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  <front>
    <journal-meta><journal-id journal-id-type="publisher">TC</journal-id><journal-title-group>
    <journal-title>The Cryosphere</journal-title>
    <abbrev-journal-title abbrev-type="publisher">TC</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">The Cryosphere</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1994-0424</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/tc-12-3477-2018</article-id><title-group><article-title>Repeat mapping of snow depth across an alpine catchment with RPAS
photogrammetry</article-title><alt-title>Repeat mapping of snow depth across an alpine catchment</alt-title>
      </title-group><?xmltex \runningtitle{Repeat mapping of snow depth across an alpine catchment}?><?xmltex \runningauthor{T.~A.~N. Redpath et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Redpath</surname><given-names>Todd A. N.</given-names></name>
          <email>todd.redpath@otago.ac.nz</email>
        <ext-link>https://orcid.org/0000-0001-9322-0245</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Sirguey</surname><given-names>Pascal</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Cullen</surname><given-names>Nicolas J.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8877-1325</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Department of Geography, University of Otago, Dunedin, 9016, New
Zealand</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>National School of Surveying, University of Otago, Dunedin, 9016, New
Zealand</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Todd A. N. Redpath (todd.redpath@otago.ac.nz)</corresp></author-notes><pub-date><day>8</day><month>November</month><year>2018</year></pub-date>
      
      <volume>12</volume>
      <issue>11</issue>
      <fpage>3477</fpage><lpage>3497</lpage>
      <history>
        <date date-type="received"><day>14</day><month>May</month><year>2018</year></date>
           <date date-type="rev-request"><day>6</day><month>June</month><year>2018</year></date>
           <date date-type="rev-recd"><day>8</day><month>September</month><year>2018</year></date>
           <date date-type="accepted"><day>3</day><month>October</month><year>2018</year></date>
      </history>
      <permissions>
        
        
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018.html">This article is available from https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018.html</self-uri><self-uri xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018.pdf">The full text article is available as a PDF file from https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018.pdf</self-uri>
      <abstract>
    <p id="d1e104">Being dynamic in time and space, seasonal snow represents a difficult target
for ongoing in situ measurement and characterisation. Improved understanding
and modelling of the seasonal snowpack requires mapping snow depth at fine
spatial resolution. The potential of remotely piloted aircraft system (RPAS)
photogrammetry to resolve spatial variability of snow depth is evaluated
within an alpine catchment of the Pisa Range, New Zealand. Digital surface
models (DSMs) at 0.15 m spatial resolution in autumn (snow-free reference)
winter (2 August 2016) and spring (10 September 2016) allowed mapping of snow
depth via DSM differencing. The consistency and accuracy of the RPAS-derived
surface was assessed by the propagation of check point residuals from the
aero-triangulation of constituent DSMs and via comparison of snow-free
regions of the spring and autumn DSMs. The accuracy of RPAS-derived snow
depth was validated with in situ snow probe measurements. Results for
snow-free areas between DSMs acquired in autumn and spring demonstrate
repeatability yet also reveal that elevation errors follow a distribution
that substantially departs from a normal distribution, symptomatic of the
influence of DSM co-registration and terrain characteristics on vertical
uncertainty. Error propagation saw snow depth mapped with an accuracy of <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.08</mml:mn></mml:mrow></mml:math></inline-formula> m (90 % c.l.). This is lower than the characterization of
uncertainties on snow-free areas (<inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.14</mml:mn></mml:mrow></mml:math></inline-formula> m). Comparisons between RPAS
and in situ snow depth measurements confirm this level of performance of RPAS
photogrammetry while also highlighting the influence of vegetation on snow
depth uncertainty and bias. Semi-variogram analysis revealed that the RPAS
outperformed systematic in situ measurements in resolving fine-scale spatial
variability. Despite limitations accompanying RPAS photogrammetry, which are
relevant to similar applications of surface and volume change analysis, this
study demonstrates a repeatable means of accurately mapping snow depth for an
entire, yet relatively small, hydrological catchment (<?xmltex \hack{\mbox\bgroup}?><inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula><?xmltex \hack{\egroup}?> km<inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> at very high resolution. Resolving snowpack features
associated with redistribution and preferential accumulation and ablation,
snow depth maps provide geostatistically robust insights into seasonal snow
processes, with unprecedented detail. Such data will enhance understanding of
physical processes controlling spatial distributions of seasonal snow and
their relative importance on varying spatial and temporal scales.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e158">Seasonal snow provides a globally important water resource (Mankin et al.,
2015; Sturm et al., 2017), which is highly variable in space and time (Clark
et al., 2011). Difficulties associated with collecting field observations
limit the characterisation and understanding of spatial variability in snow
depth and, in turn, our ability to improve spatially distributed modelling
of seasonal snow. While insight can be gained via modelling on moderate to
large scales (Winstral et al., 2013), resolving the fine-scale variability
and its controlling processes remains limited by the ability to capture such
variability in the field (Clark et al., 2011). Since water storage within a
snowpack is a function of snow depth and density, and the former exhibits
higher spatial variability than the latter, advances in measuring snow depth
at high spatial resolution offer promise for improved estimates of snow
water equivalent (SWE) (Harder et al., 2016).</p>
      <?pagebreak page3478?><p id="d1e161">Historically, studies of seasonal snow processes have relied on in situ
observations. With biweekly temporal resolution, Anderson et al. (2014)
gained substantial insights into physical controls on seasonal snow
processes, albeit with a dependence on statistical scaling to relate transect-scale observations to basin-scale processes. Alternatively, the nature of
automated snow measurement instrumentation often precludes continuous in situ
measurement across networks sufficiently dense to characterise fine-scale
spatial variability. Kinar and Pomeroy (2015) provide a comprehensive review
of instrumentation and techniques for measuring snow depth and characterising
snowpacks. In summary, while instrumentation and methodologies exist for
obtaining accurate and temporally continuous, measurements of snow depth and
related snowpack properties at point locations, adequately resolving the high
spatial variability of snow depth remains a challenge. This is exacerbated by
local field conditions, such as exposure to wind or the complexity of the
topography and vegetation further increasing the spatial variability in snow
depth (Clark et al., 2011; Kerr et al., 2013; Winstral and Marks, 2014).</p>
      <p id="d1e164">Remote sensing has provided substantial advances in quantification of
seasonal snow variability, with imaging sensors supporting spatial and
temporal resolutions that allow a range of scales to be explored.
Space-borne satellite imagers provide a synoptic view and accompanying
step-change capability in capturing properties of snow-covered areas,
although trade-offs exist between competing spatial, spectral and temporal
resolutions (Dozier, 1989; Nolin and Dozier, 1993; Hall et al., 2002, 2015;
Sirguey et al., 2009; Malenovský et al., 2012; Rittger et al., 2013; Roy
et al., 2014; Bessho et al., 2016). Passive and active microwave sensors
offer the capacity to retrieve estimates of snow water equivalent directly
from space-borne platforms but also suffer substantial limitations,
including coarse spatial resolution in the case of passive microwave
sensors and complexities in successfully processing snow signals and
accounting for complex terrain in the case of both passive and active
sensors (Lemmetyinen et al., 2018). Despite the progress in remotely mapping
snow, reliable determination of snow depth, particularly in complex terrain,
remains challenging. Modern, very high-resolution stereo-capable imagers
show promise for retrieving snow depth over large areas from space, although
the influence of topography on uncertainties and complications introduced
by shadows in alpine terrain demand attention (Marti et al., 2016).</p>
      <p id="d1e167">Advances in light detection and ranging (lidar) technologies have become
increasingly relevant for measurement of snow depth, firstly from air (Deems
et al., 2013; Painter et al., 2016) and more recently from space-borne
platforms (Treichler and Kääb, 2017). Of the three modes of lidar
data capture, terrestrial laser scanning (TLS) (e.g. Revuelto et al., 2016)
offers the best performance in terms of precision and accuracy. TLS can
resolve snow depth on a fine scale across relatively large areas but remains
limited by view-obstruction and logistical challenges of placing equipment in
situ in complex terrain. Airborne lidar provides a balance of spatial
resolution and accurate surface elevation measurement and, combined with
density estimates, can provide SWE estimates on the catchment scale across
substantial areas of hundreds of square kilometres (Painter et al., 2016).
High financial costs and logistical challenges, however, preclude regular
airborne lidar data capture in many regions globally. Treichler and
Kääb (2017) assessed ICESat lidar data, which is designed primarily
for measuring surface elevation over polar regions to characterise seasonal
snow depth in subpolar southern Norway. Despite reasonable estimates of snow
depth, measurements were accompanied by relatively large errors for most
temperate locations. ICESat measurements are also limited by their punctual
nature and footprint, yielding a relatively sparse and coarse spatial
distribution, in turn complicating inferences about spatial variability.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><caption><p id="d1e173">Location and hypsometry of the study catchment within the Pisa
Range, New Zealand.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018-f01.jpg"/>

      </fig>

      <p id="d1e182">Recent technological advances, including the miniaturisation of imaging and
positioning sensors, as well as improvements in battery power and autonomous
navigation have significantly lowered the barriers associated with a remotely
piloted aircraft system (RPAS, also known as unmanned aerial systems,
UAS, and unmanned aerial vehicles) operation (Watts et al., 2012).
This, combined with ever-increasing computing power and significant
improvements in machine-vision for dense photogrammetric reconstruction
(Hirschmuller, 2008; Lindeberg, 2015), provides new opportunities to map small
areas photogrammetrically at very high resolution in a temporally flexible,
on-demand, fashion. Examples of RPAS use related to mapping snow depth are
promising but tend to apply to sub-catchment scales and to not fully
characterise the uncertainty associated with photogrammetric modelling
(Vander Jagt et al., 2015; Bühler et al., 2016; De Michele et al., 2016;
Harder et al., 2016, Cimoli et al., 2017; Avanzi et al., 2018). Furthermore,
most RPAS studies of snow depth to date have mapped terrain of relatively low
complexity (e.g. Avanzi et al., 2018; Fernandes et al., 2018). Additionally,
with a few exceptions (e.g. Harder et al., 2016; Bühler et al., 2017;
Marti et al., 2016), previous studies have often relied on multirotor
platforms despite their relatively short endurance and reduced spatial
coverage relative to fixed-wing alternatives. Merit remains in characterising
fine-scale variability in snow depth distribution across an entire catchment,
a scale that fixed-wing RPAS can more easily capture. However, increased
terrain complexity and the magnitude of the image block can, in turn,
challenge photogrammetric modelling. Determination of snow depth via RPAS
photogrammetry relies first on the reconstruction of three-dimensional scenes
from a set of overlapping images and then on the principal of differencing
between temporally subsequent surfaces, provided by point clouds or digital
surface models (DSMs) (Vander Jagt et al., 2015; Harder et al., 2016). A
snow-free surface provides a reference data set for absolute snow depth, while
changes in snow distribution through winter can be assessed by<?pagebreak page3479?> comparing
surfaces obtained while snow cover is present in the catchment. Because
changes in snow depth through time, either through processes of accumulation,
ablation or redistribution, may be subtle, the repeatability and vertical
accuracy achieved by photogrammetric modelling is paramount. The aim of this
paper is to test a methodology for retrieving snow depth across an entire
catchment via RPAS photogrammetry from a fixed-wing platform. We seek to
evaluate the performance, limitations and usefulness of this approach and
assess how well snow depth can be resolved on the catchment scale. Associated
challenges include minimising spatial uncertainties sufficiently to reliably
detect changes in snow depth over time, with a decimetre level of vertical
accuracy targeted, while also reducing the need and complication of extensive
in situ collection of ground control points (GCPs). This approach was
assessed during a campaign of winter RPAS-based photogrammetric surveys of an
alpine catchment in the Pisa Range, New Zealand, was undertaken.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p id="d1e188">Timing details for RPAS flights during 2016. All flights were
completed between noon and early afternoon.</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="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:colspec colnum="5" colname="col5" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Mission/flight</oasis:entry>
         <oasis:entry colname="col2">Date</oasis:entry>
         <oasis:entry colname="col3">Season</oasis:entry>
         <oasis:entry colname="col4">Snow cover</oasis:entry>
         <oasis:entry colname="col5">Sky conditions</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">M001f01</oasis:entry>
         <oasis:entry colname="col2">17 May 2016</oasis:entry>
         <oasis:entry colname="col3">Autumn</oasis:entry>
         <oasis:entry colname="col4">Minimal – remaining traces of early snowfall</oasis:entry>
         <oasis:entry colname="col5">Clear sky, light winds</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">M002f01</oasis:entry>
         <oasis:entry colname="col2">2 Aug 2016</oasis:entry>
         <oasis:entry colname="col3">Midwinter</oasis:entry>
         <oasis:entry colname="col4">Extensive – winter snowpack, high surface roughness</oasis:entry>
         <oasis:entry colname="col5">Thin high cloud, light winds</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">M003f01</oasis:entry>
         <oasis:entry colname="col2">10 Sep 2016</oasis:entry>
         <oasis:entry colname="col3">Spring</oasis:entry>
         <oasis:entry colname="col4">Spring melt underway, extensive snow-free areas.</oasis:entry>
         <oasis:entry colname="col5">Clear sky, light winds</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">Reduced snow surface roughness</oasis:entry>
         <oasis:entry colname="col5"/>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e299">The paper describes the field site, field and photogrammetric methods, as
well as the quality and accuracy assessment. Results are considered in terms
of the validation and repeatability of the method, as well as considering
the spatial distribution of snow within the catchment. The discussion
addresses the performance of RPAS photogrammetry in this context, sources
and nature of the associated uncertainty as well as pitfalls and limitations
that were encountered, before demonstrating the insight that RPAS-derived
data can provide for the study of seasonal snow. While primarily exploring
and assessing the potential of RPAS photogrammetry for measuring seasonal
snowpack, this study has broader implications for the wider field of modern
close-range photogrammetry, as typically implemented from low-cost (relative
to manned systems) unmanned systems. While considered here in terms of
seasonal snow, the characterisation of RPAS photogrammetry performance
presented also applies to other applications involving three-dimensional
surface and/or volume change analysis.</p>
</sec>
<sec id="Ch1.S2">
  <title>Study site</title>
      <p id="d1e308">The study catchment (Fig. 1), a tributary of the Leopold Burn located in the
Pisa Range of the Southern Alps/Kā Tiritiri-o-te-Moana of New Zealand
(44.882<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 169.081<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E), is 0.41 km<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> in size and has
been the subject of prior snow-hydrology investigations (Sims and Orwin,
2011). Elevation of the catchment ranges between 1440 and 1580 m a.s.l.
with a near-uniform area-elevation distribution (Fig. 1). The average slope is
moderate, with 80 % of the catchment having a surface slope of
24<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> or less. The catchment runs north to south and is drained by a
small stream. While east of the Main Divide of the Southern Alps, the Pisa
Range is representative of several large fault-block mountain ranges that
dominate the eastern portion of the Clutha Catchment within the Otago region.
These ranges are bounded by moderately steep slopes, rising to broad
continuous ridge and plateau systems, in turn dissected by relatively<?pagebreak page3480?> shallow
gullies, basins and gorges. These ranges feature relatively large areas above
the winter snowline, with complex micro-terrain features, which are of
interest in the context of redistribution, preferential accumulation and
ablation of seasonal snow. In combination with typically windy conditions,
the topography is expected to produce complex, highly variable spatial
distributions of seasonal snow, convolved with and potentially overtaking
the role of elevation in influencing variability in snow depth. The catchment
mapped in this study is larger than areas mapped for similar studies
published to date (Vander Jagt et al., 2015; Bühler et al., 2016; De
Michele et al., 2016; Harder et al., 2016) and has a relatively complex
topography, with several gullies dissecting the main slopes, separated by
broad, steep-sided ridges. Visual assessment of Landsat, Sentinel-2, and
MODIS imagery revealed that, while the catchment could be considered to be in
the marginal snow zone, snow cover persists from June to late September in most
years, thus providing opportunities for repeated mapping and the capture of
the snowpack in various states.</p>
</sec>
<sec id="Ch1.S3">
  <title>Data and methods</title>
<sec id="Ch1.S3.SS1">
  <title>Field approach</title>
<sec id="Ch1.S3.SS1.SSS1">
  <title>RPAS platform and payload</title>
      <p id="d1e363">We used the Trimble UX5 Unmanned Aircraft System, a fixed-wing RPAS
manufactured by Trimble Navigation for photogrammetric applications. A single
two-blade propeller, driven by a 700 W electric motor, propels the platform.
Power is supplied from a 14.8 V, 6000 mAh lithium-polymer battery allowing
a flight endurance of 50 min. Autonomous navigation is supported by a single-channel GPS receiver, which also provides approximate coordinates for each
photo centre, while an accelerometer logs orientation data.</p>
      <p id="d1e366">Imagery is captured by a large-sensor (APS-C) Sony NEX 5R mirrorless reflex
digital camera providing a maximum imaging resolution of 4912 pixels by
3264 pixels or about 0.04 m GSD at 400 ft (122 m) a.g.l. The camera is
fitted with a Voigtlander Super Wide-Heliar 15 mm <inline-formula><mml:math id="M9" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula>/4.5 Aspherical II
lens, with focus fixed to infinity. Appropriate exposure to ensure suitable
contrast on the range of imaged targets was achieved with maximum aperture,
high shutter speeds between <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1000</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">4000</mml:mn></mml:mrow></mml:math></inline-formula> s to minimize forward-motion
blurring and automatic ISO sensitivity. Camera settings were checked prior
to each flight to accommodate varying light conditions and the relative share
of ground cover (vegetation vs. snow).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p id="d1e402">Typical flight path for the mapping of the study catchment using the
Trimble UX5, GCP network established for each flight mission, and reference
snow depth locations. Flight log is from the spring flight mission. The
configuration of the ground control point (GCP) and check point (CP)
assignment for the triangulation of each flight is shown in the panels on the
right-hand side.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018-f02.png"/>

