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  <front>
    <journal-meta>
<journal-id journal-id-type="publisher">ESurf</journal-id>
<journal-title-group>
<journal-title>Earth Surface Dynamics</journal-title>
<abbrev-journal-title abbrev-type="publisher">ESurf</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Earth Surf. Dynam.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">2196-632X</issn>
<publisher><publisher-name>Copernicus Publications</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>

    <article-meta>
      <article-id pub-id-type="doi">10.5194/esurf-4-627-2016</article-id><title-group><article-title><?xmltex \hack{\vspace*{-1mm}}?>How does grid-resolution modulate the topographic expression of geomorphic processes?</article-title>
      </title-group><?xmltex \runningtitle{How does grid-resolution modulate geomorphic processes?}?><?xmltex \runningauthor{S.~W.~D.~Grieve et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Grieve</surname><given-names>Stuart W. D.</given-names></name>
          <email>s.grieve@ed.ac.uk</email>
        <ext-link>https://orcid.org/0000-0003-1893-7363</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Mudd</surname><given-names>Simon M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1357-8501</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Milodowski</surname><given-names>David T.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8419-8506</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Clubb</surname><given-names>Fiona J.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Furbish</surname><given-names>David J.</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>School of GeoSciences, University of Edinburgh, Drummond Street, Edinburgh, EH8 9XP, UK</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Earth and Environmental Sciences, Vanderbilt University, Nashville, TN, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Stuart W. D. Grieve (s.grieve@ed.ac.uk)</corresp></author-notes><pub-date><day>8</day><month>August</month><year>2016</year></pub-date>
      
      <volume>4</volume>
      <issue>3</issue>
      <fpage>627</fpage><lpage>653</lpage>
      <history>
        <date date-type="received"><day>10</day><month>May</month><year>2016</year></date>
           <date date-type="rev-request"><day>13</day><month>May</month><year>2016</year></date>
           <date date-type="rev-recd"><day>13</day><month>July</month><year>2016</year></date>
           <date date-type="accepted"><day>25</day><month>July</month><year>2016</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under a Creative Commons Attribution 3.0 Unported License. To view a copy of this license, visit <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by/3.0/">http://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
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</permissions><self-uri xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016.html">This article is available from https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016.html</self-uri>
<self-uri xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016.pdf">The full text article is available as a PDF file from https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016.pdf</self-uri>


      <abstract>
    <p>In many locations, our ability to study the processes which shape
the Earth are greatly enhanced through the use of high-resolution digital
topographic data. However, although the availability of such datasets has
markedly increased in recent years, many locations of significant geomorphic
interest still do not have high-resolution topographic data available. Here,
we aim to constrain how well we can understand surface processes through
topographic analysis performed on lower-resolution data. We generate digital
elevation models from point clouds at a range of grid resolutions from 1 to
30 m, which covers the range of widely used data resolutions available
globally, at three locations in the United States. Using these data, the
relationship between curvature and grid resolution is explored, alongside the
estimation of the hillslope sediment transport coefficient (<inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>, in
m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) for each landscape. Curvature, and consequently <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>, values
are shown to be generally insensitive to grid resolution, particularly in
landscapes with broad hilltops and valleys. Curvature distributions, however,
become increasingly condensed around the mean, and theoretical considerations
suggest caution should be used when extracting curvature from landscapes with
sharp ridges. The sensitivity of curvature and topographic gradient to grid
resolution are also explored through analysis of one-dimensional
approximations of curvature and gradient, providing a theoretical basis for
the results generated using two-dimensional topographic data. Two methods of
extracting channels from topographic data are tested. A geometric method of
channel extraction that finds channels by detecting threshold values of
planform curvature is shown to perform well at resolutions up to 30 m in all
three landscapes. The landscape parameters of hillslope length and relief are
both successfully extracted at the same range of resolutions. These
parameters can be used to detect landscape transience and our results suggest
that such work need not be confined to high-resolution topographic data. A
synthesis of the results presented in this work indicates that although high-resolution (e.g., 1 m) topographic data do yield exciting possibilities
for geomorphic research, many key parameters can be understood in lower-resolution data, given careful consideration of how analyses are performed.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>Geomorphologists have always made use of topographic data, from initial
qualitative observations of surface morphology and its link to process
<xref ref-type="bibr" rid="bib1.bibx31" id="paren.1"><named-content content-type="pre">e.g.,</named-content></xref> to directly measuring landscape
geometries from contour maps, constraining river dynamics and morphometric
relationships (e.g., <xref ref-type="bibr" rid="bib1.bibx39" id="altparen.2"/>, <xref ref-type="bibr" rid="bib1.bibx106" id="altparen.3"/>, and <xref ref-type="bibr" rid="bib1.bibx10" id="altparen.4"/>). Further quantitative analyses
of the Earth's surface were facilitated through the advent of gridded
topographic data. Work to generate digital elevation models (DEMs) from
photogrammetry, contour maps, and active remote sensing platforms
<xref ref-type="bibr" rid="bib1.bibx129 bib1.bibx126 bib1.bibx94 bib1.bibx123" id="paren.5"/>
produced datasets at tens to thousands of meters' grid resolution, along with geomorphic analyses designed for such datasets
<xref ref-type="bibr" rid="bib1.bibx77 bib1.bibx113 bib1.bibx69 bib1.bibx8 bib1.bibx112" id="paren.6"/>.
Algorithms have subsequently been developed which exploit the higher-resolution topographic data now available, predominantly from light detection
and ranging (lidar), which not only refined existing techniques
<xref ref-type="bibr" rid="bib1.bibx79 bib1.bibx80 bib1.bibx12" id="paren.7"/> but also allowed the study of hitherto unresolvable
features on landscapes <xref ref-type="bibr" rid="bib1.bibx115 bib1.bibx122 bib1.bibx100 bib1.bibx15 bib1.bibx114 bib1.bibx65" id="paren.8"/>.</p>
      <p>Presently, lidar data coverage is predominantly focused around locations of
particular scientific interest or infrastructural importance, as can be seen
on many lidar data portals <xref ref-type="bibr" rid="bib1.bibx56" id="paren.9"><named-content content-type="pre">e.g.,</named-content></xref>. It
is unlikely that global lidar coverage can be achieved in the near future,
leaving the provision of commercially available 12 m TanDEM-X data
<xref ref-type="bibr" rid="bib1.bibx55" id="paren.10"/> and freely available 30 m Shuttle Radar
Topography Mission (SRTM) data <xref ref-type="bibr" rid="bib1.bibx94" id="paren.11"/> as the best
available data options for many study sites.</p>
      <p>As a consequence of this data availability it is crucial to understand the
limitations of lower-resolution data when performing topographic analysis for
geomorphic research. Extracting channels from topography is a common
requirement of many analyses, and it is expected that the accuracy of
extracted channel networks will be affected by increasing grid resolution
<xref ref-type="bibr" rid="bib1.bibx78" id="paren.12"/>. <xref ref-type="bibr" rid="bib1.bibx99" id="text.13"/>,
<xref ref-type="bibr" rid="bib1.bibx44" id="text.14"/>, and <xref ref-type="bibr" rid="bib1.bibx33" id="text.15"/> used
measurements of hillslope length and relief to identify signals of landscape
transience. However, all such work was performed on high-resolution
topography and the impact of grid resolution on these metrics is unknown.
<xref ref-type="bibr" rid="bib1.bibx99" id="text.16"/> and <xref ref-type="bibr" rid="bib1.bibx42" id="text.17"/> demonstrated
that the curvature of ridgelines measured from high-resolution topography can
be used as a proxy for erosion rates in soil-mantled landscapes. This
observation has been used in many studies in which cosmogenic radionuclide-derived erosion rates are unavailable <xref ref-type="bibr" rid="bib1.bibx82 bib1.bibx45 bib1.bibx44 bib1.bibx33" id="paren.18"/>.
However, it can also be used in locations with an independent constraint on
erosion rates in order to quantify a sediment transport coefficient that
relates hillslope sediment flux to the topographic gradient, which is set by the
material properties of soils <xref ref-type="bibr" rid="bib1.bibx26" id="paren.19"/>. Therefore,
understanding the effect of grid resolution on the extraction of curvature is
crucial in order to evaluate the applicability of calculating the sediment
transport coefficient from coarse-resolution data.</p>
      <p>Here, we grid topographic data at a range of resolutions in order to test the
sensitivity of these techniques to decreasing grid resolution, with the aim
of placing constraints on the estimation of common geomorphic parameters when
lidar topographic data are unavailable. Through an analysis of one-dimensional curvature and topographic gradient approximations, the changes in
fidelity as grid resolution decreases for both curvature and topographic
gradient are examined and placed within the context of the two-dimensional
results of this study and the wider literature.</p>
<sec id="Ch1.S1.SS1">
  <title>Previous work</title>
      <p>It has long been recognized that the scale of topographic data used in an
analysis or model will have an impact on the scale of the processes which can
be measured <xref ref-type="bibr" rid="bib1.bibx121" id="paren.20"/>. It is intuitive that in order to
measure the properties of hillslope processes the resolution of the data must
be high enough that variations in hillslope form can be captured adequately.
The resolution of topographic data defines the Nyquist frequency, given as
<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mtext>Res</mml:mtext><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> where “Res” is the grid resolution of the dataset
<xref ref-type="bibr" rid="bib1.bibx124" id="paren.21"/>. The inverse of this frequency yields the
minimum wavelength resolvable from a given dataset. In the example of a 1 m
grid resolution, the smallest features that could be resolved would
have a length scale of 2 m. Recognizing this, many authors have
attempted to quantify this uncertainty, aiming to answer the following question: at
what point does a dataset become unsuitable for a given analysis?
<xref ref-type="bibr" rid="bib1.bibx93" id="paren.22"><named-content content-type="pre">e.g.,</named-content></xref>.</p>
      <p>Many attempts to constrain the error content of topographic measurements have
focused on comparisons between elevation values taken from differing
resolution data products, often in conjunction with field survey data, with
the aim of discriminating between DEM generation methods.
<xref ref-type="bibr" rid="bib1.bibx123" id="text.23"/> performed a comparison of DEMs generated
using cartometric and photogrammetric methods against field-surveyed elevation data. They demonstrated that at grid resolutions of 6.25, 12.5, and
25 m the cartometric DEM produced less error than the photogrammetric
DEM when compared to the field-surveyed data, collected at 3.25 m
intervals.</p>
      <p>The advent of lidar-derived topographic data provided a new technique and
increased the range of possible grid resolutions to evaluate.
<xref ref-type="bibr" rid="bib1.bibx38" id="text.24"/> assessed the quality of high-resolution
topographic data sourced from interferometry and lidar for a heavily
vegetated catchment in North Carolina. This analysis demonstrated that, under
such conditions, the lidar-derived DEM outperformed the interferometric data
in addition to both classes of USGS DEM product. However, concerns were
raised about the overall accuracy of the lidar data with a requirement for
improved methodologies to be developed to process multistory vegetation.
Further work was carried out in North Carolina to constrain the minimum
number of lidar returns required to generate a DEM at a given grid resolution
<xref ref-type="bibr" rid="bib1.bibx1" id="paren.25"/>. This work indicated that a 5 m grid (the
finest resolution used) required approximately 115 points ha<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>,
whereas at 30 m grid resolution the requirement reduced to approximately 35
points ha<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.</p>
      <p><xref ref-type="bibr" rid="bib1.bibx121" id="text.26"/> resampled a 1 m lidar-derived DEM to a range of
grid resolutions up to 25 m and assessed the accuracy of elevation
values for each of these resampled grids when compared to a 1 m
resolution field survey. It was found that there was little variation in the
distribution of elevation values between the resampled data sets. However,
when the data was compared with 25 m DEMs generated from topographic maps
and contour generalization, there were considerable errors, supporting
earlier authors' conclusions that lidar-derived topographic data contain more
useful geomorphic information than other methods of topographic data
collection.</p>
      <p>Topographic gradient (or slope) is one of the most fundamental topographic
derivatives across the disparate disciplines which utilize topographic data.
This measurement has been used in geomorphology
<xref ref-type="bibr" rid="bib1.bibx8" id="paren.27"><named-content content-type="pre">e.g.,</named-content></xref>, ecology
<xref ref-type="bibr" rid="bib1.bibx64" id="paren.28"><named-content content-type="pre">e.g.,</named-content></xref>, soil science
<xref ref-type="bibr" rid="bib1.bibx76" id="paren.29"><named-content content-type="pre">e.g.,</named-content></xref>, and hydrology
<xref ref-type="bibr" rid="bib1.bibx132" id="paren.30"><named-content content-type="pre">e.g.,</named-content></xref>. <xref ref-type="bibr" rid="bib1.bibx126" id="text.31"/>
endeavored to constrain the accuracy with which this parameter can be
calculated as grid resolution is increased from 100 to 1000 m and showed
that as the grid resolution is decreased, there is a clear reduction in the
slope values produced for a landscape. Similar wide-scale analysis has also
been performed within the context of global hydrological analysis
(e.g., <xref ref-type="bibr" rid="bib1.bibx46" id="altparen.32"/>, and <xref ref-type="bibr" rid="bib1.bibx49" id="altparen.33"/>),
indicating that from meter to kilometer scale the reduction in quality of
slope measurements is an issue which must be considered when working with
topographic data.</p>
      <p><xref ref-type="bibr" rid="bib1.bibx30" id="text.34"/> considered the accuracy of slope measurements at
locations manually classified as valleys, peaks, and ridges. They found an
initially small increase in the error of slope measurements at intermediate
resolutions (10–20 m) and a much more rapid increase in error between
20 and 30 m resolution, suggesting a threshold minimum resolution for
analysis of these landforms. More recent work has considered how high-resolution lidar data impact the quality of slope measurements.
<xref ref-type="bibr" rid="bib1.bibx121" id="text.35"/> demonstrated a similar trend to previous authors
working with lower-resolution data: as grid resolution is decreased from 1 to
25 m, there is a considerable reduction in the slope values generated
for a landscape. <xref ref-type="bibr" rid="bib1.bibx124" id="text.36"/> evaluated the reliability of
slope measurements by contrasting 10 methods of gradient calculation against
field measurements of topographic gradient. The error between DEM and
field-derived slope measurements was shown to increase with decreasing grid
resolution (from 1 to 12 m), resulting in the recommendation to increase
data resolution wherever possible to decrease errors in topographic analysis.</p>
      <p>Numerous authors have considered the impact of grid resolution on
hydrological applications, which often require slope calculation as a
fundamental processing step. It has been demonstrated across many landscapes
and scales that as grid resolution is decreased the upslope contributing area
will increase and the local slope will decrease, which will have a
significant impact on any hydrological analysis
<xref ref-type="bibr" rid="bib1.bibx127 bib1.bibx132 bib1.bibx128" id="paren.37"/>. Similarly, from
the perspective of modeling global-scale sediment fluxes to the oceans,
<xref ref-type="bibr" rid="bib1.bibx57" id="text.38"/> noted that measurements of slope dropped
logarithmically with increasing grid resolution, and failing to account for
this may lead to a substantial underestimate of the contribution of steep,
montane regions.</p>
      <p><xref ref-type="bibr" rid="bib1.bibx52" id="text.39"/> performed analyses on the accuracy of
hydrological networks generated through photogrammetry and radar
interferometry at 5 and 30 m grid resolution, respectively. Their error
analysis was extended to consider the vertical errors generated both through
the downsampling of the topographic data, as well as from the techniques used
to capture the topographic information. Predicted catchment runoff was up to
7 % larger in the lower-resolution datasets, considered to be driven by both
the vertical errors and the reduction in spatial resolution increasing
variables such as upslope drainage area.</p>
      <p>Topographic wetness index (TWI), calculated as <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>A</mml:mi><mml:mo>/</mml:mo><mml:mi>S</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math display="inline"><mml:mi>A</mml:mi></mml:math></inline-formula> is the
specific upslope area and <inline-formula><mml:math display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula> is the slope, is used as a single variable to
compare the hydrological setting of differing parts of the landscape,
providing insight into factors including groundwater properties and overland
flow rates. <xref ref-type="bibr" rid="bib1.bibx109" id="text.40"/> used lidar data to test the
robustness of TWI calculations on spatial scales ranging from 5 to 50 m,
concluding that the most sensitive part of the TWI calculation was the
specific upslope area measurements. This sensitivity resulted in significant
variation in the TWI values across the range of resolutions tested. Predicted
slope stability, modeled in part as a function of TWI, was assessed by
<xref ref-type="bibr" rid="bib1.bibx116" id="text.41"/>, who demonstrated that, for large-scale landsliding,
a lidar-derived DEM downsampled to 10 m resolution was more suitable to
identify landslide hazard than the highest-resolution data available. This
highlights the requirement to consider the scale of the process being studied
when selecting the appropriate grid resolution for a study and corresponds
to the challenges of selecting the correct size of smoothing window to
capture processes on a suitable scale (e.g., <xref ref-type="bibr" rid="bib1.bibx100" id="altparen.42"/>, <xref ref-type="bibr" rid="bib1.bibx42" id="altparen.43"/>, and <xref ref-type="bibr" rid="bib1.bibx33" id="altparen.44"/>).</p>
      <p>The accuracy of channel network extraction from topographic data was tested
by <xref ref-type="bibr" rid="bib1.bibx75" id="text.45"/>, who tested a 1 m lidar DEM and a 10 m
photogrammetrically generated DEM against a field-mapped channel network in a
catchment in Alberta, Canada. The 1 m lidar-derived channel network was
found to be the best representation of the field-mapped channel network,
exceeding the quality of an additional channel network mapped by hand from
aerial photographs. However, as no intermediate datasets were tested, it is
not possible to understand at what resolution the degradation in channel
network extraction quality occurs for this location.</p>
      <p>As models of agricultural soil loss depend heavily on topographic variables
such as slope, work has been carried out to understand the influence of grid
resolution on calculated rates of soil loss.
<xref ref-type="bibr" rid="bib1.bibx105" id="text.46"/> tested data resolutions from 1 to 81 m
and demonstrated that in all cases, rates of predicted soil loss
increased with grid resolution. However, the rates of soil loss were also
influenced by the type of flow routing utilized, with the multiple flow
direction algorithm (e.g., <xref ref-type="bibr" rid="bib1.bibx25" id="altparen.47"/>, and <xref ref-type="bibr" rid="bib1.bibx93" id="altparen.48"/>) proving most
sensitive to resolution decreases. Work by <xref ref-type="bibr" rid="bib1.bibx23" id="text.49"/>
considering models of crop yields in Colorado, USA, demonstrated that on
relatively flat surfaces, such as agricultural fields, the spatial resolution
is less important than the vertical accuracy when predicting crop yields,
with significant errors being produced due to centimeter-scale vertical
displacements. Decreasing the grid resolution from 5 to 30 m had
limited effect on the yield calculations.</p>
      <p>Although considerable work has been carried out on the sensitivity of various
factors to grid resolution, much of it has been focused on a specific
application (e.g., <xref ref-type="bibr" rid="bib1.bibx127" id="altparen.50"/>, <xref ref-type="bibr" rid="bib1.bibx105" id="altparen.51"/>, <xref ref-type="bibr" rid="bib1.bibx23" id="altparen.52"/>, and
<xref ref-type="bibr" rid="bib1.bibx109" id="altparen.53"/>) with few studies considering the impact of DEM grid resolution within a
geomorphic context. Here we aim to extend existing methodologies to constrain
the utility of low-resolution data products across a suite of geomorphic
analyses to understand the following: (1) how hillslope length, topographic curvature, and
relief vary with grid resolution; (2) how best to extract channel networks in
lower-resolution datasets in order to minimize errors; and (3) whether it is
possible to estimate sediment transport coefficients from low-resolution
topographic data, where an independent constraint on erosion rate is
available.</p>
</sec>
</sec>
<sec id="Ch1.S2">
  <title>Theory and methods</title>
<sec id="Ch1.S2.SS1">
  <title>Generating topographic data</title>
      <p>Previous studies that have explored the impact of changing grid resolution on
topographic or geomorphic parameters have typically produced coarser-resolution topographic data by downsampling the highest-resolution data
product available for their study sites (e.g., <xref ref-type="bibr" rid="bib1.bibx118" id="altparen.54"/>, <xref ref-type="bibr" rid="bib1.bibx1" id="altparen.55"/>, <xref ref-type="bibr" rid="bib1.bibx11" id="altparen.56"/>, and <xref ref-type="bibr" rid="bib1.bibx109" id="altparen.57"/>).
Work has been undertaken to understand the influence of various re-gridding
schemes on topographic measurements <xref ref-type="bibr" rid="bib1.bibx128" id="paren.58"/>, with focus placed
upon understanding the use of downsampling high-resolution data in order to
facilitate computationally expensive analysis on larger spatial areas with
minimal loss in data fidelity. However, as computational power increases,
cost decreases and more efficient algorithms are developed
<xref ref-type="bibr" rid="bib1.bibx117 bib1.bibx92 bib1.bibx7 bib1.bibx107" id="paren.59"/>, the need to downsample data for computational
convenience becomes reduced. Instead, it becomes more important to understand
the limitations of available data products, to facilitate geomorphic analysis
in locations in which high-resolution topographic data are not available. This
is of particular importance in many studies of natural hazards (e.g., <xref ref-type="bibr" rid="bib1.bibx102" id="altparen.60"/>, and <xref ref-type="bibr" rid="bib1.bibx9" id="altparen.61"/>) in which data
quality is limited. It will also open geomorphic research up to communities
which do not have the resources to acquire high-resolution topographic data.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1"><caption><p>Lidar point cloud metadata.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{0.95}[0.95]?><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row>  
         <oasis:entry colname="col1">Location</oasis:entry>  
         <oasis:entry colname="col2">Point density</oasis:entry>  
         <oasis:entry colname="col3">Vertical</oasis:entry>  
         <oasis:entry colname="col4">Horizontal</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">(points m<inline-formula><mml:math 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>)</oasis:entry>  
         <oasis:entry colname="col3">accuracy</oasis:entry>  
         <oasis:entry colname="col4">accuracy</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3">(m)</oasis:entry>  
         <oasis:entry colname="col4">(m)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Santa Cruz Island</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>8.27</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:msup><mml:mn>0.067</mml:mn><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:msup><mml:mn>1.07</mml:mn><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Gabilan Mesa</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>5.56</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.20</mml:mn><mml:mo>±</mml:mo><mml:mn>0.15</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>0.11</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Oregon Coast Range</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>6.55</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.07</mml:mn><mml:mo>±</mml:mo><mml:mn>0.03</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>0.06</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table><?xmltex \begin{scaleboxenv}{0.95}[0.95]?><table-wrap-foot><p><inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula> Accuracy is the 95 % confidence level of the root mean
squared error of measurements compared to static GPS control points.</p></table-wrap-foot><?xmltex \end{scaleboxenv}?></table-wrap>

