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  <front>
    <journal-meta>
<journal-id journal-id-type="publisher">NHESS</journal-id>
<journal-title-group>
<journal-title>Natural Hazards and Earth System Sciences</journal-title>
<abbrev-journal-title abbrev-type="publisher">NHESS</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Nat. Hazards Earth Syst. Sci.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1684-9981</issn>
<publisher><publisher-name>Copernicus Publications</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>

    <article-meta>
      <article-id pub-id-type="doi">10.5194/nhess-17-225-2017</article-id><title-group><article-title>Dealing with deep uncertainties in landslide modelling for disaster risk
reduction under climate change</article-title>
      </title-group><?xmltex \runningtitle{Dealing with deep uncertainties in landslide modelling}?><?xmltex \runningauthor{S. Almeida et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Almeida</surname><given-names>Susana</given-names></name>
          <email>susana.almeida@bristol.ac.uk</email>
        <ext-link>https://orcid.org/0000-0003-3539-5578</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Holcombe</surname><given-names>Elizabeth Ann</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8517-6130</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Pianosi</surname><given-names>Francesca</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1516-2163</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Wagener</surname><given-names>Thorsten</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3881-5849</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Department of Civil Engineering, University of Bristol, Bristol, BS8
1TR, UK</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Cabot Institute, University of Bristol, Bristol, BS8 1TR, UK</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Susana Almeida (susana.almeida@bristol.ac.uk)</corresp></author-notes><pub-date><day>21</day><month>February</month><year>2017</year></pub-date>
      
      <volume>17</volume>
      <issue>2</issue>
      <fpage>225</fpage><lpage>241</lpage>
      <history>
        <date date-type="received"><day>18</day><month>August</month><year>2016</year></date>
           <date date-type="rev-request"><day>12</day><month>September</month><year>2016</year></date>
           <date date-type="accepted"><day>31</day><month>January</month><year>2017</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under a Creative Commons Attribution 3.0 Unported License. To view a copy of this license, visit <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by/3.0/">http://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://nhess.copernicus.org/articles/.html">This article is available from https://nhess.copernicus.org/articles/.html</self-uri>
<self-uri xlink:href="https://nhess.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://nhess.copernicus.org/articles/.pdf</self-uri>