          </fig>

</sec>
<sec id="Ch1.S3.SS1.SSS2">
  <title>RPAS flights</title>
      <p id="d1e417">Three RPAS missions were undertaken with identical planning and differing
states of snow cover in the catchment (Table 1). Flight planning was carried
out using the Trimble Aerial Imaging software. All flights imaged 15 strips,
aligned along the major axis of the study catchment (Fig. 2). The study area
was imaged with 90/80 % forward/sideward overlap with respect to the
lowest elevation to ensure that sufficient overlap was maintained when
mapping rising ground. Exposure locations are determined automatically by the
software to achieve the desired overlap, with the camera being triggered
accordingly during flight using on-board Global Navigation Satellite System (GNSS) navigation. The duration of
each flight was <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">35</mml:mn></mml:mrow></mml:math></inline-formula> min, with about 900 images being captured per
flight. The average flying altitude of the flights was 1650 m a.s.l., with a
standard deviation of less than 1.5 m during the mapping phase of the flight.
For both the winter and spring flights, the snow surface had considerable
texture, with a greater surface roughness overall for winter missions.
Wind-affected recent fresh snow was present for the winter flight. It is
recognised that homogeneous snow surfaces may represent particularly
challenging targets for photogrammetry (Bühler et al., 2017).
Nevertheless, the imaging quality and dynamic range of the camera used in
this study provided sufficient contrast for all flights, across snow as well
as when imaging mixed snow-bare ground conditions. Subsequently, full
photogrammetric restitution could be completed without the need for image
post-processing (e.g. Cimoli et al., 2017).</p>
</sec>
<sec id="Ch1.S3.SS1.SSS3">
  <title>Ground control survey</title>
      <p id="d1e436">Achieving a robust constraint of exterior orientation parameters during
aero-triangulation (AT) depends on the availability of a set of high-quality
ground control points (GCPs). This is particularly true if the imaging
platform lacks a precise-point-positioning capability (e.g. it carries
only single-frequency GPS and is not capable of determining differentially
corrected positions). Such code-only GPS navigation is accompanied by
uncertainties 2 orders of magnitude<?pagebreak page3481?> greater than the expected accuracy of
the models. Ground control networks were established for each RPAS flight
mission using real-time kinematic (RTK)
GNSS surveying with a Trimble R7 base station and R6 rover units. GCP
locations were measured with accuracy of the order of <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.02</mml:mn></mml:mrow></mml:math></inline-formula>–0.03 m.
GCPs were signalled with <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> m mats painted with a high-contrast
circular quadrant pattern for the autumn and winter flights. For the spring
flight, chalk powder was used with a stencil to mark the target directly on
the snow surface, using the same pattern as for previous flights. The use of
chalk powder eliminated the need to retrieve GCP targets following RPAS
flights. All survey work, as well as production of deliverables from
photogrammetry, was carried out in terms of the New Zealand Transverse
Mercator (NZTM) reference system. All RTK survey work utilised a base station
established on a common benchmark, established for this project, the position
of which was differentially corrected with respect to nearby continually
operating reference stations. GNSS data were processed using Trimble
Business Center (TBC) v3.40 software.</p>
      <p id="d1e461">It is well established that photogrammetric control is best achieved within
the bounds of the GCP network (Linder, 2016), while the uncertainty
associated with the geolocation of resected points increases beyond the
control network. To constrain the area within the study catchment for
photogrammetric processing, the GCP network was distributed around the
catchment perimeter, as well as through the central area of the catchment.
Additionally, the placement of GCPs on the valley floor and at mid-elevation
within the catchment ensured that the network also sampled the elevation
range of the catchment. An extensive GCP network was established for the
first flight with no snow on the ground, which permitted the robustness of AT
to be tested under different GCP scenarios, as discussed further in
Sect. 3.2.1. This allowed the network to be refined and reduced in size for
subsequent missions, a matter of practical importance when working in alpine
areas during the winter. Control point networks for<?pagebreak page3482?> each mission are
illustrated in Fig. 2. A new GCP network was established for each survey
campaign due to the inability to establish permanent markers (e.g. on poles)
due to the conservation status of the study area. Although the layout of the
network was similar for each mission, there were no common GCPs shared
between different flights, with the only common setting being the set-up of
the base station for each RTK survey.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS4">
  <title>Reference snow depth measurements</title>
      <p id="d1e470">To assess the quality of snow depth data derived from RPAS photogrammetry,
independent measurements were collected by manual snow probing on
10 September 2016, the same day as the spring RPAS mission. This approach has
been established as standard practice in similar studies (e.g. Nolan et al.,
2015; De Michele et al., 2016). Aluminium avalanche probes with 0.01 m
graduations, providing a nominal precision of 0.01 m, were used. The
sampling strategy involved the measurement of snow depth every 50 m along
three elevation contours within the study catchment, namely 1460, 1500 and
1540 m (Fig. 2). This strategy ensured that snow depth was measured across a
representative sample of slope aspect and elevation, while optimizing
navigation across the catchment. Snow depths were measured at each location
by probing 5 times within arm's reach, and the location of the central
measurement was surveyed with RTK GNSS, under the same protocol and achieving the
same level of accuracy as the GCP survey. This provided 430 measurements of
snow depth, with the mean snow depth at each of the 86 locations providing a
sample for comparisons with RPAS-derived snow depth.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Data processing</title>
<sec id="Ch1.S3.SS2.SSS1">
  <title>Photogrammetric processing</title>
      <p id="d1e485">The goal of aero-triangulation (AT) in photogrammetry is to transform a set
of images into a scene in which geometrically accurate measurements can be
made in three-dimensional, often geographic, space. This georeferencing
process requires a transformation from the inherent coordinate system of the
device capturing imagery (a camera) to an appropriate geographic coordinate
system (Vander Jagt et al., 2015; Linder, 2016). While traditional
photogrammetry has long relied on metric (calibrated) cameras, the use of
off-the-shelf non-metric cameras requires the simultaneous solving of both
interior orientation (the camera model) and exterior orientation. This
process, known as self-calibration, applies a bundle-block adjustment to
solve the camera model describing the precise focal length (<inline-formula><mml:math id="M15" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula>), the offset
between the principal point of autocollimation and the centre of the
imaging sensor plane (<inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), and the departure between the image
point coordinate (<inline-formula><mml:math id="M18" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M19" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula>) and the idealized linear projection due to lens
distortion. Camera calibration parameterises radial and decentering
distortion with models such as that of Brown (1971):

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M20" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E1"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mover accent="true"><mml:mrow><mml:msup><mml:mi>x</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mfenced open="(" close=")"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:msub><mml:mi>K</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msub><mml:mi>K</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">5</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msub><mml:mi>K</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">7</mml:mn></mml:msup></mml:mrow></mml:mfenced><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi>T</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mover accent="true"><mml:mrow><mml:mi>x</mml:mi><mml:mi>y</mml:mi></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>+</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msup><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mtr><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mover accent="true"><mml:mrow><mml:msup><mml:mi>y</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mfenced open="(" close=")"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:msub><mml:mi>K</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msub><mml:mi>K</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">5</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msub><mml:mi>K</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">7</mml:mn></mml:msup></mml:mrow></mml:mfenced><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi>T</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi>x</mml:mi><mml:mi>y</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msup><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>

              in which <inline-formula><mml:math id="M21" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> terms are the radial distortion coefficients, <inline-formula><mml:math id="M22" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> terms are the
tangential distortion coefficients, and

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M23" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E2"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E3"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mi>y</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E4"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:msup><mml:mover accent="true"><mml:mi>x</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mi>y</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              Image coordinates corrected for lens distortion are then used in the set of
collinearity equations relating object point coordinates (<inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi>A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>)
to the corresponding image point coordinates (<inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mrow><mml:msup><mml:mi>x</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi>A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>,
<inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mrow><mml:msup><mml:mi>y</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi>A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) to solve for the exterior orientation (Vander Jagt et
al., 2015; Linder, 2016):

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M29" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E5"><mml:mtd/><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mfenced close=")" open="("><mml:mtable class="array" columnalign="left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mover accent="true"><mml:mrow><mml:msup><mml:mi>x</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi>A</mml:mi></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mover accent="true"><mml:mrow><mml:msup><mml:mi>y</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi>A</mml:mi></mml:msub></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><mml:mo>=</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mtr><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mfenced open="(" close=")"><mml:mtable rowspacing="5.690551pt" class="array" columnalign="left"><mml:mtr><mml:mtd><mml:mrow><mml:mi>f</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mn mathvariant="normal">11</mml:mn></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mn mathvariant="normal">12</mml:mn></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mn mathvariant="normal">13</mml:mn></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mn mathvariant="normal">31</mml:mn></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mn mathvariant="normal">32</mml:mn></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mn mathvariant="normal">33</mml:mn></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mi>f</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mn mathvariant="normal">21</mml:mn></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mn mathvariant="normal">22</mml:mn></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mn mathvariant="normal">23</mml:mn></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mn mathvariant="normal">31</mml:mn></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mn mathvariant="normal">32</mml:mn></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mn mathvariant="normal">33</mml:mn></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>

