.</p>
</sec>
</sec>
</sec>
<?pagebreak page1574?><sec id="Ch1.S3">
  <title>Results</title>
<sec id="Ch1.S3.SS1">
  <title>Simulated line characteristics</title>
      <p id="d1e1470">Figure <xref ref-type="fig" rid="Ch1.F5"/> shows the results of kite line shape simulations
with different wind speeds, line characteristics and physical processes
taken into account.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><caption><p id="d1e1477">Comparison of the shapes on the 300 m lines (black bold) with perfect ones
(thin grey) on a kite flown under different wind conditions and with different line
materials. Simulations were performed at five wind speeds from 3
to 11 m s<inline-formula><mml:math id="M61" 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> in steps of 2 m s<inline-formula><mml:math id="M62" 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>. The load of the rig
(Fig. <xref ref-type="fig" rid="Ch1.F2"/> – right) for the simulation is 500 g. Perfect lines
(thin grey) were modelled with negligible weight and drag. <bold>(a)</bold> Dyneema<sup>®</sup>
line (0.39 g m<inline-formula><mml:math id="M63" 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>). <bold>(b)</bold> Polyester line (3 g m<inline-formula><mml:math id="M64" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>).</p></caption>
          <?xmltex \igopts{width=213.395669pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018-f05.png"/>

        </fig>

      <p id="d1e1546">This figure revealed the following three findings: (i) with light and thin lines,
the kite line is almost straight, and the flying angle is maximal; (ii) when the
kite is flown in sufficiently strong wind, wind speed variations cause only small
effective flight angle variations; and (iii) the latter observation is all the more
true when the kite line is thin and light. These conclusions corroborate the field
observations, which made us choose a thin and light line for photogrammetric acquisitions.
Using a thin and light kite line – and a kite adapted to the actual wind conditions
at the time of image acquisition – is hence a key condition for obtaining a steady
flight angle and the required stable position of the kite relative to the operator.</p>
      <p id="d1e1549">Figure <xref ref-type="fig" rid="Ch1.F6"/> shows the simulated flight angle as a function of
the line length for the Dyneema<sup>®</sup>  line and polyester line.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><caption><p id="d1e1560">Simulation of the variation in flight angle with the line length for different
winds and line materials. Simulations were performed with five wind speeds from
3 to 11 m s<inline-formula><mml:math id="M65" 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> in steps of
2 m s<inline-formula><mml:math id="M66" 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>. <bold>(a)</bold> Dyneema<sup>®</sup> line. <bold>(b)</bold> Polyester line.</p></caption>
          <?xmltex \igopts{width=213.395669pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018-f06.png"/>

        </fig>

      <p id="d1e1602">For both cases, the simulations showed that the flight angle dropped with
increasing line length. The drop was slight for the Dyneema<sup>®</sup>
but critical for the polyester line due to the stronger “banana shape” of the
line observed in Fig. <xref ref-type="fig" rid="Ch1.F5"/>. Hence, the use of thin and light
kite lines such as Dyneema<sup>®</sup>  lines allows for kite flights
with a steady flight angle at a given line length (Fig. <xref ref-type="fig" rid="Ch1.F5"/>)
but also with various line lengths (Fig. <xref ref-type="fig" rid="Ch1.F6"/>). This steady flight angle makes the line
length the only factor influencing the variation in the kite position relative to
the operator. As a consequence, kite flights can effectively be planned and
then properly realised. However, it is recommended to use a margin of
security, considering the slight drop in flight angle for greatest line
lengths. These findings were confirmed by the field experiments presented in
the following section.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Observed kite flight angles</title>
      <p id="d1e1623">Figure <xref ref-type="fig" rid="Ch1.F7"/> shows the measured effective flight angles
for the two kites used with the Dyneema<sup>®</sup>  line for different
line lengths and different wind conditions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p id="d1e1633">Observed flight angles for the two kites and various wind speed
conditions and line lengths. Wind conditions (in italics) are expressed in
the Beaufort scale. Measured flight angles were grouped in min/max boxes for
each flight. Blue boxes represent the behaviour of the 10 m<inline-formula><mml:math id="M67" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> kite and black boxes represent the behaviour of the 4 m<inline-formula><mml:math id="M68" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> kite.</p></caption>
          <?xmltex \igopts{width=213.395669pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018-f07.png"/>