      <abstract>
    <p>Landslides have large negative economic and societal
impacts, including loss of life and damage to infrastructure. Slope
stability assessment is a vital tool for landslide risk management, but high
levels of uncertainty often challenge its usefulness. Uncertainties are
associated with the numerical model used to assess slope stability and its
parameters, with the data characterizing the geometric, geotechnic and
hydrologic properties of the slope, and with hazard triggers (e.g.
rainfall). Uncertainties associated with many of these factors are also
likely to be exacerbated further by future climatic and socio-economic
changes, such as increased urbanization and resultant land use change. In
this study, we illustrate how numerical models can be used to explore the
uncertain factors that influence potential future landslide hazard using a
bottom-up strategy. Specifically, we link the Combined Hydrology And
Stability Model (CHASM) with sensitivity analysis and Classification And
Regression Trees (CART) to identify critical thresholds in slope properties
and climatic (rainfall) drivers that lead to slope failure. We apply our
approach to a slope in the Caribbean, an area that is naturally susceptible
to landslides due to a combination of high rainfall rates, steep slopes, and
highly weathered residual soils. For this particular slope, we find that
uncertainties regarding some slope properties (namely thickness and
effective cohesion of topsoil) are as important as the uncertainties
related to future rainfall conditions. Furthermore, we show that 89 % of
the expected behaviour of the studied slope can be characterized based on
only two variables – the ratio of topsoil thickness to cohesion and the
ratio of rainfall intensity to duration.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>Landslide hazards and their impacts on human lives, economies and
infrastructure present a growing challenge globally (Dai et al., 2002).
Approximately 300 million people worldwide are estimated to be exposed to
landslides  (Dilley et al., 2005) with the greatest absolute
economic losses experienced in Europe and the overwhelming majority of
injuries and fatalities in Asia, South and Central America and the Caribbean
(UNU, 2006; Petley, 2012). The susceptibility of slopes to landslides is
known to increase with urban development activities such as vegetation
removal, construction of earthworks (cuts and fills), buildings and roads,
and altered drainage  (Smyth and Royle, 2000). Similarly, another
major factor affecting landslide occurrence is rainfall event intensity.
Climate change is projected to increase the occurrence of extreme
precipitation events in many regions worldwide, and therefore may also have
important implications for the frequency of rainfall-triggered landslides
(Ibsen and Brunsden, 1996; Borgatti and Soldati, 2010; Crozier, 2010;
Kendon et al., 2014).</p>
      <p>Landslide hazard assessment forms the basis for disaster risk reduction
decisions such as the design of physical landslide hazard mitigation
measures, planning controls and early warning systems for hazard avoidance,
vulnerability reduction (resilience) approaches, or insurance. The spatial
scale and the purpose of the hazard assessment, as well as the data
available, determine which methods or slope stability models can be applied.
Available assessment methods include inventory-based susceptibility mapping
or regional forecasting, and statistical, heuristic and physically based
modelling (either spatially distributed or site specific)
(Soeters and van Westen, 1996; Dai and Lee, 2001). These
methods require data in some or all of the following categories: (i) <italic>inventories</italic> of past landslide locations, types and triggers;
(ii) <italic>preparatory factors</italic> determining the inherent susceptibility of a
slope to landslides, such as slope geometry (slope angles and heights,
convergence/divergence, soil and parent material depths), the geotechnical
and hydrological properties of slope material, and land-use; and (iii) <italic>triggering factors</italic> such as rainfall intensity, duration and
frequency.</p>
      <p>The challenge of acquiring these data in sufficient quantity, quality and
resolution is currently hindering the production of “actionable” landslide
hazard information for decision makers      (Aitsi-Selmi et
al., 2015). With the exception of particular regions such as Hong Kong,
there is generally a lack of systematic landslide data collection even in
the most landslide-prone countries  (Corominas et al., 2014). Especially
high-frequency, low-intensity events may be missed out due to their small
spatial scale and impact. Existing databases are therefore often spatially
and temporally biased or incomplete  (for discussion about landslide
inventories, the reader is referred to Malamud et al., 2004). Lack of data
on past landslides limits our ability to build inventory-based and
statistical models for predicting likely locations, timing or impacts of
future landslides. In comparison, the advantage of physically based slope
stability models is their smaller reliance on observations of past events
and an ability to mechanistically represent the preparatory and triggering
processes driving slope failure. This latter characteristic also allows them
to assess the impact of higher intensity rainfall events than a region might
have experienced in the past, or of possible urbanization scenarios.
Landslide hazard researchers and civil engineers currently employ
physically based models to diagnose existing stability conditions, design
new slopes and determine landslide probabilities. Nevertheless, when using
physically based models to assess slope stability it is important to note
that care should always be taken to ensure that the selected model
adequately represents the key processes determining slope stability for the
chosen study site.</p>
      <p>The mechanistic ability of physically based models comes at a cost. The
detailed representation of slope processes in the model requires detailed
information on slope properties such as soils and topography. The more
complex, high-resolution and comprehensive the representation of slope
processes in the model, the more data regarding the physical site
characteristics are required. Parsimonious models are therefore often
selected that are consistent with data availability and with the required
level of process representation. Even then, data are rarely available in
sufficient detail, and this introduces uncertainty into the model
parameterization. Sources of uncertainty include those associated with
slopes geometries and material strata depths  (Lumb, 1975; Corominas et
al., 2014), soil properties  (Cho, 2007; Beven and Germann, 2013), and a
limited understanding of how measured variables relate to model parameters
(the commensurability issue – Beven, 1989; Wagener and Gupta, 2005;
Beven, 2006). The lack in accuracy of forcing boundary conditions, such as
the temporal and areal variability of historical rainfall, introduces
further uncertainty that needs to be considered  (Minder et al., 2009; von
Ruette et al., 2014). Studies have assessed the impact of uncertainties
associated with such models  (Hall et al., 2004; Arnone et al., 2016) for
both site-specific and spatially distributed landslide hazard predictions –
though such information is rarely used to support risk reduction
decision-making.</p>
      <p>Additional uncertainty is introduced by the poorly known potential
implications of future climate or land use change. Such uncertainties are
different from the ones listed above, because they cannot be easily
characterized by probability distributions that different experts could
agree on, i.e. they are often called <italic>deep uncertainties</italic>  (Bankes,
2002; Lempert et al., 2003; Stein and Stein, 2013). The standard approach to
dealing with deep uncertainties is through scenario-led strategies, also
called top-down approaches. In these approaches, climate change projections
of a general circulation model (GCM) are downscaled to derive local rainfall
intensities and frequencies, as well as other climatic variables. These
scenarios are then used to drive a slope stability model in a top-down
manner  (Collison et al., 2000; Melchiorre and Frattini, 2012). Studies
that have attempted to quantify the uncertainty in the estimation of climate
variables derived in this manner have found them to be prohibitively large
in many cases  (e.g. Collins et al., 2012; Ning et al., 2012). As a
result, one usually finds that the uncertainty in the final predicted
impacts is also quite large and that a wide range of possible outcomes is
feasible, which is of little practical use for decision-making or for
identifying an “optimal” management solution  (Bankes, 2002; Wilby and
Dessai, 2010; Hallegatte et al., 2012; Herman et al., 2014). To reduce the
range of possible outcomes, a smaller subset of the many possible potential
future scenarios can be selected. However, this approach is problematic as
arbitrary selection of scenarios or of the downscaled simulations will
undermine the credibility of the results   (e.g. Kim et al.,
2015).</p>
      <p>Given that such deep uncertainties are unavoidable, a shift from
“top-down” to “bottom-up” approaches has been suggested to derive
actionable information for decision makers  (Groves and Lempert, 2007;
Wilby and Dessai, 2010; Singh et al., 2014; Ray and Brown, 2015). While
“top-down” approaches simulate system behaviour under potential future
conditions in a predictive manner (e.g. to estimate probability of slope
failure given one or more climate change scenarios), “bottom-up”
approaches focus on exploring the vulnerabilities of the system, i.e. on
finding those combinations of factors values that would produce unwanted
outcomes (e.g. slope failure). Bottom-up approaches are therefore
stakeholder driven since they start with the stakeholder who has to define
what threshold separates acceptable from unwanted outcomes. A wide range of
possible values of the uncertain factors can then be considered (i.e.
propagated through the model) and mapped onto the regions of vulnerability
of the output space. We can use statistical data-mining algorithms to
quantify the link between inputs and outputs, i.e. the mapping stage.
Commonly used algorithms to implement the mapping required for bottom-up
approaches include Friedman and Fisher's (1999) Patient Rule
Induction Method (PRIM) and Classification and Regression Trees (CART)
developed by   Breiman et al. (1984). The bottom-up strategy is very
similar to the problem of mapping in Global Sensitivity Analysis, where one
tries to understand which parts of the input factor space produce a
particular model output, for example output values exceeding a certain
threshold  (e.g. Saltelli et al., 2008; Pianosi et al., 2016).</p>
      <p>In this study, we apply a bottom-up approach to a landslide hazard
assessment model in order to address the following three questions:
<list list-type="order"><list-item>
      <p>Can we identify the dominant preparatory and triggering factors driving
slope instability (i.e. slope geometry, geotechnical and hydrological
parameters or rainfall drivers) in data-scarce locations?</p></list-item><list-item>
      <p>Does deep uncertainty in future landslide triggers, such as climate change,
exceed other uncertainties, such as those related to slope properties, in
determining our ability to predict slope failure?</p></list-item><list-item>
      <p>What are the implications of uncertainty for data acquisition and assessment
of future hazard?</p></list-item></list></p>
</sec>
<sec id="Ch1.S2">
  <title>Model and study site</title>
      <p>We select a physically based model and study site to represent the landslide
hazard assessment and risk reduction challenges typical of data-scarce and
resource-limited locations (Fig. 1). The model is representative of those
used by civil engineers and slope stability modellers. It can be
parameterized using study site data and has a track-record of successful
application in data-scarce locations (references provided in Sect. 2.2). The
methodology we develop around this case study is transferable to other
locations and other types of physically based slope stability assessment
models.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p>Typical informal housing on a landslide-prone slope in the eastern
Caribbean (photograph by Holcombe, 2007).</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/17/225/2017/nhess-17-225-2017-f01.jpg"/>