      <p>As a consequence of these constraints we have generated topographic data for
our three study sites without downsampling or re-gridding high-resolution
data products, as is commonly performed
<xref ref-type="bibr" rid="bib1.bibx118 bib1.bibx1 bib1.bibx11 bib1.bibx109" id="paren.62"/>.
Instead we have followed established techniques to grid the processed lidar
point cloud data provided by OpenTopography
(<uri>http://www.OpenTopography.org</uri>) at a range of data resolutions which
span from 1 m, considered to be the limit of the Oregon Coast Range dataset
by <xref ref-type="bibr" rid="bib1.bibx32" id="text.63"/> to 30 m, which is equal to the grid resolution of
the global SRTM dataset <xref ref-type="bibr" rid="bib1.bibx94" id="paren.64"/> and the Advanced Spaceborne
Thermal Emission and Reflection Radiometer (ASTER) dataset
<xref ref-type="bibr" rid="bib1.bibx129" id="paren.65"/> and in excess of the TanDEM-X dataset
<xref ref-type="bibr" rid="bib1.bibx55" id="paren.66"/> and as such should span the vast majority of
grid resolutions used in modern geomorphic research. The direct comparison
between elevation products generated using differing methodologies is
challenging <xref ref-type="bibr" rid="bib1.bibx13" id="paren.67"><named-content content-type="pre">e.g.,</named-content></xref>, and more work is
required within the context of geomorphic research to understand limitations
in topographic datasets, such as SRTM and TanDEM-X, which arise from data
capture and processing rather than purely from resolution constraints. By
generating the topographic data from the same source, we aim to isolate the
signal of decreasing data resolution, without the introduction of new sources
of error which may arise from data collected using a different instrument.
The error estimates of the raw point clouds used in this re-gridding process
are provided by OpenTopography and can be found in Table <xref ref-type="table" rid="Ch1.T1"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><caption><p>Example shaded reliefs of the same section of Santa Cruz Island at
increasing grid resolutions. All coordinates are in UTM Zone 11<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N.
Panels <bold>(a)–(f)</bold> represent resolutions of 1, 2, 5, 10, 20, and 30 m. Tick
spacing is in meters. The red box outlines an extensively gullied first-order
drainage, clearly visible in the highest-resolution data, but as the grid
resolution is decreased, this feature and its internal structure become indistinguishable from the surrounding hillslopes.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016-f01.png"/>