              (<inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) are the coordinates of the perspective centre of the
image frame in the ground coordinate system. The <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> terms represent the
<inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mn mathvariant="normal">3</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> rotation matrix relating the sensor coordinate system
orientation to the ground coordinate system. Since the UX5 camera is fixed
with respect to the platform, the latter combines the roll, pitch and yaw
(<inline-formula><mml:math id="M35" display="inline"><mml:mi mathvariant="italic">ω</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M36" display="inline"><mml:mi mathvariant="italic">φ</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M37" display="inline"><mml:mi mathvariant="italic">κ</mml:mi></mml:math></inline-formula>) of the platform at the time of exposure.
The nature of bundle-block adjustment with camera self-calibration dictates
that the quality of the final photogrammetric model is highly sensitive to
errors in both sensor position and orientation as well as inaccurate
refinements of the interior orientation parameters (Ebner and Fritz,
1980).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><caption><p id="d1e1318">Summary results of alternative ground control point (GCP) and check
point (CP) scenarios tested for aero-triangulation within UAS Master.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="9">
     <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" colsep="1"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry rowsep="1" namest="col2" nameend="col5" align="center" colsep="1">GCP RMSE (m) </oasis:entry>
         <oasis:entry rowsep="1" namest="col6" nameend="col9" align="center">CP RMSE (m) </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Scenario</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M38" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M39" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M40" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M41" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M42" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M43" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8"><inline-formula><mml:math id="M44" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col9"><inline-formula><mml:math id="M45" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">1</oasis:entry>
         <oasis:entry colname="col2">23</oasis:entry>
         <oasis:entry colname="col3">0.0069</oasis:entry>
         <oasis:entry colname="col4">0.0076</oasis:entry>
         <oasis:entry colname="col5">0.0055</oasis:entry>
         <oasis:entry colname="col6">0</oasis:entry>
         <oasis:entry colname="col7">N/A</oasis:entry>
         <oasis:entry colname="col8">N/A</oasis:entry>
         <oasis:entry colname="col9">N/A</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">2</oasis:entry>
         <oasis:entry colname="col2">14</oasis:entry>
         <oasis:entry colname="col3">0.0017</oasis:entry>
         <oasis:entry colname="col4">0.0010</oasis:entry>
         <oasis:entry colname="col5">0.0004</oasis:entry>
         <oasis:entry colname="col6">9</oasis:entry>
         <oasis:entry colname="col7">0.0119</oasis:entry>
         <oasis:entry colname="col8">0.0184</oasis:entry>
         <oasis:entry colname="col9">0.0320</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">3</oasis:entry>
         <oasis:entry colname="col2">6</oasis:entry>
         <oasis:entry colname="col3">0.0033</oasis:entry>
         <oasis:entry colname="col4">0.0039</oasis:entry>
         <oasis:entry colname="col5">0.0009</oasis:entry>
         <oasis:entry colname="col6">17</oasis:entry>
         <oasis:entry colname="col7">0.0263</oasis:entry>
         <oasis:entry colname="col8">0.0207</oasis:entry>
         <oasis:entry colname="col9">0.0575</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <title>Software and workflow</title>
      <p id="d1e1533">Initially, AT was carried out using the photogrammetry module of
Trimble Business Center, v3.40 (TBC), which relies on a simplified
implementation of the adjustment process from Inpho UAS Master. Deliverables
produced using TBC, however, suffered from severe elevation artefacts which
limited their usefulness for further analysis. This is discussed further in
Sect. 5.3.</p>
      <p id="d1e1536">Following the identification of shortfalls in TBC, AT was carried out using
Trimble Inpho UAS Master<sup>®</sup> v8.0 (UAS Master). UAS Master is a
feature-rich photogrammetry package that is targeted to RPAS applications
(Trimble, 2015, 2016) and is a comprehensive alternative to
software often used in similar studies such as Pix4D or Agisoft<?pagebreak page3483?> Photoscan.
The AT solution is initialised by the positional parameters (<inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)
for each photo centre, as provided by the on-board GPS receiver. Relative
adjustment is achieved after automatic tie point (TP) collection. TPs are
common targets recognised in multiple overlapping images, which allow the
relative position and orientation of images within the block to be
determined. Subsequent measurement of GCP positions in images enables
absolute adjustment. GCPs may be collected manually or automatically via
feature recognition. In this case, targets marking GCPs were identified and
selected manually. The absolute bundle-block adjustment then concurrently
refines the exterior and interior orientation
parameters.</p>
      <p id="d1e1575">The robustness of photogrammetric modelling was assessed by testing several
alternate control scenarios, based on the autumn mission when 23 GCPs were
placed and measured in the field. The following scenarios were evaluated:
<list list-type="order"><list-item>
      <p id="d1e1580">all 23 control points as horizontal and vertical GCPs,</p></list-item><list-item>
      <p id="d1e1584">14 control points as horizontal and vertical GCPs,</p></list-item><list-item>
      <p id="d1e1588">6 control points as horizontal and vertical GCPs.</p></list-item></list></p>
      <p id="d1e1591">In each scenario, the balance of the control points was provided as check
points (CPs). In retaining GCPs, we ensured that the perimeter of the study
catchment remained fully constrained within the network. As the number of
GCPs decreased, the root mean square error (RMSE) for CPs provided an
indication of AT robustness. It was found that as few as 14 GCPs provided an
acceptable triangulation across the study area, with some degradation
apparent when only six GCPs were used, primarily in terms of <inline-formula><mml:math id="M49" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula> (Table 2). No
spatial structure was evident in the distribution of GCP or CP error. This
assessment aided the determination of an optimal number of GCPs to minimise
the time required to place and survey control points when snow is present in
the catchment. On this basis, 14 control points were placed and measured in
the field for each of the winter and spring missions. For all missions, the
AT from which deliverables were produced utilised all surveyed points as
GCPs. A second AT was carried out using a subset of control points as CPs, as
shown in Table 3. Thus, the RMSE provided by CPs is expected to be
conservative compared to the quality of the deliverables obtained from the
fully constrained AT.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS3">
  <title>Intermediate deliverables</title>
      <p id="d1e1607">Standard deliverables from the photogrammetric modelling included a dense
point cloud; a digital surface model, interpolated to 0.15 m spatial
resolution; and an ortho-mosaic, resampled to 0.05 m spatial resolution. The
DSM and the ortho-mosaic are the principal products
for further analysis. Each DSM provides the basis for determining snow
depth, while the ortho-mosaics allow for assessment of the snow-covered
area, and for snow-free areas to be identified when assessing the quality
and repeatability of DSMs between flight missions.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><caption><p id="d1e1613">Summary statistics for each of the triangulations used to produce
DSMs and ortho-mosaics from each of the three flight missions for ground
control points (GCPs) and check points (CPs).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="12">
     <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:colspec colnum="8" colname="col8" align="right" colsep="1"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:colspec colnum="10" colname="col10" align="right"/>
     <oasis:colspec colnum="11" colname="col11" align="right"/>
     <oasis:colspec colnum="12" colname="col12" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Flight</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M50" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> images</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M51" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> images</oasis:entry>
         <oasis:entry colname="col4"/>
         <oasis:entry rowsep="1" namest="col5" nameend="col8" align="center">GCP RMSE (m) </oasis:entry>
         <oasis:entry rowsep="1" namest="col9" nameend="col12" align="center">CP RMSE (m) </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">captured</oasis:entry>
         <oasis:entry colname="col3">used</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M52" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> TP</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M53" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M54" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M55" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8"><inline-formula><mml:math id="M56" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col9"><inline-formula><mml:math id="M57" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col10"><inline-formula><mml:math id="M58" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col11"><inline-formula><mml:math id="M59" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col12"><inline-formula><mml:math id="M60" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">1</oasis:entry>
         <oasis:entry colname="col2">885</oasis:entry>
         <oasis:entry colname="col3">885</oasis:entry>
         <oasis:entry colname="col4">100 390</oasis:entry>
         <oasis:entry colname="col5">14</oasis:entry>
         <oasis:entry colname="col6">0.0083</oasis:entry>
         <oasis:entry colname="col7">0.0073</oasis:entry>
         <oasis:entry colname="col8">0.0034</oasis:entry>
         <oasis:entry colname="col9">9</oasis:entry>
         <oasis:entry colname="col10">0.0134</oasis:entry>
         <oasis:entry colname="col11">0.0163</oasis:entry>
         <oasis:entry colname="col12">0.0220</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">2</oasis:entry>
         <oasis:entry colname="col2">920</oasis:entry>
         <oasis:entry colname="col3">917</oasis:entry>
         <oasis:entry colname="col4">98 730</oasis:entry>
         <oasis:entry colname="col5">8</oasis:entry>
         <oasis:entry colname="col6">0.0067</oasis:entry>
         <oasis:entry colname="col7">0.0085</oasis:entry>
         <oasis:entry colname="col8">0.0018</oasis:entry>
         <oasis:entry colname="col9">6</oasis:entry>
         <oasis:entry colname="col10">0.0368</oasis:entry>
         <oasis:entry colname="col11">0.0293</oasis:entry>
         <oasis:entry colname="col12">0.0409</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">3</oasis:entry>
         <oasis:entry colname="col2">891</oasis:entry>
         <oasis:entry colname="col3">889</oasis:entry>
         <oasis:entry colname="col4">88 791</oasis:entry>
         <oasis:entry colname="col5">8</oasis:entry>
         <oasis:entry colname="col6">0.0105</oasis:entry>
         <oasis:entry colname="col7">0.0108</oasis:entry>
         <oasis:entry colname="col8">0.0028</oasis:entry>
         <oasis:entry colname="col9">6</oasis:entry>
         <oasis:entry colname="col10">0.0246</oasis:entry>
         <oasis:entry colname="col11">0.0247</oasis:entry>
         <oasis:entry colname="col12">0.0457</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S3.SS2.SSS4">
  <title>Derivation of snow depth</title>
      <p id="d1e1901">Snow depth was derived by differencing DSM of flights 2 and 3 from the
baseline obtained during flight 1 (ref) as follows:
              <disp-formula id="Ch1.E6" content-type="numbered"><mml:math id="M61" display="block"><mml:mrow><mml:msub><mml:mtext>dDSM</mml:mtext><mml:mi>n</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mtext>DSM</mml:mtext><mml:mi>n</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mtext>DSM</mml:mtext><mml:mtext>ref</mml:mtext></mml:msub><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            Equation (6) provides a map of difference between the two DSMs, henceforth
referred to as the dDSM (after Nolan et al., 2015). Values of the dDSM are
considered to represent snow depth, with the associated uncertainty considered
in Sect. 3.3.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS3">
  <title>Quality and accuracy assessment</title>
      <p id="d1e1938">Summary statistics, typically based on the rms error of GCPs and CPs from
the AT, indicate the expected accuracy of deliverables. Since snow depth is
determined by differencing two DSMs, error propagation can provide an
assessment of uncertainty associated with the dDSM. The overall accuracy of
the DSM differencing approach should also be validated against independent
reference data (e.g. snow depth measured in situ), temporally coincident with RPAS
measurements. Areas of snow-free terrain during Flight 3 further supplement
snow depth observations by providing an extensive source of samples with which to
assess the repeatability of the photogrammetric modelling process.</p>
      <p id="d1e1941">Previous studies have considered the accuracy of RPAS-derived snow depth by
comparison with reference data from in situ snow depth alone (Bühler et al.,
2016; De Michele et al., 2016; Harder et al., 2016) while ignoring the
uncertainty<?pagebreak page3484?> inherent to each photogrammetric model and their propagation
into the dDSM. Here, the accuracy of photogrammetrically derived snow depth
is assessed by exploring both approaches. Relating photogrammetric model
quality, as inferred from GCPs and CPs, to observed uncertainties in the
determination of snow depth provides the basis for realistically informing
uncertainties in snow depth from ongoing RPAS measurements. This in turn
allows rigorous inferences about the evolution of snow depth to be made,
without the need for further campaigns of in situ validation. While high-resolution
reference elevation data, such as lidar-derived elevation or surface models
would provide a useful benchmark for assessing RPAS DSM quality, no such
data were available for the study area.</p>
<sec id="Ch1.S3.SS3.SSS1">
  <title>Uncertainty associated with RPAS-derived snow depth</title>
      <p id="d1e1949">Since snow depth is determined via DSM differencing as a linear combination
of two independently measured variables (Eq. 6), the uncertainty
associated with snow depth (SD), measured in the vertical dimension, for
each measurement date (<inline-formula><mml:math id="M62" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>) can be obtained via Gaussian error propagation
(James et al., 2012) as follows:
              <disp-formula id="Ch1.E7" content-type="numbered"><mml:math id="M63" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mtext>dDSM</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">ε</mml:mi><mml:mi>n</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">ε</mml:mi><mml:mtext>ref</mml:mtext><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:msqrt><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M64" display="inline"><mml:mi mathvariant="italic">ε</mml:mi></mml:math></inline-formula> for each DSM is the elevation error determined from the
AT as the RMSE<inline-formula><mml:math id="M65" display="inline"><mml:msub><mml:mi/><mml:mi>Z</mml:mi></mml:msub></mml:math></inline-formula> value for the set of CPs. Inherent in this simple
approach is the assumption that the planimetric accuracy of each constituent
DSM has negligible contribution to <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mtext>dDSM</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>. Calculating
<inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mtext>dDSM</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> provides a single estimate of uncertainty assumed to
apply equally throughout the map of RPAS-derived snow depth for each date.
Under the assumption that errors are normally distributed and bias-free, the
RMSE<inline-formula><mml:math id="M68" display="inline"><mml:msub><mml:mi/><mml:mi>z</mml:mi></mml:msub></mml:math></inline-formula> derived from CPs identifies the standard deviation <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>z</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>,
allowing the 90 % confidence level of <inline-formula><mml:math id="M70" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula> to be determined as <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.65</mml:mn><mml:mo>×</mml:mo><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>Z</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. In turn, inferences associated with uncertainties for
elevation differences, <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mtext>dDSM</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, also depend on the
Gaussian assumption to provide the 90 % confidence level.</p>
      <p id="d1e2084">In reality, perfect co-registration between constituent DSMs and the
Gaussian assumption are unwarranted. Subsequently, inferences associated
with the evolution of snow depth may be compromised due to confidence
intervals being conservative or immoderate. Therefore, we use dDSM for
snow-free areas to characterise the experimental distribution of errors and
assess the validity of the Gaussian assumption in this context.</p>
</sec>
<sec id="Ch1.S3.SS3.SSS2">
  <title>Validation against reference snow depth measurements</title>
      <p id="d1e2093">The approach above provides a means to determine the expected accuracy of
snow depth derived from RPAS photogrammetric surveys. In order to validate
this estimate, a reference data set of in situ observations was sampled in the
field using snow probes, with a nominal precision of <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula> m, as
described in Sect. 3.1.4. De Michele et al. (2016) assessed the accuracy of
RPAS-derived snow depths against snow depth surfaces interpolated from 12
point measurements. This approach, however, may be limited by an inability to
accurately resolve the spatial variability of snow depth, as well as the
compounding effects of uncertainty associated with the interpolation scheme,
particularly beyond the domain defined by the measured points.</p>
      <p id="d1e2106">Here, 430 measurements of snow depth provided 86 mean reference values, with
the standard deviation of each set of five measurements providing 95 %
confidence intervals. The aim of this sampling strategy was to assess and
account for co-location uncertainty and spatial variability between the RPAS
and reference snow depth data sets. Reference snow depths were compared with
those from the spatially coincident pixels from the map of RPAS-derived snow
depth. RPAS-derived snow depth quality was assessed in terms of residuals and
weighted linear regression between reference and RPAS-derived snow depths.</p>
</sec>
<sec id="Ch1.S3.SS3.SSS3">
  <title>Repeatability of photogrammetric modelling</title>
      <p id="d1e2116">Emergence of snow-free areas at the time of the spring flight facilitated
comparison between autumn and spring DSMs on those areas. As the same
terrain surface mapped from two independent flights should yield identical
DSMs, the residual between them provides a means to characterise the
distribution of errors in the photogrammetric processing, which can be
readily compared to the assessment made from CPs.</p>
      <p id="d1e2119">Snow-covered and snow-free areas were segmented using an unsupervised
classification of the spring ortho-image using the Iso Cluster classification tool in
ArcGIS v10.3. With five output classes, this approach enabled<?pagebreak page3485?> discrimination
between illuminated snow pixels, shaded snow pixels, and vegetation and soil-dominated snow-free pixels. Snow-free pixel classes were then grouped to
provide a mask within which the distribution of spring dDSM values could be
characterized. While this approach relies on the characterisation of
repeatability for snow areas, good image contrast and the high overall
density of TPs generated across the image block, regardless of the presence
or absence of snow, indicates that photogrammetric reconstruction
performance should be comparable for both snow-free and snow-covered areas.
This is a product of the camera properties, which maintain high dynamic
range across scenes of mixed land cover and extensive snow cover. Therefore,
this residual represents a measure of the repeatability of the technique for
measuring surface height change, including derivation of snow depth.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p id="d1e2124">Processed ortho-mosaics for autumn <bold>(a)</bold>, winter <bold>(b)</bold>
and spring <bold>(c)</bold> flights, with corresponding autumn hill-shaded
DSM <bold>(d)</bold> and maps of snow depth derived for winter <bold>(e)</bold> and
spring <bold>(f)</bold>.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018-f03.jpg"/>

          </fig>

</sec>
<sec id="Ch1.S3.SS3.SSS4">
  <title>Resolution of fine-scale spatial variability</title>
      <p id="d1e2158">A primary motivation for exploring the use of RPAS photogrammetry for mapping
a snowpack is the ability to resolve fine-scale spatial variability in snow
depth. This capability was assessed by computing and comparing the
semi-variograms of reference and RPAS-derived snow depths from the autumn
flight. While the sample size for reference snow depths remained fixed
(<inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">86</mml:mn></mml:mrow></mml:math></inline-formula>), the semi-variogram of RPAS-derived snow depths could be calculated
from many more samples. Two random samples were extracted from the spring
dDSM map (<inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1000</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5000</mml:mn></mml:mrow></mml:math></inline-formula>), each yielding a semi-variogram
capturing the spatial variability of snow depth with increasing detail, which
were compared to that of the in situ observations.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S4">
  <title>Results</title>
<sec id="Ch1.S4.SS1">
  <title>Photogrammetric processing</title>
<sec id="Ch1.S4.SS1.SSS1">
  <title>Quality of the triangulation</title>
      <p id="d1e2215">Since GCPs are used to solve the photogrammetric model, they do not provide
an independent assessment of accuracy. Such an assessment is provided by the
CPs, the RMSE of which was of the order of centimetres for all flights
(Table 3). Planimetric RMSE (i.e. <inline-formula><mml:math id="M77" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M78" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula>) was always substantially less
than the GSD. Vertical RMSE (<inline-formula><mml:math id="M79" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula>) tended to be about double that achieved
planimetrically but never exceeded 0.05 m. The final models were produced
from a second and more constrained AT with all surveyed points used as GCPs,
thus making the assessment conservative relative to the final products.</p>
      <p id="d1e2239">While the RMSE of CPs increased for the winter and spring flights, possibly
due to a less constrained model, the level of accuracy achieved is compatible
with expectations for the determination of snow depth. Additionally, the more
tightly constrained first AT reduced the error for the baseline model, in
turn contributing a reduced uncertainty in derived snow depths, despite the
reduced control for subsequent ATs. For all flight missions, the
photogrammetric processing performed well in the correlation of images and
the construction of the image block, as indicated in Table 3. Tie point (TP)
generation relies on the successful match of unique targets across multiple
images, which was achieved despite the complicated contrast over snow. For
all flights <inline-formula><mml:math id="M80" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 80 000, TPs were generated across the imaged area.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p id="d1e2251">Residuals between snow depths measured by RPAS photogrammetry and
probing for all probe locations (“all”, blue) and non-tussock probe
locations (“n-t”, red) <bold>(a)</bold>, and bi-square (bisq.) weighted
regression between snow depth derived from a 0.15 m RPAS grid and probed
snow depths <bold>(b)</bold>. Vertical error bars are determined from the error
propagation associated with DSM differencing and have a magnitude of <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.094</mml:mn></mml:mrow></mml:math></inline-formula> m, while horizontal error bars are calculated from the standard
deviation of probe measurements made at each reference sampling location.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018-f04.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p id="d1e2279">Map <bold>(a)</bold> and histogram <bold>(b)</bold> of the vertical residual
for snow-free areas for surface models derived from the autumn and spring
flights. The histogram includes fitted normal and <inline-formula><mml:math id="M82" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> location-scale (<inline-formula><mml:math id="M83" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>)
distributions.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018-f05.png"/>