      </fig>

<sec id="Ch1.S2.SS1">
  <title>An urban study site in the humid tropics</title>
      <p>The selected study site is situated on the lower slope of a ravine on a
hillside in the city of Castries, Saint Lucia (eastern Caribbean), in which
informal construction of houses has led to increased landslide risk. The
slope section is approximately 50 m in height and has an overall angle of
about 30<inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. The material strata comprise up to 6 m of residual
soils overlying a similar depth of decomposed rock  (weathering
grades III–IV; after GEO, 1988) overlying volcanic bedrock. As is typical
for the humid tropics, the dominant landslide trigger in the Caribbean is
rainfall        (Lumb, 1975; De Graff et al., 1989), and
shallow rotational slides are the most common type of landslide in the deep
weathered tropical residual soils on the mid to lower slopes of steep
hillsides (Migon, 2010). Such locations tend to be the only land
available to the most socio-economically vulnerable families, so even small
landslide events can have a high societal impact (UNISDR, 2015). These
“everyday disasters” are also increasingly seen as indicators of risk
accumulation (low disaster resilience) and represent a potential hindrance
to national economic development     (Bull-Kamanga et al.,
2003).</p>
      <p>In 2011 a landslide hazard reduction project was implemented at the study
site location using a community-based approach – Management of Slope
Stability in Communities (Mossaic) – developed by
Anderson and Holcombe (2006). At the time, estimates of
geotechnical, hydrological and geometrical parameters for the study site
were derived from a combination of: topographic maps, site surveys,
interviews with residents to estimate soil strata depths and weathering
grades (based on their experiences of excavating the soils to construct
house foundations), elicitation of local engineering knowledge of soils, and
information from shear box and ring infiltrometer testing of similar soils
in Saint Lucia. Soil properties were also benchmarked against extensive
triaxial and permeameter test data for similar undisturbed tropical residual
soils in Hong Kong  (GCO, 1982).</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>A physically based model for rainfall-triggered landslides</title>
      <p>Deterministic physically based modelling of slope stability has previously
been carried out at the study site using the Combined Hydrology And slope
Stability Model (CHASM) to diagnose landslide drivers and estimate the
benefit–cost ratio of landslide mitigation  (Holcombe et al., 2012). In a
validation exercise in Hong Kong CHASM was shown to be numerically robust
and capable of correctly classifying 78 % of failed slopes and 68 % of
stable slopes (i.e. true positives, TP <inline-formula><mml:math id="M2" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 78 %; false positives,
FP <inline-formula><mml:math id="M3" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 22 %; true negatives, TN <inline-formula><mml:math id="M4" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 68 %; false negatives, FN <inline-formula><mml:math id="M5" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 32 %) for
a specified rainfall event  (Anderson, 1990), corresponding to an
accuracy of 72.5 % ((TP <inline-formula><mml:math id="M6" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> TN) <inline-formula><mml:math id="M7" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> (total observed failed slopes <inline-formula><mml:math id="M8" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> total
observed stable slopes)). This is comparable with, or exceeds, the
performance of spatially distributed GIS-based models such as a statistical
analysis of landslide susceptibility in Central America (using the Hurricane
Mitch landslide inventory) that attained an accuracy of 68 %
(Kirschbaum et al., 2012); and a physically based infinite-slope analysis
(using modified SINMAP) in the data-rich region of Calabria, Italy, that
achieved a maximum TP rate of 71 % and accuracy of 72 %
(Formetta et al., 2014, p. 639). This level of accuracy
might typically enable disaster risk managers and practitioners (such as
engineers and planners) to identify slopes exhibiting potentially high
hazard and prioritize further investigation and/or risk reduction
accordingly. CHASM has been extensively used by slope stability researchers
and practitioners to assess landslide hazards along roads and in urban and
rural areas, and to propose appropriate mitigation in Malaysia, Indonesia,
the eastern Caribbean, United Kingdom and New Zealand  (Anderson et al.,
1997; Lloyd et al., 2001; Wilkinson et al., 2002a, b).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p>Conceptual model of the experimental slope. CHASM uses the Bishop
method of slices to perform slope stability analysis, which involves a
numerical search for the slip surface.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/17/225/2017/nhess-17-225-2017-f02.pdf"/>

        </fig>

      <p>A brief overview of CHASM is given here – full descriptions of the
numerical scheme and principal equations can be found in Anderson
and Lloyd (1991) and  Wilkinson et al. (2002b). CHASM
represents the slope cross-section as a regular two-dimensional mesh of
columns and cells with geotechnical and hydrological parameters specified
for each soil type (Fig. 2). Initial hydrological conditions are the matric
suctions (negative pore pressure) in the top cells of each column and the
water table position. Subsequent dynamic forcing conditions are rainfall
events of specified intensities and durations imposed on the top cells. For
each hydrological time step (usually 10–60 s) a forward-explicit
finite difference scheme is used to solve Richards' equation
(Richards, 1931) and Darcy's law  (Darcy, 1856) for
rainfall infiltration, unsaturated and saturated groundwater flows. Cell
moisture conditions, pressure heads and unsaturated hydraulic conductivities
are updated at each time step using soil moisture characteristic curves and
the Millington–Quirk procedure  (Millington and Quirk, 1959). At the
end of each simulation hour the pressure head fields are used to calculate
pore water pressures (positive and negative) for input to a two-dimensional
limit equilibrium method (LEM) calculation of slope stability. In LEM
analysis the slope factor of safety (<inline-formula><mml:math id="M9" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula>) is calculated as the ratio of
destabilising forces to resisting forces for a potential landslide slip
surface location, such that <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mi>F</mml:mi><mml:mi mathvariant="italic">&lt;</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> indicates failure. In CHASM either
Bishop's simplified circular method of slices  (Bishop, 1955) or
Janbu's non-circular method  (Janbu, 1954) is implemented using an
automated search algorithm to identify the location of the slip surface with
the minimum value of <inline-formula><mml:math id="M11" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> for that hour.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Methods</title>
      <p>Our study aims to advance understanding of the critical uncertainties
driving rainfall-triggered landslides. To this end, the simulation model,
CHASM, is run with 10 000 different combinations of values for the 28
uncertain input factors. Such combinations are generated via random sampling
from a set of probability distributions that characterize the uncertainty in
the slope properties, and uniform distributions with very wide ranges for
the intensity and duration of future rainfall events, so as to
reproduce the (practically) unconstrained nature of “deep” uncertainties.
Model simulations are performed using the BlueCrystal Phase 3
high-performance cluster at the University of Bristol, which contains 16 <inline-formula><mml:math id="M12" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.6 GHz
Sandy Bridge cores. Each simulation is classified as corresponding to
stable or unstable slope based on the resulting slope factor of safety, <inline-formula><mml:math id="M13" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula>
(model output) being above or below 1 at any stage during the simulated time
period. We first perform a preliminary visual analysis of the simulations to
identify influential factors that lead to slope failure. We then apply
Classification And Regression Trees (CART) to formally determine
combinations of factors and their thresholds values for which the model
predicts slope failure in a bottom-up strategy. The Matlab SAFE toolbox
(Pianosi et al., 2015) and the CART functions in the Matlab
Statistics and Machine Learning Toolbox  (Mathworks, 2015) are used to
perform our analysis.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p>CHASM parameters and their distributions.</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>  
         <oasis:entry colname="col1">Parameter</oasis:entry>  
         <oasis:entry colname="col2">Symbol/Unit</oasis:entry>  
         <oasis:entry rowsep="1" namest="col3" nameend="col5" align="center">Values </oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3">Grade V–VI<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4">Grade III–IV<inline-formula><mml:math id="M26" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5">Grade I–II<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3">residual soil (0)</oasis:entry>  
         <oasis:entry colname="col4">weathered material (1)</oasis:entry>  
         <oasis:entry colname="col5">bedrock (2)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Slope height</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M28" display="inline"><mml:mi>H</mml:mi></mml:math></inline-formula> (m)</oasis:entry>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M29" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> (48, 49)</oasis:entry>  
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Slope angle</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M30" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> (degrees)</oasis:entry>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M31" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> (27, 30)</oasis:entry>  
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Thickness of strata</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (m)</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M33" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> (2, 6)</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M34" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> (2, 6)</oasis:entry>  
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Depth of initial water table<inline-formula><mml:math id="M35" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col2">DWT (%)</oasis:entry>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M36" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> (60, 95)</oasis:entry>  
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Saturated hydraulic conductivity</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (m s<inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3">ln <italic>N</italic> (<inline-formula><mml:math id="M39" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>11.055, 0.373)</oasis:entry>  
         <oasis:entry colname="col4">ln <italic>N</italic> (<inline-formula><mml:math id="M40" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>13.357, 0.373)</oasis:entry>  
         <oasis:entry colname="col5">1 <inline-formula><mml:math id="M41" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M42" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Saturated soil moisture content</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (m<inline-formula><mml:math id="M44" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"><italic>N</italic> (0.413, 0.074)</oasis:entry>  
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Van Genuchten suction–moisture curve <inline-formula><mml:math id="M46" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M47" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> (m<inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4">ln <italic>N</italic> (1.264, 1.076)</oasis:entry>  
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Van Genuchten suction–moisture curve <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:msup><mml:mi>n</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M50" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> (–)</oasis:entry>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4">ln <italic>N</italic> (0.364, 0.358)</oasis:entry>  
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Residual soil moisture content<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">d</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (m<inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4">ln <italic>N</italic> (<inline-formula><mml:math id="M55" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.974, 0.376)</oasis:entry>  
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Initial surface suction</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">Ψ</mml:mi><mml:mi mathvariant="normal">init</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M57" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M58" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.5, <inline-formula><mml:math id="M59" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.5)</oasis:entry>  
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Dry unit weight<inline-formula><mml:math id="M60" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">e</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (kN m<inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math id="M63" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> (16, 18)</oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math id="M64" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> (18, 20)</oasis:entry>  
         <oasis:entry colname="col5">23</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Effective cohesion<inline-formula><mml:math id="M65" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">f</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msup><mml:mi>c</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> (kPa)</oasis:entry>  
         <oasis:entry colname="col3"><italic>N</italic> (8, 3.3)</oasis:entry>  
         <oasis:entry colname="col4"><italic>N</italic> (25, 1.7)</oasis:entry>  
         <oasis:entry colname="col5">80</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Effective friction angle</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">ϕ</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> (degrees)</oasis:entry>  
         <oasis:entry colname="col3"><italic>N</italic> (25, 1.7)</oasis:entry>  
         <oasis:entry colname="col4"><italic>N</italic> (35, 3.3)</oasis:entry>  
         <oasis:entry colname="col5">60</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p><inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula>  Weathering grades defined according to
GEO (1988).
<?xmltex \hack{\\}?><inline-formula><mml:math id="M15" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula>  Water table height is defined as a percentage of slope height measured to the toe of the slope. <?xmltex \hack{\\}?><inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">c</mml:mi></mml:msup></mml:math></inline-formula>  <inline-formula><mml:math id="M17" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> is always greater than 1. <?xmltex \hack{\\}?><inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mi mathvariant="normal">d</mml:mi></mml:msup><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is always greater than 0; <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> greater than <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. <?xmltex \hack{\\}?><inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mi mathvariant="normal">e</mml:mi></mml:msup><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the saturated unit weight. <?xmltex \hack{\\}?><inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">f</mml:mi></mml:msup></mml:math></inline-formula>  Effective cohesion is always greater than 0. <?xmltex \hack{\\}?><inline-formula><mml:math id="M24" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula>, uniform distribution; <italic>N</italic>, normal distribution; ln <italic>N</italic>, log-normal distribution.</p></table-wrap-foot></table-wrap>