        </fig>

      <p>The point clouds are gridded using Points2Grid, which employs a local binning
algorithm, searching for points within a circular window of radius defined by
<xref ref-type="bibr" rid="bib1.bibx53" id="text.68"/> as
            <disp-formula id="Ch1.E1" content-type="numbered"><mml:math display="block"><mml:mrow><mml:mtext>Radius</mml:mtext><mml:mo>=</mml:mo><mml:mo>⌈</mml:mo><mml:msqrt><mml:mn mathvariant="normal">2</mml:mn></mml:msqrt><mml:mtext>Res</mml:mtext><mml:mo>⌉</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p>An inverse distance-weighted averaging approach is then performed to assign
an elevation value to each grid cell. This approach, which has been employed
in previous studies <xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx33" id="paren.69"/>,
yields a reliable representation of the topographic surface, with few data
gaps and a minimal amount of interpolation. The level of interpolation
performed is controlled by the density of lidar ground returns within each
search window, consequently more interpolation may be performed in areas of
high vegetation density such as the Oregon Coast Range. This is an additional
source of error which must be considered when processing lidar data, and this
consideration informed the selection of 1 m as the maximum resolution used
in this study as it is the highest resolution these datasets can have been
gridded to in the past (e.g., <xref ref-type="bibr" rid="bib1.bibx87" id="altparen.70"/>, and <xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx33" id="altparen.71"/>).</p>
      <p>The topographic data used in this study have been gridded at 20 resolutions,
and Fig. <xref ref-type="fig" rid="Ch1.F1"/> provides representative hillshades of a
section of Santa Cruz Island, highlighting the degradation of topographic
information as grid resolution is decreased.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>Measuring curvature from topography</title>
      <p>Landscape curvature has long been recognized as a key geomorphic
characteristic of landscapes, from Gilbert's
(<xref ref-type="bibr" rid="bib1.bibx31" id="year.72"/>) qualitative observations of hilltop
convexity to more recent approaches to quantify landform curvature using
digital topography (e.g., <xref ref-type="bibr" rid="bib1.bibx103" id="altparen.73"/>, and <xref ref-type="bibr" rid="bib1.bibx42" id="altparen.74"/>).
However, unlike other key landscape properties such as gradient
<xref ref-type="bibr" rid="bib1.bibx30 bib1.bibx126 bib1.bibx124 bib1.bibx121" id="paren.75"/>,
hydrology
<xref ref-type="bibr" rid="bib1.bibx127 bib1.bibx132 bib1.bibx75 bib1.bibx128" id="paren.76"/>, or soil characteristics
<xref ref-type="bibr" rid="bib1.bibx105 bib1.bibx23" id="paren.77"/>, the influence of
grid resolution on curvature has not been fully explored, particularly within
a geomorphic context.</p>
      <p>This is particularly important with the proliferation of high-resolution
topographic data from lidar, allowing the analysis of curvature on increasingly fine scales. Recent developments in channel extraction
techniques
<xref ref-type="bibr" rid="bib1.bibx58 bib1.bibx79 bib1.bibx80 bib1.bibx12" id="paren.78"/>
typically require the identification of topographic convergence in high-resolution topography using a curvature threshold. <xref ref-type="bibr" rid="bib1.bibx96" id="text.79"/>
and <xref ref-type="bibr" rid="bib1.bibx42" id="text.80"/> demonstrated that hilltop curvature scales with
erosion rate and as such demonstrated the importance of accurately
constraining the impact of grid resolution on this landscape parameter. Its
importance is highlighted by an increasing number of studies using this
relationship as a proxy for erosion rate
<xref ref-type="bibr" rid="bib1.bibx82 bib1.bibx45 bib1.bibx44 bib1.bibx33" id="paren.81"/>.
Hilltop curvature can also be used to constrain the sediment transport
coefficient of a landscape where an independent constraint on erosion rate is
available <xref ref-type="bibr" rid="bib1.bibx45" id="paren.82"/>.</p>
      <p>The measured curvature of a topographic surface depends on the orientation of
the measurement. Here, we consider two common types of curvature, with the
following definitions: (1) total curvature (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>Total</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>) – the curvature
of a surface calculated in two dimensions
<xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx130 bib1.bibx70" id="paren.83"/>
– and (2) tangential curvature (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>Tan</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>) – the curvature calculated
normal to the slope gradient <xref ref-type="bibr" rid="bib1.bibx66" id="paren.84"/>. These two
measures are employed to extract hilltop curvature and channel networks,
respectively. However, these definitions vary between studies and software
packages; see <xref ref-type="bibr" rid="bib1.bibx103" id="text.85"/> for a full review of the
varying nomenclature and definitions of curvature measurements used in the
literature.</p>
      <p>Work by <xref ref-type="bibr" rid="bib1.bibx103" id="text.86"/> utilized 10 m resolution DEMs to
evaluate the most accurate method for calculating curvature from digital
topographic data. It was concluded that curvature could be most accurately
calculated when a nine-term polynomial was fitted to the elevation surface, with
the caveat that this will only be effective where the data quality is high
enough. In cases in which the data are of lower accuracy,
<xref ref-type="bibr" rid="bib1.bibx103" id="text.87"/> recommended using quadratics to fit the
elevation data. This work was extended by <xref ref-type="bibr" rid="bib1.bibx42" id="text.88"/> to
consider whether these patterns held for high-resolution topographic data, and it
was found that fitting a six-term quadratic or nine-term polynomial yielded
similar results. Therefore, <xref ref-type="bibr" rid="bib1.bibx42" id="text.89"/> chose to use the six-term
quadratic to compute curvature. For this study we also chose to use the six-term quadratic in order to reduce computation time and, more importantly, to
provide more robust curvature values as the data quality is degraded to
resolutions below 10 m <xref ref-type="bibr" rid="bib1.bibx103" id="paren.90"/>.</p>
      <p>We calculate curvature using a circular window passed across the landscape,
with a radius defined by identifying scaling breaks in the standard deviation
and interquartile range of curvature calculated at increasing window sizes,
consistent with the length scales of individual hillslopes
<xref ref-type="bibr" rid="bib1.bibx58 bib1.bibx100 bib1.bibx42 bib1.bibx32 bib1.bibx33" id="paren.91"/>.
Consequently, curvature measurements on the hillslope scale can only be
considered at data resolutions high enough to resolve individual hillslope
features, considered here to be no more than 10 m, based on the window sizes
identified for each landscape. A quadratic function of the form
            <disp-formula id="Ch1.E2" content-type="numbered"><mml:math display="block"><mml:mrow><mml:mi mathvariant="italic">ζ</mml:mi><mml:mo>=</mml:mo><mml:mi>a</mml:mi><mml:msup><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mi>b</mml:mi><mml:msup><mml:mi>y</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mi>c</mml:mi><mml:mi>x</mml:mi><mml:mi>y</mml:mi><mml:mo>+</mml:mo><mml:mi>d</mml:mi><mml:mi>x</mml:mi><mml:mo>+</mml:mo><mml:mi>e</mml:mi><mml:mi>y</mml:mi><mml:mo>+</mml:mo><mml:mi>f</mml:mi></mml:mrow></mml:math></disp-formula>
          is then fitted to the elevation values within the window by least squares
regression <xref ref-type="bibr" rid="bib1.bibx24" id="paren.92"/>, where <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">ζ</mml:mi></mml:math></inline-formula> is the elevation, <inline-formula><mml:math display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>
and <inline-formula><mml:math display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> are horizontal coordinates, and <inline-formula><mml:math display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> through <inline-formula><mml:math display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> are fitting
coefficients. The fitted coefficients of this polynomial can be used to
calculate differing types of curvature:
            <disp-formula id="Ch1.E3" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>Total</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi>a</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi>b</mml:mi></mml:mrow></mml:math></disp-formula>
          and
            <disp-formula id="Ch1.E4" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>Tan</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mi>a</mml:mi><mml:msup><mml:mi>e</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi>c</mml:mi><mml:mi>d</mml:mi><mml:mi>e</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi>b</mml:mi><mml:msup><mml:mi>d</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:msup><mml:mi>d</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>)</mml:mo><mml:msqrt><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:msup><mml:mi>d</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:msqrt></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p>From the measure of <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>Total</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> for every cell in a DEM, we can also
extract a subset of curvature values from the hilltops. The value of
curvature at a hilltop (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>HT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>) can be readily evaluated if the
positions of the hilltops are known. To extract hilltops we follow
<xref ref-type="bibr" rid="bib1.bibx42" id="text.93"/> in defining a hilltop as the boundary between two
drainage basins of the same stream order. These points in the landscape can
be algorithmically extracted once a channel network is defined through the
identification of points in the landscape where two channels of the same
Strahler order meet and the identification of that point's upslope
contributing area. Each of these areas defines a basin of a given order, and
by repeating this process across the range of Strahler orders found in the
landscape, a network of hilltops can be defined. This network is then used to
sample the curvature values at these locations to provide the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>HT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>
values across the landscape. To ensure consistency between <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>HT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>
measurements at changing grid resolutions, the same channel network,
generated using the geometric method described in
Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/> from 1 m resolution data, is used as the
basis of the hilltop extraction algorithm.</p>
      <p>For our data on hilltop curvature, <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>HT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, hilltops with a gradient
exceeding 0.4 are excluded as <xref ref-type="bibr" rid="bib1.bibx42" id="text.94"/> demonstrated that this
gradient is the point at which <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn> 15</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of sediment transport is
nonlinear. Under nonlinear sediment flux hilltop curvature scales nonlinearly
with erosion rate <xref ref-type="bibr" rid="bib1.bibx96" id="paren.95"/> and consequently cannot be used
as a proxy for erosion rates. As hilltops have a convex form, their curvature
should be negative, so as a final step any points identified as hilltops
which have a positive curvature are excluded from further analysis.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Channel extraction</title>
      <p>Extracting channel networks from digital topographic data remains a
fundamental challenge for many areas of topographic analysis. Without the
ability to discriminate between fluvial and hillslope domains, it is not
possible extract many topographic metrics such as hillslope length
<xref ref-type="bibr" rid="bib1.bibx32" id="paren.96"/>, mean basin slope <xref ref-type="bibr" rid="bib1.bibx14" id="paren.97"/>, or
hilltop curvature <xref ref-type="bibr" rid="bib1.bibx42" id="paren.98"/>, and the accuracy of each of these
metrics will be influenced by the accuracy of the channel network extracted.
At a more fundamental level, the ability to identify where channels initiate
will facilitate better understanding of the processes acting at the
transition between diffusive (hillslope) and advective (fluvial) sediment
transport <xref ref-type="bibr" rid="bib1.bibx84" id="paren.99"/>.</p>
      <p>Many authors have made use of field-mapped channel heads both as a basis for
geomorphic analysis and as a method for evaluating channel extraction methods
<xref ref-type="bibr" rid="bib1.bibx68 bib1.bibx78 bib1.bibx50 bib1.bibx47 bib1.bibx12" id="paren.100"/>.
Prior to the availability of high-resolution topographic data, contributing
area and slope-area scaling thresholds were commonly used to define the
location of channel heads directly from DEMs
<xref ref-type="bibr" rid="bib1.bibx61 bib1.bibx77 bib1.bibx68 bib1.bibx113 bib1.bibx17 bib1.bibx18" id="paren.101"/>.
The influence of decreasing grid resolution on such channel extraction
methods was evaluated by <xref ref-type="bibr" rid="bib1.bibx78" id="text.102"/>, who demonstrated
a strong sensitivity in predicted channel head location to grid resolution,
suggesting that coarser-resolution data may not be suitable for channel
extraction through an area threshold. We apply the method described by
<xref ref-type="bibr" rid="bib1.bibx78" id="text.103"/> to quantify the accuracy of an extracted
channel network, detailed in Sect. <xref ref-type="sec" rid="Ch1.S2.SS4"/>.</p>
      <p>Several methods have been proposed to identify channel heads from high-resolution topography. Typically these methods exploit the high-resolution
nature of topographic data to resolve morphometric or process-based
signatures of channel initiation or the transition between the hillslope and
fluvial domain
<xref ref-type="bibr" rid="bib1.bibx58 bib1.bibx79 bib1.bibx80 bib1.bibx12" id="paren.104"/>.
Here we evaluate how two techniques – one geometric method built upon work by
<xref ref-type="bibr" rid="bib1.bibx80" id="text.105"/> and <xref ref-type="bibr" rid="bib1.bibx79" id="text.106"/> and one
process-based method, the DrEICH algorithm, developed by
<xref ref-type="bibr" rid="bib1.bibx12" id="text.107"/> – are influenced by decreasing grid resolution.</p>
      <p>The DrEICH method was selected for evaluation as the technique on which it is
based has been shown to operate successfully in lower-resolution data
<xref ref-type="bibr" rid="bib1.bibx73" id="paren.108"/>. The DrEICH method makes use of <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula>
analysis, performed by integrating drainage area along a river profile to
facilitate comparisons between river profiles of differing drainage area,
with fewer uncertainties than traditional slope-area analysis
<xref ref-type="bibr" rid="bib1.bibx101 bib1.bibx83" id="paren.109"/>. When plotting the <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula>
value against elevation for a river profile, river channels will plot as
linear segments, whereas hillslopes will display nonlinear segments. The