          </fig>

</sec>
<sec id="Ch1.S4.SS1.SSS2">
  <title>Determination of snow depth</title>
      <p id="d1e2314">Snow depth was found to be highly variable across the study catchment for
both winter and spring (Fig. 3). The midwinter flight mapped near-complete
snow cover across the study catchment, while large snow-free areas developed
by the spring flight, where snow-covered area was reduced by about one-third
(Fig. 3a and b). Where snow was present, depths ranged from less than
0.10 m, typically on exposed ridgelines and broad elevated slopes, to 2 m
or more where cornices formed along ridgelines, as well as in gullies.
Average snow depth was greater for winter, although maximum depths were
comparable between winter and spring. Between winter and spring, considerable
ablation was observed. Areas of deepest snow were spatially coincident
between winter and spring, with the greatest retention of snow in cornices
and gullies. Where shallow snow was present on ridgelines in winter, it was
largely lost by spring.</p>
</sec>
</sec>
<sec id="Ch1.S4.SS2">
  <title>Accuracy assessment and validation of snow depth</title>
<sec id="Ch1.S4.SS2.SSS1">
  <title>Propagation of aero-triangulation error</title>
      <p id="d1e2329">Propagation of errors under the Gaussian assumption, based on the RMSE from
each AT, yielded vertical uncertainties for snow depths at the 90 %
confidence level of <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.077</mml:mn></mml:mrow></mml:math></inline-formula> m for the winter flight and <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.084</mml:mn></mml:mrow></mml:math></inline-formula> m
for the spring flight. This one-dimensional approach to error propagation
assumes that the planimetric geolocation of individual surfaces, and
subsequently the co-registration of surface pairs, does not contribute
significantly to the vertical uncertainty.</p>
</sec>
<sec id="Ch1.S4.SS2.SSS2">
  <title>Assessment against reference probe data</title>
      <p id="d1e2358">Comparison of RPAS-derived and reference snow depth yielded a mean residual
of <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.069</mml:mn></mml:mrow></mml:math></inline-formula> m, indicating that, on average, reference depths were greater
than RPAS-derived depths. Filtering the reference data set to exclude
reference measurements that were made in areas occupied by tussock
(<italic>Chionochloa rigida</italic>) vegetation, however, improved the mean residual
to <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula> m (Fig. 4a). The small residual is indicative of good agreement
between the two data sets while also indicating that, overall, snow depths
measured by probing may be overestimated. Limitations of probing and
uncertainty introduced due to the presence of vegetation is discussed further
in Sect. 5.2.1.</p>
      <?pagebreak page3486?><p id="d1e2384">Good agreement between data sets is further demonstrated in Fig. 4b.
Relatively large horizontal error bars accompanying the reference
measurements (Fig. 4b) reflect the substantial spatial variability in snow
depth measured by probing, even within arm's reach. Substantial departure
occurs for reference snow depths between 0.20 and 0.60 m which tend to
exceed RPAS measurements. Negative depths in the RPAS-derived data set is a
product of co-registration uncertainty, particularly in areas where the
surface model represents large vegetation or is influenced by rock outcrops,
as well as spurious values from the constituent DSMs. Agreement between
reference and RPAS-derived data sets improved with the removal of reference
measurements made above tussocks. This filtering saw the <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> value
improve by 22 %, while RMSE decreased by 23 % (Table 4). The 1 : 1
ratio line was contained within the 95 % confidence interval of the
weighted (bi-square) regression between RPAS-derived and filtered reference
snow depths. Some disagreement between RPAS derived and probed snow depths is
likely due to the varying areas over which snow depth was sampled by the two
techniques, and resulting spatial uncertainty in comparing the two data sets.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4"><caption><p id="d1e2401">Parameters of weighted regression between reference and RPAS-derived
snow depths.</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"/>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M89" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">RMSE</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M93" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">All points</oasis:entry>
         <oasis:entry colname="col2">86</oasis:entry>
         <oasis:entry colname="col3">0.92</oasis:entry>
         <oasis:entry colname="col4">0.80</oasis:entry>
         <oasis:entry colname="col5">14.7</oasis:entry>
         <oasis:entry colname="col6">0.67</oasis:entry>
         <oasis:entry colname="col7">0.000</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Non-tussock</oasis:entry>
         <oasis:entry colname="col2">52</oasis:entry>
         <oasis:entry colname="col3">1.69</oasis:entry>
         <oasis:entry colname="col4">0.86</oasis:entry>
         <oasis:entry colname="col5">11.3</oasis:entry>
         <oasis:entry colname="col6">0.82</oasis:entry>
         <oasis:entry colname="col7">0.000</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S4.SS2.SSS3">
  <title>Comparison of DSMs from independent RPAS flights</title>
      <p id="d1e2548">The emergence of snow-free areas for the September flight permitted a
comparison of height derived on snow-free<?pagebreak page3487?> surfaces between the pre-winter and
spring flights (Fig. 5). The small magnitude of the residuals, compatible
with errors consistent with the uncertainty of the triangulation CPs,
demonstrates the repeatability in the derivation of snow-free surfaces.
Furthermore, the absence of any spatially structured trend in the
distribution of the residual indicates robust photogrammetric modelling from
the RPAS platform. At 0.15 m resolution, the snow-free pixels from the
spring mission provided a large sample (<inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 5 936 428). The mean
residual (bias) detected with respect to the pre-winter DSM was 0.024 m
(<inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.239</mml:mn></mml:mrow></mml:math></inline-formula> m) (Fig. 5).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><caption><p id="d1e2575">Mean, <inline-formula><mml:math id="M96" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> <bold>(a)</bold>, standard deviation, <inline-formula><mml:math id="M97" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> <bold>(b)</bold>
and distribution kurtosis <bold>(c)</bold> for the residual, in terms of discrete
classes of slope (5<inline-formula><mml:math id="M98" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> width), up to the 90th percentile of slope.
Kurtosis is plotted on a log-scale and is accompanied by a standard error of
606. The slope histogram has been clipped to the 90th percentile.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018-f06.png"/>

          </fig>

      <?pagebreak page3488?><p id="d1e2617">The set of residuals departed substantially from the Gaussian distribution
and was better represented by the Student's <inline-formula><mml:math id="M99" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> location-scale distribution
(Fig. 6):
              <disp-formula id="Ch1.E8" content-type="numbered"><mml:math id="M100" display="block"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Γ</mml:mi><mml:mfenced close=")" open="("><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mi>v</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mfenced></mml:mrow><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:msqrt><mml:mrow><mml:mi>v</mml:mi><mml:mi mathvariant="italic">π</mml:mi></mml:mrow></mml:msqrt><mml:mi mathvariant="normal">Γ</mml:mi><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>v</mml:mi><mml:mo>+</mml:mo><mml:mfenced close=")" open="("><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="italic">μ</mml:mi></mml:mrow><mml:mi mathvariant="italic">σ</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced></mml:mrow><mml:mi>v</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced><mml:mrow><mml:mo>-</mml:mo><mml:mfenced close=")" open="("><mml:mstyle scriptlevel="+1"><mml:mfrac><mml:mrow><mml:mi>v</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mfenced></mml:mrow></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M101" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M102" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M103" display="inline"><mml:mi>v</mml:mi></mml:math></inline-formula> are the location, scale and shape parameters,
respectively. Large kurtosis (calculated <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1956</mml:mn></mml:mrow></mml:math></inline-formula>) associated with the
histogram of residuals in Fig. 6 shows significant departure from a Gaussian
law (for which <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula>) of equal standard deviation, <inline-formula><mml:math id="M106" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>. The
leptokurtic experimental distribution results in a narrower 90 %
confidence interval than that estimated under the Gaussian assumption with
<inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.24</mml:mn></mml:mrow></mml:math></inline-formula> m, while the probability of large residuals is larger than
predicted by a Gaussian distribution. Overall, the mean residual (<inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.02</mml:mn></mml:mrow></mml:math></inline-formula> m) and the precision of <inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.14</mml:mn></mml:mrow></mml:math></inline-formula> m (90 % confidence level,
calculated from the distribution 90th percentile; Fig. 6) exceeds the
uncertainties estimated from error propagation alone (<inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.08</mml:mn></mml:mrow></mml:math></inline-formula> m at
90 % confidence level; see Sect. 4.1.1) yet support the suitable
repeatability of the photogrammetric modelling. Importantly, the significant
departure from a normal distribution shows that assessing the variability
from a Gaussian fit on stable targets (<inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.39</mml:mn></mml:mrow></mml:math></inline-formula> m at the 90 % level)
would significantly overestimate the confidence interval. On the other hand,
the 90% confidence interval calculated from the fitted Student's <inline-formula><mml:math id="M112" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>
location-scale is <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.10</mml:mn></mml:mrow></mml:math></inline-formula> m (Table 5). The significance of this result
with respect to statistical inferences is discussed further in Sect. 5.2.2.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T5"><caption><p id="d1e2847">Observed (calculated under Gaussian assumption) and fitted normal
and <inline-formula><mml:math id="M114" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> location-scale (<inline-formula><mml:math id="M115" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> l-s) parameters for the residual distributions
shown in Fig. 5b.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Parameter</oasis:entry>
         <oasis:entry colname="col2">Distribution</oasis:entry>
         <oasis:entry colname="col3">Value</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Observed</oasis:entry>
         <oasis:entry colname="col3">0.024</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M116" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> (m)</oasis:entry>
         <oasis:entry colname="col2">Normal fit</oasis:entry>
         <oasis:entry colname="col3">0.036</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M117" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> l-s fit</oasis:entry>
         <oasis:entry colname="col3">0.019</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Observed</oasis:entry>
         <oasis:entry colname="col3">0.239</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M118" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> (m)</oasis:entry>
         <oasis:entry colname="col2">Normal fit</oasis:entry>
         <oasis:entry colname="col3">0.236</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M119" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> l-s fit</oasis:entry>
         <oasis:entry colname="col3">0.056</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M120" display="inline"><mml:mi mathvariant="italic">ν</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M121" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> l-s fit</oasis:entry>
         <oasis:entry colname="col3">2.579</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p id="d1e3011">Comparison of histograms and accompanying descriptive statistics for
the residual between DSMs for slopes between 5 and 10<inline-formula><mml:math id="M122" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and slopes
between 70 and 75<inline-formula><mml:math id="M123" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. Flatter slopes are found to exhibit extreme
kurtosis relative to steeper slopes. Normal and <inline-formula><mml:math id="M124" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> location-scale (<inline-formula><mml:math id="M125" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>)
distributions are shown.</p></caption>
            <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018-f07.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><caption><p id="d1e3054">Semi-variograms for snow depth, based on measurements provided by
probing (86 samples), and two random samples drawn from RPAS-derived snow
depth of 1000 and 5000 observations.</p></caption>
            <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018-f08.png"/>

          </fig>

      <p id="d1e3063">The non-Gaussian nature of the residual distribution deserves further
scrutiny. Similar distributions have been identified for comparable
repeatability assessments of photogrammetric dDSMs used for mapping snow
depth (Nolan et al., 2015), but have not been explored in detail. Analysing
the variability of the mean and standard deviation of the residual for discrete classes of slope, as well
as the<?pagebreak page3489?> kurtosis of the residual distribution,
provided insight into the role of terrain. For classes of slope up to
65<inline-formula><mml:math id="M126" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> the mean residual remains within the standard error, before
becoming increasingly negative for the remaining classes (Fig. 6). Standard
deviation exhibits a similar trend, remaining largely within the overall
standard error for slope classes up to 45<inline-formula><mml:math id="M127" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, beyond which variability
increases.</p>
      <p id="d1e3084">The observed pattern in the mean and standard deviation of the residual
indicates that larger and more variable errors are associated with steeper
slopes. Reduced kurtosis accompanying the error distribution on larger slopes
(Fig. 6) reveals a tendency towards a Gaussian distribution of residuals as
mean slope increases. Here, for slopes <inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M129" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, kurtosis was reduced
below 100, and for slopes <inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">85</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M131" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, kurtosis was less than 10,
approaching that of the normal distribution. Therefore, the statistical
distribution of error, while non-normal, also varies significantly with
terrain characteristics, as highlighted by the comparison of the residual
histogram for discrete classes of slope (Fig. 7 and Table 6). Subsequently, the overall
distribution of residuals (Fig. 5b) is the result of a convolution between
non-normal distributions and the hypsometry of the area (i.e. area-elevation
distribution).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T6"><caption><p id="d1e3127">Observed (calculated under Gaussian assumption) and fitted normal
and <inline-formula><mml:math id="M132" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> location-scale (<inline-formula><mml:math id="M133" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> l-s) parameters for the residual distributions
shown in Fig. 7.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry rowsep="1" namest="col3" nameend="col4" align="center">Slope class </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Parameter</oasis:entry>
         <oasis:entry colname="col2">Distribution</oasis:entry>
         <oasis:entry colname="col3">5–10<inline-formula><mml:math id="M134" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">70–75<inline-formula><mml:math id="M135" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Observed</oasis:entry>
         <oasis:entry colname="col3">0.026</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.022</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M137" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> (m)</oasis:entry>
         <oasis:entry colname="col2">Normal fit</oasis:entry>
         <oasis:entry colname="col3">0.026</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.022</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M139" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> l-s fit</oasis:entry>
         <oasis:entry colname="col3">0.021</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.118</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Observed</oasis:entry>
         <oasis:entry colname="col3">0.186</oasis:entry>
         <oasis:entry colname="col4">0.892</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M141" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> (m)</oasis:entry>
         <oasis:entry colname="col2">Normal fit</oasis:entry>
         <oasis:entry colname="col3">0.186</oasis:entry>
         <oasis:entry colname="col4">0.892</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M142" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> l-s fit</oasis:entry>
         <oasis:entry colname="col3">0.046</oasis:entry>
         <oasis:entry colname="col4">0.376</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M143" display="inline"><mml:mi mathvariant="italic">ν</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M144" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> l-s fit</oasis:entry>
         <oasis:entry colname="col3">4.104</oasis:entry>
         <oasis:entry colname="col4">2.093</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S4.SS2.SSS4">
  <title>Characterising the spatial variability of snow depth</title>
      <p id="d1e3372">The semi-variograms for RPAS-derived snow depth, compared to that from the
reference measurements, are shown Fig. 8. They exemplify the new insight that
high-resolution mapping provides into the spatial variability of snow depth.
Both the 1000 and 5000 random point samples captured a comparable structure
of spatial auto-correlation with a range of ca. 40 m. The 5000-point sample
improved the resolution of the semi-variogram, with an improved signal-to-noise ratio. In contrast, the reference data, despite being demanding in
fieldwork, performed poorly at capturing the spatial variability, as most
measurements were separated by a minimum distance of 50 m. A lack of spatial
auto-correlation in the reference data confirms a posteriori that probing
samples could be assumed to be independent of each other, which is desirable
for the accuracy assessment. Additionally, it also reveals that probing
failed to capture most of the spatial structure of<?pagebreak page3490?> the snow depth field, thus
stressing a limitation of this classical method to characterise the snowpack.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S5">
  <title>Discussion</title>
<sec id="Ch1.S5.SS1">
  <title>Performance of RPAS photogrammetry for resolving snow depth</title>
      <p id="d1e3389">Overall, RPAS photogrammetry is found to be suitable for determining snow
depth via DSM differencing. Primarily, the achievement of uncertainties <inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.14</mml:mn></mml:mrow></mml:math></inline-formula> m at the 90 % confidence level for derived snow depth,
demonstrated empirically by the repeatability analysis (Fig. 5), provides a
basis for useful data capture, and robust inferences and interpretations. The
reported magnitudes of uncertainties account for the sources discussed further
below, and compare favourably with other similar studies (Vander Jagt et al.,
2015; Bühler et al., 2016; De Michele et al., 2016; Harder et al., 2016).
Decimetre levels of uncertainty appear to be an emerging benchmark for snow
depths measured by RPAS photogrammetry and also considered as standard for
airborne lidar (Deems et al., 2013). In terms of comparisons with in situ
data, Fig. 4 shows good agreement between RPAS and reference snow depth, and
that RPAS photogrammetry performance improves as snow depth increases. At the
same time, use of probed snow depths as references for validating such data
can be compromised by the nature of the underlying vegetation.</p>
      <p id="d1e3402">Mapping snow depth continuously at 0.15 m resolution, across an entire
hydrological catchment, represents a new contribution to the quantification
and characterisation of spatial variability in snow depth on this scale,
which is up to 2 orders of magnitude greater than many similar studies to
date. Before considering the broader implications of this in terms of snow
processes, uncertainty, limitations and pitfalls of the approach are
considered.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <title>Sources and nature of uncertainty</title>
<sec id="Ch1.S5.SS2.SSS1">
  <title>Vegetation</title>
      <p id="d1e3416">Vegetation contributes to uncertainty, particularly when validating
RPAS-derived snow depths against reference snow depths. As described in
Sect. 4.2.2, the agreement between RPAS-derived and probed snow depths
improved substantially when areas of large tussock vegetation were excluded.
It is likely that the presence of tussock introduces a bias into the snow
depth measurement, whereby a probe may penetrate the tussock foliage, and
possibly also a sub-vegetation void, before striking the ground surface. This
is similar to the cavity effect highlighted for airborne lidar measurement of
snow (Painter et al., 2016), and similar challenges have been documented by
Vander Jagt et al. (2015). High-resolution dDSMs, on the other hand, resolve
the vegetation surface, and so vegetation height is inherently better
accounted for.</p>
      <p id="d1e3419">As identified by Nolan et al. (2015), photogrammetrically derived snow depths
may also be affected by the compaction of vegetation below the snowpack,
which may introduce an anomalous signal of surface height change, to the
point of returning false negative snow depths. Correcting observed surface
height change would not be straightforward, and is not possible with the data
acquired within this study. The effects of vegetation compaction are likely
to be greatest in the early winter. As grass typically does not rebound until
after the complete removal of the winter snowpack, ongoing subsidence of
vegetation below the snowpack through midwinter and spring is expected to be
minimal. Ongoing future measurement of snow depth via surface differencing
(regardless of the source of DSMs) will benefit from the development and
incorporation of vegetation compaction and cavity models.</p>
      <p id="d1e3422">Ultimately, this study suggests that, for areas dominated by tussock
vegetation, RPAS photogrammetry may provide a more reliable means of
measurement than probing. A lack of knowledge regarding the specific location
of sub-snow vegetation when making measurements by probing is likely to
provide a systematic overestimation of snow depth (Fig. 4). In the New
Zealand context, almost all seasonal snow occurs above the treeline, so the
inability of photogrammetry to penetrate the forest canopy is a lesser concern
than for the Northern Hemisphere.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p id="d1e3427">The vertical residual between two elevation profiles, extracted from
the same DSM, along a common transect and offset horizontally by
0.5 m <bold>(a)</bold>, and the resulting residuals plotted as a function of
terrain surface slope, for the applied offset of 0.5 m, and a range of other
offsets (d<inline-formula><mml:math id="M146" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>) <bold>(b)</bold>.</p></caption>
            <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018-f09.png"/>