<sec id="Ch1.S3.SS1">
  <title>Characterization of uncertain input factors</title>
      <p>The study site slope cross-section, as represented in CHASM, is illustrated
in Fig. 2. Slope input factors (slope geometry, geotechnical and
hydrological properties) are assumed to be random variables characterized by
different statistical distributions. These distributions and their
statistical parameters have been obtained from different sources as
described in Sect. 2.1, and summarized in Table 1. For each set of CHASM
input factors generated via random sampling, checks are undertaken to ensure
that any combination of the input factor values that is physically
unrealistic (for example, with saturated unit weight smaller than
unsaturated unit weight) is discarded from further analysis (and replaced by
another randomly generated, feasible combination). The complete list of such
feasibility checks is given in the footnote of Table 1. For the purposes of
this study the model discretization parameters – such as the cell size
(1 m <inline-formula><mml:math id="M68" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1 m), hydrological time step (60 s), and slip search grid location
and dimensions – and physical and mathematical constants are not varied.
These discretization parameters are selected based on preliminary model
simulations and our previous experience of applying CHASM to similar slopes,
and they ensure the numerical stability and conservation of mass (water) of
the hydrological component throughout the simulation period. These choices
are thus meant to minimize the number of failed model runs during the Monte
Carlo simulation process.</p>
      <p>The dynamic hydrological scheme of CHASM requires the specification of
hourly rainfall intensities to drive the dynamic hydrological component of
CHASM for the selected hydrological time step (60 s). While the
uncertainties in slope properties are characterized by probability
distributions based on past experience of applying the model to the study
area, the potential variability of future rainfall is difficult to define
with a probability distribution, hence the term of “deep” uncertainty. We
therefore represent our lack of knowledge by varying rainfall
intensity–duration combinations widely to ensure that any feasible future
design storm in a changing climate is captured in our sampling. The ranges
of rainfall intensity and duration used in this analysis are based on
intensity–duration–frequency (IDF) relationships derived for the design of
the Roseau Dam in Saint Lucia (Fig. 3). Engineering consultants,
Klohn-Crippen (1995), applied Gumbel analysis of 40 years of daily
rainfall data from weather stations around the island to estimate the
intensities and durations of <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> to 1 : 500-year return periods events. From
these IDF relationships we define ranges of possible rainfall intensities of
0 to 200 mm h<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and durations of 0 to 72 h, which we sample
independently and uniformly.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p>Rainfall intensity–duration–frequency curves for Saint Lucia
developed by Klohn-Crippen (1995) using Gumbel analysis of 40 years of
hourly rainfall data from 15 rainfall gauges.</p></caption>
          <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/17/225/2017/nhess-17-225-2017-f03.pdf"/>

