<?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-382-493-2020</article-id><title-group><article-title>Modelling subsidence due to Holocene soft-sediment deformation in the
Netherlands  under <?xmltex \hack{\break}?> dynamic water table conditions
</article-title><alt-title>Modelling subidence under dynamic water table conditions</alt-title>
      </title-group><?xmltex \runningtitle{Modelling subidence under dynamic water table conditions}?><?xmltex \runningauthor{H. Kooi and G. Erkens}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Kooi</surname><given-names>Henk</given-names></name>
          <email>henk.kooi@deltares.nl</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Erkens</surname><given-names>Gilles</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Deltares Research Institute, P.O. Box 85467, 3508 AL Utrecht, the
Netherlands</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Faculty of Geosciences, Utrecht University, P.O. Box 80115, 3508 TC
Utrecht, the Netherlands</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Henk Kooi (henk.kooi@deltares.nl)</corresp></author-notes><pub-date><day>22</day><month>April</month><year>2020</year></pub-date>
      
      <volume>382</volume>
      <fpage>493</fpage><lpage>498</lpage>
      
      <permissions>
        <copyright-statement>Copyright: © 2020 Henk Kooi</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/382/493/2020/piahs-382-493-2020.html">This article is available from https://piahs.copernicus.org/articles/382/493/2020/piahs-382-493-2020.html</self-uri><self-uri xlink:href="https://piahs.copernicus.org/articles/382/493/2020/piahs-382-493-2020.pdf">The full text article is available as a PDF file from https://piahs.copernicus.org/articles/382/493/2020/piahs-382-493-2020.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e84">Local and regional governments in The Netherlands are
increasingly faced with the question how to adjust and optimize groundwater
table conditions in urban areas to minimize ongoing subsidence and its
consequences. To help addressing this question, a model was developed that
includes soft-soil deformation by creep. In this paper, a study is presented
in which the model was used to investigate and intercompare the
effectiveness of measures that (a) prevent anomalous water table drop during
a drought, (b) suppress the seasonal variability of the water table, and (c) involve a permanent rise of the mean water table.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e96">Urban areas in the western part of The Netherlands commonly show persistent
subsidence over multiple decades at rates between 0–10 mm yr<inline-formula><mml:math id="M1" 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>. At the same
time, buildings with a foundation in Pleistocene strata usually show much
smaller to negligible subsidence, indicating that the land surface
subsidence is mainly caused by slow deformation of clay and peat deposits in
the Holocene strata. In contrast to areas with peat oxidation, in urban
areas, the persistent nature of the subsidence is thought to be the
expression of viscous behaviour (creep) of the subsurface, under periodic
addition of fill at the surface to compensate for elevation loss and/or
water table lowering. The subsidence causes damage to pipes and cables,
damage to buildings and infrastructure without pile foundation, damage to
buildings due to decay of wooden pile foundations if the water table is
lowered, nuisance flooding, and high maintenance costs of public space
functions. Because (ground)water level change can provoke subsidence, and
local and regional governments are responsible for groundwater levels in the
public space, these governments are faced with the question how to adjust
and optimize water table conditions to minimize the subsidence and its
consequences. To be able to choose among potential measures, questions they
seek answers to include: How much subsidence can be prevented by:
<list list-type="custom"><list-item><label>a.</label>
      <p id="d1e113">preventing excessive water table lowering during an occasional drought;</p></list-item><list-item><label>b.</label>
      <p id="d1e117">permanent damping of seasonal water table variations;</p></list-item><list-item><label>c.</label>
      <p id="d1e121">raising of the
mean water table?</p></list-item></list></p>
      <p id="d1e124">In this study, modelling was used to address these questions.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Model formulation</title>
      <p id="d1e142">A 1-dimensional mathematical model was built that quantifies the concepts
depicted in Fig. 1. The model domain consists of Holocene peat and clay
layers. Coupled groundwater flow and deformation (consolidation/swelling)
are calculated in these layers, resulting in vertical land movement relative
to the underlying Pleistocene aquifer. The natural Holocene stack is
overlain by an anthropogenic cover layer (fill), generally consisting of
debris and sand that was added in the course of history. The phreatic water
table sits within the cover layer and varies in response to weather
conditions and<?pagebreak page494?> human interference. The water table variations directly
impact the pore pressure and the geostatic stress in the underlying layers
due to the changes in cover layer weight (water content change), and
indirectly impact pore pressures by the changing head at the base of the
cover layer, which acts as the upper drainage boundary for consolidation and
swelling in the peat and clay stack.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><label>Figure 1</label><caption><p id="d1e147">Conceptual model.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://piahs.copernicus.org/articles/382/493/2020/piahs-382-493-2020-f01.png"/>