          </fig>

</sec>
<sec id="Ch1.S5.SS2.SSS2">
  <title>Geolocation and co-registration</title>
      <p id="d1e3455">In mapping snow depth across a catchment with relatively complex terrain, we
have been able to characterise the influence of terrain on dDSM uncertainty.
The assumption that error associated with physical measurements is normally
distributed and often underpins subsequent statistical inferences. As
demonstrated in Sect. 4.2.3, the error associated with the bias between
independently acquired DSMs significantly departed from normal and was
better approximated by the Student's <inline-formula><mml:math id="M147" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> location-scale distribution. This
extremely leptokurtic distribution of residuals reflects the influence of
relatively low frequency, but high-magnitude residuals beyond the probability
of the normal law, despite an overall dominance of residuals about and close
to the mean. A possible source of large residuals between two DSMs is their
relative planimetric accuracy and subsequent co-registration quality
(Kääb, 2005). For steep terrain in particular, a horizontal
displacement between DSMs could add a component to dDSM uncertainty beyond
the vertical accuracy of constituent DSMs. The residual (<inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:math></inline-formula>) between
two surface profiles, which are identical but horizontally displaced by
0.5 m, is shown in Fig. 9a. The error introduced to DSM differencing
resulting from co-registration uncertainty increases with steepening slope.
Maximum residuals coincide with the steepest terrain (near-vertical areas
associated with rock outcrops) and exceed 2 m. The sign of the error
is aspect dependent, assuming a uniform horizontal displacement.</p>
      <?pagebreak page3491?><p id="d1e3475">Consistent with Kääb (2005), the vertical error introduced by a
uniform, one-dimensional (e.g. horizontal) offset, is given by the following:
              <disp-formula id="Ch1.E9" content-type="numbered"><mml:math id="M149" display="block"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>h</mml:mi><mml:mo>=</mml:mo><mml:mtext>d</mml:mtext><mml:mi>x</mml:mi><mml:mi>tan⁡</mml:mi><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where d<inline-formula><mml:math id="M150" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> is the offset between transects (i.e. 0.5 m in this case), and
<inline-formula><mml:math id="M151" display="inline"><mml:mi mathvariant="italic">θ</mml:mi></mml:math></inline-formula> is the surface slope in degrees, as seen in Fig.  9b. It is clear
from Fig. 9b that where the average slope of target surfaces is low and
co-registration quality is good, the error introduced to a dDSM as a product
of co-registration will be minimal. Increasing slope and/or co-registration
uncertainty is accompanied by increased vertical uncertainty in the dDSM.
This relationship is consistent with the findings of Sect. 4.2.3, resulting in
the distribution of residuals departing substantially from the Gaussian
distribution when the proportion of steep slopes is low. These findings
provide context for the effect noted by Nolan et al. (2015), whereby a
non-normal distribution of residuals associated with photogrammetric mapping
of snow depth was found to narrow further when the area considered was
restricted to a frozen lake (i.e. near planar) surface.</p>
      <p id="d1e3514">Complicating this effect is the fact that co-registration uncertainty exists
in two dimensions. Subsequently, it will become dependent on aspect as well
as slope (Nuth and Kääb, 2011), with neither possessing a uniform
spatial distribution. This effect is expected to be more pronounced with very
high-resolution (i.e. sub-metre) surface models due to a greater frequency
and magnitude of breaks in surface slope being resolved compared to coarser
models. The modification of surface slope for constituent DSMs (e.g. through
the addition of snow) further convolves the propagation of vertical
uncertainty. Despite this, the leptokurtic observed error distribution
indicates that the reliance on statistics that assume a Gaussian distribution
of errors will provide an overestimated characterisation of the expected
accuracy. Overestimation of uncertainties may in turn affect statistical
inferences and the computation of uncertainties on derived parameters.</p>
      <p id="d1e3517">The convolution of vertical and planimetric accuracy stresses the importance
of ensuring a robust AT and the benefits of utilising high-quality ground
control. With new photogrammetric platforms leveraging non-metric cameras
and resulting image blocks prone to suboptimal photogrammetric modelling
(Sirguey et al., 2016), there is a need to be wary of systematic
bias or spatial structure in the distribution of errors, which may not be
revealed readily by residuals from the AT alone. These considerations are
especially important where a relatively high level of precision is required,
and the signal-to-noise ratio may be low when assessing relatively subtle
surface height and/or volume changes from dDSMs. Utilising independent ATs
as the control of co-registration quality, rather than explicitly
co-registering DSMs, has the further advantage of simplifying the processing
chain from data acquisition to change detection, mitigating against the risk
of introducing gross error when co-registering DSMs and avoiding the need
for snow-free (or stable) reference areas within the analysis region.</p>
</sec>
</sec>
<?pagebreak page3492?><sec id="Ch1.S5.SS3">
  <title>Pitfalls and limitations of RPAS photogrammetry</title>
      <p id="d1e3527">Initial processing using the photogrammetry module of Trimble Business
Center (v3.40) produced strong striping artefacts in the dDSM. Striping
involved a periodic bias in surface height change, aligned with the 15 image
strips. This was readily revealed because identical flight plans between
successive surveys made constructive errors obvious, rather than convoluted
with terrain variability. This systematic error was severe and problematic,
particularly when considering the surface change resulting from the addition
of snow cover to the ground. Extensive snow cover concealed stable
references, precluding characterisation of the error and its empirical
removal from the real signal of surface height change (e.g. Albani and
Klinkenberg, 2003; Berthier et al., 2007). Products derived using UAS Master
(v8.0) did not exhibit such artefacts, allowing the potential source of error
associated with AT from TBC to be investigated.</p>
      <p id="d1e3530">The absence of systematic bias in dDSMs derived using UAS Master indicates a
more reliable AT. Thus, the UAS Master triangulation provided a reference
surface for further exploration of the nature of the bias propagated in the
TBC triangulation. Comparisons from the winter flight are presented here.
The nature of the photogrammetric problem described in Sect. 3.2.1  dictates
that small errors in the interior orientation and/or the rotational components
of the exterior orientation can result in large, spatially structured errors in the adjusted image block
(Sirguey et al., 2016).</p>
      <p id="d1e3533">Cimoli et al. (2017) reported an improved performance in mapping snow depth
with the application of a radial lens distortion correction. In our case, no
significant difference was detected between the distortion models provided
for each of the two software calibrations of the same camera, for the same
flight. (Fig. 11a). Minimal divergence in lens distortion was observed beyond
10 mm radius, reaching 1 % at 14.5 mm. Agreement between lens
distortion models indicated that differing interior orientation solutions
between TBC and UAS Master were not the source of the artefacts seen in
products of the TBC triangulation.</p>
      <p id="d1e3536">Since the observed artefact was propagated along the flight lines, the roll
parameter (<inline-formula><mml:math id="M152" display="inline"><mml:mi mathvariant="italic">ω</mml:mi></mml:math></inline-formula>) was considered. Bias in the estimation of this
parameter could lead to a systematic elevation offset of resected points
between flight lines, either raising or lowering the terrain,
as documented in the case of stereo-satellite imagery by Berthier et
al. (2007). Occurrence of this for multiple flights with near-identical
flight lines would exacerbate constructive biases, resulting in the striping
in the dDSM. Alternatively, pitch and yaw parameters are unlikely to produce
such an artefact along the flight direction (Ebner and Fritz, 1980). The
residual of <inline-formula><mml:math id="M153" display="inline"><mml:mi mathvariant="italic">ω</mml:mi></mml:math></inline-formula> for individual photo centres between each of the two
software packages confirmed that a positive bias existed in the <inline-formula><mml:math id="M154" display="inline"><mml:mi mathvariant="italic">ω</mml:mi></mml:math></inline-formula> value as
estimated by TBC v3.40 relative to that provided by UAS Master. The mean
residual (<inline-formula><mml:math id="M155" display="inline"><mml:mover accent="true"><mml:mrow><mml:mi>r</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula>) was found to be 0.014<inline-formula><mml:math id="M156" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>.</p>
      <p id="d1e3583">The impact of bias in <inline-formula><mml:math id="M157" display="inline"><mml:mi mathvariant="italic">ω</mml:mi></mml:math></inline-formula> on the resected height <inline-formula><mml:math id="M158" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula> for a target with
respect to a photo centre can be estimated simply as a right-angled triangle,
since values of <inline-formula><mml:math id="M159" display="inline"><mml:mi mathvariant="italic">ω</mml:mi></mml:math></inline-formula> are small compared to the baseline length, <inline-formula><mml:math id="M160" display="inline"><mml:mi>l</mml:mi></mml:math></inline-formula>,
which is equal to half the distance between adjacent flight lines (see
Fig. 12):

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M161" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E10"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>tan⁡</mml:mi><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>h</mml:mi><mml:mi>l</mml:mi></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E11"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi>tan⁡</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>-</mml:mo><mml:mover accent="true"><mml:mrow><mml:mi>r</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>h</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>h</mml:mi></mml:mrow><mml:mi>l</mml:mi></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E12"><mml:mtd/><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>h</mml:mi><mml:mo>=</mml:mo><mml:mi>h</mml:mi><mml:mo>-</mml:mo><mml:mi>l</mml:mi><mml:mi>tan⁡</mml:mi><mml:mfenced open="(" close=")"><mml:mover accent="true"><mml:mrow><mml:mi>r</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mfenced></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E13"><mml:mtd/><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>h</mml:mi><mml:mo>=</mml:mo><mml:mi>h</mml:mi><mml:mo>-</mml:mo><mml:mi>l</mml:mi><mml:mi>tan⁡</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:mi>arctan⁡</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>h</mml:mi><mml:mi>l</mml:mi></mml:mfrac></mml:mstyle><mml:mover accent="true"><mml:mrow><mml:mi>r</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mrow></mml:mfenced><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            Using the observed value of 0.014<inline-formula><mml:math id="M162" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> for <inline-formula><mml:math id="M163" display="inline"><mml:mover accent="true"><mml:mrow><mml:mi>r</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula>, <inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:math></inline-formula> was calculated for a range of typical values of <inline-formula><mml:math id="M165" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula>, yielding the
relationship between <inline-formula><mml:math id="M166" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:math></inline-formula> as shown in Fig. 11b. Bias in the
estimation of the <inline-formula><mml:math id="M168" display="inline"><mml:mi mathvariant="italic">ω</mml:mi></mml:math></inline-formula> parameter during the AT can introduce a
significant vertical error, dependent (non-linearly) on flying height (<inline-formula><mml:math id="M169" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula>),
propagating an error of <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.12</mml:mn></mml:mrow></mml:math></inline-formula> m at a flying height of 110 m. The
increase in error with flying height above ground level was consistent with
the observed propagation of striping artefacts in DSM products, whereby the
magnitude of the observed bias decreased as terrain height increased
(Fig. 10), while absolute flying height remained approximately constant.</p>
      <p id="d1e3830">The observed propagation reinforces the need for vigilance when working with
such data sets, particularly those delivered from “off the shelf”
photogrammetry packages, which are becoming increasingly popular. Artefacts
such as the striping identified here, and evidence of non-optimal AT, are
likely to be less obvious as the complexity of the mapped terrain increases.
As RTK GPS-equipped RPAS become more common, increased precision of initial
AT parameters may mitigate the risk of error introduced by spurious
solutions for refined parameters. Currently, however, RTK systems have an
increased power demand, which can substantially reduce the flight time.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><caption><p id="d1e3835">Map of the systematic artefacts in surface height change (dh)
(expected to represent snow depth), propagated when differencing digital
surface models (DSMs) resulting from aerial-triangulation in TBC v3.40
<bold>(a)</bold> compared with the dDSM from UAS Master <bold>(b)</bold>. Vertical
(north–south aligned) striping is highlighted in <bold>(c)</bold>, which shows the residual
between dDSMs derived from TBC and UAS Master.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018-f10.jpg"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><caption><p id="d1e3855">Comparison of lens distortion characterised by individual
triangulations of data from the same flight carried out in two different
software packages, TBC and UAS Master <bold>(a)</bold>, and the error in surface
height propagated by a bias in the roll parameter, <inline-formula><mml:math id="M171" display="inline"><mml:mi mathvariant="italic">ω</mml:mi></mml:math></inline-formula>, in relation to
flying height <bold>(b)</bold>. The distortion residual was only apparent at
radial distances <inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">12</mml:mn></mml:mrow></mml:math></inline-formula> mm <bold>(a)</bold>, while the observed mean bias in
<inline-formula><mml:math id="M173" display="inline"><mml:mi mathvariant="italic">ω</mml:mi></mml:math></inline-formula> that was propagated by TBC results in substantial errors in surface
height <bold>(b)</bold>.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018-f11.png"/>

        </fig>

</sec>
<sec id="Ch1.S5.SS4">
  <title>Spatial and temporal trends in snow cover</title>
      <p id="d1e3907">Figure 8 demonstrates the new insight that RPAS photogrammetry can provide
over probing for resolving spatial variability in snow depth, particularly on
fine scales. Therefore, RPAS photogrammetry can provide a basis for improving
spatially distributed snowpack models. In turn, this contribution will
further improve understanding of seasonal snow processes, where there has
been a dependency on point-based observations over glaciers to characterise
atmospheric controls on seasonal snow (e.g. Cullen and Conway, 2015). While
knowledge of the atmospheric controls on ablation processes has improved
(Conway and Cullen, 2016), our understanding of the redistribution of snow
and preferential accumulation have not kept pace. RPAS photogrammetry
represents a valuable avenue for determining how these<?pagebreak page3493?> processes are
represented in existing and new snow and glacier models, which will enable
short-term hydrological forecasts and climate projections in snow-covered
areas to be improved. Such data can also facilitate the use of geostatistical
approaches for examining controls on spatial distribution of snow, such as
that applied to the Brewster Glacier, New Zealand (Cullen et al., 2017). In
this case, the density of measurements provides insights into spatial
variability on scales that would allow consideration of terrain and
meteorological controls on snow distribution on micro-scales, extending
understanding beyond the spatial co-variance between snow depth and
elevation.</p>
      <?pagebreak page3494?><p id="d1e3910">The ability to resolve fine-scale variability reliably from continuous raster
snow maps lessens the dependence on interpolation through areas of sparse
data for interpreting controls on spatial distribution of snow. While
previous studies have been able to correlate between snow and terrain
properties (e.g. Anderson et al., 2014), such studies rely on the inference
of catchment-scale processes from transect-scale observations. The ability to
produce spatially continuous maps of snow depth across an entire catchment
at a resolution of 0.15 m bridges this gap and reduces the reliance on
inferences when scaling up from point- or transect-based in situ observations
to catchment-scale processes. Such data sets provide an opportunity to build
on previous work in understanding the relationships between snow
redistribution, preferential accumulation and ablation, terrain and
meteorology (Winstral et al., 2002, 2013; Webster et al., 2015; Revuelto et
al., 2016). While RPAS photogrammetry is severely limited in spatial scale
compared to airborne lidar, resolving snow depth in this way across an entire
catchment facilitates robust integration into hydrological models, enhanced
by validation against catchment discharge (e.g. from streamflow data).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12"><caption><p id="d1e3915">Schematic of the relationship between height (<inline-formula><mml:math id="M174" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula>), baseline length
(<inline-formula><mml:math id="M175" display="inline"><mml:mi>l</mml:mi></mml:math></inline-formula>) and the interior angle (<inline-formula><mml:math id="M176" display="inline"><mml:mi mathvariant="italic">θ</mml:mi></mml:math></inline-formula>) that may be affected by a bias
(<inline-formula><mml:math id="M177" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:math></inline-formula>) for a terrain point position resected from images centred at p1
and p2, when the mean bias (<inline-formula><mml:math id="M178" display="inline"><mml:mover accent="true"><mml:mrow><mml:mi>r</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula>) is small (e.g.
0.014<inline-formula><mml:math id="M179" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> in this case).</p></caption>
          <?xmltex \igopts{width=113.811024pt}?><graphic xlink:href="https://tc.copernicus.org/articles/12/3477/2018/tc-12-3477-2018-f12.png"/>

