<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing with OASIS Tables v3.0 20080202//EN" "journalpub-oasis3.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0"><?xmltex \bartext{Tenth International Symposium on Land Subsidence (TISOLS)}?>
  <front>
    <journal-meta><journal-id journal-id-type="publisher">PIAHS</journal-id><journal-title-group>
    <journal-title>Proceedings of the International Association of Hydrological Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">PIAHS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Proc. IAHS</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2199-899X</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/piahs-382-443-2020</article-id><title-group><article-title>Parameterisation of the Koppejan settlement<?xmltex \hack{\break}?> prediction model using cone
penetration<?xmltex \hack{\break}?> testing and gradient boosting</article-title><alt-title>Parameterisation of the Koppejan settlement prediction model</alt-title>
      </title-group><?xmltex \runningtitle{Parameterisation of the Koppejan settlement prediction model}?><?xmltex \runningauthor{K.~Duffy et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Duffy</surname><given-names>Kevin</given-names></name>
          <email>kevin.duffy@ucdconnect.ie</email>
        <ext-link>https://orcid.org/0000-0002-7918-2171</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Siderius</surname><given-names>Klaas</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Long</surname><given-names>Mike</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>School of Civil Engineering, University College Dublin, Dublin, Ireland</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Fugro NL Land B.V., Groningen, the Netherlands</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Kevin Duffy (kevin.duffy@ucdconnect.ie)</corresp></author-notes><pub-date><day>22</day><month>April</month><year>2020</year></pub-date>
      
      <volume>382</volume>
      <fpage>443</fpage><lpage>447</lpage>
      
      <permissions>
        <copyright-statement>Copyright: © 2020 Kevin Duffy et al.</copyright-statement>
        <copyright-year>2020</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://piahs.copernicus.org/articles/382/443/2020/piahs-382-443-2020.html">This article is available from https://piahs.copernicus.org/articles/382/443/2020/piahs-382-443-2020.html</self-uri><self-uri xlink:href="https://piahs.copernicus.org/articles/382/443/2020/piahs-382-443-2020.pdf">The full text article is available as a PDF file from https://piahs.copernicus.org/articles/382/443/2020/piahs-382-443-2020.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e95">This study examines how cone penetration test (CPT)
parameters, such as cone tip resistance and friction sleeve resistance, can
be used to assess the compressibility of fine-grained soils across the
Netherlands based on a database of 286 paired CPTs and oedometer tests from
across the country. This is done with the aim of refining and simplifying
the parameterisation of the Koppejan consolidation coefficients, a procedure
which can yield significant error and is prone to misinterpretation. It was
found that there is significant potential in using gradient boosting methods
to obtain a relationship between the CPT parameters and the Koppejan
parameters, with further investigation required into the noise within the
dataset and the acquisition of additional high-quality samples. The use of
such methods will offer a means of reducing the influence of human error or
misinterpretation on the prediction of settlement and provide further
confidence in the use of machine learning methods in engineering practice.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e107">Appropriately assessing the consolidation of soil under applied loads has
long been a challenge for geotechnical engineers. In the case of the
Netherlands, soft clays and organic soils dominate the subsurface and the
heterogeneity and high compressibility of these materials has resulted in a
significant margin of error being associated with settlement calculations,
in the range of <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> % for Dutch practice  (CROW, 2004).
This is exacerbated by the effect of human subjectivity on the
parameterisation of variables associated with settlement prediction models,
a process which is highly dependent on the experience and interpretation of
the engineer. Furthermore, given the sporadic and random nature of soil
sampling and the sample disturbance that may also result, there is also a
need to correlate these variables to continuous, in situ tests in order to
obtain a more representative parameter for a soil layer. The cone
penetration test (CPT) is an example of such a test and involves penetrating
the ground with an instrumented steel cone and rod, measuring the cone tip
resistance <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and friction sleeve resistance <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> as it penetrates
through the ground. It is used almost ubiquitously throughout the
Netherlands and many other countries worldwide due to the many correlations
its parameters have with basic soil properties along with its ability to
delineate soil stratigraphy to a high resolution.</p>
      <p id="d1e142">Of the settlement prediction models in the Netherlands, the Koppejan model
(Koppejan, 1948) is the most prevalent, largely due to its
simplicity and cost effectiveness in comparison to the more advanced models
such as the <inline-formula><mml:math id="M4" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M5" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M6" display="inline"><mml:mi>c</mml:mi></mml:math></inline-formula> isotache model  (Den Haan, 1992, 1994) or the
NEN-Bjerrum model (Bjerrum, 1967). The model has also been
extensively implemented in Dutch geotechnical practice and thus, many Dutch
engineers have a high competence with the model. The model is based on a
combination of the logarithmic compression law proposed by Terzaghi (1925) and the creep law proposed by Buisman (1936). The
Koppejan parameters can be obtained directly from incremental loading
oedometer tests, a procedure which assesses the one-dimensional
consolidation of a small soil specimen through the application of increasing
vertical loads over time on top of the specimen.</p>
      <?pagebreak page444?><p id="d1e166">Hence, this study aims to explore the relationship between the CPT and the
Koppejan compressibility parameters using both simple linear regression and
machine learning, based on a database of fine-grained clay soils obtained
from sites across the Netherlands.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><label>Figure 1</label><caption><p id="d1e172">Borehole–CPT pairings across the Netherlands (©OpenStreetMap contributors YEAR. Distributed under a Creative Commons BY-SA License, see <uri>https://www.openstreetmap.org/copyright</uri>, last access: 29 August 2019).</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://piahs.copernicus.org/articles/382/443/2020/piahs-382-443-2020-f01.png"/>