DrEICH algorithm identifies the transition between these linear and nonlinear
segments as the best-fit location of the channel head.</p>
      <p>The geometric method, used by <xref ref-type="bibr" rid="bib1.bibx33" id="text.110"/>, removes
noise from the raw topographic data using a Wiener filter
<xref ref-type="bibr" rid="bib1.bibx125" id="paren.111"/>, as recommended by
<xref ref-type="bibr" rid="bib1.bibx80" id="text.112"/>. This smoothed topography is then processed to
identify channelized portions of the landscape using a tangential curvature
threshold <xref ref-type="bibr" rid="bib1.bibx80" id="paren.113"><named-content content-type="pre">e.g.,</named-content></xref>, selected using the
deviation of the probability density function of curvature from a normal
distribution on a quantile–quantile plot (e.g., <xref ref-type="bibr" rid="bib1.bibx58" id="altparen.114"/>, and <xref ref-type="bibr" rid="bib1.bibx79" id="altparen.115"/>). The
identified areas of channelization are then combined into a contiguous
channel network by employing a connected-components algorithm
<xref ref-type="bibr" rid="bib1.bibx34" id="paren.116"/> and thinned into a final channel network skeleton
using the algorithm of <xref ref-type="bibr" rid="bib1.bibx131" id="text.117"/>.</p>
      <p>Channels were extracted from the 5, 10, 20, and 30 m DEMs generated in
Sect. <xref ref-type="sec" rid="Ch1.S2.SS1"/> using both of the channel extraction
methodologies. Parameters required in the operation of each algorithm were
selected based on values used in previous studies
<xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx33" id="paren.118"/>, and these values can be
found in Appendix <xref ref-type="sec" rid="App1.Ch1.S1"/>.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <title>Comparing channel networks</title>
      <p>To assess the accuracy of the channel networks extracted using both methods,
we employ two measures of quality described by
<xref ref-type="bibr" rid="bib1.bibx78" id="text.119"/>. These measures operate on classifications
of the predicted location of channel heads placing each channel head into one
of three categories: true positives (TPs), false positives (FPs), and false
negatives (FNs). A TP is where a predicted channel head from low-resolution
data occupies the same spatial location as the channel head derived from 1 m
resolution topography. An FP is where a predicted channel head is placed in a
location where there is no channel head in the high-resolution data. An FN is
when a channel head from high-resolution topography does not have a predicted
channel head from low-resolution topography in the same spatial location.</p>
      <p>We follow <xref ref-type="bibr" rid="bib1.bibx78" id="text.120"/> in employing a 30 m search
radius around the 1 m derived channel heads and consider a low-resolution
channel head falling within this radius to be spatially coincident. This has
the effect of normalizing the size of each channel head point, to ensure that
we can perform comparisons between predictions made at different spatial
resolutions.</p>
      <p>The reliability, <inline-formula><mml:math display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula>, of a channel extraction method is the ability of a
method to not predict channel heads in areas where none are located and is
calculated as
            <disp-formula id="Ch1.E5" content-type="numbered"><mml:math display="block"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∑</mml:mo><mml:mtext>TP</mml:mtext></mml:mrow><mml:mrow><mml:mo>∑</mml:mo><mml:mtext>TP</mml:mtext><mml:mo>+</mml:mo><mml:mtext>FP</mml:mtext></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math display="inline"><mml:mo>∑</mml:mo></mml:math></inline-formula> TP is the total number of true positives and <inline-formula><mml:math display="inline"><mml:mo>∑</mml:mo></mml:math></inline-formula> FP is the
total number of false positives. The sensitivity, <inline-formula><mml:math display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula>, of a channel
extraction methodology is given by
            <disp-formula id="Ch1.E6" content-type="numbered"><mml:math display="block"><mml:mrow><mml:mi>s</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∑</mml:mo><mml:mtext>TP</mml:mtext></mml:mrow><mml:mrow><mml:mo>∑</mml:mo><mml:mtext>TP</mml:mtext><mml:mo>+</mml:mo><mml:mo>∑</mml:mo><mml:mtext>FN</mml:mtext></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math display="inline"><mml:mo>∑</mml:mo></mml:math></inline-formula> FN is the total number of false negatives. The sensitivity is
the ability of a method to predict all of the channel heads expected. Using
these two indexes it is possible to quantify the quality of channel heads
predicted using low-resolution data, as well as understand why a particular
method fails, by distinguishing between methods which fail due to either
over- or underpredicting the number of channel heads in a landscape or by simply
placing channel heads in the wrong spatial location.</p>
</sec>
<sec id="Ch1.S2.SS5">
  <title>Estimating the hillslope sediment transport coefficient from hilltop curvature</title>
      <p>The sediment transport coefficient, <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> [<inline-formula><mml:math display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">L</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:msup><mml:mi mathvariant="normal">T</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>]
(dimensions of mass [<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">M</mml:mi></mml:math></inline-formula>], length [<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">L</mml:mi></mml:math></inline-formula>], and time [<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">T</mml:mi></mml:math></inline-formula>]
denoted in square brackets), of a landscape is a
measure of its sediment transport efficiency and was demonstrated by
<xref ref-type="bibr" rid="bib1.bibx26" id="text.121"/> to be controlled by the material properties
of soil such as grain size, cohesion, and thickness. The value of <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> within a
landscape will exert a control on the morphology of hillslopes
<xref ref-type="bibr" rid="bib1.bibx97" id="paren.122"><named-content content-type="pre">e.g.,</named-content></xref>. Diffusion-like hillslope evolution
can be modeled using a 1-D mass conservation equation, assuming that the
contribution to surface lowering from chemical processes is negligible when
contrasted with the signal of surface lowering from physical processes
(e.g., <xref ref-type="bibr" rid="bib1.bibx97" id="altparen.123"/>, and <xref ref-type="bibr" rid="bib1.bibx72" id="altparen.124"/>):
            <disp-formula id="Ch1.E7" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mtext>s</mml:mtext></mml:msub><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi mathvariant="italic">ζ</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mtext>s</mml:mtext></mml:msub><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mtext>s</mml:mtext></mml:msub></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mtext>r</mml:mtext></mml:msub><mml:mi>U</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">ζ</mml:mi></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:mi mathvariant="normal">L</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> is the elevation of the land surface,
<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mtext>s</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mtext>r</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:mi mathvariant="normal">M</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">L</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> are
densities of dry soil and rock, respectively, and <inline-formula><mml:math display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula>
<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:mi mathvariant="normal">L</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">T</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> is the uplift rate. In steady-state landscapes, where <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>U</mml:mi><mml:mo>=</mml:mo><mml:mi>E</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∂</mml:mo><mml:mi mathvariant="italic">ζ</mml:mi><mml:mo>/</mml:mo><mml:mo>∂</mml:mo><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>,
Eq. (<xref ref-type="disp-formula" rid="Ch1.E7"/>) simplifies to
            <disp-formula id="Ch1.E8" content-type="numbered"><mml:math display="block"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mtext>r</mml:mtext></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mtext>s</mml:mtext></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>E</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mtext>s</mml:mtext></mml:msub></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          with <inline-formula><mml:math display="inline"><mml:mi>E</mml:mi></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:mi mathvariant="normal">L</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">T</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> denoting the erosion rate. To solve
this equation, a statement of the volumetric sediment flux per unit contour
length, <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mtext>s</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:msup><mml:mi mathvariant="normal">L</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">T</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>, must be derived. A
nonlinear relationship between sediment flux and topographic gradient has
been proposed by a number of authors
<xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx54 bib1.bibx2 bib1.bibx41 bib1.bibx97 bib1.bibx98 bib1.bibx81" id="paren.125"/>.
Support for such models has been found from both tests of the resulting
topographic predictions
<xref ref-type="bibr" rid="bib1.bibx99 bib1.bibx42 bib1.bibx32" id="paren.126"/> as well as
through independent measurements of sediment flux across hillslopes
<xref ref-type="bibr" rid="bib1.bibx98 bib1.bibx96" id="paren.127"/>.</p>
      <p>The nonlinear model proposed by <xref ref-type="bibr" rid="bib1.bibx3" id="text.128"/> and
<xref ref-type="bibr" rid="bib1.bibx97" id="text.129"/> is of the form
            <disp-formula id="Ch1.E9" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mtext>s</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mtext>DS</mml:mtext><mml:msup><mml:mfenced close="]" open="["><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>|</mml:mo><mml:mi>S</mml:mi><mml:mo>|</mml:mo></mml:mrow><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mtext>c</mml:mtext></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mfenced><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mtext>c</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is a critical gradient, and as the hillslope gradient
approaches this threshold, <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mtext>s</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> asymptotes towards infinity.</p>
      <p>At low hillslope gradients (e.g., on hilltops), the term within brackets in
Eq. (<xref ref-type="disp-formula" rid="Ch1.E9"/>) approximates to unity <xref ref-type="bibr" rid="bib1.bibx42" id="paren.130"/>.
Equation (<xref ref-type="disp-formula" rid="Ch1.E9"/>) can therefore be substituted into
Eq. (<xref ref-type="disp-formula" rid="Ch1.E8"/>) and can be solved for <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> on low-gradient hilltops,
assuming that an independent constraint on <inline-formula><mml:math display="inline"><mml:mi>E</mml:mi></mml:math></inline-formula> is available,
            <disp-formula id="Ch1.E10" content-type="numbered"><mml:math display="block"><mml:mrow><mml:mi>D</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>E</mml:mi><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mtext>r</mml:mtext></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>HT</mml:mtext></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mtext>s</mml:mtext></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
</sec>
<sec id="Ch1.S2.SS6">
  <title>Hillslope length and relief</title>
      <p>Hillslope length (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>H</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>) is a crucial landscape parameter to
constrain as it controls the rate of mass flux by overland flow within
catchments <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx22 bib1.bibx119" id="paren.131"/>,
influences rates of soil erosion <xref ref-type="bibr" rid="bib1.bibx59" id="paren.132"/>, and presents a first-order control on the maximum source area of landslides
<xref ref-type="bibr" rid="bib1.bibx43" id="paren.133"/>. Furthermore, it may be used to demonstrate
nonlinearity in hillslope sediment flux
<xref ref-type="bibr" rid="bib1.bibx97 bib1.bibx99 bib1.bibx32 bib1.bibx33" id="paren.134"/>.</p>
      <p>Many studies have attempted to calculate hillslope length through the
inversion of drainage density <xref ref-type="bibr" rid="bib1.bibx120" id="paren.135"/>, analysis of
plots of local slope against drainage area <xref ref-type="bibr" rid="bib1.bibx99" id="paren.136"/>,
direct measurements from topographic maps
<xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx111" id="paren.137"/>, and by measuring the length
of overland flow from ridgeline to channel
<xref ref-type="bibr" rid="bib1.bibx42 bib1.bibx32" id="paren.138"/>. <xref ref-type="bibr" rid="bib1.bibx32" id="text.139"/>
demonstrated that the most geomorphologically suitable technique to use,
particularly in the context of hillslope sediment transport, was that of
measuring the length of overland flow. An additional measure which can be
derived from this technique is the topographic relief, which is the
difference in elevation between a hilltop and channel connected by a
hillslope flow path. Topographic relief has been estimated in a number of
ways and is frequently used in studies of tectonic geomorphology (e.g., <xref ref-type="bibr" rid="bib1.bibx27" id="altparen.140"/>, <xref ref-type="bibr" rid="bib1.bibx37" id="altparen.141"/>, <xref ref-type="bibr" rid="bib1.bibx28" id="altparen.142"/>, and <xref ref-type="bibr" rid="bib1.bibx29" id="altparen.143"/>).
Furthermore, topographic relief may be used to generate dimensionless erosion
and relief plots
<xref ref-type="bibr" rid="bib1.bibx99 bib1.bibx42 bib1.bibx110 bib1.bibx33" id="paren.144"/>,
which can be used to identify landscape transience
<xref ref-type="bibr" rid="bib1.bibx44 bib1.bibx71" id="paren.145"/>. Consequently, we intend
to test the robustness of measuring hillslope length and relief as grid
resolution decreases, with the aim of facilitating increased confidence in
geomorphic analyses performed in locations where high-resolution topography
is unavailable.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p><bold>(a)</bold> Map showing the location of each of the study sites
within the USA. <bold>(b–d)</bold> Shaded reliefs of representative sections of
each study site, generated from 1 m resolution data. Tick spacing is in
meters. All coordinates are in UTM. <bold>(b)</bold> Gabilan Mesa, California,
UTM Zone 10<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N. <bold>(c)</bold> Santa Cruz Island, California, UTM Zone
11<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N. <bold>(d)</bold> Oregon Coast Range, Oregon, UTM Zone
10<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016-f02.jpg"/>