        </fig>

      <p id="d1e156">Deformation is calculated employing an isotache-based, viscoelastic
compression model that is used in certified geotechnical software for
settlement modelling in The Netherlands and other countries. The viscous
deformation is referred to as creep. The creep strain in the isotache model
is a generalization of, and therefore replaces, the ideal-plastic
deformation of Terzaghi's classical elastoplastic compression model. That
is, all irreversible deformation in the isotache model is caused by creep.
The model uses three compression parameters: swelling constant <inline-formula><mml:math id="M2" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula>,
compression constant <inline-formula><mml:math id="M3" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>, secondary compression constant <inline-formula><mml:math id="M4" display="inline"><mml:mi>c</mml:mi></mml:math></inline-formula>; and an
(initial) overconsolidation ratio OCR. For a given set of values of the
compression parameters, the momentary viscous (creep) time rate of (natural)
strain <inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">cr</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is a function of OCR:
            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M6" display="block"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">cr</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>c</mml:mi><mml:mi mathvariant="italic">τ</mml:mi></mml:mfrac></mml:mstyle><mml:mspace linebreak="nobreak" width="1em"/><mml:mspace width="1em" linebreak="nobreak"/><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">τ</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub><mml:msup><mml:mi mathvariant="normal">OCR</mml:mi><mml:mstyle scriptlevel="+1"><mml:mfrac><mml:mrow><mml:mi>b</mml:mi><mml:mo>-</mml:mo><mml:mi>a</mml:mi></mml:mrow><mml:mi>c</mml:mi></mml:mfrac></mml:mstyle></mml:msup></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">τ</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> d. <inline-formula><mml:math id="M8" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> is intrinsic time, which can be taken as
an apparent age of the clay or peat, where young age corresponds to high,
and old age to low creep rates. For a comprehensive description of the
model, see Den Haan (1994) or Kooi et al. (2018). The model equations are
solved with FlexPDE 6.50, a scripted finite element solution environment for
partial differential equations.</p>
      <p id="d1e269">The model does not account for shrink and swell associated with seasonal
desiccation and wetting of clay-rich units in the unsaturated zone (e.g., te
Brake et al., 2013).</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Parameter values</title>
      <p id="d1e280">Table 1 lists the parameter values that were used for peat, clay and the
anthropogenic cover layer in the calculations presented here. Deformation of
the cover layer is assumed to be negligible. Hydraulic conductivity of peat
and clay was assigned a fixed value of 5 mm d<inline-formula><mml:math id="M9" 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>. These are
representative values that provide a fair impression of the impacts of the
water table scenarios. The values of OCR were varied (by specifying <inline-formula><mml:math id="M10" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula>) in order to vary the background (initial) subsidence rate by creep. A
comprehensive sensitivity analysis is beyond the scope of this paper.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e305">Parameter values per lithology.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.9}[.9]?><oasis:tgroup cols="6">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M11" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M12" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M13" display="inline"><mml:mi>c</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi mathvariant="normal">sat</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi mathvariant="normal">unsat</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(–)</oasis:entry>
         <oasis:entry colname="col3">(–)</oasis:entry>
         <oasis:entry colname="col4">(–)</oasis:entry>
         <oasis:entry colname="col5">(kN m<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col6">(kN m<inline-formula><mml:math id="M17" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">anthropogenic</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
         <oasis:entry colname="col5">20.4</oasis:entry>
         <oasis:entry colname="col6">18.4</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">peat</oasis:entry>
         <oasis:entry colname="col2">0.017</oasis:entry>
         <oasis:entry colname="col3">0.13</oasis:entry>
         <oasis:entry colname="col4">0.009</oasis:entry>
         <oasis:entry colname="col5">11.5</oasis:entry>
         <oasis:entry colname="col6">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">clay</oasis:entry>
         <oasis:entry colname="col2">0.005</oasis:entry>
         <oasis:entry colname="col3">0.065</oasis:entry>
         <oasis:entry colname="col4">0.003</oasis:entry>
         <oasis:entry colname="col5">18.5</oasis:entry>
         <oasis:entry colname="col6"/>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Model runs</title>
      <p id="d1e504">The model was run for the three-layer configuration shown in Fig. 1, with a
thickness of 3, 7 and 2 m for the anthropogenic, peat and clay layer,
respectively. This layering approximates subsurface conditions in the city
of Gouda (Van Laarhoven, 2017). Seasonal water table variations are
represented by a sine-function. In reference runs, the mean annual water
table is 1 m below land surface and the amplitude 0.5 m. Table 2 summarizes
the three modified water table scenarios “dry summer”, “damping”, and
“raising” that were used to study their impacts. The magnitude of the
applied perturbations is rather large compared to what is generally feasible
in practice. This was done to bring out the impacts more clearly.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e510">Scenarios for the perturbation applied to the reference ground
water table condition.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">scenario</oasis:entry>
         <oasis:entry colname="col2">description</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">drought</oasis:entry>
         <oasis:entry colname="col2">amplitude <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula> m <italic>in</italic> dry season year 8</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">damping</oasis:entry>
         <oasis:entry colname="col2">amplitude <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula> m applied <italic>after</italic> year 9</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">raising</oasis:entry>
         <oasis:entry colname="col2">annual mean <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> m applied <italic>after</italic> year 9</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e603">Note that for “drought” the reference and the scenario should formally be
swapped to evaluate the impact of mitigation measures that prevent excessive
water table lowering during the drought. In the runs hydraulic head at the
base of the clay is kept constant and equal to the mean ground water table.
A period of 25 years is simulated.</p>
      <?pagebreak page495?><p id="d1e607">To study how impacts of water table scenarios vary as a function of the
background (or initial) subsidence rate, values of 10, 20 and 100 years were
assigned to the initial intrinsic time <inline-formula><mml:math id="M21" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> for both the peat and clay
layer. These <inline-formula><mml:math id="M22" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> values can be converted to corresponding values of
OCR using Eq. (1) and the parameter values listed in Table 1.
<?xmltex \hack{\newpage}?></p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
      <p id="d1e634">Figure 2 presents the calculated vertical land movement of the reference
runs. <inline-formula><mml:math id="M23" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> values of 100, 20 and 10 years yield initial subsidence rates of
about 1, 3 and 5 mm yr<inline-formula><mml:math id="M24" 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>, respectively. The total movement includes
oscillations with an amplitude of about 5 mm that are predominantly caused
by the elastic response of the peat and the clay to the seasonal stress
changes. The accumulated irreversible, inelastic subsidence is labelled
“creep”. It includes subtle seasonal variations indicating that the creep
rate accelerates (with some delay) when the water table declines and
decelerates when the water table rises.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><label>Figure 2</label><caption><p id="d1e658">Calculated subsidence for the reference runs.</p></caption>
        <?xmltex \igopts{width=221.931496pt}?><graphic xlink:href="https://piahs.copernicus.org/articles/382/493/2020/piahs-382-493-2020-f02.png"/>