        </fig>

      <p id="d1e3978">The mapping of snow depth effectively provides a volumetric view of the
snowpack across the catchment (i.e. depth <inline-formula><mml:math id="M180" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> area). The snowpack
mass balance in terms of SWE can be calculated based on in situ measurements
of snow density. While snow depth was only determined for two dates in this
case, emergent trends within the data can be explored. Between the winter and
spring flights, the catchment snow-covered area (SCA) decreased from
100 % to 67 %. Bulk snowpack densities, measured gravimetrically at
a single snow pit for the winter flight (314 kg m<inline-formula><mml:math id="M181" 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>), and two snow
pits for the spring flight (391 kg m<inline-formula><mml:math id="M182" 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>), allow catchment SWE to be
calculated, revealing a 20 % reduction in SWE between flights. This
highlights the importance of effective concentration of snow in preferred
areas, and the complex spatial distribution that results. The ability to
detect this, even with a temporally limited data set, indicates the potential
for RPAS photogrammetry as a measurement approach for improving resolution
and understanding of snow hydrology. In particular, such data sets may offer a
unique opportunity to assess the performance of models forced by remotely
sensed data of coarser resolution in estimating SWE from estimates of
subpixel fractional SCA (Bair et al., 2016).</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <title>Conclusions and outlook</title>
      <p id="d1e4019">This study has demonstrated that RPAS photogrammetry provides a suitable,
repeatable means of reliably determining snow depth in an alpine catchment
of low relief that possesses some terrain complexity. Achieving decimetre-level accuracy for measuring snow depth provides a basis for monitoring
seasonal snowpacks and associated processes, especially considering the
capacity to provide very high-resolution, spatially continuous measurements
across an entire hydrological catchment. This ability to characterise the
seasonal snowpack will provide an important stepping stone for improved
modelling of seasonal snow and associated processes, especially through
accurate mapping of an entire hydrological catchment.</p>
      <p id="d1e4022">Challenges encountered through this deployment provide important points for
consideration in this and other applications of close-range photogrammetry,
especially from RPAS platforms, for surface and volume change analysis.
Specifically, a small but persistent bias in photogrammetric solutions for the
roll parameter exemplifies the possibility of suboptimal solutions in
processing software. Such a bias can introduce substantial systematic errors
which may be difficult to correct and can compromise further analysis.</p>
      <p id="d1e4025">We show that uncertainty analysis from the AT only, based on a limited
number of check points, may underestimate the uncertainty. Alternatively, an
assessment of repeatability of photogrammetric modelling on stable ground
can support a more detailed uncertainty analysis. It reveals, however, that
the statistical distribution of the error of differentiated surface models
is more complex than normal and governed by terrain parameters. The
leptokurtic residual distribution demonstrates that an assumption of
Gaussian law can substantially overestimate confidence intervals, in turn
compromising inferences. This result has important practical applications for
the computation of uncertainties in studies that characterise volume change
from repeated surface modelling.</p>
      <p id="d1e4028">Finally, there is scope to further refine the characterisation of
uncertainty associated with RPAS photogrammetry in order to ensure that all
potential sources of error are captured, and that statistical analysis is
appropriate to the distributions within underlying data. Existing methods
for mitigating the impact of co-registration uncertainty of coarser products
may<?pagebreak page3495?> permit modelling and correction of such errors in the very
high-resolution products that are now available.</p>
</sec>

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

      <p id="d1e4035">The data used in this research are available on request
from Todd A. N. Redpath.</p>
  </notes><notes notes-type="authorcontribution">

      <p id="d1e4041">TR and PS designed the study and collected the data. TR processed and
analysed the data and wrote the manuscript with input from PS and NC. PS and
NC supervised the research.</p>
  </notes><notes notes-type="competinginterests">

      <p id="d1e4047">The authors declare that they have no conflict of
interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e4053">The authors are grateful to those who provided assistance in the field:
Julien Boeuf, Kelly Gragg, Mike Denham, Craig MacDonell, Aubrey Miller, Sam
West, Thomas Ibbotson and Alia Khan. Sean Fitzsimons provided helpful
feedback on the draft manuscript. This research was carried out under the
Department of Conservation Research &amp; Collection Authorisation 53609-GEO.
This research was funded by a University of Otago Doctoral Scholarship with
support from the Department of Geography and an internal grant of the
National School of Surveying, as well as a fieldwork grant from the New
Zealand Hydrological Society. The authors thank the editor, Martin
Schneebeli, and two anonymous reviewers, whose thorough and thoughtful
comments improved this manuscript.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?> Edited by:
Martin Schneebeli<?xmltex \hack{\newline}?> Reviewed by: two anonymous referees</p></ack><ref-list>
    <title>References</title>