      </fig>

</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data source</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Geology of the Netherlands</title>
      <p id="d1e199">The Netherlands is situated in a delta formed by the Rhine, Maas and Schelde
rivers with much of the country being flat and altered anthropogenically,
evident from its canalised streams, polders and dikes protecting the
coastline and inland regions. Most of the country is dominated by Quartenary
deposits, with the western half of the country immediately underlain by a very soft
Holocene layer and the east by a firm sandy Pleistocene layer (Maljers et
al., 2015). In the context of engineering applications, the western Holocene
layer is particularly troublesome due to its high compressibility, with
structures generally requiring long piles extending down towards the
Pleistocene layer below (Houkes, 2016).</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Data description</title>
      <p id="d1e211">The data originates primarily from road and rail projects executed by Fugro
throughout the Netherlands between 2008 and 2018 (see Fig. 1). For each
location, sampling boreholes were automatically paired with CPT locations
less than 25 m away, with the closest CPT location chosen where applicable.
Given the size of the dataset, an individual geological assessment of each
site was deemed infeasible and hence, a Python algorithm was developed for
the oedometer–CPT test pairing process (Duffy, 2019).</p>
      <p id="d1e214">In total, 286 oedometer–CPT pairs were used for the analysis, with the
Koppejan's general constant of compressibility at stresses greater than the
preconsolidation pressure <inline-formula><mml:math id="M7" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula>, the CPT cone resistance <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the
friction sleeve resistance <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> brought forward for further analysis.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Linear regression analysis</title>
      <p id="d1e255">A direct visual relationship between <inline-formula><mml:math id="M10" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and the CPT parameters was not
evident, with simple linear and multiple linear regression models affirming
the lack of correlation, an example of which is shown in Fig. 2.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><label>Figure 2</label><caption><p id="d1e267">Plot of the Koppejan <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:msup><mml:mi>C</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> values against the
corresponding cone resistance <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, indicating the lack
of a distinct visual relationship.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://piahs.copernicus.org/articles/382/443/2020/piahs-382-443-2020-f02.png"/>