        </fig>

      <p id="d1e1660">This figure corroborates the simulation results shown in Fig. <xref ref-type="fig" rid="Ch1.F6"/>:
during field experiments, the flight angle
dropped slightly but significantly with line length. This drop must hence be
taken into account in preparation for image acquisition. We also noted that
the smaller kite – which has a tail –<?pagebreak page1575?> flew at a significantly lower angle
than the larger one. These experiments also included a flight (the leftmost
blue box in Fig. <xref ref-type="fig" rid="Ch1.F7"/>) with insufficient wind strength
to fly the 10 m<inline-formula><mml:math id="M69" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> kite, which resulted in a
wider range of flight angles and greater variability in the camera position
relative to the operator. This result confirms that even with a thin and
light line, the kite must fly within the appropriate wind conditions so that
the flight angle remains steady.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <title>DEM quality</title>
      <p id="d1e1682">The quantitative assessment of the DEM quality is reported in Table <xref ref-type="table" rid="Ch1.T3"/>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3"><caption><p id="d1e1690">DEM altimetric error statistics.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Mean (m)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M70" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.06</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Median (m)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M71" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.07</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Standard deviation (m)</oasis:entry>
         <oasis:entry colname="col2">0.22</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">90 % confidence interval (m)</oasis:entry>
         <oasis:entry colname="col2">[<inline-formula><mml:math id="M72" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.29; 0.81]</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Sample size</oasis:entry>
         <oasis:entry colname="col2">469</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e1769">The error statistics demonstrated good agreement between the kite DEM and the
independent DGPS-surveyed validation data set. In particular, the mean error
and median error were smaller than the pixel size and the standard deviation
of the error was of the order of the pixel size. These figures show that the
DEM acquired by kite constitutes a reliable model of the catchment
topography.</p>
      <p id="d1e1772">Moreover, a qualitative assessment of the kite DEM was carried out with a
manual inspection of full-resolution DEM shaded views with three close-ups
(Fig. <xref ref-type="fig" rid="Ch1.F8"/>). The assessment showed that the kite DEM planimetric and
altimetric resolutions allow for the visual detection of numerous landscape
features, including most man-made structures (roads, tracks, buildings) and
gully heads that were identified in the field (e.g. Fig. <xref ref-type="fig" rid="Ch1.F8"/>a and b). The plot locations and limits were also clearly depicted
(Fig. <xref ref-type="fig" rid="Ch1.F8"/>a). Indeed, the boundaries between two separate adjacent
plots are not exposed to tillage erosion and finally form small humps that
are visible in the DEM. In the main thalweg (Fig. <xref ref-type="fig" rid="Ch1.F8"/>c), marks of
regressive erosion were visible, and headcut locations could easily be
identified. The potential of the kite DEM for use in extensive gully mapping
within an area of several square kilometres is quantitatively evaluated in
the next section.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p id="d1e1786">Shaded images of the computed DEM over the Kamech test site. The main
image is a classical shading of the DEM computed with a unique illumination
source located in the east. The three zoomed-in panels are shaded images computed
as the portion of visible sky at each point. This latter type of shading
highlights local features such as steep slopes and areas of high curvature:
<bold>(a)</bold> shows some cultivated plots with the plot borders easily visible and a
gully head downstream of the plots; <bold>(b)</bold> shows a gully head; and <bold>(c)</bold> shows the main
thalweg headcut, which is experiencing slow regressive erosion processes.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018-f08.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS4">
  <title>Assessment of 3-D gully modelling</title>
      <p id="d1e1810">An assessment of the gully network delineation was conducted at the scale of
the whole channel network, and the 3-D restitution of the internal morphology
of a gully was assessed at the scale of a single gully. Figure <xref ref-type="fig" rid="Ch1.F9"/>
shows the final gully map obtained by the proposed method
superimposed on the shaded DEM and a map of the validation results.
Statistics of the comparison between the network extracted from the DEM and
the field reference network are presented in Table <xref ref-type="table" rid="Ch1.T4"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p id="d1e1819">Results of the gully mapping algorithm. <bold>(a)</bold> The gully network
identified from the kite DEM is represented in red and superimposed on the
shaded DEM. <bold>(b)</bold> Comparison with ground survey: yellow lines represent the
part of the network correctly detected by our algorithm; black thick lines
represent gullies detected by our algorithm where no gully was surveyed in
the field (overdetection); blue lines represent gullies that were identified
on the ground but not detected by our algorithm (underdetection); green
lines represent gullies that were identified on ground but not used for error
statistics, because they were outside the Kamech catchment area or their
heads were outside of the area covered by the kite DEM.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018-f09.png"/>

        </fig>

<table-wrap id="Ch1.T4"><caption><p id="d1e1836">Error statistics of the comparison at the scale of the channel
network (Fig. <xref ref-type="fig" rid="Ch1.F9"/>).</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="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:thead>
       <oasis:row>

         <oasis:entry colname="col1"/>

         <oasis:entry namest="col2" nameend="col3" align="center">Gully length </oasis:entry>