      </fig>

      <p id="d1e667">Figures 3–5 present the calculated vertical land movement for the three
water table scenarios. To visualize the impact of the changed conditions,
the creep component of the reference runs (Fig. 2) is shown for reference.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><?xmltex \currentcnt{3}?><label>Figure 3</label><caption><p id="d1e673">Calculated subsidence for scenario “dry summer”. The creep of the
reference runs is depicted as “ref. creep”.</p></caption>
        <?xmltex \igopts{width=213.395669pt}?><graphic xlink:href="https://piahs.copernicus.org/articles/382/493/2020/piahs-382-493-2020-f03.png"/>

      </fig>

<?xmltex \hack{\newpage}?><?xmltex \floatpos{t}?><fig id="Ch1.F4"><?xmltex \currentcnt{4}?><label>Figure 4</label><caption><p id="d1e685">Calculated subsidence for scenario “damping”. The creep of the
reference runs is depicted as “ref. creep”.</p></caption>
        <?xmltex \igopts{width=213.395669pt}?><graphic xlink:href="https://piahs.copernicus.org/articles/382/493/2020/piahs-382-493-2020-f04.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><label>Figure 5</label><caption><p id="d1e696">Calculated subsidence for scenario “raising”. The creep of the
reference runs is depicted as “ref. creep”.</p></caption>
        <?xmltex \igopts{width=213.395669pt}?><graphic xlink:href="https://piahs.copernicus.org/articles/382/493/2020/piahs-382-493-2020-f05.png"/>