      </fig>

      <?pagebreak page445?><p id="d1e298">Based on the correlation devised by Buisman and Huizinga (1944)
shown in Eq. (1), an assessment was made of the relationship between
<inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mi>C</mml:mi><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the in situ vertical effective stress parameter <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> which describes the vertical stress transmitted between soil
particles at a certain depth as a result of the weight of soil above that
same depth. In obtaining <inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>, the saturated unit weight
correlation for Dutch soils derived by Lengkeek et al. (2018) was used, assuming a water table of one metre
throughout.
          <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M17" display="block"><mml:mrow><mml:mi>C</mml:mi><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
        where <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the constrained modulus cone factor.</p>
      <p id="d1e406">The results of this localised assessment are shown in Table 1. Results of
this study have been quantified using both the root mean square error (RMSE)
and the coefficient of determination (<inline-formula><mml:math id="M19" 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>), a coefficient which
expresses the proportion of variance explained by the statistical model and
is given in its generalised form in Eq. (2):
          <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M20" display="block"><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">1</mml:mn><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="normal">SS</mml:mi><mml:mi mathvariant="normal">res</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="normal">SS</mml:mi><mml:mi mathvariant="normal">tot</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>
        where SS<inline-formula><mml:math id="M21" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">res</mml:mi></mml:msub></mml:math></inline-formula> is the sum of squares of the residuals and SS<inline-formula><mml:math id="M22" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">tot</mml:mi></mml:msub></mml:math></inline-formula> is
the total sum of squares.</p>
      <p id="d1e469">Indeed, although <inline-formula><mml:math id="M23" 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> is the square of the correlation coefficient <inline-formula><mml:math id="M24" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> in
the case of simple linear regression, it may also be negative in other
statistical models, indicating that the mean of the data provides a better
fit to the outcome than the fitted statistical model itself.</p>
      <p id="d1e490">For the most part, the correlation performs relatively well. The choice of
an <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> coefficient can also be supported by look-up tables such as
that by Mitchell and Gardner (1975) which uses the soil plasticity, water
content and primary description. However, in the case of a single
engineering project where CPT and laboratory data is significantly more
limited, obtaining a robust <inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> value may prove to be relatively
challenging. Hence it would be optimal if a more universal correlation for
the Netherlands could be found.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e518">Results of the project by project analysis.</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="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Project</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M28" 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="col4">RMSE</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Leeuwarden</oasis:entry>
         <oasis:entry colname="col2">1</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M29" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.51</oasis:entry>
         <oasis:entry colname="col4">11.75</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Amsterdam</oasis:entry>
         <oasis:entry colname="col2">1</oasis:entry>
         <oasis:entry colname="col3">0.43</oasis:entry>
         <oasis:entry colname="col4">4.38</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Arnhem I</oasis:entry>
         <oasis:entry colname="col2">1.5</oasis:entry>
         <oasis:entry colname="col3">0.46</oasis:entry>
         <oasis:entry colname="col4">11.90</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Geldermalsen</oasis:entry>
         <oasis:entry colname="col2">2</oasis:entry>
         <oasis:entry colname="col3">0.65</oasis:entry>
         <oasis:entry colname="col4">9.90</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Groningen</oasis:entry>
         <oasis:entry colname="col2">1.5</oasis:entry>
         <oasis:entry colname="col3">0.73</oasis:entry>
         <oasis:entry colname="col4">4.19</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Rotterdam</oasis:entry>
         <oasis:entry colname="col2">1.5</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M30" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.05</oasis:entry>
         <oasis:entry colname="col4">2.80</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Leiden</oasis:entry>
         <oasis:entry colname="col2">1</oasis:entry>
         <oasis:entry colname="col3">0.38</oasis:entry>
         <oasis:entry colname="col4">9.26</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Arnhem II</oasis:entry>
         <oasis:entry colname="col2">1</oasis:entry>
         <oasis:entry colname="col3">0.50</oasis:entry>
         <oasis:entry colname="col4">7.14</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Enschede</oasis:entry>
         <oasis:entry colname="col2">2</oasis:entry>
         <oasis:entry colname="col3">0.56</oasis:entry>
         <oasis:entry colname="col4">5.41</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Machine learning</title>
      <p id="d1e730">In order to explore more complex non-linear patterns in the dataset, machine
learning methods have been explored, including artificial neural networks,
gradient boosting and XGBoost. A preliminary assessment found that gradient
boosting produced the strongest results  (Duffy, 2019).</p>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Decision trees and gradient boosting</title>
      <p id="d1e740">At an elementary level, decision trees are akin to a flow chart in that each
“node” represents a variable, each “branch” represents a decision and
each “leaf” represents an outcome. It can be used effectively for
classification and regression purposes, with an example of a simple decision
tree shown in Fig. 3.</p>
      <p id="d1e743">In the process of creating a decision tree, the algorithm partitions the
dataset into subsets of variables of similar magnitudes, ascertaining the
effectiveness of potential splits as it moves through the tree. In other
words, the tree assesses the improvement in model score (or reduction in
error) caused by creating the split. The algorithm converges when it can no
longer gain further information through the creation of more splits or when
it reaches a pre-specified limit imposed on the model, known as the model's
“hyperparameters”. An example of a hyperparameter may include the number
of levels in the tree or the minimum number of samples required in a leaf
node.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><?xmltex \currentcnt{3}?><label>Figure 3</label><caption><p id="d1e748">Example of a basic decision tree.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://piahs.copernicus.org/articles/382/443/2020/piahs-382-443-2020-f03.png"/>