      <ref id="bib1.bib1"><label>1</label><mixed-citation>Albani, M. and Klinkenberg, B.: A spatial filter for the removal of striping
artifacts in digital elevation models, Photogramm. Eng. Remote, 69, 755–765,
<ext-link xlink:href="https://doi.org/10.14358/PERS.69.7.755" ext-link-type="DOI">10.14358/PERS.69.7.755</ext-link>, 2003.</mixed-citation></ref>
      <ref id="bib1.bib2"><label>2</label><mixed-citation>Anderson, B. T., McNamara, J. P., Marshall, H.-P., and Flores, A. N.:
Insights into the physical processes controlling correlations between snow
distribution and terrain properties, Water. Resour. Res., 50, 4545–4563,
<ext-link xlink:href="https://doi.org/10.1002/2013WR013714" ext-link-type="DOI">10.1002/2013WR013714</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib3"><label>3</label><mixed-citation>Avanzi, F., Bianchi, A., Cina, A., De Michele, C., Maschio, P., Pagliari, D.,
Passoni, D., Pinto, L., Piras, M., and Rossi, L.: Centimetric accuracy in
snow depth using unmanned aerial system photogrammetry and a multistation,
Remote Sensing, 10, 1–16, <ext-link xlink:href="https://doi.org/10.3390/rs10050765" ext-link-type="DOI">10.3390/rs10050765</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib4"><label>4</label><mixed-citation>Bair, E. H., Rittger, K., Davis, R. E., Painter, T. H., and Dozier, J.:
Validating reconstruction of snow water equivalent in California's Sierra
Nevada using measurements from the NASA Airborne Snow Observatory, Water.
Resour. Res., 52, 8437–8460, <ext-link xlink:href="https://doi.org/10.1002/2016WR018704" ext-link-type="DOI">10.1002/2016WR018704</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib5"><label>5</label><mixed-citation>Berthier, E., Arnaud, Y., Kumar, R., Ahmad, S., Wagnon, P., and Chevallier,
P.: Remote sensing estimates of glacier mass balances in the Himachal Pradesh
(Western Himalaya, India), Remote Sens. Environ., 108, 327–338,
<ext-link xlink:href="https://doi.org/10.1016/j.rse.2006.11.017" ext-link-type="DOI">10.1016/j.rse.2006.11.017</ext-link>, 2007.</mixed-citation></ref>
      <ref id="bib1.bib6"><label>6</label><mixed-citation>Bessho, K., Date, K., Hayashi, M., Ikeda, A., Imai, T., Inoue, H., Kumagai,
Y., Miyakawa, T., Murata, H., Ohno, T., Okuyama, A., Oyama, R., Sasaki, Y.,
Shimazu, Y., Shimoji, K., Sumida, Y., Suzuki, M., Taniguchi, H., Tsuchiyama,
H., Uesawa, D., Yokota, H., and Yoshida, R.: An Introduction to Himawari-8/9
– Japan's New-Generation Geostationary Meteorological Satellites, J.
Meteorol. Soc. Jpn. Ser. II, 94, 151–183, <ext-link xlink:href="https://doi.org/10.2151/jmsj.2016-009" ext-link-type="DOI">10.2151/jmsj.2016-009</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib7"><label>7</label><mixed-citation>
Brown, D. C.: Close-range camera calibration, Photogramm. Eng., 37, 855–866,
1971.</mixed-citation></ref>
      <ref id="bib1.bib8"><label>8</label><mixed-citation>Bühler, Y., Adams, M. S., Bösch, R., and Stoffel, A.: Mapping snow
depth in alpine terrain with unmanned aerial systems (UASs): potential and
limitations, The Cryosphere, 10, 1075–1088,
<ext-link xlink:href="https://doi.org/10.5194/tc-10-1075-2016" ext-link-type="DOI">10.5194/tc-10-1075-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib9"><label>9</label><mixed-citation>Bühler, Y., Adams, M. S., Stoffel, A., and Boesch, R.: Photogrammetric
reconstruction of homogenous snow surfaces in alpine terrain applying
near-infrared UAS imagery, Int. J. Remote Sens., 38, 3135–3158,
<ext-link xlink:href="https://doi.org/10.1080/01431161.2016.1275060" ext-link-type="DOI">10.1080/01431161.2016.1275060</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib10"><label>10</label><mixed-citation>Cimoli, E., Marcer, M., Vandecrux, B., Bøggild, C. E., Williams, G., and Simonsen, S. B.: Application of Low-Cost UASs and Digital
Photogrammetry for High-Resolution Snow Depth Mapping in the Arctic, Remote Sens., 9, 1142,
<ext-link xlink:href="https://doi.org/10.3390/rs9111144" ext-link-type="DOI">10.3390/rs9111144</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib11"><label>11</label><mixed-citation>Clark, M. P., Hendrikx, J., Slater, A. G., Kavetski, D., Anderson, B.,
Cullen, N. J., Kerr, T., Hreinsson, E. Ö., and Woods, R. A.:
Representing spatial variability of snow water equivalent in hydrologic and
land-surface models?: A review, Water. Resour. Res., 47, W07539,
<ext-link xlink:href="https://doi.org/10.1029/2011WR010745" ext-link-type="DOI">10.1029/2011WR010745</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bib12"><label>12</label><mixed-citation>Conway, J. P. and Cullen, N. J.: Cloud effects on surface energy and mass
balance in the ablation area of Brewster Glacier, New Zealand, The
Cryosphere, 10, 313–328, <ext-link xlink:href="https://doi.org/10.5194/tc-10-313-2016" ext-link-type="DOI">10.5194/tc-10-313-2016</ext-link>, 2016</mixed-citation></ref>
      <ref id="bib1.bib13"><label>13</label><mixed-citation>Cullen, N. J. and Conway, J. P.: A 22 month record of surface meteorology and
energy balance from the ablation zone of Brewster Glacier, New Zealand, J.
Glaciol., 61, 931–946, <ext-link xlink:href="https://doi.org/10.3189/2015JoG15J004" ext-link-type="DOI">10.3189/2015JoG15J004</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib14"><label>14</label><mixed-citation>Cullen, N. J., Anderson, B., Sirguey, P., Stumm, D., Mackintosh, A., Conway,
J. P., Horgan, H. J., Dadic, R., Fitzsimons, S. J., and Lorrey, A.: An
11-year record of mass balance of Brewster Glacier, New Zealand, determined
using a geostatistical approach, J. Glaciol., 63, 199–217,
<ext-link xlink:href="https://doi.org/10.1017/jog.2016.128" ext-link-type="DOI">10.1017/jog.2016.128</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib15"><label>15</label><mixed-citation>Deems, J. S., Painter, T. H., and Finnegan, D. C.: Lidar measurement of snow
depth: A review, J. Glaciol., 59, 467–479, <ext-link xlink:href="https://doi.org/10.3189/2013JoG12J154" ext-link-type="DOI">10.3189/2013JoG12J154</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib16"><label>16</label><mixed-citation>De Michele, C., Avanzi, F., Passoni, D., Barzaghi, R., Pinto, L., Dosso, P.,
Ghezzi, A., Gianatti, R., and Della Vedova, G.: Using a fixed-wing UAS to map
snow depth distribution: an evaluation at peak accumulation, The Cryosphere,
10, 511–522, <ext-link xlink:href="https://doi.org/10.5194/tc-10-511-2016" ext-link-type="DOI">10.5194/tc-10-511-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib17"><label>17</label><mixed-citation>
Dozier, J.: Spectral signature of alpine snow cover from the Landsat Thematic
Mapper, Remote Sens. Environ., 22, 9–22, 1989.</mixed-citation></ref>
      <?pagebreak page3496?><ref id="bib1.bib18"><label>18</label><mixed-citation>
Ebner, H. and Fritz, L.: Aerotriangulation, in: Manual of Photogrammetry, 4th
edn., edited by: Slama, C. C., American Society of Photogrammetry, Falls
Church, 453–518, 1980.</mixed-citation></ref>
      <ref id="bib1.bib19"><label>19</label><mixed-citation>Fernandes, R., Prevost, C., Canisius, F., Leblanc, S. G., Maloley, M., Oakes,
S., Holman, K., and Knudby, A.: Monitoring snow depth change across a range
of landscapes with ephemeral snow packs using Structure from Motion applied
to lightweight unmanned aerial vehicle videos, The Cryosphere Discuss.,
<ext-link xlink:href="https://doi.org/10.5194/tc-2018-82" ext-link-type="DOI">10.5194/tc-2018-82</ext-link>, in review, 2018.</mixed-citation></ref>
      <ref id="bib1.bib20"><label>20</label><mixed-citation>Hall, D. K., Crawford, C. J., Di Girolamo, N. E., Riggs, G. A., and Foster,
J. L.: Detection of earlier snowmelt in the Wind River Range, Wyoming, using
Landsat imagery, 1972–2013, Remote Sens. Environ., 162, 45–54,
<ext-link xlink:href="https://doi.org/10.1016/j.rse.2015.01.032" ext-link-type="DOI">10.1016/j.rse.2015.01.032</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib21"><label>21</label><mixed-citation>Hall, D. K., Riggs, G. A., Salomonson, V. V, Di Girolamo, N. E., and Bayr, K.
J.: MODIS snow-cover products, Remote Sens. Environ., 83, 181–194,
<ext-link xlink:href="https://doi.org/10.1016/S0034-4257(02)00095-0" ext-link-type="DOI">10.1016/S0034-4257(02)00095-0</ext-link>, 2002.</mixed-citation></ref>
      <ref id="bib1.bib22"><label>22</label><mixed-citation>Harder, P., Schirmer, M., Pomeroy, J., and Helgason, W.: Accuracy of snow
depth estimation in mountain and prairie environments by an unmanned aerial
vehicle, The Cryosphere, 10, 2559–2571,
<ext-link xlink:href="https://doi.org/10.5194/tc-10-2559-2016" ext-link-type="DOI">10.5194/tc-10-2559-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib23"><label>23</label><mixed-citation>Hirschmuller, H.: Accurate and efficient stereo processing by semi-global
matching and mutual information, IEEE. T. Pattern Anal., 2, 807–814,
<ext-link xlink:href="https://doi.org/10.1109/CVPR.2005.56" ext-link-type="DOI">10.1109/CVPR.2005.56</ext-link>, 2008.</mixed-citation></ref>
      <ref id="bib1.bib24"><label>24</label><mixed-citation>James, L. A., Hodgson, M. E., Ghoshal, S., and Latiolais, M. M.: Geomorphic
change detection using historic maps and DEM differencing: The temporal
dimension of geospatial analysis, Geomorphology, 137, 181–198,
<ext-link xlink:href="https://doi.org/10.1016/j.geomorph.2010.10.039" ext-link-type="DOI">10.1016/j.geomorph.2010.10.039</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib25"><label>25</label><mixed-citation>
Kääb, A.: Remote Sensing of Mountain Glaciers and Permafrost Creep.
Zürich: Geographisches Institut der Universiturich, Zürich, 2005.</mixed-citation></ref>
      <ref id="bib1.bib26"><label>26</label><mixed-citation>Kerr, T., Clark, M., Hendrikx, J., and Anderson, B.: Snow distribution in a
steep mid-latitude alpine catchment, Adv. Water Resour., 55, 17–24,
<ext-link xlink:href="https://doi.org/10.1016/j.advwatres.2012.12.010" ext-link-type="DOI">10.1016/j.advwatres.2012.12.010</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib27"><label>27</label><mixed-citation>Kinar, N. J. and Pomeroy, J. W.: Measurement of the physical properties of
the snowpack, Rev. Geophys., 53, 481–544, <ext-link xlink:href="https://doi.org/10.1002/2015RG000481" ext-link-type="DOI">10.1002/2015RG000481</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib28"><label>28</label><mixed-citation>Lemmetyinen, J., Derksen, C., Rott, H., Macelloni, G., King, J., Schneebeli,
M., Wiesmann, A., Leppänen, L., Kontu, A., and Pulliainen, J.:
Retrieval of Effective Correlation Length and Snow Water Equivalent from
Radar and Passive Microwave Measurements, Remote Sens., 10, 170,
<ext-link xlink:href="https://doi.org/10.3390/rs10020170" ext-link-type="DOI">10.3390/rs10020170</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib29"><label>29</label><mixed-citation>Lindeberg, T.: Image Matching Using Generalized Scale-Space Interest Points,
J. Math. Imaging Vis., 52, 3–36, <ext-link xlink:href="https://doi.org/10.1007/s10851-014-0541-0" ext-link-type="DOI">10.1007/s10851-014-0541-0</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib30"><label>30</label><mixed-citation>
Linder, W.: Digital Photogrammetry: A Practical Course, 4th edn., Heidelberg,
Springer, 2016.</mixed-citation></ref>
      <ref id="bib1.bib31"><label>31</label><mixed-citation>Malenovský, Z., Rott, H., Cihlar, J., Schaepman, M. E.,
García-Santos, G., Fernandes, R., and Berger, M.: Sentinels for science:
Potential of Sentinel-1, -2, and -3 missions for scientific observations of
ocean, cryosphere, and land, Remote Sens. Environ., 120, 91–101,
<ext-link xlink:href="https://doi.org/10.1016/j.rse.2011.09.026" ext-link-type="DOI">10.1016/j.rse.2011.09.026</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib32"><label>32</label><mixed-citation>Mankin, J. S., Viviroli, D., Singh, D., Hoekstra, A. Y., and Diffenbaugh, N.
S.: The potential for snow to supply human water demand in the present and
future, Environ. Res. Lett., 10, 114016, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/10/11/114016" ext-link-type="DOI">10.1088/1748-9326/10/11/114016</ext-link>,
2015.</mixed-citation></ref>
      <ref id="bib1.bib33"><label>33</label><mixed-citation>Marti, R., Gascoin, S., Berthier, E., de Pinel, M., Houet, T., and Laffly,
D.: Mapping snow depth in open alpine terrain from stereo satellite imagery,
The Cryosphere, 10, 1361–1380, <ext-link xlink:href="https://doi.org/10.5194/tc-10-1361-2016" ext-link-type="DOI">10.5194/tc-10-1361-2016</ext-link>,
2016.</mixed-citation></ref>
      <ref id="bib1.bib34"><label>34</label><mixed-citation>Nolan, M., Larsen, C., and Sturm, M.: Mapping snow depth from manned aircraft
on landscape scales at centimeter resolution using structure-from-motion
photogrammetry, The Cryosphere, 9, 1445–1463,
<ext-link xlink:href="https://doi.org/10.5194/tc-9-1445-2015" ext-link-type="DOI">10.5194/tc-9-1445-2015</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib35"><label>35</label><mixed-citation>Nolin, A. W. and Dozier, J.: Estimating snow grain size using AVIRIS data,
Remote Sens. Environ., 44, 231–238, <ext-link xlink:href="https://doi.org/10.1016/0034-4257(93)90018-S" ext-link-type="DOI">10.1016/0034-4257(93)90018-S</ext-link>, 1993.</mixed-citation></ref>
      <ref id="bib1.bib36"><label>36</label><mixed-citation>Nuth, C. and Kääb, A.: Co-registration and bias corrections of
satellite elevation data sets for quantifying glacier thickness change, The
Cryosphere, 5, 271–290, <ext-link xlink:href="https://doi.org/10.5194/tc-5-271-2011" ext-link-type="DOI">10.5194/tc-5-271-2011</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bib37"><label>37</label><mixed-citation>Painter, T. H., Berisford, D. F., Boardman, J. W., Bormann, K. J., Deems, J.
S., Gehrke, F., Hedrick, A., Joyce, M., Laidlaw, R., Marks, D., Mattmann, C.,
McGurk, B., Ramirez, P., Richardson, M., Skiles, S. M. K., Seidel, F. C., and
Winstral, A.: The Airborne Snow Observatory: Fusion of scanning lidar,
imaging spectrometer, and physically-based modeling for mapping snow water
equivalent and snow albedo, Remote Sens. Environ., 184, 139–152,
<ext-link xlink:href="https://doi.org/10.1016/j.rse.2016.06.018" ext-link-type="DOI">10.1016/j.rse.2016.06.018</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib38"><label>38</label><mixed-citation>Revuelto, J., Vionnet, V., López-Moreno, J. I., Lafaysse, M., and Morin,
S.: Combining snowpack modeling and terrestrial laser scanner observations
improves the simulation of small scale snow dynamics, J. Hydrol., 533,
291–307, <ext-link xlink:href="https://doi.org/10.1016/j.jhydrol.2015.12.015" ext-link-type="DOI">10.1016/j.jhydrol.2015.12.015</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib39"><label>39</label><mixed-citation>Rittger, K., Painter, T. H., and Dozier, J. : Assessment of methods for
mapping snow cover from MODIS, Adv. Water Resour., 51, 367–380,
<ext-link xlink:href="https://doi.org/10.1016/j.advwatres.2012.03.002" ext-link-type="DOI">10.1016/j.advwatres.2012.03.002</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib40"><label>40</label><mixed-citation>Roy, D. P., Wulder, M. A., Loveland, T. R., C.E., W., Allen, R. G., Anderson,
M. C., Helder, D., Irons, J. R., Johnson, D. M., Kennedy, R., Scambos, T. A.,
Schaaf, C. B., Schott, J. R., Sheng, Y., Vermote, E. F., Belward, A. S.,
Bindschadler, R., Cohen, W. B., Gao, F., Hipple, J. D., Hostert, P.,
Huntington, J., Justice, C. O., Kilic, A., Kovalskyy, V., Lee, Z. P.,
Lymburner, L., Masek, J. G., McCorkel, J., Shuai, Y., Trezza, R., Vogelmann,
J., Wynne, R. H., and Zhu, Z.: Landsat-8: Science and product vision for
terrestrial global change research, Remote Sens. Environ., 145, 154–172,
<ext-link xlink:href="https://doi.org/10.1016/j.rse.2014.02.001" ext-link-type="DOI">10.1016/j.rse.2014.02.001</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib41"><label>41</label><mixed-citation>
Sims, C. and Orwin, J. F.: Snowmelt generation on a hydrologically sensitive
mountain range, Pisa Range, Central Otago, New Zealand, J. Hydrol., 50,
383–405, 2011.</mixed-citation></ref>
      <ref id="bib1.bib42"><label>42</label><mixed-citation>
Sirguey, P., Boeuf, J., Cambridge, R., and Mills, S.: Evidence of sub-optimal
photogrammetric modelling in RPAS-based aerial surveys, in: Proceedings of
the GeoCart'2016 and ICA Symposium on Cartography, edited by: Moore, A. and
Drecki, I., New Zealand Cartographic Society Inc., 91–98, 2016.</mixed-citation></ref>
      <ref id="bib1.bib43"><label>43</label><mixed-citation>Sirguey, P., Mathieu, R., and Arnaud, Y.: Subpixel monitoring of the seasonal
snow cover with MODIS at 250 m spatial resolution in the Southern Alps of
New Zealand: Methodology and accuracy assessment, Remote Sens. Environ., 113,
160–181, <ext-link xlink:href="https://doi.org/10.1016/j.rse.2008.09.008" ext-link-type="DOI">10.1016/j.rse.2008.09.008</ext-link>, 2009.</mixed-citation></ref>
      <?pagebreak page3497?><ref id="bib1.bib44"><label>44</label><mixed-citation>Sturm, M., Goldstein, M. A., and Parr, C.: Water and life from snow: A
trillion dollar science question, Water. Resour. Res., 53, 3534–3544,
<ext-link xlink:href="https://doi.org/10.1002/2017WR020840" ext-link-type="DOI">10.1002/2017WR020840</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib45"><label>45</label><mixed-citation>Treichler, D. and Kääb, A.: Snow depth from ICESat laser altimetry –
A test study in southern Norway, Remote Sens. Environ., 191, 389–401,
<ext-link xlink:href="https://doi.org/10.1016/j.rse.2017.01.022" ext-link-type="DOI">10.1016/j.rse.2017.01.022</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib46"><label>46</label><mixed-citation>
Trimble: UAS Master 7.0: Tutorial, Trimble Germany, 2015.</mixed-citation></ref>
      <ref id="bib1.bib47"><label>47</label><mixed-citation>
Trimble: Release Notes for UASMaster 8.0.0, Trimble Navigation Limited, 2016.</mixed-citation></ref>
      <ref id="bib1.bib48"><label>48</label><mixed-citation>Vander Jagt, B., Lucieer, A., Wallace, L., Turner, D., and Durand, M.: Snow
depth retrieval with UAS using photogrammetric techniques, Geosciences, 5,
264–285, <ext-link xlink:href="https://doi.org/10.3390/geosciences5030264" ext-link-type="DOI">10.3390/geosciences5030264</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib49"><label>49</label><mixed-citation>Watts, A. C., Ambrosia, V. G., and Hinkley, E. A.: Unmanned aircraft systems
in remote sensing and scientific research: Classification and considerations
of use, Remote Sens., 4, 1671–1692, <ext-link xlink:href="https://doi.org/10.3390/rs4061671" ext-link-type="DOI">10.3390/rs4061671</ext-link>, 2012.
</mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bib50"><label>50</label><mixed-citation>Webster, C. S., Kingston, D. G., and Kerr, T.: Inter-annual variation in the
topographic controls on catchment-scale snow distribution in a maritime
alpine catchment, New Zealand, Hydrol. Process., 29, 1096–1109,
<ext-link xlink:href="https://doi.org/10.1002/hyp.10224" ext-link-type="DOI">10.1002/hyp.10224</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib51"><label>51</label><mixed-citation>Winstral, A., Elder, K., and Davis, R. E.: Spatial Snow Modeling of
Wind-Redistributed Snow Using Terrain-Based Parameters, J. Hydrometeorol., 3,
524–538, <ext-link xlink:href="https://doi.org/10.1175/1525-7541(2002)003&lt;0524:SSMOWR&gt;2.0.CO;2" ext-link-type="DOI">10.1175/1525-7541(2002)003&lt;0524:SSMOWR&gt;2.0.CO;2</ext-link>, 2002.</mixed-citation></ref>
      <ref id="bib1.bib52"><label>52</label><mixed-citation>Winstral, A. and Marks, D.: Long-term snow distribution observations in a
mountain catchment: Assessing variability, time stability, and the
representativeness of an index site, Water. Resour. Res., 50, 293–305,
<ext-link xlink:href="https://doi.org/10.1002/2012WR013038" ext-link-type="DOI">10.1002/2012WR013038</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib53"><label>53</label><mixed-citation>Winstral, A., Marks, D., and Gurney, R.: Simulating wind-affected snow
accumulations at catchment to basin scales, Adv. Water Resour., 55, 64–79,
<ext-link xlink:href="https://doi.org/10.1016/j.advwatres.2012.08.011" ext-link-type="DOI">10.1016/j.advwatres.2012.08.011</ext-link>, 2013.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>Repeat mapping of snow depth across an alpine catchment with RPAS photogrammetry</article-title-html>
<abstract-html><p>Being dynamic in time and space, seasonal snow represents a difficult target
for ongoing in situ measurement and characterisation. Improved understanding
and modelling of the seasonal snowpack requires mapping snow depth at fine
spatial resolution. The potential of remotely piloted aircraft system (RPAS)
photogrammetry to resolve spatial variability of snow depth is evaluated
within an alpine catchment of the Pisa Range, New Zealand. Digital surface
models (DSMs) at 0.15&thinsp;m spatial resolution in autumn (snow-free reference)
winter (2 August 2016) and spring (10 September 2016) allowed mapping of snow
depth via DSM differencing. The consistency and accuracy of the RPAS-derived
surface was assessed by the propagation of check point residuals from the
aero-triangulation of constituent DSMs and via comparison of snow-free
regions of the spring and autumn DSMs. The accuracy of RPAS-derived snow
depth was validated with in situ snow probe measurements. Results for
snow-free areas between DSMs acquired in autumn and spring demonstrate
repeatability yet also reveal that elevation errors follow a distribution
that substantially departs from a normal distribution, symptomatic of the
influence of DSM co-registration and terrain characteristics on vertical
uncertainty. Error propagation saw snow depth mapped with an accuracy of ±0.08&thinsp;m (90&thinsp;% c.l.). This is lower than the characterization of
uncertainties on snow-free areas (±0.14&thinsp;m). Comparisons between RPAS
and in situ snow depth measurements confirm this level of performance of RPAS
photogrammetry while also highlighting the influence of vegetation on snow
depth uncertainty and bias. Semi-variogram analysis revealed that the RPAS
outperformed systematic in situ measurements in resolving fine-scale spatial
variability. Despite limitations accompanying RPAS photogrammetry, which are
relevant to similar applications of surface and volume change analysis, this
study demonstrates a repeatable means of accurately mapping snow depth for an
entire, yet relatively small, hydrological catchment (<span style="" class="text"> ∼ 0.4</span>&thinsp;km<sup>2</sup>) at very high resolution. Resolving snowpack features
associated with redistribution and preferential accumulation and ablation,
snow depth maps provide geostatistically robust insights into seasonal snow
processes, with unprecedented detail. Such data will enhance understanding of
physical processes controlling spatial distributions of seasonal snow and
their relative importance on varying spatial and temporal scales.</p></abstract-html>
<ref-html id="bib1.bib1"><label>1</label><mixed-citation>
Albani, M. and Klinkenberg, B.: A spatial filter for the removal of striping
artifacts in digital elevation models, Photogramm. Eng. Remote, 69, 755–765,
<a href="https://doi.org/10.14358/PERS.69.7.755" target="_blank">https://doi.org/10.14358/PERS.69.7.755</a>, 2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>2</label><mixed-citation>
Anderson, B. T., McNamara, J. P., Marshall, H.-P., and Flores, A. N.:
Insights into the physical processes controlling correlations between snow
distribution and terrain properties, Water. Resour. Res., 50, 4545–4563,
<a href="https://doi.org/10.1002/2013WR013714" target="_blank">https://doi.org/10.1002/2013WR013714</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>3</label><mixed-citation>
Avanzi, F., Bianchi, A., Cina, A., De Michele, C., Maschio, P., Pagliari, D.,
Passoni, D., Pinto, L., Piras, M., and Rossi, L.: Centimetric accuracy in
snow depth using unmanned aerial system photogrammetry and a multistation,
Remote Sensing, 10, 1–16, <a href="https://doi.org/10.3390/rs10050765" target="_blank">https://doi.org/10.3390/rs10050765</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>4</label><mixed-citation>
Bair, E. H., Rittger, K., Davis, R. E., Painter, T. H., and Dozier, J.:
Validating reconstruction of snow water equivalent in California's Sierra
Nevada using measurements from the NASA Airborne Snow Observatory, Water.
Resour. Res., 52, 8437–8460, <a href="https://doi.org/10.1002/2016WR018704" target="_blank">https://doi.org/10.1002/2016WR018704</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>5</label><mixed-citation>
Berthier, E., Arnaud, Y., Kumar, R., Ahmad, S., Wagnon, P., and Chevallier,
P.: Remote sensing estimates of glacier mass balances in the Himachal Pradesh
(Western Himalaya, India), Remote Sens. Environ., 108, 327–338,
<a href="https://doi.org/10.1016/j.rse.2006.11.017" target="_blank">https://doi.org/10.1016/j.rse.2006.11.017</a>, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>6</label><mixed-citation>
Bessho, K., Date, K., Hayashi, M., Ikeda, A., Imai, T., Inoue, H., Kumagai,
Y., Miyakawa, T., Murata, H., Ohno, T., Okuyama, A., Oyama, R., Sasaki, Y.,
Shimazu, Y., Shimoji, K., Sumida, Y., Suzuki, M., Taniguchi, H., Tsuchiyama,
H., Uesawa, D., Yokota, H., and Yoshida, R.: An Introduction to Himawari-8/9
– Japan's New-Generation Geostationary Meteorological Satellites, J.
Meteorol. Soc. Jpn. Ser. II, 94, 151–183, <a href="https://doi.org/10.2151/jmsj.2016-009" target="_blank">https://doi.org/10.2151/jmsj.2016-009</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>7</label><mixed-citation>
Brown, D. C.: Close-range camera calibration, Photogramm. Eng., 37, 855–866,
1971.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>8</label><mixed-citation>
Bühler, Y., Adams, M. S., Bösch, R., and Stoffel, A.: Mapping snow
depth in alpine terrain with unmanned aerial systems (UASs): potential and
limitations, The Cryosphere, 10, 1075–1088,
<a href="https://doi.org/10.5194/tc-10-1075-2016" target="_blank">https://doi.org/10.5194/tc-10-1075-2016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>9</label><mixed-citation>
Bühler, Y., Adams, M. S., Stoffel, A., and Boesch, R.: Photogrammetric
reconstruction of homogenous snow surfaces in alpine terrain applying
near-infrared UAS imagery, Int. J. Remote Sens., 38, 3135–3158,
<a href="https://doi.org/10.1080/01431161.2016.1275060" target="_blank">https://doi.org/10.1080/01431161.2016.1275060</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>10</label><mixed-citation>
Cimoli, E., Marcer, M., Vandecrux, B., Bøggild, C. E., Williams, G., and Simonsen, S. B.: Application of Low-Cost UASs and Digital
Photogrammetry for High-Resolution Snow Depth Mapping in the Arctic, Remote Sens., 9, 1142,
<a href="https://doi.org/10.3390/rs9111144" target="_blank">https://doi.org/10.3390/rs9111144</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>11</label><mixed-citation>
Clark, M. P., Hendrikx, J., Slater, A. G., Kavetski, D., Anderson, B.,
Cullen, N. J., Kerr, T., Hreinsson, E. Ö., and Woods, R. A.:
Representing spatial variability of snow water equivalent in hydrologic and
land-surface models?: A review, Water. Resour. Res., 47, W07539,
<a href="https://doi.org/10.1029/2011WR010745" target="_blank">https://doi.org/10.1029/2011WR010745</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>12</label><mixed-citation>
Conway, J. P. and Cullen, N. J.: Cloud effects on surface energy and mass
balance in the ablation area of Brewster Glacier, New Zealand, The
Cryosphere, 10, 313–328, <a href="https://doi.org/10.5194/tc-10-313-2016" target="_blank">https://doi.org/10.5194/tc-10-313-2016</a>, 2016
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>13</label><mixed-citation>
Cullen, N. J. and Conway, J. P.: A 22 month record of surface meteorology and
energy balance from the ablation zone of Brewster Glacier, New Zealand, J.
Glaciol., 61, 931–946, <a href="https://doi.org/10.3189/2015JoG15J004" target="_blank">https://doi.org/10.3189/2015JoG15J004</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>14</label><mixed-citation>
Cullen, N. J., Anderson, B., Sirguey, P., Stumm, D., Mackintosh, A., Conway,
J. P., Horgan, H. J., Dadic, R., Fitzsimons, S. J., and Lorrey, A.: An
11-year record of mass balance of Brewster Glacier, New Zealand, determined
using a geostatistical approach, J. Glaciol., 63, 199–217,
<a href="https://doi.org/10.1017/jog.2016.128" target="_blank">https://doi.org/10.1017/jog.2016.128</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>15</label><mixed-citation>
Deems, J. S., Painter, T. H., and Finnegan, D. C.: Lidar measurement of snow
depth: A review, J. Glaciol., 59, 467–479, <a href="https://doi.org/10.3189/2013JoG12J154" target="_blank">https://doi.org/10.3189/2013JoG12J154</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>16</label><mixed-citation>
De Michele, C., Avanzi, F., Passoni, D., Barzaghi, R., Pinto, L., Dosso, P.,
Ghezzi, A., Gianatti, R., and Della Vedova, G.: Using a fixed-wing UAS to map
snow depth distribution: an evaluation at peak accumulation, The Cryosphere,
10, 511–522, <a href="https://doi.org/10.5194/tc-10-511-2016" target="_blank">https://doi.org/10.5194/tc-10-511-2016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>17</label><mixed-citation>
Dozier, J.: Spectral signature of alpine snow cover from the Landsat Thematic
Mapper, Remote Sens. Environ., 22, 9–22, 1989.
</mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>18</label><mixed-citation>
Ebner, H. and Fritz, L.: Aerotriangulation, in: Manual of Photogrammetry, 4th
edn., edited by: Slama, C. C., American Society of Photogrammetry, Falls
Church, 453–518, 1980.
</mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>19</label><mixed-citation>
Fernandes, R., Prevost, C., Canisius, F., Leblanc, S. G., Maloley, M., Oakes,
S., Holman, K., and Knudby, A.: Monitoring snow depth change across a range
of landscapes with ephemeral snow packs using Structure from Motion applied
to lightweight unmanned aerial vehicle videos, The Cryosphere Discuss.,
<a href="https://doi.org/10.5194/tc-2018-82" target="_blank">https://doi.org/10.5194/tc-2018-82</a>, in review, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>20</label><mixed-citation>
Hall, D. K., Crawford, C. J., Di Girolamo, N. E., Riggs, G. A., and Foster,
J. L.: Detection of earlier snowmelt in the Wind River Range, Wyoming, using
Landsat imagery, 1972–2013, Remote Sens. Environ., 162, 45–54,
<a href="https://doi.org/10.1016/j.rse.2015.01.032" target="_blank">https://doi.org/10.1016/j.rse.2015.01.032</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>21</label><mixed-citation>
Hall, D. K., Riggs, G. A., Salomonson, V. V, Di Girolamo, N. E., and Bayr, K.
J.: MODIS snow-cover products, Remote Sens. Environ., 83, 181–194,
<a href="https://doi.org/10.1016/S0034-4257(02)00095-0" target="_blank">https://doi.org/10.1016/S0034-4257(02)00095-0</a>, 2002.
</mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>22</label><mixed-citation>
Harder, P., Schirmer, M., Pomeroy, J., and Helgason, W.: Accuracy of snow
depth estimation in mountain and prairie environments by an unmanned aerial
vehicle, The Cryosphere, 10, 2559–2571,
<a href="https://doi.org/10.5194/tc-10-2559-2016" target="_blank">https://doi.org/10.5194/tc-10-2559-2016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>23</label><mixed-citation>
Hirschmuller, H.: Accurate and efficient stereo processing by semi-global
matching and mutual information, IEEE. T. Pattern Anal., 2, 807–814,
<a href="https://doi.org/10.1109/CVPR.2005.56" target="_blank">https://doi.org/10.1109/CVPR.2005.56</a>, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>24</label><mixed-citation>
James, L. A., Hodgson, M. E., Ghoshal, S., and Latiolais, M. M.: Geomorphic
change detection using historic maps and DEM differencing: The temporal
dimension of geospatial analysis, Geomorphology, 137, 181–198,
<a href="https://doi.org/10.1016/j.geomorph.2010.10.039" target="_blank">https://doi.org/10.1016/j.geomorph.2010.10.039</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>25</label><mixed-citation>
Kääb, A.: Remote Sensing of Mountain Glaciers and Permafrost Creep.
Zürich: Geographisches Institut der Universiturich, Zürich, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>26</label><mixed-citation>
Kerr, T., Clark, M., Hendrikx, J., and Anderson, B.: Snow distribution in a
steep mid-latitude alpine catchment, Adv. Water Resour., 55, 17–24,
<a href="https://doi.org/10.1016/j.advwatres.2012.12.010" target="_blank">https://doi.org/10.1016/j.advwatres.2012.12.010</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>27</label><mixed-citation>
Kinar, N. J. and Pomeroy, J. W.: Measurement of the physical properties of
the snowpack, Rev. Geophys., 53, 481–544, <a href="https://doi.org/10.1002/2015RG000481" target="_blank">https://doi.org/10.1002/2015RG000481</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>28</label><mixed-citation>
Lemmetyinen, J., Derksen, C., Rott, H., Macelloni, G., King, J., Schneebeli,
M., Wiesmann, A., Leppänen, L., Kontu, A., and Pulliainen, J.:
Retrieval of Effective Correlation Length and Snow Water Equivalent from
Radar and Passive Microwave Measurements, Remote Sens., 10, 170,
<a href="https://doi.org/10.3390/rs10020170" target="_blank">https://doi.org/10.3390/rs10020170</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>29</label><mixed-citation>
Lindeberg, T.: Image Matching Using Generalized Scale-Space Interest Points,
J. Math. Imaging Vis., 52, 3–36, <a href="https://doi.org/10.1007/s10851-014-0541-0" target="_blank">https://doi.org/10.1007/s10851-014-0541-0</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>30</label><mixed-citation>
Linder, W.: Digital Photogrammetry: A Practical Course, 4th edn., Heidelberg,
Springer, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>31</label><mixed-citation>
Malenovský, Z., Rott, H., Cihlar, J., Schaepman, M. E.,
García-Santos, G., Fernandes, R., and Berger, M.: Sentinels for science:
Potential of Sentinel-1, -2, and -3 missions for scientific observations of
ocean, cryosphere, and land, Remote Sens. Environ., 120, 91–101,
<a href="https://doi.org/10.1016/j.rse.2011.09.026" target="_blank">https://doi.org/10.1016/j.rse.2011.09.026</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>32</label><mixed-citation>
Mankin, J. S., Viviroli, D., Singh, D., Hoekstra, A. Y., and Diffenbaugh, N.
S.: The potential for snow to supply human water demand in the present and
future, Environ. Res. Lett., 10, 114016, <a href="https://doi.org/10.1088/1748-9326/10/11/114016" target="_blank">https://doi.org/10.1088/1748-9326/10/11/114016</a>,
2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>33</label><mixed-citation>
Marti, R., Gascoin, S., Berthier, E., de Pinel, M., Houet, T., and Laffly,
D.: Mapping snow depth in open alpine terrain from stereo satellite imagery,
The Cryosphere, 10, 1361–1380, <a href="https://doi.org/10.5194/tc-10-1361-2016" target="_blank">https://doi.org/10.5194/tc-10-1361-2016</a>,
2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>34</label><mixed-citation>
Nolan, M., Larsen, C., and Sturm, M.: Mapping snow depth from manned aircraft
on landscape scales at centimeter resolution using structure-from-motion
photogrammetry, The Cryosphere, 9, 1445–1463,
<a href="https://doi.org/10.5194/tc-9-1445-2015" target="_blank">https://doi.org/10.5194/tc-9-1445-2015</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>35</label><mixed-citation>
Nolin, A. W. and Dozier, J.: Estimating snow grain size using AVIRIS data,
Remote Sens. Environ., 44, 231–238, <a href="https://doi.org/10.1016/0034-4257(93)90018-S" target="_blank">https://doi.org/10.1016/0034-4257(93)90018-S</a>, 1993.
</mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>36</label><mixed-citation>
Nuth, C. and Kääb, A.: Co-registration and bias corrections of
satellite elevation data sets for quantifying glacier thickness change, The
Cryosphere, 5, 271–290, <a href="https://doi.org/10.5194/tc-5-271-2011" target="_blank">https://doi.org/10.5194/tc-5-271-2011</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>37</label><mixed-citation>
Painter, T. H., Berisford, D. F., Boardman, J. W., Bormann, K. J., Deems, J.
S., Gehrke, F., Hedrick, A., Joyce, M., Laidlaw, R., Marks, D., Mattmann, C.,
McGurk, B., Ramirez, P., Richardson, M., Skiles, S. M. K., Seidel, F. C., and
Winstral, A.: The Airborne Snow Observatory: Fusion of scanning lidar,
imaging spectrometer, and physically-based modeling for mapping snow water
equivalent and snow albedo, Remote Sens. Environ., 184, 139–152,
<a href="https://doi.org/10.1016/j.rse.2016.06.018" target="_blank">https://doi.org/10.1016/j.rse.2016.06.018</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>38</label><mixed-citation>
Revuelto, J., Vionnet, V., López-Moreno, J. I., Lafaysse, M., and Morin,
S.: Combining snowpack modeling and terrestrial laser scanner observations
improves the simulation of small scale snow dynamics, J. Hydrol., 533,
291–307, <a href="https://doi.org/10.1016/j.jhydrol.2015.12.015" target="_blank">https://doi.org/10.1016/j.jhydrol.2015.12.015</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>39</label><mixed-citation>
Rittger, K., Painter, T. H., and Dozier, J. : Assessment of methods for
mapping snow cover from MODIS, Adv. Water Resour., 51, 367–380,
<a href="https://doi.org/10.1016/j.advwatres.2012.03.002" target="_blank">https://doi.org/10.1016/j.advwatres.2012.03.002</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>40</label><mixed-citation>
Roy, D. P., Wulder, M. A., Loveland, T. R., C.E., W., Allen, R. G., Anderson,
M. C., Helder, D., Irons, J. R., Johnson, D. M., Kennedy, R., Scambos, T. A.,
Schaaf, C. B., Schott, J. R., Sheng, Y., Vermote, E. F., Belward, A. S.,
Bindschadler, R., Cohen, W. B., Gao, F., Hipple, J. D., Hostert, P.,
Huntington, J., Justice, C. O., Kilic, A., Kovalskyy, V., Lee, Z. P.,
Lymburner, L., Masek, J. G., McCorkel, J., Shuai, Y., Trezza, R., Vogelmann,
J., Wynne, R. H., and Zhu, Z.: Landsat-8: Science and product vision for
terrestrial global change research, Remote Sens. Environ., 145, 154–172,
<a href="https://doi.org/10.1016/j.rse.2014.02.001" target="_blank">https://doi.org/10.1016/j.rse.2014.02.001</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>41</label><mixed-citation>
Sims, C. and Orwin, J. F.: Snowmelt generation on a hydrologically sensitive
mountain range, Pisa Range, Central Otago, New Zealand, J. Hydrol., 50,
383–405, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>42</label><mixed-citation>
Sirguey, P., Boeuf, J., Cambridge, R., and Mills, S.: Evidence of sub-optimal
photogrammetric modelling in RPAS-based aerial surveys, in: Proceedings of
the GeoCart'2016 and ICA Symposium on Cartography, edited by: Moore, A. and
Drecki, I., New Zealand Cartographic Society Inc., 91–98, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>43</label><mixed-citation>
Sirguey, P., Mathieu, R., and Arnaud, Y.: Subpixel monitoring of the seasonal
snow cover with MODIS at 250&thinsp;m spatial resolution in the Southern Alps of
New Zealand: Methodology and accuracy assessment, Remote Sens. Environ., 113,
160–181, <a href="https://doi.org/10.1016/j.rse.2008.09.008" target="_blank">https://doi.org/10.1016/j.rse.2008.09.008</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>44</label><mixed-citation>
Sturm, M., Goldstein, M. A., and Parr, C.: Water and life from snow: A
trillion dollar science question, Water. Resour. Res., 53, 3534–3544,
<a href="https://doi.org/10.1002/2017WR020840" target="_blank">https://doi.org/10.1002/2017WR020840</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>45</label><mixed-citation>
Treichler, D. and Kääb, A.: Snow depth from ICESat laser altimetry –
A test study in southern Norway, Remote Sens. Environ., 191, 389–401,
<a href="https://doi.org/10.1016/j.rse.2017.01.022" target="_blank">https://doi.org/10.1016/j.rse.2017.01.022</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>46</label><mixed-citation>
Trimble: UAS Master 7.0: Tutorial, Trimble Germany, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>47</label><mixed-citation>
Trimble: Release Notes for UASMaster 8.0.0, Trimble Navigation Limited, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>48</label><mixed-citation>
Vander Jagt, B., Lucieer, A., Wallace, L., Turner, D., and Durand, M.: Snow
depth retrieval with UAS using photogrammetric techniques, Geosciences, 5,
264–285, <a href="https://doi.org/10.3390/geosciences5030264" target="_blank">https://doi.org/10.3390/geosciences5030264</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib49"><label>49</label><mixed-citation>
Watts, A. C., Ambrosia, V. G., and Hinkley, E. A.: Unmanned aircraft systems
in remote sensing and scientific research: Classification and considerations
of use, Remote Sens., 4, 1671–1692, <a href="https://doi.org/10.3390/rs4061671" target="_blank">https://doi.org/10.3390/rs4061671</a>, 2012.