      </fig>

</sec>
<?pagebreak page496?><sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Discussion and conclusions</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Elucidation of results of the scenarios</title>
<sec id="Ch1.S4.SS1.SSS1">
  <label>4.1.1</label><title>Drought scenario</title>
      <p id="d1e727">Figure 3 shows that a single dry season with 1 m extra water table
lowering, has a distinct subsidence impact (up to about 1 cm). However, most
of this subsidence is due to elastic deformation and is recovered by the end
of the drought. The net impact of the drought – defined here by the
difference between the “creep” and “ref. creep” curves – is induced by
enhancement of the rate of creep during the period in which the water table
is anomalously low. The duration of this period (6 months in the
simulation), therefore, is an important factor that determines the magnitude
of the post-drought impact. The results further show that the impact is more
significant for low values of <inline-formula><mml:math id="M25" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> (low OCR and high background subsidence
rate). Furthermore, the loading and unloading caused by the drought and its
recovery leaves the peat and clay mildly overconsolidated after the drought.
That<?pagebreak page497?> is, the OCR is slightly enhanced, and the creep rate slightly reduced
after the drought. This is visible in Fig. 3c where the “creep” and “ref.
creep” curve very slowly converge over the years after the drought. The net
impact of the drought is very small relative to the background subsidence.</p>
</sec>
<sec id="Ch1.S4.SS1.SSS2">
  <label>4.1.2</label><title>Damping scenario</title>
      <p id="d1e745">The reduction of the amplitude of seasonal water table variation by 0.4 m
(80 %) moderates the seasonal variation of the total land surface
movement by approximately the same amount, and the annual average creep rate
is slightly reduced (Fig. 4). The impact of the latter, in terms of
millimetres of subsidence prevented, takes many years to decades to develop.
The reduction of the annual creep rate is the result of opposing
contributions of the wet and the dry season. The raised water table during
the dry period compared to the reference condition, reduces the creep rate
in that season. However, during the wet season, the lower water table
compared to the reference condition enhances the creep rate during that
time. The contribution of the dry season prevails in the net impact. This
indicates that the effectiveness would be larger if only the dry season
water table would be raised, and the wet season water table would be left
untouched. The net impact of the drought is very small relative to the
background subsidence.</p>
</sec>
<sec id="Ch1.S4.SS1.SSS3">
  <label>4.1.3</label><title>Raising scenario</title>
      <p id="d1e756">The permanent increase of the mean water table by 0.4 m has both a direct
and a secular effect on the land surface elevation (Fig. 5). The direct
effect consists of elastic uplift/heave of about 5 mm. The secular effect
consists of the reduction of the creep rate. The reduction of the creep rate
is permanent and applies to both the wet and the dry season (the amplitude
of water table variation is not modified in this scenario). Comparison with
Figs. 3 and  4 reveals that the impact of permanently raising of the
water table is larger than for the other two scenarios. The greater impact
is due to the permanent reduction of the creep rate. However, since water
tables are already maintained at rather shallow depth in parts of The
Netherlands that contain Holocene soft-soils, localities where water table
can be raised by several decimetres or more without causing damage are
probably very limited.</p>
</sec>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Need for field- and laboratory testing</title>
      <p id="d1e768">The isotache model employed in this study, includes modern-day concepts of
the soil mechanics of Holocene peat and clay. This model has been developed
for the modelling of, and is primarily tested against, settlement caused by
large loads such as dikes, and surcharge that is applied in areas where new
residential areas are being built. It is presently unclear to what extent
the model also accurately represents creep rates and creep behaviour for the
small loads associated with the water table scenarios considered in this
manuscript. Dedicated field- and laboratory tests are needed to shed more
light on creep rates and creep behaviour for effective stress levels at or
below the preconsolidation stress, and to test the validity of presented
results.</p>
</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>Conclusions</title>
      <p id="d1e779">Modelling employing an isotache-based viscoelastic compression model adopted
from certified geotechnical software for settlement modelling allows
quantitative assessment of the subsidence impact of interferences in water
table conditions in urban areas.</p>
      <p id="d1e782">Model results indicate that:
<list list-type="bullet"><list-item>
      <p id="d1e787">The absolute subsidence impact of measures increases with increasing
background subsidence rate.</p></list-item><list-item>
      <p id="d1e791">The effectiveness of measures increases with the duration of the period
during which water tables are raised. That is, permanent raising tends to be
more effective than periodic or occasional prevention of water table drops.</p></list-item><list-item>
      <p id="d1e795">For conditions that exist in urban areas in The Netherlands, water table
interventions are predicted to prevent a fraction of the subsidence that
would have occurred without the intervention.</p></list-item></list></p>
</sec>
</sec>