        </fig>

      <p id="d1e758">Boosting methods are an extension of the basic decision tree algorithm
whereby the algorithm uses a combination of trees, with each new tree
learning from the mistakes of previous trees. In this way, the model
constantly aims to remove or reduce any pattern that may be preeminent in
the residuals or the error. This is a core principle of the gradient
boosting algorithm (Friedman, 2001).</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Input parameters</title>
      <p id="d1e769">In order to produce a result that is reliable and not a product of
overfitting, 80 % of the data was randomly designated as training data,
with the remaining 20 % being designated as unseen testing data. This
split was chosen in order to retain a sufficient amount of testing data so a
more robust and reliable result could be produced.</p>
      <p id="d1e772">The input parameters chosen were <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the ratio between <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (also known as the friction ratio <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>,
with <inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> chosen in lieu of <inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> so that the possibility of any
interpretability issues associated with the collinearity between <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> was avoided. <inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:msup><mml:mi>C</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> was used as the output parameter.</p>
      <?pagebreak page446?><p id="d1e890"><?xmltex \hack{\newpage}?>The gradient boosting model used as part of this study was implemented using
the MLPRegressor class of the scikit-learn toolbox version 0.20.3
(Pedregosa et al., 2011), with 5-fold cross-validation used for
hyperparameter tuning.</p>
</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>Results</title>
      <p id="d1e902">The model produced an <inline-formula><mml:math id="M41" 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> score of 0.73 and 0.37 for the training and
testing sets respectively, with 5-fold cross validation returning a mean
score of 0.36 with standard deviation of 0.115. In the context of
geotechnical engineering, this can be described as a “medium to strong
correlation” as per the guidelines set out by Jakobsen (2014).</p>
      <p id="d1e916">This model also returned feature importances of 0.34, 0.13 and 0.53 for
<inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> respectively. These scores highlight
the role each variable plays in the calculation of the <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:mi>C</mml:mi><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>, with <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
and <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> being the more dominant features in determining the
model output, perhaps largely due to the relative inaccuracy associated with
friction sleeve measurements (Lunne et al., 1997).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><?xmltex \currentcnt{4}?><label>Figure 4</label><caption><p id="d1e997">Learning curves for the gradient boosting model.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://piahs.copernicus.org/articles/382/443/2020/piahs-382-443-2020-f04.png"/>

        </fig>

      <p id="d1e1007">Notwithstanding, Fig. 4 shows that both the training and testing curves fail
to converge together at higher sample sizes. This is indicative of variance
within the model, a problem that may be resolved by increasing the number of
samples and thus allowing the learning curves to converge more closely,
redolent of a well-fitted model.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><label>Figure 5</label><caption><p id="d1e1012">Histogram of results for the random state analysis.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://piahs.copernicus.org/articles/382/443/2020/piahs-382-443-2020-f05.png"/>