</mixed-citation></ref-html>
<ref-html id="bib1.bib50"><label>50</label><mixed-citation>
Webster, C. S., Kingston, D. G., and Kerr, T.: Inter-annual variation in the
topographic controls on catchment-scale snow distribution in a maritime
alpine catchment, New Zealand, Hydrol. Process., 29, 1096–1109,
<a href="https://doi.org/10.1002/hyp.10224" target="_blank">https://doi.org/10.1002/hyp.10224</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib51"><label>51</label><mixed-citation>
Winstral, A., Elder, K., and Davis, R. E.: Spatial Snow Modeling of
Wind-Redistributed Snow Using Terrain-Based Parameters, J. Hydrometeorol., 3,
524–538, <a href="https://doi.org/10.1175/1525-7541(2002)003&lt;0524:SSMOWR&gt;2.0.CO;2" target="_blank">https://doi.org/10.1175/1525-7541(2002)003&lt;0524:SSMOWR&gt;2.0.CO;2</a>, 2002.
</mixed-citation></ref-html>
<ref-html id="bib1.bib52"><label>52</label><mixed-citation>
Winstral, A. and Marks, D.: Long-term snow distribution observations in a
mountain catchment: Assessing variability, time stability, and the
representativeness of an index site, Water. Resour. Res., 50, 293–305,
<a href="https://doi.org/10.1002/2012WR013038" target="_blank">https://doi.org/10.1002/2012WR013038</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib53"><label>53</label><mixed-citation>
Winstral, A., Marks, D., and Gurney, R.: Simulating wind-affected snow
accumulations at catchment to basin scales, Adv. Water Resour., 55, 64–79,
<a href="https://doi.org/10.1016/j.advwatres.2012.08.011" target="_blank">https://doi.org/10.1016/j.advwatres.2012.08.011</a>, 2013.
</mixed-citation></ref-html>--></article>