        </fig>

      <p>Using the 20 topographic datasets generated in
Sect. <xref ref-type="sec" rid="Ch1.S2.SS1"/> for each of the three landscapes, hillslope
length measurements were generated following the methods outlined in
<xref ref-type="bibr" rid="bib1.bibx32" id="text.146"/>. We measured hillslope length on each dataset using
two different channel networks. Firstly, channel heads were extracted from
the highest-resolution data set, in each case 1 m, using the geometric
method outlined in Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/>. These high-resolution
channel heads were mapped onto the coarser-resolution topographic data, to
ensure that changing channel extraction results will not have an influence on
the measures of hillslope length. This allows improved isolation of the
factors driving variations in hillslope length as grid resolution is
decreased. Secondly, the analysis was performed using coarser-resolution
channel networks extracted using the geometric method of channel extraction.
We use the geometric method as opposed to the DrEICH method because, as we
will show below, the geometric method is less sensitive to grid resolution.
These two channel networks effectively provide upper and lower bounds for the
accuracy of hillslope length and relief measurements.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Study sites</title>
      <p>Three study sites from the United States have been selected for this study:
Santa Cruz Island, California; Gabilan Mesa, California; and the Oregon Coast
Range, Oregon. The first two sites have regularly spaced valleys at a range
of length scales, particularly Gabilan Mesa, which has been the focus of
previous work in this context
<xref ref-type="bibr" rid="bib1.bibx85 bib1.bibx86" id="paren.147"/>. Santa Cruz Island, while
less studied in the context of topographic analysis than Gabilan Mesa,
has a wider range of hilltop curvatures (Fig. <xref ref-type="fig" rid="Ch1.F2"/>). The
Oregon Coast Range has been considered to be very regular, with uniform first-order drainage areas <xref ref-type="bibr" rid="bib1.bibx97 bib1.bibx99" id="paren.148"/>.
However, more recent work has demonstrated the spatial variability of many
topographic measurements in this landscape
<xref ref-type="bibr" rid="bib1.bibx62 bib1.bibx33" id="paren.149"/>, and as such it provides a more challenging test case for our analyses. Furthermore, these
sites were selected as they each have high-resolution lidar data covering a
large spatial area and have been the subject of many previous studies
<xref ref-type="bibr" rid="bib1.bibx95 bib1.bibx97 bib1.bibx98 bib1.bibx67 bib1.bibx89 bib1.bibx99 bib1.bibx86 bib1.bibx87 bib1.bibx88 bib1.bibx62 bib1.bibx32 bib1.bibx33" id="paren.150"/>, which should provide a good basis for the evaluation of the results of this
study in a wider geomorphic context.</p>
<sec id="Ch1.S3.SS1">
  <title>Gabilan Mesa</title>
      <p>Gabilan Mesa, a section of the Central Coast Ranges in California, USA
(Fig. <xref ref-type="fig" rid="Ch1.F2"/>b), is a highly regular landscape with very gentle
transitions between hillslopes and channels, which correspond to topographic
predictions of diffusion-like sediment transport
<xref ref-type="bibr" rid="bib1.bibx99" id="paren.151"/>. The area's semiarid climate supports a range
of vegetation from oak savanna to chaparral shrubland
<xref ref-type="bibr" rid="bib1.bibx108 bib1.bibx99" id="paren.152"/>. The nature of this
lower-density vegetation allows a larger proportion of lidar pulses to reach
the ground, requiring less processing and interpolation to generate a final
bare-earth DEM for analysis <xref ref-type="bibr" rid="bib1.bibx60 bib1.bibx63" id="paren.153"/>.</p>
      <p>A series of large, linear canyons running northeast to southwest are fed by
parallel tributaries which flow perpendicular to the main trunk channel.
These regularly spaced valleys present two distinct length scales in the
landscape which have been observed both qualitatively
<xref ref-type="bibr" rid="bib1.bibx19 bib1.bibx20" id="paren.154"/> and
quantitatively through measurements of hillslope length distributions
<xref ref-type="bibr" rid="bib1.bibx32" id="paren.155"/>. Relationships between dimensionless erosion rate and
relief, the uniformity of hilltop curvatures, and the regularity of valley
spacing have all been used to assert that much of this landscape is in steady
state
<xref ref-type="bibr" rid="bib1.bibx99 bib1.bibx86 bib1.bibx33" id="paren.156"/>,
although localized observations of a relict plateau surface add complexity to
this steady-state observation.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p>Maps showing the spatial variation in total curvature measurements
as grid resolution is decreased for the same section of Santa Cruz Island as
displayed in Fig. <xref ref-type="fig" rid="Ch1.F1"/>. All coordinates are in UTM Zone
11<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N. Panels <bold>(a)</bold>–<bold>(f)</bold> represent resolutions of 1,
2, 5, 10, 20, and 30 m. Tick spacing is in meters. The black boxes outline
the same features as highlighted in Fig. <xref ref-type="fig" rid="Ch1.F1"/>, showing the
reduction in the curvature signal with grid resolution for such a feature.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016-f03.jpg"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS2">
  <title>Santa Cruz Island</title>
      <p>Santa Cruz Island (Fig. <xref ref-type="fig" rid="Ch1.F2"/>c), the largest of the eight
California Channel Islands located to the west of California, USA, is divided
by a large east–west trending valley, which follows the Santa Cruz fault
<xref ref-type="bibr" rid="bib1.bibx91 bib1.bibx74" id="paren.157"/>. Parallel to this valley
are two large ridges – one to the north and one to the south – which exhibit
regularly spaced parallel channels draining north to south
<xref ref-type="bibr" rid="bib1.bibx90 bib1.bibx89" id="paren.158"/>; this regular pattern is
particularly evident in the northwest section of the study area. The Santa
Cruz Fault has been demonstrated to have left-lateral strike slip motion,
which deflects channels away from the perpendicular to the main valley in the
center of the island <xref ref-type="bibr" rid="bib1.bibx90" id="paren.159"/>. Studies of marine terraces in
the region suggest that the Channel Islands have been steadily uplifted
through the late Quaternary <xref ref-type="bibr" rid="bib1.bibx74" id="paren.160"/>.</p>
      <p>The island has a Mediterranean climate similar to that of Gabilan Mesa
<xref ref-type="bibr" rid="bib1.bibx89" id="paren.161"/>, supporting extensive grassland with
occasional patches of pine forest and chaparral vegetation
<xref ref-type="bibr" rid="bib1.bibx89 bib1.bibx87 bib1.bibx88" id="paren.162"/>.
Human activities led to overgrazing across the island at the turn of the 19th
century, causing a period of gullying and rapid erosion, particularly evident
in the southwest of the island
<xref ref-type="bibr" rid="bib1.bibx89 bib1.bibx88" id="paren.163"/>. The lidar data collected
for this location have been extensively tested and ground truthed, ensuring
that they are suitable for use in a geomorphic context
<xref ref-type="bibr" rid="bib1.bibx87" id="paren.164"/> and for performing topographic analysis at
high spatial resolutions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p>Plots of the distribution of <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>Total</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> <bold>(a, c, e)</bold> and <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>Tan</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> <bold>(b, d, f)</bold> measurements as resolution is decreased for each of the study
landscapes. Whiskers are the 2nd and 98th percentiles; the box covers the
25th and 75th percentiles; the blue bar is the mean and the red bar is the
median. The gray outline is the probability density function of each
dataset.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016-f04.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS3">
  <title>Oregon Coast Range</title>
      <p>The Oregon Coast Range in Oregon (Fig. <xref ref-type="fig" rid="Ch1.F2"/>d), USA, is a
densely vegetated upland landscape, dominated by coniferous and hardwood
forests <xref ref-type="bibr" rid="bib1.bibx104" id="paren.165"/>, with a humid climate
<xref ref-type="bibr" rid="bib1.bibx97" id="paren.166"/>. Qualitative observations of the landscape
suggest that the valleys are regularly spaced, with a particular uniformity
found in the dimensions of first-order drainage basins
<xref ref-type="bibr" rid="bib1.bibx97 bib1.bibx99 bib1.bibx62" id="paren.167"/>.
Such observations have been supported by measurements of hillslope length
across the landscape <xref ref-type="bibr" rid="bib1.bibx32" id="paren.168"/>. However, comparisons of the
dimensionless relief and erosion rate performed by
<xref ref-type="bibr" rid="bib1.bibx33" id="text.169"/> highlight the small-scale topographic
variability inherent in this otherwise regular landscape. The Oregon Coast
Range is considered to be in steady state due to the correlation between
uplift rates from marine terrace data <xref ref-type="bibr" rid="bib1.bibx51" id="paren.170"/> and
erosion rates from cosmogenic radionuclides
<xref ref-type="bibr" rid="bib1.bibx4 bib1.bibx95 bib1.bibx5 bib1.bibx35" id="paren.171"/>.
The hillslopes are steeper and the ridgelines sharper than in Gabilan Mesa,
consistent with observations of debris flows and shallow landsliding across
the range
<xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx35 bib1.bibx67" id="paren.172"/>,
which have the potential to create a distinct topographic signature
<xref ref-type="bibr" rid="bib1.bibx6" id="paren.173"/>.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <title>Results</title>
<sec id="Ch1.S4.SS1">
  <title>Curvature</title>
      <p>Figure <xref ref-type="fig" rid="Ch1.F3"/> illustrates the variations in total curvature
with grid resolution for a section of Santa Cruz Island. As the grid
resolution is decreased, the range of <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>Total</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> measurements are
reduced, with much of the landscape becoming apparently planar. Within the
black box, which covers the same spatial area as the boxes in
Fig. <xref ref-type="fig" rid="Ch1.F1"/>, the impact of degrading resolution on small
topographic features is observed, with the curvature signal of this first-order feature being lost as the grid resolution approaches 30 m.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p>Plots of the reduction in range between the 2nd and 98th percentiles
(blue triangles) and the interquartile range (red circles) of
<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>Total</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> <bold>(a, c, e)</bold> and <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>Tan</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>
<bold>(b, d, f)</bold> measurements as resolution is
decreased for each of the study landscapes.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016-f05.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p>Representative sections of each landscape's channel network
displaying the extent of each network as grid resolution is decreased. Panels <bold>(a)</bold>, <bold>(b)</bold>, and <bold>(c)</bold> are generated using the DrEICH
method of channel extraction. Panels <bold>(d)</bold>, <bold>(e)</bold>, and <bold>(f)</bold> are
generated using the geometric method. All coordinates are in UTM. Tick
spacing is in meters. The left column is from Santa Cruz Island, UTM Zone
11<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, the central column is from Gabilan Mesa, UTM Zone
10<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, and the right column is from the Oregon Coast Range, UTM Zone
10<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016-f06.jpg"/>

        </fig>

      <p>Figure <xref ref-type="fig" rid="Ch1.F4"/> displays the variations in the distribution of total
and tangential curvature measurements with grid resolution for each of the
study landscapes. Santa Cruz Island shows little variation in mean and median
curvature with resolution, with the majority of the changes in each
distribution with resolution occurring at the extremes of the curvature
distribution for each dataset, as the representation of ridgelines and
channel bottoms becomes increasingly diffuse. As resolution is decreased, the
range between 2nd and 98th percentiles and the 1st and 3rd quartiles
decreases, with a more rapid reduction in the more extreme values than in the
quartiles (Fig. <xref ref-type="fig" rid="Ch1.F5"/>). While this effect is most marked at
the extremes, the distributions are condensed across all percentile intervals
as grid resolution is increased beyond 3–4 m. This behavior is observed for
both <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>Total</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>Tan</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> as grid resolution is decreased.</p>
      <p>In the Oregon Coast Range for both measurements of curvature, there is little
variation between the 1, 2, and 3 m datasets, with a broad range of
measurements shown in the probability distributions. Beyond this point the
mean and median do not significantly change, but as in Santa Cruz Island, the
overall distribution of measurements compresses towards the average value for
the landscape. The Gabilan Mesa data show similar trends to those of Santa
Cruz Island but exhibit less variability at lower resolutions. The
probability distributions of each measurement also exhibit less change with
resolution than the other two datasets, indicating a reduced sensitivity to
grid resolution at this location.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p>The variations in reliability (Eq. <xref ref-type="disp-formula" rid="Ch1.E5"/>) and
sensitivity (Eq. <xref ref-type="disp-formula" rid="Ch1.E6"/>) of each channel network with decreasing
grid resolution. Panels <bold>(a)</bold>, <bold>(c)</bold>, and <bold>(e)</bold> are generated
using the geometric method of channel extraction. Panels <bold>(b)</bold>,
<bold>(d)</bold>, and <bold>(f)</bold> are generated using the DrEICH method. The top row is from
Gabilan Mesa, the middle row is from Santa Cruz Island, and the bottom row is
from the Oregon Coast Range. The full results from this analysis can be found
in Tables <xref ref-type="table" rid="Ch1.T3"/> and <xref ref-type="table" rid="Ch1.T4"/>.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016-f07.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS2">
  <title>Channel networks</title>
      <p>Figure <xref ref-type="fig" rid="Ch1.F6"/> provides a qualitative overview of the changes
of channel network extent with decreasing grid resolution for both methods,
across the three test landscapes. In each case the general patterns are that
as the grid resolution is decreased, the lowest-order channels are lost, as
they exist on a spatial scale below that of the data resolution. In contrast,
large parts of the predicted networks appear to occupy similar spatial locations in
larger, higher-order channels where the topographic signal of a channel is
more pronounced. The geometric method shows less reduction in drainage
density than the DrEICH method, as data resolution is decreased.</p>
      <p>Figure <xref ref-type="fig" rid="Ch1.F7"/> provides a quantitative assessment of channel
extraction quality by presenting the indexes of reliability and sensitivity
for both the geometric channel extraction and extraction based on DrEICH, as
the grid resolution is decreased. In Gabilan Mesa the channels extracted by
the geometric method exhibit a high reliability which does not decrease
considerably with decreasing grid resolution, suggesting that for each
resolution step a large proportion of the predicted channel heads are
spatially coincident with the channel heads generated from the 1 m data. The
sensitivity values for this method and location are lower and decline more
steadily with decreasing grid resolution, suggesting an increasing number of
channel heads being missed by the algorithm as grid resolution is decreased.
The DrEICH method does not perform as well in Gabilan Mesa, with lower index
values for the 5 m data than the geometric method, and a rapid decline
towards index values of 0, suggesting that the predicted channel heads bear
little relation to the channel heads from the 1 m data.</p>
      <p>In Santa Cruz Island the geometric method's reliability index is similar to
Gabilan Mesa; however, the sensitivity index is not as high, which indicates that a
large number of channel heads are being missed, but where a prediction is
made, it is typically accurate. The DrEICH method exhibits a similarly large
reliability initially but again shows more rapid degradation in the index
value as grid resolution is decreased. The sensitivity values again decline
more rapidly and reach a 0 value at 20 m grid resolution.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p>Changes in the estimated sediment transport coefficient, <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>,
calculated using Eq. (<xref ref-type="disp-formula" rid="Ch1.E10"/>) and parameters in
Table <xref ref-type="table" rid="Ch1.T2"/> for each of the three study landscapes, with
decreasing data resolution. The error bars on each data point represent the
uncertainties reported for each landscape's erosion rate data.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016-f08.png"/>

        </fig>

<?xmltex \floatpos{th!}?><table-wrap id="Ch1.T2" specific-use="star"><caption><p>Published parameters used to calculate diffusivity.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="left"/>
     <oasis:thead>
       <oasis:row>  
         <oasis:entry colname="col1">Location</oasis:entry>  
         <oasis:entry colname="col2">Soil density</oasis:entry>  
         <oasis:entry colname="col3">Rock density</oasis:entry>  
         <oasis:entry colname="col4">Erosion rate</oasis:entry>  
         <oasis:entry colname="col5">Reference</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">(kg m<inline-formula><mml:math 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 display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3">(kg m<inline-formula><mml:math 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 display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4">(mm yr<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>  
         <oasis:entry colname="col5"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Santa Cruz Island</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>1.4</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>2.4</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.069</mml:mn><mml:mo>±</mml:mo><mml:mn>0.007</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5">
                    <xref ref-type="bibr" rid="bib1.bibx88" id="text.175"/>
                  </oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Gabilan Mesa</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>1.4</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>2.4</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.36</mml:mn><mml:mstyle scriptlevel="+1"><mml:mtable class="substack"><mml:mtr><mml:mtd><mml:mo>+</mml:mo><mml:mn>0.38</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mo>-</mml:mo><mml:mn>0.22</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:mstyle></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5">
                    <xref ref-type="bibr" rid="bib1.bibx99" id="text.176"/>
                  </oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Oregon Coast Range</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>1.4</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>2.4</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.1</mml:mn><mml:mo>±</mml:mo><mml:mn>0.05</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5">
                    <xref ref-type="bibr" rid="bib1.bibx97" id="text.177"/>
                  </oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p><inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula> Soil and rock densities are representative of typical
measurements of the field sites and are taken from
<xref ref-type="bibr" rid="bib1.bibx36" id="text.174"/>.</p></table-wrap-foot></table-wrap>