        </fig>

      <p id="d1e1021">Furthermore, as illustrated by Fig. 5, there is significant fluctuation in
the <inline-formula><mml:math id="M48" 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> score as the random state of the model is changed.   In other words,
if different training and testing sets are taken and if the model learns
slightly differently compared to its last execution, the model score changes
significantly. Based on a collective assessment of one hundred different
random states, the median and maximum <inline-formula><mml:math id="M49" 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> scores obtained were 0.33 and
0.68 respectively. It is surmised that this instability is indicative of the
variability and noise within the dataset, consequently leading to the
presence of many local minima as the algorithms undergo gradient descent
along the objective function. As a result of this, the model may be
particularly prone to converging within these local minima, resulting in the
dispersion of results as the random state is changed.</p>
      <p id="d1e1046">Consequently, it is recommended that further high-quality samples are
sourced for the continued development of such an algorithm in order to yield
a more complete convergence of the learning curves and to investigate the
effect of the change of random state on the <inline-formula><mml:math id="M50" 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> score. Further
development is also required into the automated process of pairing the CPTs
to the oedometer tests, with a manual assessment taken where appropriate.</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d1e1070">A major challenge in the geotechnical engineering industry is reducing the
significant amount of error associated with settlement calculations. This
research has aimed to minimise the error associated with settlement
prediction models by refining the parameterisation process and reducing
their subjectivity by implementing a gradient boosting model, returning the
appropriate Koppejan parameter based on an input of solely CPT data.</p>
      <p id="d1e1073">The model produced has indicated that there is some promise in using such a
method in developing a universal correlation for fine-grained soils in the
Netherlands and is readily extendible to other settlement prediction models
upon the provision of appropriate data. However, it is apparent that further
high-quality samples are required in order to produce a more robust and
stable model.</p>
      <p id="d1e1076">Nonetheless, the results show that machine learning methods offer a means of
discovering patterns in data which simpler regression methods are unable to
discover and with the<?pagebreak page447?> refinement of the CPT data, more accurate models can
be developed.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e1083">The dataset generated from this study is not publicly available due to commercial restrictions, however is available from the corresponding author on reasonable request.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e1089">KS and KD were involved in the data collection and data curation. KD performed the formal analysis using statistical models and visualisation under the supervision of KS and ML. KD wrote the paper with reviews by KS and ML. KS was involved in project administration.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e1095">The authors declare that they have no conflict of interest.</p>
  </notes><notes notes-type="sistatement"><title>Special issue statement</title>

      <p id="d1e1101">This article is part of the special issue “TISOLS: the Tenth International Symposium On Land Subsidence – living with subsidence”. It is a result of the Tenth International Symposium on Land Subsidence, Delft, the Netherlands, 17–21 May 2021.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e1107">The authors are extremely grateful for the support of colleagues at Fugro and University College Dublin. Special thanks go to Thijs Lukkezen of Fugro for his advice on the machine learning segment of the research, along with the supervisory committee at University College Dublin.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e1112">This research has been kindly supported by Fugro and forms part of the Master of Engineering programme at University College Dublin.</p>
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  </ref-list></back>
    <!--<article-title-html>Parameterisation of the Koppejan settlement prediction model using cone penetration testing and gradient boosting</article-title-html>
<abstract-html><p>This study examines how cone penetration test (CPT)
parameters, such as cone tip resistance and friction sleeve resistance, can
be used to assess the compressibility of fine-grained soils across the
Netherlands based on a database of 286 paired CPTs and oedometer tests from
across the country. This is done with the aim of refining and simplifying
the parameterisation of the Koppejan consolidation coefficients, a procedure
which can yield significant error and is prone to misinterpretation. It was
found that there is significant potential in using gradient boosting methods
to obtain a relationship between the CPT parameters and the Koppejan
parameters, with further investigation required into the noise within the
dataset and the acquisition of additional high-quality samples. The use of
such methods will offer a means of reducing the influence of human error or
misinterpretation on the prediction of settlement and provide further
confidence in the use of machine learning methods in engineering practice.</p></abstract-html>
<ref-html id="bib1.bib1"><label>1</label><mixed-citation>
Bjerrum, L.: Engineering geology of Norwegian normally-consolidated marine
clays as related to settlements of buildings, Géotechnique, 17, 83–118,
<a href="https://doi.org/10.1680/geot.1967.17.2.83" target="_blank">https://doi.org/10.1680/geot.1967.17.2.83</a>, 1967.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>2</label><mixed-citation>
Buisman, A. S.: Results of long duration settlement tests, in: Proceedings of the 1st International Conference on Soil Mechanics and Foundation Engineering, Cambridge, Massachusetts, 22–26 June 1936, 103–107, 1936.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>3</label><mixed-citation>
Buisman, A. S. K. and Huizinga, T. K.: Grondmechanica, Leerboek der
Toegepaste Mechanica: Deel IV, Waltman, Delft, the Netherlands, 281 pp., 1944 (in
Dutch).