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

         <oasis:entry colname="col1"/>

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

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

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

         <oasis:entry colname="col1">Field reference</oasis:entry>

         <oasis:entry colname="col2">18 237</oasis:entry>

         <oasis:entry colname="col3">100 %</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">Good fit</oasis:entry>

         <oasis:entry colname="col2">13 549</oasis:entry>

         <oasis:entry colname="col3">74 %</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">False positives</oasis:entry>

         <oasis:entry colname="col2" morerows="1">1513</oasis:entry>

         <oasis:entry colname="col3" morerows="1">8 %</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">(Overdetection)</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">False negatives</oasis:entry>

         <oasis:entry colname="col2" morerows="1">4688</oasis:entry>

         <oasis:entry colname="col3" morerows="1">26 %</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">(Underdetection)</oasis:entry>

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

      <p id="d1e1938">The analysis of the gully map and the statistics showed a very good agreement
between the detected gullies and the field reference. The overall accuracy
was 74 %, with 8 % overdetection and 26 % of the network length unmapped.
An inspection of the comparison map showed that most gullies that were not
detected by our algorithm were located on the left bank (i.e. the
south-eastern half), where gullies are less incised than those located on the
right bank. Furthermore,<?pagebreak page1576?> most overdetections (gullies found by our algorithm
but not surveyed on the ground) consisted of small gully segments mainly
located on the right bank of the catchment.</p>
      <p id="d1e1942">Next, validation of the 3-D gully map was performed at the local scale and at
very high resolution. Figure <xref ref-type="fig" rid="Ch1.F10"/> shows a 3-D comparison
between a gully modelled by the kite DEM and dense measurements from a total station survey.</p>

      <?xmltex \floatpos{htbp}?><fig id="Ch1.F10"><caption><p id="d1e1949">Comparison of the kite DEM with the ground survey. <bold>(a)</bold> Plan of
the gully showing a gauging station at the gully outlet (white), two dense
shrub patches of approximately 1 m height on the sides of the gully
(dark black) and three patches of recent manure application (brown) in the
field on the left bank of the gully; the graduated black line shows where
profiles have been extracted. <bold>(b)</bold> Comparison of kite DEM (red) and ground
survey (black) profiles; the vertical dashed lines delimit areas covered with
shrubs. <bold>(c)</bold> Difference between the kite DEM and the ground survey along the
same profile. Error statistics computed on this area are reported in Table
<xref ref-type="table" rid="Ch1.T5"/>.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/18/1567/2018/nhess-18-1567-2018-f10.png"/>

        </fig>

      <p id="d1e1969">Comparison of the profiles extracted from the kite DEM and from the surveyed
DEM showed good agreement along the whole profile, except for areas covered
by vegetation. The influence of vegetation was clearly detected (Fig. <xref ref-type="fig" rid="Ch1.F10"/>c), with elevation differences significantly differing
from the surrounding noise. These observations were supported by the
associated error statistics (Table <xref ref-type="table" rid="Ch1.T5"/>),
with a mean error of <inline-formula><mml:math id="M73" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.08 m, which decreases to <inline-formula><mml:math id="M74" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.002 m when not taking into
account zones covered by vegetation (parts of the profiles surrounded by
vertical dashed lines in Fig. <xref ref-type="fig" rid="Ch1.F10"/>b and <xref ref-type="fig" rid="Ch1.F10"/>c). These results indicate that the kite DEM constitutes a
reliable source of topographic data for the description of gully erosion
forms. These findings seem likely to be extended for other gullies
considering the good accordance between error statistics shown in Tables <xref ref-type="table" rid="Ch1.T5"/>
and <xref ref-type="table" rid="Ch1.T3"/>.</p>