<?xmltex \floatpos{th!}?><table-wrap id="Ch1.T3" specific-use="star"><caption><p>Reliability and sensitivity metrics for the DrEICH method of channel
extraction.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">Location</oasis:entry>  
         <oasis:entry colname="col2">Resolution (m)</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mo>∑</mml:mo></mml:math></inline-formula> TP</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mo>∑</mml:mo></mml:math></inline-formula> FP</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mo>∑</mml:mo></mml:math></inline-formula> FN</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Gabilan Mesa</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">5</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>555</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>982</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>1489</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.36</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.27</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>210</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>879</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>1875</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.19</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.1</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>20</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>42</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>734</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>2088</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.05</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.02</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>30</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>13</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>609</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>2122</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.02</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.01</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Santa Cruz Island</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">5</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>3295</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>1971</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>4799</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.63</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.41</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>2454</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>793</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>6865</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.76</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.26</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>20</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>69</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>838</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>8235</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.08</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.01</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>30</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>27</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>915</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>8284</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.03</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.0</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Oregon Coast Range</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">5</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>507</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>1718</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>1131</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.23</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.31</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>144</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>445</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>1462</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.24</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.09</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>20</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>16</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>105</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>1623</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.13</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.01</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>30</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">2</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>442</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>1639</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.0</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.0</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \floatpos{th!}?><table-wrap id="Ch1.T4" specific-use="star"><caption><p>Reliability and sensitivity metrics for the geometric method of
channel extraction.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">Location</oasis:entry>  
         <oasis:entry colname="col2">Resolution (m)</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mo>∑</mml:mo></mml:math></inline-formula> TP</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mo>∑</mml:mo></mml:math></inline-formula> FP</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mo>∑</mml:mo></mml:math></inline-formula> FN</oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Gabilan Mesa</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">5</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>1019</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>519</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>987</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.66</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.51</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>712</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>380</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>1301</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.65</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.35</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>20</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>448</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>332</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>1592</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.57</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.22</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>30</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>292</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>333</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>1775</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.48</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.14</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Santa Cruz Island</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">5</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>4280</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>991</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>3109</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.81</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.57</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>2473</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>777</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>4998</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.76</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.33</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>20</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>334</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>505</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>7861</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.4</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.04</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>30</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>475</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>470</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>7659</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.5</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.06</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Oregon Coast Range</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">5</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>792</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>1438</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>788</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.36</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.5</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>562</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>602</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>938</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.48</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.37</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>20</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>276</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>374</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>1275</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.42</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.18</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mn>30</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mn>475</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mn>277</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mn>1418</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mn>0.38</mml:mn></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mn>0.11</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p>The data for the Oregon Coast Range show similar patterns for both methods,
although the geometric method exhibits systematically larger index values. In
each case the reliability increases slightly from 5 to 10 m resolution and
then declines gradually towards 30 m resolution. The sensitivity indexes for
both methods begin at a larger value than the reliability indexes and
steadily decline towards 0. A sensitivity value exceeding the reliability
value suggests that in this landscape there are fewer missed channel heads in
the 5 m data but at the expense of too many predicted channel heads in
locations where there are none predicted in the 1 m data.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p>Plots of the distribution of hillslope length <bold>(a, c)</bold> and
relief <bold>(b, d)</bold> measurements as resolution is decreased for Santa Cruz
Island. Whiskers are the 2nd and 98th percentiles; the box covers the 25th
and 75th percentiles; the blue bar is the mean and the red bar is the median.
The gray outline is the probability density function of each dataset. The top
row presents the best-case scenario, where an independent constraint on the
channel network is available for the lower-resolution data, and the bottom row
uses the channel networks extracted using the geometric method outlined in
Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/> for each resolution step.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016-f09.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS3">
  <title>Sediment transport coefficient</title>
      <p>Using the values for hilltop curvature generated in Sect. <xref ref-type="sec" rid="Ch1.S4.SS1"/>,
published parameters for erosion rate and material properties outlined in
Table <xref ref-type="table" rid="Ch1.T2"/> and Eq. (<xref ref-type="disp-formula" rid="Ch1.E10"/>), the average sediment
transport coefficient (<inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>) of each landscape can be calculated as a function
of grid resolution. Figure <xref ref-type="fig" rid="Ch1.F8"/> displays the relationship between
diffusivity and grid resolution for each of the three study sites. The data
for Santa Cruz Island and Oregon Coast Range both show a gradual increase in
diffusivity with decreasing grid resolution, the rate of which reduces with
decreasing grid resolution. The Gabilan Mesa data do not exhibit the same
trend, with little variability in calculated <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> values as resolution is
decreased. Although the Oregon Coast Range and Santa Cruz Island datasets
exhibit an increase in estimated <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>, all of the values for each location
fall within the range of values for <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> compiled by
<xref ref-type="bibr" rid="bib1.bibx45" id="text.178"/>.</p>
</sec>
<sec id="Ch1.S4.SS4">
  <title>Hillslope length and relief</title>
      <p>The hillslope length measurements for Santa Cruz Island calculated using 1 m
channel heads (Fig. <xref ref-type="fig" rid="Ch1.F9"/>a) show little variation in the
distribution of the data up to 10 m resolution, with the main difference
being the decrease with grid resolution in the 2nd percentile measurements,
which is a trend observed within each of the datasets. The mean and median
values also gradually decrease towards the 10 m resolution dataset, before
gradually increasing towards the 30 m resolution step. However, these
variations are very small, with the overall distributions of hillslope length
and relief not varying considerably between resolution steps. When the same
hillslope length algorithm is applied using channel networks extracted using
the geometric method for each resolution step (Fig. <xref ref-type="fig" rid="Ch1.F9"/>c), there
is little change in the distribution or average values of <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>H</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> until
beyond the 10 m resolution step. Beyond this point the measurements of
hillslope length are clearly affected by the reduction in accuracy of the
channel network. The relief measurements for both channel head methods
(Fig. <xref ref-type="fig" rid="Ch1.F9"/>b, d) in Santa Cruz Island exhibit little resolution
dependence up to 10 m grid resolution, beyond which point the values
increase steadily. In the case of the 1 m channel heads, the distribution
becomes compressed around the average values at lower resolutions, whereas
with the variable channel head dataset the distribution of values increases
with decreasing resolution.</p>
      <p>In Gabilan Mesa the hillslope length measurements calculated using 1 m
channel heads (Fig. <xref ref-type="fig" rid="Ch1.F10"/>a) show a gradual reduction in mean and
median values between the highest-resolution data and the 8 m resolution
data before a small plateau and then a small increase until the 30 m
dataset. The average relief values calculated for the same dataset increase
steadily by approximately 20 m between the highest- and lowest-resolution
datasets (Fig. <xref ref-type="fig" rid="Ch1.F10"/>b). The distribution of relief measurements are
broadly consistent between 1 and 5 m resolutions before reducing about the
median as grid resolution is decreased. The same trends are apparent in the
hillslope length and relief data calculated using the variable channel heads
(Fig. <xref ref-type="fig" rid="Ch1.F10"/>c, d) with little change between the two pairs of
datasets.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F10" specific-use="star"><caption><p>Plots of the distribution of hillslope length <bold>(a, c)</bold> and
relief <bold>(b, d)</bold> measurements as resolution is decreased for Gabilan
Mesa. Whiskers are the 2nd and 98th percentiles; the box covers the 25th and
75th percentiles; the blue bar is the mean and the red bar is the median. The
gray outline is the probability density function of each dataset. The top row
presents the best-case scenario, where an independent constraint on the
channel network is available for the lower-resolution data, and the bottom row
uses the channel networks extracted using the geometric method outlined in
Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/> for each resolution step.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016-f10.png"/>

        </fig>

      <?xmltex \floatpos{p}?><fig id="Ch1.F11" specific-use="star"><caption><p>Plots of the distribution of hillslope length <bold>(a, c)</bold> and
relief <bold>(b, d)</bold> measurements as resolution is decreased for the Oregon
Coast Range. Whiskers are the 2nd and 98th percentiles; the box covers
the 25th and 75th percentiles; the blue bar is the mean and the red bar
is the median. The gray outline is the probability density function of each
dataset. The top row presents the best case scenario, where an independent
constraint on the channel network is available for the lower-resolution data, and the bottom row uses the channel networks extracted using the geometric
method outlined in Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/> for each resolution step.
At higher-resolution steps the 98th percentile data is not shown in the
plot, to better highlight the distribution of measurements between the 25th
and 75th percentiles, which make up the majority of the data points.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016-f11.png"/>

        </fig>

      <p>The hillslope length measurements for the Oregon Coast Range with channel
heads from the 1 m data (Fig. <xref ref-type="fig" rid="Ch1.F11"/>a) again show a gradual
reduction in the median values with a gradual increase in the mean values
until 20 m grid resolution. Beyond this point the data become considerably
more variable, with a large increase in both the mean and median results. The
relief data shown in Fig. <xref ref-type="fig" rid="Ch1.F11"/>b are the most consistent of the
three landscapes, with very little variation in the values until they begin
increasing with grid resolution at approximately 20 m resolution. The data
presented in Fig. <xref ref-type="fig" rid="Ch1.F11"/>c and d show the most sensitivity to grid
resolution of the three landscapes. Average hillslope length values reduce
towards 10 m before stabilizing and then rapidly increasing in the same
manner as the fixed channel head data. The relief measurements show a gradual
decline in mean relief across the range of resolutions from 1 to 10 m, where
the fixed data show much less variation.</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <title>Discussion</title>
<sec id="Ch1.S5.SS1">
  <title>Curvature and the problem of resolution-dependent filtering</title>
      <p>Across the three landscapes the variance of the distributions of both total
and tangential curvature values are systematically reduced as resolution is
decreased, an effect that is particularly notable after the grid resolution
exceeds 3–4 m (Fig. <xref ref-type="fig" rid="Ch1.F4"/>). In each of the three datasets, the
interquartile ranges remain relatively constant, whereas beyond 4 m
resolution in each case the range between the 2nd and 98th percentiles
reduces rapidly (Fig. <xref ref-type="fig" rid="Ch1.F5"/>), demonstrating that the majority
of the loss of curvature information occurs at the extremes of the
distribution.</p>
      <p>In producing a DEM, we are sampling a complex two-dimensional elevation
signal, in which spatial variations in geomorphic processes drive variations in
topographic amplitude at different wavelengths <xref ref-type="bibr" rid="bib1.bibx85" id="paren.179"/>.
Decreasing the grid resolution of DEMs acts as a low-pass filter on this
topographic signal, which preferentially degrades features in the topography
that have significant amplitude at small wavelengths, such as sharp
ridgelines, narrow valley bottoms, and local topographic roughness generated
by, for example, landslides, tree throw, and rock exposure
(Figs. <xref ref-type="fig" rid="Ch1.F1"/> and <xref ref-type="fig" rid="Ch1.F3"/>). While the position of
ridges and valleys is preserved in coarser-resolution data, the magnitude of
their associated curvature values is reduced as resolution decreases; this
effect is particularly marked for hillslopes in which curvature is focused at
the ridge crest and valley bottoms, a common characteristic of more rapidly
eroding landscapes <xref ref-type="bibr" rid="bib1.bibx97 bib1.bibx99" id="paren.180"/>. For
first-order landscape features, such as gullies, landslide scars, and first-order channels, decreasing grid resolution eventually results in the complete
loss of topographic information, as highlighted in Figs. <xref ref-type="fig" rid="Ch1.F1"/>
and <xref ref-type="fig" rid="Ch1.F3"/>.</p>
<sec id="Ch1.S5.SS1.SSS1">
  <title>Topographic filtering and its implications for curvature and slope measurements</title>
      <p>We can explain some of the observed behavior in Figs. <xref ref-type="fig" rid="Ch1.F4"/>
and <xref ref-type="fig" rid="Ch1.F5"/> through spectral analysis. Spectral analysis assumes
that data can be approximated as the sum of sine waves of varying frequency.
One can apply a spectral filter to any dataset: this simply means that one
transforms input data into output data using linear functions (that is, we
can multiply the input data by a series of weights). Any filter will have a
<italic>gain</italic>, which is the ratio between the filtered amplitude and the
original amplitude. A filter will also have a <italic>fidelity</italic>, which is the
ratio between the continuous gain and the discrete gain. We are using
discrete data, so the fidelity measures how well our discrete filter is able
to reproduce a theoretical signal that is continuous. We can never have
continuous data since lidar is not continuous: our filters will always
represent an imperfect version of nature and fidelity quantifies just how
imperfect it is. Hopefully our readers will not be put off by this foray into
jargon, and we can move on to practical application of spectral filters for
use in topographic applications.</p>
      <p>We will examine the spectral behavior of a simplified one-dimensional system.
We acknowledge that a 1-D approach cannot fully describe complex two-dimensional topography of real landscapes, but a one-dimensional system is
amenable to mathematical treatment that can at least give us qualitative
insight into trends observed in our data. In addition, some of the features
of interest, for example ridgelines and channels, can be roughly approximated
as one-dimensional structures within a two-dimensional landscape.</p>
      <p>Curvature in one dimension, <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> [<inline-formula><mml:math display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">L</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>], is often approximated
with the differencing equation:
              <disp-formula id="Ch1.E11" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ζ</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi mathvariant="italic">ζ</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">ζ</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">ζ</mml:mi></mml:math></inline-formula> [<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">L</mml:mi></mml:math></inline-formula>] is the elevation of the land surface, <inline-formula><mml:math display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>
[<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">L</mml:mi></mml:math></inline-formula>] is a location in space, <inline-formula><mml:math 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 curvature at location
<inline-formula><mml:math display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:math></inline-formula> [<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">L</mml:mi></mml:math></inline-formula>] is the grid interval. The subscripts
denote the discrete locations where elevation is evaluated.
Equation (<xref ref-type="disp-formula" rid="Ch1.E11"/>) is in fact a spectral filter. The
original data is <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">ζ</mml:mi></mml:math></inline-formula>, which is distributed in space, and the weights in
the filter are <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for data points at <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>,
respectively. From this filter, we can calculate the <italic>wave number response function</italic>. A full description of the theory and significance of a
wave number response function can be found in <xref ref-type="bibr" rid="bib1.bibx48" id="text.181"/>.
For our purposes, it is sufficient to know that this function must be
calculated if we are to calculate the gain and fidelity of the filter (which
here is a measure of curvature of our elevation data). The wave number
response function (<inline-formula><mml:math display="inline"><mml:mrow><mml:mi>H</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mo>;</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>) from this filter, given by
<xref ref-type="bibr" rid="bib1.bibx48" id="text.182"/> in their Eq. (7.3.7), is
              <disp-formula id="Ch1.E12" content-type="numbered"><mml:math display="block"><mml:mrow><mml:mi>H</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mo>;</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">2</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>[</mml:mo><mml:mi>cos⁡</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>]</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="italic">ω</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">π</mml:mi><mml:mo>/</mml:mo><mml:mi>L</mml:mi><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mo>[</mml:mo><mml:msup><mml:mi mathvariant="normal">L</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>] is the wave number with wavelength
<inline-formula><mml:math display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula> [<inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">L</mml:mi></mml:math></inline-formula>]. Higher wave numbers correspond to shorter wavelengths.
Using this function, we can calculate the gain, <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>G</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mo>;</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>. Again,
the gain measures the ratio of the amplitude of the filtered signal (in this
case curvature) to the amplitude of the original signal (in this case
elevation) at the wave number <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">ω</mml:mi></mml:math></inline-formula>. The theoretical gain for continuous
waveforms of curvature (i.e., not discrete filters like
Eq. <xref ref-type="disp-formula" rid="Ch1.E11"/>) is <inline-formula><mml:math display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">ω</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>. The gain of a discrete
filter is the modulus of the wave number response function <xref ref-type="bibr" rid="bib1.bibx48" id="paren.183"><named-content content-type="pre">see p. 296
in</named-content></xref>, so in the case of
Eq. (<xref ref-type="disp-formula" rid="Ch1.E12"/>) the resultant gain, <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>G</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mo>;</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is
              <disp-formula id="Ch1.E13" content-type="numbered"><mml:math display="block"><mml:mrow><mml:mi>G</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mo>;</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">2</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>[</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi>cos⁡</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msup><mml:mi>cos⁡</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:msup><mml:mo>]</mml:mo><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p>In the case of our curvature filter (Eq. <xref ref-type="disp-formula" rid="Ch1.E11"/>), the
gain function reveals how high-frequency waveforms (e.g., ridge crests,
tree throw mounds, local roughness) in the elevation data involve relatively
large values of curvature, whereas low-frequency elevation waveforms (e.g.,
ridge–valley features or geologic folds) with the same amplitude involve
relatively small curvatures. Crucially, however, the discrete filter does not
retain all of the high-frequency information. Some of this information is
lost in the discretization process (i.e., it is lost because we are sampling
the data at fixed intervals rather than having continuous information about
the surface). We can calculate what information is lost by calculating the
fidelity, which is the ratio between discrete gain (Eq. <xref ref-type="disp-formula" rid="Ch1.E13"/>) and the
theoretical gain (<inline-formula><mml:math display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">ω</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>):