        </fig>

      <p>For this experiment the first 168 h of rainfall forcing are set to an
intensity of 0 mm h<inline-formula><mml:math id="M71" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> to allow the moisture distribution within the
unsaturated zone to be established based on the suction–moisture curve. This
is necessary because the initial moisture content in each unsaturated cell
at time step zero is a linearly interpolated value between the initial
surface suction and position of the estimated water table (where the
pressure head is 0 m). Then after the first iteration of the hydrological
function in CHASM the Millington–Quirk equation is used to update the
moisture content based on the suction–moisture curve. The implementation of
a 168 h start-up (zero rainfall) period should be sufficient to establish
a representative moisture distribution and potentially steady-state seepage
(equilibrium). However, if hydrological equilibrium is not attained, this is
still an acceptable representation of the physical processes that may be
observed in such slopes. For instance, it may replicate the high groundwater
tables that often exist in our study area towards the end of a rainy season.</p>
      <p>Rainfall of the selected intensity and duration is then imposed on the slope
to determine the stability of the slope for that storm event. In the absence
of information on typical hourly rainfall rates for events longer than 1 h, rainfall intensity is assumed to be uniform across the rainfall
duration sampled. The storm is followed by a further 168 h of
zero-rainfall simulation time to consider the continued effects of the
groundwater response on slope stability.</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Classification and regression trees (CART)</title>
      <p>While different algorithms have been used to implement the mapping step in
bottom-up approaches in past studies, we have chosen to use classification
and regression trees (CART). Comparison between the most popular algorithms,
CART and PRIM, did not show either algorithm to be superior
(Lempert et al., 2008), while CART has the advantages of simplicity
and an ability to work with minimal input from the user. CART is a
machine-learning method for constructing prediction models from data
(Breiman et al., 1984). In our application, such model takes the form of
a binary tree, where a categorical dependent outcome (i.e. slope failure
versus stability) is predicted from a set of continuous independent
variables (i.e. slope and design storm properties). The tree is composed of
nodes and branches. At each node, an if-then condition is applied to one of
the independent variables (e.g. “slope angle above or below 30 degrees”)
to generate two different branches. Several strata of nodes and branches
compose the tree up to a stratum of terminal nodes (leaf nodes) where a
prediction of the categorical dependent outcome is made (e.g. “slope
fails”).</p>
      <p>A CART is constructed through a recursive algorithm applied to a sample of
independent variables (inputs) and associated categorical outcomes
(outputs). In this study, the input/output sample is generated by the Monte
Carlo simulation of CHASM. The algorithm automatically selects which input
variable and threshold value to use at every node. The selection is based on
maximizing the homogeneity of the output samples in the subsequent nodes.
The level of homogeneity can be measured by different criteria. Here, we use
the Gini impurity measure, which is defined  as
            <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M72" display="block"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>m</mml:mi></mml:munderover><mml:msup><mml:mi>p</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mfenced open="(" close=")"><mml:mi>i</mml:mi></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M73" display="inline"><mml:mi>m</mml:mi></mml:math></inline-formula> is the number of categories for the output (2 in our case), and
<inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mfenced close=")" open="("><mml:mi>i</mml:mi></mml:mfenced></mml:mrow></mml:math></inline-formula> is the fraction of output samples in the node belonging
to category <inline-formula><mml:math id="M75" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. A Gini impurity index equal to 0 corresponds to a pure
node, i.e. a node where all output samples belong to the same category. In
general, pure nodes cannot be obtained, but the algorithm seeks to minimize
the Gini impurity index.</p>
      <p>A key question in constructing a classification tree is that of the optimal
sizing (i.e. number of nodes and branches). Increasing the size of the tree
generally increases its predictive accuracy over the sample used for its
construction, but it might reduce its ability to generalize to new samples
(overfitting). Moreover, a tree with simpler structure might be easier to
interpret and communicate. Once a CART has been constructed, a machine
learning technique called “pruning” can be applied to reduce the size of
the tree by removing sections that provide little classification power. More
details about the pruning technique can be found, for example, in
Hastie et al. (2009).</p><?xmltex \hack{\newpage}?>
</sec>
</sec>
<sec id="Ch1.S4">
  <title>Results</title>
      <p>In this section, we analyse the outputs from the 10 000 CHASM simulations to
determine which factors control slope stability and whether critical
thresholds exist beyond which slope failure will occur.</p>
      <p>We perform an initial evaluation of the factors controlling slope stability
by comparing the marginal distributions of the input factors that cause
slope failure with those that do not. The approach is generally referred to
as regional sensitivity analysis  (first proposed by Spear and Hornberger,
1980; for a general introduction see Pianosi et al., 2016). We split the
10 000 model simulations into two sub-sets: those that produce slope failure
(<inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:mi>F</mml:mi><mml:mi mathvariant="italic">&lt;</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>) and those that simulate a stable slope (<inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:mi>F</mml:mi><mml:mi mathvariant="italic">&gt;</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>). For
each input factor, the (marginal) empirical cumulative distribution
functions of the two sub-sets are computed. Figure 4 shows these
distributions for a selection of factors. The grey dashed line is the
distribution corresponding to a stable slope and the black solid line is the
one corresponding to slope failure. The grey and black lines clearly deviate
(i.e. the two distributions are different) for thickness of topsoil,
effective cohesion of topsoil, rainfall intensity and rainfall duration,
implying that these factors are important determinants of slope failure. For
all other factors (including those not shown in Fig. 4), the two lines
essentially overlap, implying that the factors have no direct influence on
determining failure  (although they still may have influence through
interactions, see Saltelli et al., 2008). Besides identifying the
influential factors, Fig. 4 also provides information on the ranges of
influential factors associated with slope failure. For example, the top left
panel shows that the model is unlikely to predict failure when thickness of
topsoil is smaller than 3 m, as the black solid line is nearly flat towards
the smallest values of the original range of this factor. This initial
analysis suggests that relatively few input factors have a significant
impact on slope stability. Furthermore, it also provides initial guidance
about which values of those factors are more likely to produce failure.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p>Cumulative probability distributions (cdf) of slope failure and
stability predicted by CHASM for several different input factors. Note that
the Van Genuchten suction–moisture curve <inline-formula><mml:math id="M78" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> is shown in logarithmic
scale.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/17/225/2017/nhess-17-225-2017-f04.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p>Classification tree of slope response. Each interior node
corresponds to one of the analysed uncertain input factors (model
parameters, boundary conditions and design storm properties). The bar under
each leaf shows the proportion of simulations that resulted in slope failure
(black) or stability (grey) for that leaf.</p></caption>
        <?xmltex \igopts{width=469.470472pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/17/225/2017/nhess-17-225-2017-f05.pdf"/>

      </fig>

      <?xmltex \floatpos{p}?><fig id="Ch1.F6"><caption><p><bold>(a)</bold> Sampled values of effective cohesion of topsoil versus
thickness of topsoil. Black points correspond to simulations resulting in
slope failure, while grey crosses correspond to simulations resulting in a
stable slope. <bold>(b)</bold> As panel a, with the additional red dashed line
representing the thresholds derived from the classification tree in Fig. 5. <bold>(c)</bold> As panel a, with the additional red dashed line representing the
thresholds derived from the classification tree in Fig. 9.</p></caption>
        <?xmltex \igopts{width=193.47874pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/17/225/2017/nhess-17-225-2017-f06.png"/>