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

      <p id="d1e804">No data sets were used in this article.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e810">HK conceptualized the analysis, developed the model scripts, conducted the experiments and wrote the original draft of the manuscript. GE reviewed and edited the draft manuscript.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e816">Co-author Gilles Erkens is member of the editorial board of  the special issue but was not responsible for the acceptance of the manuscript for publication.</p>
  </notes><notes notes-type="sistatement"><title>Special issue statement</title>

      <p id="d1e822">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><ref-list>
    <title>References</title>

      <ref id="bib1.bib1"><label>1</label><?label 1?><mixed-citation>
Den Haan, E. J.: Vertical Compression of Soils, PhD Dissertation, Technical
University of Delft, 96 pp., 1994.</mixed-citation></ref>
      <ref id="bib1.bib2"><label>2</label><?label 1?><mixed-citation>Kooi, H., Bakr, M., de Lange, G., den Haan, E., and Erkens, G.: User guide to
SUB-CR; a MODFLOW package fo<?pagebreak page498?>r land subsidence and aquifer system compaction
that includes creep, Deltares internal report 11202275-008, available at: <uri>http://publications.deltares.nl/11202275_008.pdf</uri> (last access: 25 February 2020), 2018.</mixed-citation></ref>
      <ref id="bib1.bib3"><label>3</label><?label 1?><mixed-citation>te Brake, B., van der Ploeg, M. J., and de Rooij, G. H.: Water storage change estimation from in situ shrinkage measurements of clay soils, Hydrol. Earth Syst. Sci., 17, 1933–1949, <ext-link xlink:href="https://doi.org/10.5194/hess-17-1933-2013" ext-link-type="DOI">10.5194/hess-17-1933-2013</ext-link>, 2013.
</mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bib4"><label>4</label><?label 1?><mixed-citation>Van Laarhoven, S.: Influence of loading history on subsurface architecture
and subsidence potential for the historical city of Gouda, The Netherlands,
MSc Thesis, Utrecht University, 159 pp., 2017.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>Modelling subsidence due to Holocene soft-sediment deformation in the Netherlands  under  dynamic water table conditions </article-title-html>
<abstract-html><p>Local and regional governments in The Netherlands are
increasingly faced with the question how to adjust and optimize groundwater
table conditions in urban areas to minimize ongoing subsidence and its
consequences. To help addressing this question, a model was developed that
includes soft-soil deformation by creep. In this paper, a study is presented
in which the model was used to investigate and intercompare the
effectiveness of measures that (a) prevent anomalous water table drop during
a drought, (b) suppress the seasonal variability of the water table, and (c) involve a permanent rise of the mean water table.</p></abstract-html>
<ref-html id="bib1.bib1"><label>1</label><mixed-citation>
Den Haan, E. J.: Vertical Compression of Soils, PhD Dissertation, Technical
University of Delft, 96 pp., 1994.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>2</label><mixed-citation>Kooi, H., Bakr, M., de Lange, G., den Haan, E., and Erkens, G.: User guide to
SUB-CR; a MODFLOW package for land subsidence and aquifer system compaction
that includes creep, Deltares internal report 11202275-008, available at: <a href="http://publications.deltares.nl/11202275_008.pdf" target="_blank"/> (last access: 25 February 2020), 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>3</label><mixed-citation>
te Brake, B., van der Ploeg, M. J., and de Rooij, G. H.: Water storage change estimation from in situ shrinkage measurements of clay soils, Hydrol. Earth Syst. Sci., 17, 1933–1949, <a href="https://doi.org/10.5194/hess-17-1933-2013" target="_blank">https://doi.org/10.5194/hess-17-1933-2013</a>, 2013.

</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>4</label><mixed-citation>Van Laarhoven, S.: Influence of loading history on subsurface architecture
and subsidence potential for the historical city of Gouda, The Netherlands,
MSc Thesis, Utrecht University, 159 pp., 2017.
</mixed-citation></ref-html>--></article>