                  <disp-formula specific-use="align" content-type="numbered"><mml:math display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E14"><mml:mtd/><mml:mtd/><mml:mtd><mml:mrow><mml:mi>F</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mo>;</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">2</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:msup><mml:mi mathvariant="italic">ω</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>[</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi>cos⁡</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msup><mml:mi>cos⁡</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:msup><mml:mo>]</mml:mo><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12"><caption><p>Plot of fidelity (<inline-formula><mml:math display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula>) of two one-dimensional differencing
operations: curvature (Eq. <xref ref-type="disp-formula" rid="Ch1.E11"/>) and topographic
gradient (Eq. <xref ref-type="disp-formula" rid="Ch1.E15"/>) as a function dimensionless
wave number <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>/</mml:mo><mml:mi>L</mml:mi></mml:mrow></mml:math></inline-formula> to the Nyquist wave number, <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>/</mml:mo><mml:mi>L</mml:mi><mml:mo>=</mml:mo><mml:mn>0.5</mml:mn></mml:mrow></mml:math></inline-formula>.</p></caption>
            <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://esurf.copernicus.org/articles/4/627/2016/esurf-4-627-2016-f12.png"/>

          </fig>

      <p>Again, fidelity is a measure of how closely our discrete filter (here
curvature measured at discrete points in the landscape) reflects the true
curvature (that is, the curvature measured if we had a perfectly continuous
dataset). Fidelity is a function of the ratio between the grid interval and
the wavelength (Fig. <xref ref-type="fig" rid="Ch1.F12"/>). When the fidelity is unity, the
discrete filter exactly reproduces the underlying continuous function. Again,
the landscape (and its derivative metrics like curvature and gradient) has
features at different wavelengths, such as long-wavelength ridges and valleys
and short-wavelength tree throw mounds.</p>
      <p>As the frequency approaches the Nyquist wave number, defined as <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>/</mml:mo><mml:mi>L</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>, fidelity decreases (Fig. <xref ref-type="fig" rid="Ch1.F12"/>); a fidelity of only
approximately 0.4 is achieved at the Nyquist wave number itself. To achieve a
fidelity, <inline-formula><mml:math display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula>, of 0.9 requires that <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>L</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:math></inline-formula> is equal to approximately
six grid points per wavelength. A fidelity <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>F</mml:mi><mml:mo>=</mml:mo><mml:mn>0.95</mml:mn></mml:mrow></mml:math></inline-formula> requires eight points per
wavelength, and <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>F</mml:mi><mml:mo>=</mml:mo><mml:mn>0.99</mml:mn></mml:mrow></mml:math></inline-formula> requires 18. Therefore, while the grid resolution
imposes a minimum wavelength that can be resolved (defined by the Nyquist
wave number), the behavior of the fidelity function (Fig. <xref ref-type="fig" rid="Ch1.F12"/>),
clearly illustrates that curvature information will be lost when calculated
for features with wavelengths greater than but still close to the minimum
resolvable at the Nyquist wave number.</p>
      <p>What does this mean in practical terms? In our simple, one-dimensional
example, if we use 1 m resolution data we can only capture the curvature of
a one-dimensional ridgeline that had a wavelength of 3–4 m (one does not
need the entire wave to capture the peak of the waveform) but with a loss of
fidelity on the magnitude of the curvature. Or, in other words, we would
underestimate the magnitude of the curvature.</p>
      <p>Another landscape metric that is widely measured is topographic gradient. In
our study we have not computed how topographic gradient varies as a function
of grid resolution because this has been examined by many previous authors
(e.g., <xref ref-type="bibr" rid="bib1.bibx30" id="altparen.184"/>, <xref ref-type="bibr" rid="bib1.bibx124" id="altparen.185"/>, and <xref ref-type="bibr" rid="bib1.bibx121" id="altparen.186"/>).
However, our treatment of the properties of a one-dimensional filter can give
some insight into previous results. Consider a simple central-difference
approximation of the topographic gradient (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, dimensionless):
              <disp-formula id="Ch1.E15" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ζ</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">ζ</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p>Equation (<xref ref-type="disp-formula" rid="Ch1.E15"/>) is yet another spectral filter, with
weights of <inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> at <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>x</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>
at <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:math></inline-formula>. We can follow the same series of operations that we
performed on Eq. (<xref ref-type="disp-formula" rid="Ch1.E11"/>) to arrive at the fidelity of
Eq. (<xref ref-type="disp-formula" rid="Ch1.E15"/>), denoted as <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mtext>S</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, taking into
account that the theoretical gain is <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">ω</mml:mi></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx48" id="paren.187"><named-content content-type="pre">see Eq. 7.3.8
in</named-content></xref>:
              <disp-formula id="Ch1.E16" content-type="numbered"><mml:math display="block"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mtext>S</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mo>;</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mi mathvariant="italic">ω</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>[</mml:mo><mml:mi>sin⁡</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">ω</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>]</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p>Equation (<xref ref-type="disp-formula" rid="Ch1.E16"/>) formally illustrates why
estimates of slope tend to systematically decrease with increasing grid
interval <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:math></inline-formula> (Fig. <xref ref-type="fig" rid="Ch1.F12"/>). Namely, an increasing <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:math></inline-formula> is able to resolve less local (high wave number) elevation structure while
picking out the slope of more regional structure. The fidelity increases as
the ratio of the grid interval to the wavelength, <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>/</mml:mo><mml:mi>L</mml:mi></mml:mrow></mml:math></inline-formula>, decreases
(Fig. <xref ref-type="fig" rid="Ch1.F12"/>). To achieve a fidelity <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mtext>S</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn>0.9</mml:mn></mml:mrow></mml:math></inline-formula>, for
example, requires <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>L</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:math></inline-formula> or approximately eight grid points per wavelength.
A fidelity <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mtext>S</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn>0.95</mml:mn></mml:mrow></mml:math></inline-formula> requires 11 points per wavelength, and
<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mtext>S</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn>0.99</mml:mn></mml:mrow></mml:math></inline-formula> requires 18. The fidelity of the one-dimensional gradient
operator goes to 0 when approaching the Nyquist wave number (<inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>/</mml:mo><mml:mi>L</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>). These results explain the pronounced loss of gradient information in
coarse-resolution data observed by many authors
(e.g., <xref ref-type="bibr" rid="bib1.bibx30" id="altparen.188"/>, <xref ref-type="bibr" rid="bib1.bibx124" id="altparen.189"/>, and <xref ref-type="bibr" rid="bib1.bibx121" id="altparen.190"/>).</p>
</sec>
<sec id="Ch1.S5.SS1.SSS2">
  <title>Total and tangential curvature</title>
      <p>Having explored simplified one-dimensional filters, we now return to our two-dimensional results. Although real landscapes are two-dimensional and we use
polynomial fitting rather than simple differencing as in
Eq. (<xref ref-type="disp-formula" rid="Ch1.E11"/>), we can still use
Eq. (<xref ref-type="disp-formula" rid="Ch1.E14"/>) as a qualitative indicator of the grid
resolution required for appropriate curvature estimates. In the Gabilan Mesa,
where ridgelines are broad, lower-resolution data can still capture the
curvature with relatively high fidelity. However, in locations with sharper
ridgelines, such as Santa Cruz Island, the narrowest ridgelines are no longer
adequately resolved as the grid resolution is decreased, as can be seen in
Fig. <xref ref-type="fig" rid="Ch1.F3"/>.</p>
      <p>The loss of fidelity predicted by the simple one-dimensional system
(Eq. <xref ref-type="disp-formula" rid="Ch1.E14"/>) qualitatively predicts the pattern observed in
Figs. <xref ref-type="fig" rid="Ch1.F4"/> and <xref ref-type="fig" rid="Ch1.F5"/>, namely that the curvature
values are smeared over a greater length scale leading to apparently broader
ridges with resolution and a systematic underestimation of their peak
elevations. This highlights that in conjunction with data quality, landscape
morphology also exerts a control on the optimal resolution to use for a given
study, where landscapes with more gradual hillslope to valley transition
morphologies can be analyzed using coarser-resolution topographic data with
more confidence. Although the identification of landscape morphology is often
achieved through observations of high-resolution topography, it can be
achieved through field observations and the use of ancillary datasets, which
allow the qualitative checking of results obtained from a low-resolution
dataset.</p>
      <p>Santa Cruz Island and the Oregon Coast Range have the highest tangential
curvature at 1 m resolution. High tangential curvature at Santa Cruz Island
corresponds to observations of extensive gullying and hillslope erosion
<xref ref-type="bibr" rid="bib1.bibx89 bib1.bibx88" id="paren.191"/>. In the Oregon Coast
Range, features such as pit and mound topography produced by tree throw and
other biotic activity are resolved in the lidar dataset
<xref ref-type="bibr" rid="bib1.bibx100 bib1.bibx62" id="paren.192"/>, which manifests itself as an
increase in values of curvature. However, this could also be indicative of
non-topographic noise in the DEM surface produced during the processing of
the point clouds, which is particularly required in heavily forested
locations <xref ref-type="bibr" rid="bib1.bibx60 bib1.bibx63" id="paren.193"/> such as the Oregon Coast
Range. This suggests an unfortunate collinearity between the two causes of
small-wavelength topographic noise and warrants further testing in future to
disentangle synthetic and natural noise from high-resolution topographic
measurements. However, high curvature is not solely a manifestation of
stochastic disturbance in local topographic roughness but is also generated
at narrow valley bottoms and at ridgelines where erosion rates are rapid
relative to the hillslope sediment transport coefficient
<xref ref-type="bibr" rid="bib1.bibx99 bib1.bibx42" id="paren.194"/>. Gabilan Mesa exhibits much
lower curvature values than the other two locations, which is a consequence
of high landscape diffusivity, indicating that sediment transport at Gabilan
Mesa is dominated by diffusion-like processes
<xref ref-type="bibr" rid="bib1.bibx99" id="paren.195"/>, smoothing the landscape and reducing the
tangential curvature of the hillslope surface.</p>
</sec>
</sec>
<sec id="Ch1.S5.SS2">
  <title>Channel extraction</title>
      <p>It is intuitive to consider that when extracting channel networks at any data
resolution, regardless of method, the higher-order, larger channels will be
more accurately constrained than lower-order channels. This pattern is
observed in each of the study landscapes, with the majority of the variations
in channel locations occurring in first- and second-order channels. Such loss
of low-order channels from datasets has implications for studies focusing on
upland areas, in particular where detailed measurements which depend on
channel network position are performed.</p>
      <p>The contrast between the extent of channel networks and their indexes of
quality for the two methods outline that a geometric method of channel
extraction outperforms the process-based DrEICH algorithm. Due to the
relative simplicity of the geometric method of channel extraction, errors
inherent in the DEM are not compounded on the same scale as the DrEICH
algorithm, which performs more operations on topographic data. As the
geometric method identifies channels based on their tangential curvature,
although channel head features may be smoothed out of the DEM as resolution
is decreased, the channel will still express some positive curvature in lower-resolution data. The initiation point may be located downslope of the true
channel head but even in this worst case most of the channel network will be
extracted correctly. This is observed in Fig. <xref ref-type="fig" rid="Ch1.F6"/> which
shows a gradual reduction in drainage density as the grid resolution is
decreased.</p>
      <p>The indexes of quality defined by <xref ref-type="bibr" rid="bib1.bibx78" id="text.196"/> provide a
clear framework to understand the quality of channel head predictions using
these two methods as data resolution is decreased. In each case, the
geometric method outperforms the DrEICH method, both in the accuracy of the
channel heads which are predicted, and in the ability of the method to not
predict channel heads in locations where no channel exists. These indexes are
influenced by the size of the search radius around each channel head, and
reducing this radius would decrease the index values. However, the use of a
30 m search radius allows comparisons to be drawn between predictions made
at different data resolutions, and also between this study and that of
<xref ref-type="bibr" rid="bib1.bibx78" id="text.197"/>.</p>
      <p>This assessment of high-resolution methods with degraded-quality data
demonstrates the ongoing challenges that channel extraction poses to the
geomorphology community. <xref ref-type="bibr" rid="bib1.bibx78" id="text.198"/> performed
extensive testing on channel extraction using threshold channel extraction
methods and demonstrated similar limitations when channels were extracted
using lower-resolution data. Our results suggest that a geometric method of
channel extraction will provide an optimal channel network as data quality is
reduced, particularly in uniform landscapes such as Gabilan Mesa. However,
the only way to ensure the highest-quality results is to employ high-resolution data in conjunction with field mapping of channel network extents.</p>
</sec>
<sec id="Ch1.S5.SS3">
  <title>Sediment transport coefficient</title>
      <p>The predicted values of the sediment transport coefficient (<inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>) for the 1 m
data fall within the range of values compiled by
<xref ref-type="bibr" rid="bib1.bibx45" id="text.199"/> and estimated for the Oregon Coast Range and
Gabilan Mesa by <xref ref-type="bibr" rid="bib1.bibx97" id="text.200"/> and
<xref ref-type="bibr" rid="bib1.bibx99" id="text.201"/>. This suggests that this method can produce
useful estimates of <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> when employing high-resolution topography.</p>
      <p>The sediment transport coefficients calculated at the Oregon Coast Range and
Santa Cruz Island locations both increase with grid resolution, reflecting
the sensitivity of <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mtext>HT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> to grid resolution in each of these
locations. Despite the Oregon Coast Range eroding 45 % more rapidly
(Table <xref ref-type="table" rid="Ch1.T2"/>) than Santa Cruz Island, the rate of increase in <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>
measurements remains similar between the two landscapes. Gabilan Mesa data
are generally insensitive to a decrease in grid resolution, as the scale of
hilltop widths measured in Gabilan Mesa is on the order of tens of meters.
This allows datasets with grid resolutions approaching half the width of a
hilltop to provide an accurate estimate of hilltop curvature and, thus, the
sediment transport coefficient.</p>
      <p>These data suggest that estimating <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> from low-resolution topographic data
is possible in many landscapes, particularly those which have average
ridgelines broader than the grid resolution of the topographic data. In the
case of landscapes with sharper ridgelines such as Santa Cruz Island and the
Oregon Coast Range, it is more challenging to constrain <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> effectively as
the grid resolution is decreased. The magnitude of the overestimation of <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>
between the highest- and lowest-resolution diffusivity estimates,
0.0023 m<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> a<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in the case of the Oregon Coast Range, will be a
product of the uncertainty within the calculation of the erosion rate and
material densities in addition to the local variations of <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> within each
landscape.</p>
</sec>
<sec id="Ch1.S5.SS4">
  <title>Hillslope length and relief</title>
      <p>Measurements of hillslope length and relief have been used to test sediment
flux laws <xref ref-type="bibr" rid="bib1.bibx99 bib1.bibx32" id="paren.202"/> and to identify
landscape transience <xref ref-type="bibr" rid="bib1.bibx44 bib1.bibx71" id="paren.203"/>. Such
analyses have previously been restricted to high-resolution topographic data.
When considering hillslope length, we must select a grid resolution that is
at least half the median hillslope length in order to resolve any useful
information. However, in reality more than two pixels are required if any
meaningful information is to be extracted from topographic data. As the
median hillslope length for many landscapes has been shown to be in excess of
100 m <xref ref-type="bibr" rid="bib1.bibx32" id="paren.204"/>, this requirement for several pixels per
hillslope falls well within the range of many lower-resolution data products.
Therefore, our results show that meaningful hillslope length measurements can
be made from lower-resolution topographic data, with data products
approaching 30 m resolution proving suitable in some cases.</p>
      <p>The relief measurements for each landscape, however, show more sensitivity to
grid resolution, with a systematic increase in the median values in each
location beyond 10 m grid resolution. As decreasing grid resolution acts as
a low-pass filter on the landscape, the elevation of ridges are expected to
be reduced, whilst the elevation of channel beds are raised, producing a net
reduction in topographic relief. However, the increased relief observed with
decreasing grid resolution is produced by the decrease in drainage density
with decreasing resolution observed in Fig. <xref ref-type="fig" rid="Ch1.F6"/>; this
produces fewer channels reaching up towards ridgelines and leading to hillslope flow paths
traveling further downslope before reaching a channel.</p>
      <p>By contrasting the <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>H</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> results computed using fixed and
variable channel heads, it is clear that the optimal method for measuring
hillslope length and relief is to employ as accurate a channel network as
possible. However, the variable channel head data show that the signal of
average hillslope length and relief is broadly insensitive to data resolution
up to grid resolutions of at least 10 m. This would facilitate the analysis
of landscape transience using these measurements on a global scale, using
high-resolution satellite-derived DEMs, such as TanDEM-X
<xref ref-type="bibr" rid="bib1.bibx55" id="paren.205"/>. This relationship is again strongest in
Gabilan Mesa, the landscape with the least topographic complexity which
demonstrates the least sensitivity to curvature measurements and the
estimation of diffusivity. However, even in the more noisy landscape of the
Oregon Coast Range, meaningful hillslope length and relief measurements can
still be made through the use of a geometric channel extraction algorithm and
lower-resolution topographic data.</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <title>Conclusions</title>
      <p>Through the generation of topographic data spanning the range of grid resolutions
currently used in much of geomorphic research, a number of key metrics have
been evaluated for their sensitivity to grid resolution. We have demonstrated
the reduction in the range of total and tangential curvature values as grid
resolution is decreased, across three test landscapes. These curvature
measurements are important in the estimation of the hillslope sediment
transport coefficient (<inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>), in their use as a proxy for erosion rate, and in
the extraction of channel networks from topographic data. We demonstrate that
the estimation of <inline-formula><mml:math display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> from low-resolution topographic data is possible,
particularly in landscapes such as Gabilan Mesa where hilltops are broad.
Higher resolutions are required to extract meaningful curvature information
in steep landscapes with sharp ridges and narrow gullies.<?xmltex \hack{\newpage}?></p>
      <p>The extraction of channel networks from digital topographic data is a
significant challenge on all spatial scales, as the definition of a channel
network is integral in the execution of many analyses (e.g., <xref ref-type="bibr" rid="bib1.bibx15" id="altparen.206"/>, <xref ref-type="bibr" rid="bib1.bibx42" id="altparen.207"/>, and <xref ref-type="bibr" rid="bib1.bibx32" id="altparen.208"/>). We
demonstrate that the use of a geometric channel extraction algorithm produces
channel networks for all three of our landscapes which correspond well to
networks extracted from high-resolution topography. This correspondence is
tested through the computation of quality indexes for each predicted network,
which outline the suitability of this algorithm over a process-based method
at coarse DEM resolutions.</p>
      <p>Average values of hillslope length and relief for each landscape are shown to
be broadly insensitive to grid resolution up to grid resolutions which
correspond to the highest-resolution topographic data globally available.
This indicates that these measurements can be used to identify landscape
transience in locations where lidar data are unavailable. The accuracy of
these measurements is dependent on the accuracy of the channel network used,
however, as using a geometric method of channel extraction from the 1 m DEM
still provides robust measurements of hillslope length and relief.</p>
      <p>The relationships between decreasing grid resolution and the geomorphic
parameters explored here demonstrate the influence of the spatial scale of
the topographic expression of process on the quality of results which can be
extracted from lower-resolution topography. From these analyses it is
challenging to identify a clear threshold below which data become unsuitable
for use in geomorphic analysis. Rather, it is important to highlight the
influence of landscape morphology and the dominant processes acting upon it
in the selection of an appropriate data resolution for a study. Using this
work as a framework, it is now possible to place constraints on the accuracy
of results derived from coarse-resolution topographic data, particularly
where non-topographic or field data can be used to provide insight into
general landscape morphology.
<?xmltex \hack{\newpage}?></p>
</sec>
<sec id="Ch1.S7">
  <title>Code availability</title>
      <p>All of the code used in this analysis is open source and the topographic
analysis routines are available at
<uri>http://github.com/LSDtopotools/LSD_Resolution</uri>; the code to generate
the figures in this paper, alongside the raw plot data, can be downloaded from
<uri>http://github.com/sgrieve/Resolution_Paper_Figs</uri>.</p>
</sec>
<sec id="Ch1.S8">
  <title>Data availability</title>
      <p>The topographic data used in this study are freely available from
<uri>http://www.OpenTopography.org</uri>, and the specific point clouds used can
be downloaded from
<uri>http://hdl.handle.net/10283/2071</uri>.</p><?xmltex \hack{\clearpage}?>
</sec>