</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>4</label><mixed-citation>
CROW: Betrouwbaarheid van zettingsprognoses, Publication 204, CROW, Ede, the
Netherlands, 116 pp., 2004 (in Dutch).
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>5</label><mixed-citation>
Den Haan, E. J.: Denkraam voor samendrukking van verknede en natuurlijke
klei: Nieuw <i>a</i>-<i>b</i>-<i>c</i> vereenvoudigt berekening zetting, Land en Water, 32,
25–29, 1992 (in Dutch).
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>6</label><mixed-citation>
Den Haan, E. J.: Vertical compression of soils, Ph.D. thesis, TU Delft, the
Netherlands, 97 pp., 1994.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>7</label><mixed-citation>
Duffy, K.: Assessment of a soil compressibility index using cone penetration
testing and machine learning tools, M. Eng. thesis, University College
Dublin, Ireland, 134 pp., 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>8</label><mixed-citation>
Friedman, J. H.: Greedy function approximation: a gradient boosting machine,
Ann. Statist., 29, 1189–1232, <a href="https://doi.org/10.1214/aos/1013203451" target="_blank">https://doi.org/10.1214/aos/1013203451</a>, 2001.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>9</label><mixed-citation>
Houkes, C. B.: Review and validation of settlement prediction methods for
organic soft soils, on the basis of three case studies from the Netherlands,
M.Sc. thesis, TU Delft, the Netherlands, 181 pp., 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>10</label><mixed-citation>
Jakobsen, P. D.: Estimation of soft ground tool life in TBM tunnelling,
Ph.D. thesis, NTNU, Trondheim, Norway, 253 pp., 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>11</label><mixed-citation>
Koppejan, A. W.: A formula combining the Terzaghi load-compression
relationship and the Buisman secular time effect, Proceedings of the 2nd
International Conference on Soil Mechanics and Foundation Engineering,
Rotterdam, the Netherlands, 21–30 June 1948, 32–37, 1948.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>12</label><mixed-citation>
Lengkeek, H. J., de Greef, J., and Joosten, S.: CPT based unit weight
estimation extended to soft organic soils and peat, Proceedings of the 4th
International Symposium on Cone Penetration Testing (CPT'18), Delft, the
Netherlands, 21–22 June 2018, 389–394, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>13</label><mixed-citation>
Lunne, T., Robertson, P. K., and Powell, J. J. M.: Cone Penetration Testing
in Geotechnical Practice, 1st Edn., CRC Press, London, UK, 352 pp., 1997.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>14</label><mixed-citation>
Maljers, D., Stafleu, J., van der Meulen, M. J., and Dambrink, R. M.:
Advances in constructing regional geological voxel models, illustrated by
their application in aggregate resource assessments, Neth. J. Geosci., 94,
257–270, <a href="https://doi.org/10.1017/njg.2014.46" target="_blank">https://doi.org/10.1017/njg.2014.46</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>15</label><mixed-citation>
Mitchell, J. K. and Gardner, W. S.: In situ measurement of volume change
characteristics, Geotechnical Speciality Conference on In Situ Measurement
of Soil Properties, Raleigh, USA, 1–4 June 1975, 279–345, 1975.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>16</label><mixed-citation>
Pedregosa, F., Varoquaux, G., Gramfort, A., Michel, V., Bertrand, T.,
Grisel, O., Blondel, M., Prettenhofer, P., Weiss, R., Dubourg, V.,
Vanderplas, J., Passos, A., Cournapeau, D., Brucher, M., Perrot, M., and
Duchesnay, É.: Scikit-learn machine learning in Python, J. Mach. Learn.
Res., 12, 2825–2830, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>17</label><mixed-citation>
Terzaghi, K.: Erdbaumechanik auf bodenphysikalischer grundlage, 1st ed.,
Franz Deuticke, Leipzig und Wien, Germany, 399 pp., 1925 (in German).
</mixed-citation></ref-html>--></article>