      </fig>

      <p>CART analysis provides a systematic way to quantify the thresholds
separating slope failure and stability. Figure 5 shows the classification
tree obtained from the same set of simulations (see Appendix A for details
on pruning). CART results are consistent with the initial analysis of input
distributions, as evidenced by the fact that the main factors emerging in
the classification tree of Fig. 5 are the same that were shown as
influential in Fig. 4. From the 28 analysed factors (26 model parameters
plus the two design storm properties), five factors alone (thickness of topsoil, effective cohesion of topsoil, rainfall intensity, rainfall duration
and initial depth of water table) are sufficient to correctly classify
89 % of the simulations. Figure 5 also illuminates the critical thresholds
in slope properties and rainfall drivers that separate slope failure and
stability. For example, the leftmost branch shows that if the thickness of
the topsoil is less than 2.9 m and effective cohesion of this stratum is
below 2.1 kPa, the landslide model tends to predict slope failure. This
happens regardless of what values rainfall intensity and duration take. The
black/grey-shaded bar at the end of each node visualizes the fraction of
input factor combinations that produce failure/stability respectively. It
therefore provides a visual indicator of the predictive performance of the
tree at each node and shows the high predictive performance achieved.</p>
      <p>Effective cohesion and thickness of topsoil appear multiple times in the
same branch in Fig. 5 (for example, at the leftmost and the rightmost
branches), which may indicate that these two factors interact with each
other. This suspicion is confirmed if we look at the scatter plot of the
effective cohesion of topsoil samples versus the thickness of topsoil
samples for simulations that lead to slope failure (black) and stability
(grey) (Fig. 6a). The triangular pattern in Fig. 6a clearly indicates that
these two factors interact to produce slope failure, i.e. a slope with more
cohesive soil can be thicker without experiencing failure. Visualizing the
thresholds identified from the CART analysis (Fig. 5) in this scatter plot
(red dashed line in Fig. 6b) shows the inability of CART to characterize
this interaction, i.e. CART attempts to reproduce the interaction through a
sequence of vertical and horizontal separations. One can approach this
problem either by rotating the axes of this graph or by creating a new
auxiliary variable combining the interacting factors    (Dalal et
al., 2013). We create a new auxiliary variable, the ratio between effective
cohesion and thickness of the topsoil, because we believe that it is a
physically meaningful variable. We then generate a new tree based on the
original factors plus the new auxiliary variable. The resulting tree, pruned
for a similar error as the original tree, is shown in Fig. 7. It still
classifies 89 % of the simulations correctly but using a much simpler
structure than the tree in Fig. 5. Figure 7 shows that when the ratio of
cohesion to thickness of the topsoil is above 2.0 kPa m<inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, CHASM
predicts a stable slope most of the time (4611 simulations correspond to a
stable slope and only 385 simulations produce slope failure). When the topsoil cohesion to thickness ratio is below 2.0 kPa m<inline-formula><mml:math id="M80" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> then rainfall
characteristics need to be taken into account to predict slope stability.
Figure 6c also shows that the new separation line (red dashed) between failure
and stability is now more consistent with the underlying scatter plot.</p>
      <p>We further expect rainfall intensity and duration to interact in the context
of slope stability. Indeed, numerous field observations in the literature,
and empirical relationships used in regional landslide early warning systems
worldwide, show that both high-intensity/short-duration rainfall
combinations and low-intensity/long-duration combinations can result in
slope failure  (Lumb, 1975; Crosta, 1998; Martelloni et al., 2012).
Empirical rainfall intensity–duration (<inline-formula><mml:math id="M81" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>–<inline-formula><mml:math id="M82" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>) thresholds are typically
obtained by plotting observed landslide events according to their triggering
rainfall intensity and duration, and are generally linear, with a negative
gradient, when logarithmic scales are used. This log–log relationship can
also be seen in Fig. 8, which shows a separation between the rainfall <inline-formula><mml:math id="M83" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>–<inline-formula><mml:math id="M84" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>
combinations that can trigger landslides (black dots) and those that do not
(grey crosses). We therefore create a second auxiliary variable – the
negative ratio between the logarithm of rainfall intensity and the logarithm
of rainfall duration (<inline-formula><mml:math id="M85" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>log(<inline-formula><mml:math id="M86" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>)/log(<inline-formula><mml:math id="M87" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>)) – and repeat the CART analysis to see
whether it is possible to further simplify the tree. The resulting tree
(Fig. 9) is pruned based on a similar error to previous trees (Figs. 5 and 7), but with a significantly simplified structure. We consider this final
classification tree as the most effective output of the CART analysis, since
its simplicity facilitates communication with stakeholders, while preserving
the same information content.</p>
</sec>
<sec id="Ch1.S5">
  <title>Discussion</title>
      <p>We have shown that the application of a mechanistic model such as CHASM in a
combined Monte Carlo and CART analysis framework can help identify the
dominant preparatory and triggering factors driving slope instability in a
data-scarce location. Our method goes beyond previous studies by accounting
for both site-specific preparatory factors (geometrical,
geotechnical and hydrological conditions) and future uncertain rainfall
triggers. Results for our study site indicate that targeted geotechnical
data acquisition could help to constrain uncertainties in cohesion and soil
depths; and the effects of different rainfall intensities and durations
should be represented to capture both current and potential future hazard
scenarios.</p><?xmltex \hack{\newpage}?><?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><caption><p>Classification tree of slope response, when adding an auxiliary
variable (ratio between effective cohesion and thickness of topsoil) among
uncertain input factors. The bar under each leaf shows the proportion and
total number of simulations leading to slope failure (black bar, left hand
number) or a stable slope (grey bar, right hand number).</p></caption>
        <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/17/225/2017/nhess-17-225-2017-f07.pdf"/>