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

<app id="App1.Ch1.S1">
  <title>Channel extraction parameters</title>
      <p>This table provides the parameters used to generate channel networks both
using the geometric method and the DrEICH method. The drainage area value is
used to thin the initial extracted network by removing channels which have a
drainage area below the threshold value. The connected-components value
defines the point at which a group of contiguous channel pixels are
considered to be connected. The <inline-formula><mml:math display="inline"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mi>m</mml:mi><mml:mi>n</mml:mi></mml:mfrac></mml:mstyle></mml:math></inline-formula> ratio is determined using
software provided by <xref ref-type="bibr" rid="bib1.bibx73" id="text.209"/>, and its use within this
context is discussed in detail in <xref ref-type="bibr" rid="bib1.bibx12" id="text.210"/>.</p>

<?xmltex \floatpos{t}?><table-wrap id="App1.Ch1.T1"><?xmltex \hack{\hsize\textwidth}?><caption><p>Parameters used by the geometric and process-based techniques in the
extraction of channel networks.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="6">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="left"/>
     <oasis:colspec colnum="6" colname="col6" align="left"/>
     <oasis:thead>
       <oasis:row>  
         <oasis:entry colname="col1">Location</oasis:entry>  
         <oasis:entry colname="col2">Window</oasis:entry>  
         <oasis:entry colname="col3">Drainage</oasis:entry>  
         <oasis:entry colname="col4">Connected</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mi>m</mml:mi><mml:mi>n</mml:mi></mml:mfrac></mml:mstyle></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6">Reference</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">radius (<inline-formula><mml:math display="inline"><mml:mi>m</mml:mi></mml:math></inline-formula>)</oasis:entry>  
         <oasis:entry colname="col3">area (<inline-formula><mml:math display="inline"><mml:mrow><mml:msup><mml:mi>m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>  
         <oasis:entry colname="col4">components (Pixels)</oasis:entry>  
         <oasis:entry colname="col5">ratio</oasis:entry>  
         <oasis:entry colname="col6"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Santa Cruz Island</oasis:entry>  
         <oasis:entry colname="col2">4</oasis:entry>  
         <oasis:entry colname="col3">4</oasis:entry>  
         <oasis:entry colname="col4">5</oasis:entry>  
         <oasis:entry colname="col5">0.50</oasis:entry>  
         <oasis:entry colname="col6">This study</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Gabilan Mesa</oasis:entry>  
         <oasis:entry colname="col2">5</oasis:entry>  
         <oasis:entry colname="col3">4</oasis:entry>  
         <oasis:entry colname="col4">5</oasis:entry>  
         <oasis:entry colname="col5">0.45</oasis:entry>  
         <oasis:entry colname="col6">
                  <xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx33" id="text.211"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Oregon Coast Range</oasis:entry>  
         <oasis:entry colname="col2">4</oasis:entry>  
         <oasis:entry colname="col3">4</oasis:entry>  
         <oasis:entry colname="col4">5</oasis:entry>  
         <oasis:entry colname="col5">0.45</oasis:entry>  
         <oasis:entry colname="col6">
                  <xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx33" id="text.212"/>
                </oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \hack{\clearpage}?>
</app>
  </app-group><notes notes-type="authorcontribution">

      <p>Stuart W. D. Grieve, Simon M. Mudd, David T. Milodowski, and Fiona J. Clubb wrote the software. Stuart W. D. Grieve performed the
analysis. David J. Furbish and Simon M. Mudd resurrected the spectral
filtering analysis from an unpublished 2002 manuscript because they are
lovers of the long game. Stuart W. D. Grieve wrote the paper with
contributions from the other authors.</p>
  </notes><ack><title>Acknowledgements</title><p>Simon M. Mudd and Stuart W. D. Grieve are funded by NERC grant NE/J009970/1
and Simon M. Mudd is funded by US Army Research Office contract number
W911NF-13-1-0478. Fiona J. Clubb is funded by the Carnegie Foundation for the
Universities of Scotland. David T. Milodowski was funded by a NERC Doctoral
Training Grant NE/152830X/1 and NE/J500021/1. David J. Furbish was funded by
US National Science Foundation grant EAR-1420831. We thank Marie-Alice Harel,
Kristin Sweeney, Wolfgang Schwanghart, and two anonymous reviewers for
comments on earlier versions of this manuscript.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?> Edited by: R. Gloaguen<?xmltex \hack{\newline}?> Reviewed by:
K. Sweeney, W. Schwanghart, and two anonymous referees</p></ack><ref-list>
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    </app></app-group></back>
    <!--<article-title-html>How does grid-resolution modulate the topographic expression of geomorphic processes?</article-title-html>
<abstract-html><p class="p">In many locations, our ability to study the processes which shape
the Earth are greatly enhanced through the use of high-resolution digital
topographic data. However, although the availability of such datasets has
markedly increased in recent years, many locations of significant geomorphic
interest still do not have high-resolution topographic data available. Here,
we aim to constrain how well we can understand surface processes through
topographic analysis performed on lower-resolution data. We generate digital
elevation models from point clouds at a range of grid resolutions from 1 to
30 m, which covers the range of widely used data resolutions available
globally, at three locations in the United States. Using these data, the
relationship between curvature and grid resolution is explored, alongside the
estimation of the hillslope sediment transport coefficient (<i>D</i>, in
m<sup>2</sup> yr<sup>−1</sup>) for each landscape. Curvature, and consequently <i>D</i>, values
are shown to be generally insensitive to grid resolution, particularly in
landscapes with broad hilltops and valleys. Curvature distributions, however,
become increasingly condensed around the mean, and theoretical considerations
suggest caution should be used when extracting curvature from landscapes with
sharp ridges. The sensitivity of curvature and topographic gradient to grid
resolution are also explored through analysis of one-dimensional
approximations of curvature and gradient, providing a theoretical basis for
the results generated using two-dimensional topographic data. Two methods of
extracting channels from topographic data are tested. A geometric method of
channel extraction that finds channels by detecting threshold values of
planform curvature is shown to perform well at resolutions up to 30 m in all
three landscapes. The landscape parameters of hillslope length and relief are
both successfully extracted at the same range of resolutions. These
parameters can be used to detect landscape transience and our results suggest
that such work need not be confined to high-resolution topographic data. A
synthesis of the results presented in this work indicates that although high-resolution (e.g., 1 m) topographic data do yield exciting possibilities
for geomorphic research, many key parameters can be understood in lower-resolution data, given careful consideration of how analyses are performed.</p></abstract-html>
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