<table-wrap id="Ch1.T5"><caption><p id="d1e2001">Error statistics at the scale of the gully shown in
Fig. <xref ref-type="fig" rid="Ch1.F10"/>.</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="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Error statistics (m)</oasis:entry>
         <oasis:entry colname="col2">Whole gully</oasis:entry>
         <oasis:entry colname="col3">Gully without vegetation</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Minimum</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M75" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.49</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M76" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.49</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">1st quartile</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M77" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.13</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M78" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.14</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Median</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M79" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.003</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M80" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.01</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Mean</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M81" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.08</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M82" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.002</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SD</oasis:entry>
         <oasis:entry colname="col2">0.33</oasis:entry>
         <oasis:entry colname="col3">0.20</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">3rd quartile</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M83" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.19</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M84" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.14</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Maximum</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M85" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>1.52</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M86" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.66</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?pagebreak page1577?><p id="d1e2192">Moreover, a comparison of the quartiles estimated from the whole gully and
from the non-vegetated part of the gully showed that vegetation mainly
resulted in larger positive extrema, whereas the first, second and third
quartiles remained comparable. The results at this scale were very similar to
those computed with the 469 ground points sampled near the lake (Table <xref ref-type="table" rid="Ch1.T3"/>
above), with a standard deviation of the error
for the DEM statistics being closer to that for the non-vegetated case. This
result may indicate that vegetation is more likely to result in local errors
rather than in a global deviation.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <title>Discussion</title>
      <p id="d1e2204">In this study, we comprehensively assessed a cost-effective workflow to map
gullies at the scale of the elementary watershed from images acquired by
kite. Several important considerations have emerged. These considerations
refer to the image acquisition step, the quality of the kite DEM and the
accuracy of the gully map.</p>
<sec id="Ch1.S4.SS1">
  <title>Large photogrammetric data sets with kites</title>
      <p id="d1e2212">Our study showed that achieving coverage of several square kilometres with
decimetre resolution and accuracy was possible with basic equipment for the
acquisition of a photogrammetric data set. These results represent an
improvement over those presented in <xref ref-type="bibr" rid="bib1.bibx13" id="normal.53"/>, where the same
acquisition method was also used successfully over an area of only one-tenth
of that covered in this study. In other works that obtained DEMs with kites,
the maximum areas covered were also of the order of several hectares
(<xref ref-type="bibr" rid="bib1.bibx55" id="altparen.54"/>; <xref ref-type="bibr" rid="bib1.bibx23" id="altparen.55"/>; <xref ref-type="bibr" rid="bib1.bibx40" id="altparen.56"/>;
<xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx4" id="altparen.57"/>; <xref ref-type="bibr" rid="bib1.bibx10" id="altparen.58"/>). Our results clearly
constitute an extension of the kite's capability. In particular, our work
presents novel findings on the conditions that must be met to make kite
photogrammetric acquisition successful at this scale. A correct realisation
of a planned flight is hence a critical issue for tethered platforms, as has
been noted by others (<xref ref-type="bibr" rid="bib1.bibx50" id="altparen.59"/>; <xref ref-type="bibr" rid="bib1.bibx28" id="altparen.60"/>).
Numerical and field experiments have revealed that the choice of kite line
was a key factor in the success of our workflow. To the best of our
knowledge, the importance of the kite line for a proper photogrammetric
acquisition has rarely been considered with both numerical and field
experiments in previous works. <xref ref-type="bibr" rid="bib1.bibx51" id="normal.61"/> stressed out the
importance of a thin and light line on the basis of personal and external
<xref ref-type="bibr" rid="bib1.bibx6" id="paren.62"><named-content content-type="pre">e.g.</named-content></xref> empirical observations and advised the use of
Dyneema<sup>®</sup>  to mitigate line sag. Our study hence corroborated
previous empirical observations and provided new insights on the importance
of the kite line, with original numerical experiments.</p>
      <p id="d1e2251">If kites are proven to be valuable platforms for photogrammetric acquisition,
they have some limitations. The two main limitations are (i) the fact that
the line must be clear of obstacles and (ii) the need for a minimal wind
speed. We faced the first issue in the most upstream part of the catchment because of a power line.
Obstacles can also be found in densely vegetated or densely urbanised areas. Cases of obstruction
have also been discussed by <xref ref-type="bibr" rid="bib1.bibx50" id="normal.63"/>, who concluded that not every place is suitable for
performing image acquisition from tethered platforms. The second issue, also
noted by <xref ref-type="bibr" rid="bib1.bibx5" id="normal.64"/>, can be approached as in <xref ref-type="bibr" rid="bib1.bibx52" id="normal.65"/>, who
used a kite to which a small helium blimp was added. <xref ref-type="bibr" rid="bib1.bibx23" id="normal.66"/> used
kites and balloons in alternation. In our opinion, in most cases, when the
use of RPASs is not hampered by local regulations, kites associated with
small-format multi-rotor RPASs represent a relevant all-weather solution.
Indeed, the great advantage of small RPAS systems, in addition to being
fairly inexpensive platforms, is the fact that they can provide very high-resolution spatio-temporal data with reduced response times in varied
conditions <xref ref-type="bibr" rid="bib1.bibx30" id="paren.67"/>. However, typical small-format RPASs may remain
grounded during windy periods, thus preventing the requested rapid response.
The other main niche for kites is related to local regulations, either for
the flight itself or due to regulations regarding crossing borders with the
equipment.</p>
      <p id="d1e2269">On another note, kites can fly for hours when weather conditions are
appropriate. This autonomy represents a completely different paradigm
to that for most RPASs. With the equipment presented above, the
overall autonomy was only limited by the internal power supply of the camera.
Within a single flight of 3 h, several thousand overlapping images
can be acquired. This figure gives an idea of the mapping potential of this
method, which produces DEMs in the gigapixel range.</p>
</sec>
<sec id="Ch1.S4.SS2">
  <title>DEM quality</title>
      <p id="d1e2278">Beyond the ability to acquire 3-D data over several square kilometres with
kites, our aim was to demonstrate that these topographic data were reliable.
We showed that the estimated altimetric bias was lower than the pixel size
and that the estimated deviations were in the order of magnitude of pixel size. In other
words, validation with an independent ground survey showed that the produced
DEM had a decimetre resolution and accuracy.</p>
      <p id="d1e2281">Few works using kites have assessed the DEM elevation error. Our results
compare quite well with these works. <xref ref-type="bibr" rid="bib1.bibx55" id="normal.68"/> achieved a
<inline-formula><mml:math id="M87" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.13 m mean error, 0.36 m standard deviation of the error and 0.75 m<?pagebreak page1578?> maximal
error on a 0.25 m resolution DEM (one thousand validation points).
<xref ref-type="bibr" rid="bib1.bibx40" id="normal.69"/> acquired images with an estimated 0.01–0.02 m ground
sampling distance. The authors obtained a <inline-formula><mml:math id="M88" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.01 m mean error and 0.065 m
standard deviation error estimated with 399 independent validation points.
<xref ref-type="bibr" rid="bib1.bibx49" id="normal.70"/> acquired images with a 0.03–0.08 m ground sampling
distance and computed a 0.04 m resolution DEM of a test site of roughly 10 ha.
They estimated <inline-formula><mml:math id="M89" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M90" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M91" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula> errors with 61 independent validation