      </fig>

<sec id="Ch1.S5.SS1">
  <title>Preparatory and triggering factors driving slope instability</title>
      <p>For our study site the ratio of the topsoil stratum's effective cohesion to
stratum thickness is shown to be a dominant factor in the stability of the
slope. Inspection of selected model outputs indicates that the critical slip
surface generally tends to be located within this top stratum (weathering
grade V–VI) with the deepest part of the slip circle at the interface with
the weathered material stratum (grade III–IV), as illustrated in Fig. 2. The
slip surface location within the topsoil stratum is explained by the
site-specific parameters (Table 1) in which: (i) the higher strength
weathered material stratum constrains the failure surface to within the
weaker soil stratum above; and (ii) as rainfall infiltrates, the lower
hydraulic conductivity of the weathered material is likely to cause loss of
soil matric suction and thus a reduced apparent strength at the
soil/weathered material interface.</p>
      <p>Of the two topsoil stratum strength parameters, it is effective cohesion,
rather than angle of friction, that shows up in the CART analysis because
the study site slope is likely to be cohesion controlled rather than
friction controlled – i.e. the slope angle is typically greater than the
friction angle. Figure 6 shows that when the topsoil stratum is thin it can
remain stable even for very low values of effective cohesion, whereas,
thicker soils tend to require a much higher effective cohesion for
stability. This result is in keeping with other physically based modelling
studies of the relationships between the geometry of slopes, strata and
shallow landslides in cohesion controlled slopes  (Frattini and Crosta,
2013; Milledge et al., 2014). Ignoring the effects of water table location
and pore water pressures, the greater self-weight of soil at the base of a
thicker soil stratum generates higher shear stresses and requires greater
shear resistance for stability than in a shallower soil.</p>
      <p>The importance of cohesion for the stability of tropical residual soil
slopes, such as our study site, and its inclusion in stability analysis is
the subject of an ongoing debate amongst geotechnical engineering,
researchers and practitioners. Laboratory analysis of the shear strength of
remoulded clays show that the value of the effective cohesion parameter is
affected by measurement uncertainties (Parry, 2004) and that peak
cohesion is lost with seasonal cycles of dilatancy  (Take
and Bolton, 2011). The known sensitivity of slope stability to cohesion and
the uncertainties associated with its measurement thus lead some engineers
to adopt a highly conservative approach to the value of effective cohesion
used in slope design – often assigning it a value of zero
(Schofield, 2006). Yet, landslide hazard assessment
scientists and engineering practitioners in the humid tropics argue for its
inclusion as an observable strength parameter in the analysis of existing
slopes comprised of undisturbed tropical residual soils which exhibit relict
structures from the weathered parent rock     (Burland et al.,
2008). For the study site, our modelling approach supports the inclusion of
non-zero values of effective cohesion in the analysis to account for its
observable stability in the field. Our results also indicate that any data
acquisition strategy for this site should target both soil thickness and
effective cohesion values (both undisturbed and remoulded) to improve
landslide hazard predictions.</p>
      <p>The second most important factor in the stability of our study site is the
nature of rainfall events in terms of their intensity and duration. As noted
in Sect. 4, when the predicted failed and stable slopes are plotted on
log–log axes of associated rainfall intensities and durations (Fig. 8) a
negative linear threshold is found above which landslides are more likely to
occur. This relationship is observed in landslide inventories which are
widely used to generate empirical regional rainfall intensity–duration (<inline-formula><mml:math id="M88" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>–<inline-formula><mml:math id="M89" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>)
thresholds of the form <italic>I</italic> <inline-formula><mml:math id="M90" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> <italic>a</italic><inline-formula><mml:math id="M91" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> <italic>D</italic><inline-formula><mml:math id="M92" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mi>a</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, where <inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are parameters specific to a site or
region  (e.g. Larsen and Simon, 1993; Guzzetti et al., 2007). In the
absence of empirical data, physically based models may be used to generate
synthetic thresholds using Monte Carlo methods        (e.g.
Peres and Cancelliere, 2014). Our method thus demonstrates the
importance of representing the dynamic hydrological processes involved in
triggering landslides, while also providing a starting point for generating
site-specific rainfall <inline-formula><mml:math id="M95" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>–<inline-formula><mml:math id="M96" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> thresholds in data-scarce locations.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p>Sampled values of rainfall intensity versus rainfall duration when
effective cohesion over thickness of topsoil is smaller than 2.0 kPa m<inline-formula><mml:math id="M97" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.</p></caption>
          <?xmltex \igopts{width=184.942913pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/17/225/2017/nhess-17-225-2017-f08.pdf"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p>Classification tree of slope response, when adding two auxiliary
variables: the ratio between effective cohesion and thickness of topsoil,
and the negative ratio between the logarithm of rainfall intensity and the
logarithm of rainfall duration. The bar under each leaf shows the proportion
and total number of simulations leading to slope failure (black bar, left-hand number) or a stable slope (grey bar, right-hand number).</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/17/225/2017/nhess-17-225-2017-f09.pdf"/>

        </fig>

      <p>We have to reiterate that our results are valid within the context of the
assumptions made in our study. For example, changing a particular input
factor distribution may influence the importance of other factors. This is
not a limitation of our study only, but of any model-based study and
sensitivity analysis application. Particularly relevant for our study is
that we evaluate the occurrence of slope failure for individual rainfall
events and we do not consider explicitly the impacts of varying initial
hydrological conditions that may result from sequences of rainfall events.
This limitation is partially mitigated by the fact that we jointly vary the
intensity–duration of individual events and the initial depth of water
table. The approach presented here is a useful contribution for identifying
dominant landslide preparatory and triggering factors, guiding data
acquisition and refining the hazard assessment.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <title>Can deep uncertainty in future rainfall exceed other
uncertainties?</title>
      <p>In this study, we have evaluated how uncertainty about slope characteristics
and future rainfall change may influence risk of slope failure. Our findings
have demonstrated that, for our study site, physical slope properties,
namely effective cohesion and thickness of the topsoil, are significant
drivers of slope stability. For this slope, these physical properties have a
more significant impact on landslide hazard risk than variability in future
rainfall intensity and duration. Extending this type of study to other
slopes would allow further exploration of the complex interactions between
soil depth, permeability, rainfall intensity-duration, antecedent rainfall
and the resulting slide depth      (see, for example, Lumb,
1975; van Asch et al., 2009).</p>
      <p>Our findings have a number of important implications for landslide hazard
research. Previous studies typically have analysed the impacts of
uncertainty related to slope characteristics and future climate
independently.   For example, Dehn and Buma (1999),
Collison et al. (2000) and   Ciabatta et al. (2016) consider the impacts of climate change on slope stability, but ignore
uncertainty around soil properties; while  Rubio et al. (2004) account for
uncertainty introduced by slope hydrology and geotechnical properties, but
ignore uncertainty relating to design storms. However, our results suggest
that the failure to consider both sources of uncertainty simultaneously may
lead to a significant underestimation of slope susceptibility to landslides
under potential climate change. Furthermore, we have demonstrated how
physically based models, like CHASM, can be utilized to rapidly assess the
impacts of multiple interacting and uncertain drivers of landslide
occurrence in ways that would not be possible using simpler statistical
models    (e.g. Dixon and Brook, 2007).</p>
      <p><?xmltex \hack{\newpage}?>To date, only Melchiorre and Frattini (2012) have attempted to analyse
slope failure considering both uncertainty arising from slope properties and
future climate. Their research used a top-down approach to quantify the
impacts of multiple uncertainties. Specifically, they used Monte Carlo
simulations and sensitivity analysis to assess the impacts of uncertainty in
soil properties on predictions of slope stability for a pre-defined set of
precipitation scenarios. We conclude that deep uncertainty due to potential
future climate characteristics is not yet fully considered in landslide
hazard assessment, and, as a result, policy recommendations may lead to
undesirable outcomes given the difficulty in predicting impacts of climate
change on future rainfall. In contrast, bottom-up approaches, such as that
proposed in this study, consider a much wider range of possible system
drivers (rainfall) and other uncertainties, without introducing assumptions
regarding the probability of future precipitation. This insight is
particularly relevant for small islands like the Caribbean, where the
variety of different processes that contribute to rainfall change, some of
which are poorly resolved by GCMs, make it very difficult to provide
projections of future rainfall
(Seneviratne et al., 2012).</p>
</sec>
<sec id="Ch1.S5.SS3">
  <title>Implications for data acquisition and assessment of future
hazard</title>
      <p>Bottom-up approaches to natural hazard risk assessment provide valuable
knowledge to inform management decisions and to target data acquisition,
especially in situations where resources may be limited. This study has
shown how dominant physical slope properties driving landslide occurrence
for a particular class of slope can be identified. As a result,
decision makers may seek to provide funding for targeted data acquisition to
reduce uncertainty about the values of these parameters (e.g. thickness and
effective cohesion of topsoil) in order to improve understanding of how
likely a slope is to fail. Decision makers could also use the knowledge
gained from CART to target management practices to improve slope stability
(e.g. improving slope drainage or land cover) or to develop options to
mitigate consequences of slope failure (e.g. restricting development in
high-risk areas). In this regard, the methodology developed in this study
could be used to quantify the impact of different management options on
landslide occurrence thresholds, providing an objective measure of the
potential value of each strategy that can support debate amongst disaster
risk reduction practitioners.</p>
      <p>CART also has the distinct advantage that trees can provide useful knowledge
for decision makers even when uncertainties about future changes in climate
are large, as is the case with rainfall projections in the Caribbean islands
that are predominant areas where landslides occur globally. Any available
climate information can be used a posteriori to assess the
plausibility of threshold tipping points being crossed, and support the
discussion whether improved management is required to improve slope
stability in the future. Ultimately, the decision to implement any given
action depends on how risk averse stakeholders are and how much they are
willing to spend on an adaptation strategy. However, CART provides the tools
and information to enable managers to make informed choices that are robust
under a wide range of plausible future conditions, reducing the risk of
wasted investment and/or unanticipated negative outcomes.</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <title>Conclusions</title>
      <p>In this study, we used a combination of physical-based modelling and
empirical CART analysis to quantify the importance of different sources of
uncertainty when predicting landslide hazards for an example case study in
the Caribbean. Contrary to common assumptions, our findings have showed that
prediction of landslide occurrence may be more strongly influenced by
uncertainty related to physical slope properties (e.g. cohesion and
thickness of the topsoil) than by (deep) uncertainty associated with future
changes in rainfall patterns due to climate change. We suggest that failure
to account for uncertainty related to both slope properties and climate
change therefore will lead to a significant underestimation of landslide
risks and associated impacts on human populations.</p>
      <p>The methodology developed in this paper has demonstrated that bottom-up
approaches, implemented here using CART, can provide valuable information
for assessment of landslide hazards even in data-sparse environments. Our
bottom-up approach illuminates dominant drivers of slope instability,
enabling stakeholders and decision makers to target data acquisition to
reduce model prediction uncertainty. Moreover, CART analysis provides
estimates of critical rainfall thresholds at which slope failure is
predicted to occur. Using this knowledge, decision makers can assess whether
it is likely these threshold tipping points being crossed in the future
given available climate change information, and they can determine whether
improved management may be required to ensure long-term slope stability in
the face of climate change.</p>
      <p>The factors identified as drivers of slope failure in this study are
specific to the slope investigated and valid under the assumptions made
about the system representation, i.e. the choice of the CHASM model and its
resolution (spatial and temporal). While we cannot generalize our findings,
our proposed methodology can be easily applied to other sites to assess the
dominant factors affecting slope stability. Future work will seek to expand
our analysis to a broader range of slope conditions found in a wider study
region, for example to analyse effects of variable slope angles and heights
on slope stability.</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S7">
  <title>Data availability</title>
      <p>This study did not involve any underlying data.</p><?xmltex \hack{\clearpage}?>
</sec>