points and found a mean error of 0.04 m and RMSE of 0.16 m on the altitudes.
<xref ref-type="bibr" rid="bib1.bibx13" id="normal.71"/> computed a DEM with a ground sampling distance of 0.06
m. A quality check with 176 independent validation points resulted in a mean
error of <inline-formula><mml:math id="M92" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.04 m and a standard deviation of 0.07 m. Finally, with 0.004 m
resolution images acquired on a 50 by 150 m area and a final DEM ground
sampling distance of 0.05, <xref ref-type="bibr" rid="bib1.bibx4" id="normal.72"/> estimated the mean error at
<inline-formula><mml:math id="M93" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.019 m and the standard deviation at 0.055 m with 86 validation points. Our
work confirmed that the range of kites can be extended to several square
kilometres with decimetre resolution while maintaining the accuracy in the
pixel size range.</p>
</sec>
<sec id="Ch1.S4.SS3">
  <title>Gully network map and 3-D gully morphology</title>
      <p id="d1e2356">Although the overall accuracy of 74 % proved that our method was effective,
the very process of validating the gully maps obtained from high-resolution
DEM processing raises issues. To begin, validation methods are quite varied
in the literature. Most authors (<xref ref-type="bibr" rid="bib1.bibx15" id="altparen.73"/>; <xref ref-type="bibr" rid="bib1.bibx2" id="altparen.74"/>;
<xref ref-type="bibr" rid="bib1.bibx17" id="altparen.75"/>; <xref ref-type="bibr" rid="bib1.bibx8" id="altparen.76"/>) have used manual digitisation of
the gullies on the DEM as validation data and focused on different gully
characteristics: width and depth <xref ref-type="bibr" rid="bib1.bibx15" id="paren.77"/>, visual comparison
(<xref ref-type="bibr" rid="bib1.bibx2" id="altparen.78"/>; <xref ref-type="bibr" rid="bib1.bibx17" id="altparen.79"/>), and areal and volume difference
(<xref ref-type="bibr" rid="bib1.bibx17" id="altparen.80"/>; <xref ref-type="bibr" rid="bib1.bibx8" id="altparen.81"/>). Some authors (e.g. <xref ref-type="bibr" rid="bib1.bibx31" id="altparen.82"/>) did not even validate the gully mapping results.
Infrequently, studies such as <xref ref-type="bibr" rid="bib1.bibx45" id="normal.83"/> have used field surveys as
validation data for gullies that were automatically mapped from a DEM.
Similarly to their study, our validation data were in the form of a channel
network, and we used the same indicators as they did. We obtained a false
positive rate (overdetection) of 8 % and a false negative rate
(underdetection) of 26 %. Our results compare favourably to those of
<xref ref-type="bibr" rid="bib1.bibx45" id="normal.84"/>, who had false positive rates ranging from 5 to 16 %
and false negative rates ranging from 29 to 55 %. Moreover, our results
follow the same tendency, with false negatives rates being higher than false
positives. This result may be explained by the fact that all gully mapping
algorithms, including the one presented here, are based on the morphological
characteristics of gullies (i.e. what a gully is) but do not benefit from
characteristics that are known not to be shown by gullies (i.e. what a gully
is not). In our opinion, this approach would be especially useful for
avoiding confusion between gullies and man-made structures, which may be
among the most delicate features to handle. This confusion may indeed explain
some of the remaining inaccuracies we observed, and more generally, these
issues have also been faced by others <xref ref-type="bibr" rid="bib1.bibx8" id="paren.85"/>.</p>
      <p id="d1e2400">The detection of gullies in DEMs faces the difficulty of determining an
unambiguous and generic definition of what a gully is. <xref ref-type="bibr" rid="bib1.bibx8" id="normal.86"/>
indicated that to their knowledge, no one has yet assessed where gullies
“begin” in the transverse direction. Conversely, <xref ref-type="bibr" rid="bib1.bibx15" id="normal.87"/> stated that
“gully edges are the critical features for gully mapping”.
<xref ref-type="bibr" rid="bib1.bibx2" id="normal.88"/> noted that the assumptions usually used in channel-like
extraction techniques do not apply to the environment of alluvial fans in
which they propose an ad hoc gully mapping method. In brief, due to the
variety of gully shapes and the fuzzy definition of their extent, each gully
mapping algorithm in the literature so far requires the manual tuning of
parameters and/or thresholds and is preferably applied to specific
landscape types.</p>
      <p id="d1e2412">A possible workaround would be the use of multi-scale analysis, which was
still seen by <xref ref-type="bibr" rid="bib1.bibx35" id="normal.89"/> as a future research direction for
high-resolution topography analysis. For future work in this direction, our
algorithm has the advantage of being based on Fourier transforms instead of
sliding windows, which makes the computation time independent of the
characteristic size of the kernel and hence opens the door to multi-scale
filtering with controlled computation times. Computing time is indeed one
issue for DEM processing: for instance <xref ref-type="bibr" rid="bib1.bibx8" id="normal.90"/> have been unable
to process the full resolution of their largest DEM. Considering that
upcoming topographic data sets will probably be more extensive and will have
higher resolutions, this may still be an issue that will have to be
mitigated by algorithmic improvements such as the one we have proposed.</p>
      <p id="d1e2421">The interest in multi-scale approaches is as strong as the 3-D information of
such DEMs is rich, which is the case for the data obtained in our study. The
comparison of dense elevation profiles between the kite DEM and ground
reference hence showed good agreement. These findings thus confirmed, at a
very local scale, the results on DEM accuracy found at the scale of the whole
DEM. However, this detailed analysis raised the issue of vegetation cover.
This issue is present in several classical cases where image-based approaches
have limits that lidar does not have. However, with big image data sets,
SfM <inline-formula><mml:math id="M94" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> MVS DEMs can reach densities that are comparable to or even exceed
those of aerial lidar point clouds. This property would allow for the
development of vegetation filtering algorithms tailored to these dense and
multi-view image data. Second, our results can be compared to the work of
<xref ref-type="bibr" rid="bib1.bibx23" id="normal.91"/>, who used kites and balloons with a focus on two gullies.
They determined that gully morphology and even gully changes could be
assessed. In our case, with comparable sensibility and data available at the
scale of the whole catchment, this morphological information would enable the
description of different processes that occurred in different gullies or even
at<?pagebreak page1579?> different times in the same gully, such as renewed erosion in older gully
systems. Further work may then repeat our experiments to monitor ongoing
gully erosion processes. These experiments would indeed be of great help, for
instance, in understanding the source of the sediments responsible for reservoir
siltation.</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusions</title>
      <p id="d1e2442">This paper proposes a complete workflow, from image acquisition with kites to
a final gully map at the scale of a kilometre-square catchment with a careful
assessment of each step. For image acquisition, we found that a key factor
was the use of a thin and light line, which results in steady kite flight
angles and thus a proper realisation of a kite photogrammetric flight in such
large areas. Then, we showed that low-tech kite aerial photography could be
successfully used for the acquisition of a high-resolution DEM covering more
than three square kilometres with decimetre resolution and accuracy. Finally,
we demonstrated that an appropriate gully mapping algorithm developed and
applied to this DEM proved to be appropriate for the characterisation of
gullies with 3-D decimetre details. Correct matches were obtained for 74 % of
the gully lengths at the scale of an entire channel network. Still, kites
require minimal wind speeds. This technique may therefore be thought of as a
tool to be used in conjunction with small-format RPASs, especially when the
latter cannot fly because of technical or administrative obstacles. Then, the
proposed gully mapping method requires the intervention of an operator for
the digitisation of gully heads. This approach may not be adapted to contexts
with an excessive number of individual channels but proved appropriate in
pruning the false positives produced by automatic procedures on anthropogenic
features. Nevertheless, our study demonstrated that kite aerial photography
using simple but appropriate equipment and an appropriate gully mapping
algorithm represents a valuable tool for accurately surveying several hundred
gullies at the scale of a kilometre-square watershed with decimetre detail,
which may compare favourably with most ground surveys at these scales. These
findings suggest that kites, SfM <inline-formula><mml:math id="M95" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> MVS, and adequate gully mapping algorithms
provide greater access to high-resolution topographic data of
kilometre-square watersheds and will facilitate a better understanding of
gullying processes in a broader spectrum of conditions.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability">

      <p id="d1e2456">Image data and digital elevation model can be shared for collaboration purposes upon request by
contacting the corresponding author.</p>
  </notes><?xmltex \hack{\clearpage}?><app-group>

<?pagebreak page1580?><app id="App1.Ch1.S1">
  <title>MicMac workflow</title>
      <p id="d1e2468">Description of the commands used sequentially in the typical MicMac pipeline,
from images to DEMs and orthophotographs:
<list list-type="bullet"><list-item>
      <p id="d1e2473">Tapioca: SIFT points are computed and matched; image resampling ratio
affects the number of SIFT points.</p></list-item><list-item>
      <p id="d1e2477">Tapas: image orientation and auto-calibration takes place; memory requirements
grow with the number of SIFT points and images and can be prohibitive; there are possible
workarounds with RedTieP/OriRedTieP.</p></list-item><list-item>
      <p id="d1e2481">Tarama: a first raw mosaic of the area is computed; it can be used to obtain a quick estimate
of the covered area.</p></list-item><list-item>
      <p id="d1e2485">SaisieMasq: the area of interest is manually delimited.</p></list-item><list-item>
      <p id="d1e2489">SaisieAppuis: GCP positions in images are manually measured.</p></list-item><list-item>
      <p id="d1e2493">GCPBascule: the model is georeferenced.</p></list-item><list-item>
      <p id="d1e2497">Malt: dense image matching occurs; the final DEM resampling ratio and
regularisation parameters can be adjusted.</p></list-item><list-item>
      <p id="d1e2501">Tawny: orthophotograph mosaicking is completed.</p></list-item></list></p>
</app>