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

<app id="App1.Ch1.S1">
  <title>Tree pruning</title>
      <p>To avoid overfitting of data we pruned the tree using cross-validation.
Figure A1 shows the cross-validation error (i.e. the proportion of
misclassified data on the validation dataset) for different pruning levels.
The smallest cross-validation error is obtained for pruning level 23, which
corresponds to a tree with 51 leaf nodes. However, Fig. A1 shows that
choosing a much simpler tree, for example one with 25 leaf nodes (pruning
level 31), also results in a very small error. Simpler trees are easier to
interpret, and therefore in this study we select the tree with 25 leaf
nodes, which has a cross-validation error equal to 0.119.</p><?xmltex \hack{\newpage}?><?xmltex \floatpos{h!}?><fig id="App1.Ch1.F1"><caption><p>Cross-validation error of the classification tree for increasing
pruning level. The cross-validation error is computed by splitting the
available training data (10 000 CHASM model simulations in our case) at
random into 10 subsets. Ten different classification trees are then
constructed, where each tree is trained using 9 of the 10 subsets and its
misclassification rate on the remaining subset is evaluated. The average of
these 10 misclassification rates is the cross-validation error (black line).
The minimum cross-validation error is equal to 0.110 and is obtained at
pruning level 23, which corresponds to 51 leaf nodes. For the pruning level 31 (25 leaf nodes) the cross-validation error is 0.119.</p></caption>
        <?xmltex \igopts{width=184.942913pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/17/225/2017/nhess-17-225-2017-f10.pdf"/>

      </fig>

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

      <p>The authors declare that they have no conflict of
interest.</p>
  </notes><ack><title>Acknowledgements</title><p>This work was supported by the Natural Environment Research Council
(Consortium on Risk in the Environment: Diagnostics, Integration,
Benchmarking, Learning and Elicitation (CREDIBLE); grant number
NE/J017450/1). This work was carried out using the computational facilities
of the Advanced Computing Research Centre, University of Bristol –
<uri>http://www.bris.ac.uk/acrc</uri>. The SAFE Toolbox for Global Sensitivity
Analysis is freely available for research purposes from
<uri>www.bris.ac.uk/cabot/resources/safe-toolbox/</uri>. <?xmltex \hack{\newline}?><?xmltex \hack{\newline}?> Edited by: I. Main<?xmltex \hack{\newline}?> Reviewed by: T. A. Dijkstra
and one anonymous referee</p></ack><ref-list>
    <title>References</title>

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    <!--<article-title-html>Dealing with deep uncertainties in landslide modelling for disaster risk reduction under climate change</article-title-html>
<abstract-html><p class="p">Landslides have large negative economic and societal
impacts, including loss of life and damage to infrastructure. Slope
stability assessment is a vital tool for landslide risk management, but high
levels of uncertainty often challenge its usefulness. Uncertainties are
associated with the numerical model used to assess slope stability and its
parameters, with the data characterizing the geometric, geotechnic and
hydrologic properties of the slope, and with hazard triggers (e.g.
rainfall). Uncertainties associated with many of these factors are also
likely to be exacerbated further by future climatic and socio-economic
changes, such as increased urbanization and resultant land use change. In
this study, we illustrate how numerical models can be used to explore the
uncertain factors that influence potential future landslide hazard using a
bottom-up strategy. Specifically, we link the Combined Hydrology And
Stability Model (CHASM) with sensitivity analysis and Classification And
Regression Trees (CART) to identify critical thresholds in slope properties
and climatic (rainfall) drivers that lead to slope failure. We apply our
approach to a slope in the Caribbean, an area that is naturally susceptible
to landslides due to a combination of high rainfall rates, steep slopes, and
highly weathered residual soils. For this particular slope, we find that
uncertainties regarding some slope properties (namely thickness and
effective cohesion of topsoil) are as important as the uncertainties
related to future rainfall conditions. Furthermore, we show that 89 % of
the expected behaviour of the studied slope can be characterized based on
only two variables – the ratio of topsoil thickness to cohesion and the
ratio of rainfall intensity to duration.</p></abstract-html>
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