<app id="App1.Ch1.S2">
  <title>Criteria for the choice of the camera</title>

<?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.T1"><caption><p id="d1e2513">Advantages and drawbacks of three different camera technologies for
acquisition with a kite for photogrammetry. The two first criteria are
specific to kite-borne photogrammetry, while the last criteria are more
general and apply to any photogrammetric application.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.95}[.95]?><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="62.596063pt"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Criteria</oasis:entry>
         <oasis:entry colname="col2">Importance</oasis:entry>
         <oasis:entry colname="col3">Compact</oasis:entry>
         <oasis:entry colname="col4">Hybrid</oasis:entry>
         <oasis:entry colname="col5">DSLR*</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Mass</oasis:entry>
         <oasis:entry colname="col2">high</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mo>+</mml:mo><mml:mo>+</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mo>+</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M101" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Cost</oasis:entry>
         <oasis:entry colname="col2">medium</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mo>+</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M103" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M104" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Prime lens</oasis:entry>
         <oasis:entry colname="col2">medium (<inline-formula><mml:math id="M105" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>*</mml:mo><mml:mo>*</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">No</oasis:entry>
         <oasis:entry colname="col4">Yes</oasis:entry>
         <oasis:entry colname="col5">Yes</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Lens without <?xmltex \hack{\hfill\break}?>moving parts</oasis:entry>
         <oasis:entry colname="col2">high</oasis:entry>
         <oasis:entry colname="col3">No</oasis:entry>
         <oasis:entry colname="col4">Yes</oasis:entry>
         <oasis:entry colname="col5">Yes</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Camera options(<inline-formula><mml:math id="M106" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>*</mml:mo><mml:mo>*</mml:mo><mml:mo>*</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col2">high</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M107" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M108" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mo>+</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Image quality</oasis:entry>
         <oasis:entry colname="col2">medium</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M110" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mo>+</mml:mo><mml:mo>+</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mo>+</mml:mo><mml:mo>+</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table><table-wrap-foot><p id="d1e2516"><inline-formula><mml:math id="M96" display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula> Digital single-lens reflex camera. <inline-formula><mml:math id="M97" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>*</mml:mo><mml:mo>*</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> A lens with the zoom
ring scotch-tapped on is a decent workaround if no prime lens is available.
<inline-formula><mml:math id="M98" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>*</mml:mo><mml:mo>*</mml:mo><mml:mo>*</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> Includes the possibility of switching off the autofocus and the image
stabiliser, both of which make auto-calibration difficult.</p></table-wrap-foot></table-wrap>

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

<app id="App1.Ch1.S3">
  <title>Notes for future kite users</title>
      <p id="d1e2822">It is worth noting that flying large kites, especially in strong winds, can
raise security issues. Aside from <xref ref-type="bibr" rid="bib1.bibx1" id="normal.92"/> and <xref ref-type="bibr" rid="bib1.bibx51" id="normal.93"/>,
this information is still barely reported in the scientific literature. The
problems we faced appeared only under conditions of strong winds. These
problems include small burns on hands, arms or clothes when the line is
moving too fast or when the winder is temporarily out of control during a
wind gust. This problem may also occur when the kite shows erratic movement
in strongest winds when the operator is walking upwind. To avoid such
problems, the following safety measures can be adopted: (i) ensuring physical
protection of the operator with leather gloves, covering clothes and
ensuring the safety of other people by keeping the downwind zone free of
any lightweight and large equipment; (ii) keeping in mind that danger – and
necessary expertise – grows with wind strength, a clever decision may be not
to fly if conditions are not met; (iii) securing the flying gear (attaching
it with hooks, for instance); and (iv) paying attention to equipment and people.</p><?xmltex \hack{\clearpage}?>
</app>
  </app-group><notes notes-type="competinginterests">

      <p id="d1e2836">The authors declare no competing interests.</p>
  </notes><notes notes-type="sistatement">

      <p id="d1e2842">This article is part of the special issue “The use of remotely
piloted aircraft systems (RPASs) in monitoring applications and management of
natural hazards”. It is not associated with a conference.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e2848">The OMERE observatory (<uri>http://www.obs-omere.org</uri>, last access: 29 May 2018), funded by the French
institutes INRA and IRD and coordinated by INAT Tunis, INRGREF Tunis, UMR
Hydrosciences Montpellier and UMR LISAH Montpellier, is acknowledged for
providing a portion of the data used in this study. In particular, we
gratefully acknowledge Kilani Ben Hazzez M'Hamdi, Radhouane Hamdi and Michael
Schibler from IRD Tunis for the work that was carried out in the field to obtain topographic
data. This research was also supported by the TOSCA-CNES project “A-MUSE;
Analyse MUlti-temporelle de données SENTINEL 2 et 1 pour le monitoring de
caractéristiques observables de la surface du sol, en lien avec
l'infiltrabilité”(2018–2019).
<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Daniele Giordan<?xmltex \hack{\newline}?>
Reviewed by: Mitchell Bryson and four anonymous referees</p></ack><ref-list>
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    <!--<article-title-html>Using kites for 3-D mapping of gullies at decimetre-resolution over several square kilometres: a case study on the Kamech catchment, Tunisia</article-title-html>
<abstract-html><p>Monitoring agricultural areas threatened by soil erosion often requires
decimetre topographic information over areas of several square kilometres.
Airborne lidar and remotely piloted aircraft system (RPAS) imagery have the
ability to provide repeated decimetre-resolution and -accuracy digital
elevation models (DEMs) covering these extents, which is unrealistic with
ground surveys. However, various factors hamper the dissemination of these
technologies in a wide range of situations, including local regulations for
RPAS and the cost for airborne laser systems and medium-format RPAS imagery.
The goal of this study is to investigate the ability of low-tech kite aerial
photography to obtain DEMs with decimetre resolution and accuracy that permit
3-D descriptions of active gullying in cultivated areas of several square
kilometres. To this end, we developed and assessed a two-step workflow.
First, we used both heuristic experimental approaches in field and
numerical simulations to determine the conditions that make a photogrammetric flight possible and
effective over several square kilometres with a kite
and a consumer-grade camera. Second, we mapped and characterised the entire
gully system of a test catchment in 3-D. We showed numerically and
experimentally that using a thin and light line for the kite is key for
a complete 3-D coverage over several square kilometres.
We thus obtained a decimetre-resolution DEM covering 3.18&thinsp;km<sup>2</sup> with a
mean error and standard deviation of the error of +7 and
22&thinsp;cm respectively, hence achieving decimetre accuracy. With this data set,
we showed that high-resolution topographic data permit both the detection and
characterisation of an entire gully system with a high level of detail and an
overall accuracy of 74&thinsp;% compared to an independent field survey. Kite
aerial photography with simple but appropriate equipment is hence an
alternative tool that has been proven to be valuable for surveying gullies
with sub-metric details in a square-kilometre-scale catchment. This case
study suggests that access to high-resolution topographic data on these
scales can be given to the community, which may help facilitate a better
understanding of gullying processes within a broader spectrum of conditions.</p></abstract-html>
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