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  <front>
    <journal-meta><journal-id journal-id-type="publisher">HESS</journal-id><journal-title-group>
    <journal-title>Hydrology and Earth System Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">HESS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Hydrol. Earth Syst. Sci.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1607-7938</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/hess-23-4835-2019</article-id><title-group><article-title>Technical note: Water table mapping accounting for river–aquifer connectivity and human pressure</article-title><alt-title>Technical note: Water table mapping</alt-title>
      </title-group><?xmltex \runningtitle{Technical note: Water table mapping}?><?xmltex \runningauthor{M. Maillot et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Maillot</surname><given-names>Mathias</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Flipo</surname><given-names>Nicolas</given-names></name>
          <email>nicolas.flipo@mines-paristech.fr</email>
        <ext-link>https://orcid.org/0000-0002-8099-2104</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Rivière</surname><given-names>Agnès</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6002-3189</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Desassis</surname><given-names>Nicolas</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Renard</surname><given-names>Didier</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9402-0007</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Goblet</surname><given-names>Patrick</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4540-4132</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Vincent</surname><given-names>Marc</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Geosciences Department, MINES ParisTech, PSL University, Fontainebleau, France</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>EPTB Seine Grands Lacs, Paris, France</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Maillot Mathias (mathias.maillot@mines-paristech.fr) and Nicolas Flipo (nicolas.flipo@mines-paristech.fr)</corresp></author-notes><pub-date><day>27</day><month>November</month><year>2019</year></pub-date>
      
      <volume>23</volume>
      <issue>11</issue>
      <fpage>4835</fpage><lpage>4849</lpage>
      <history>
        <date date-type="received"><day>27</day><month>February</month><year>2019</year></date>
           <date date-type="rev-request"><day>10</day><month>May</month><year>2019</year></date>
           <date date-type="rev-recd"><day>20</day><month>September</month><year>2019</year></date>
           <date date-type="accepted"><day>17</day><month>October</month><year>2019</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2019 Mathias Maillot et al.</copyright-statement>
        <copyright-year>2019</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://hess.copernicus.org/articles/23/4835/2019/hess-23-4835-2019.html">This article is available from https://hess.copernicus.org/articles/23/4835/2019/hess-23-4835-2019.html</self-uri><self-uri xlink:href="https://hess.copernicus.org/articles/23/4835/2019/hess-23-4835-2019.pdf">The full text article is available as a PDF file from https://hess.copernicus.org/articles/23/4835/2019/hess-23-4835-2019.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e144">A water table mapping method that accounts for surface-water–groundwater (SW-GW) connectivity and human pressure, such as pumping and underground structures occurrence, has been elaborated and tested in the heavily urbanized Parisian area. The method developed here consists of two steps. First, hard data (hydraulic head) and soft data (dry wells) are used as conditioning points for the estimation of the SW-GW connection status. A disconnection criteria of 0.75 m is adjusted on observed unsaturated zone depth (UZD). It is a default value in areas where such data are missing. The second step consists of the final mapping of the water table. Given the knowledge of the disconnection criteria, the final map is achieved with an ordinary kriging of the UZD that integrates the surface water elevation without unsaturated zone where it is relevant. The methodology is demonstrated on two datasets of UZD observations that were collected under low- and high-flow conditions.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e156">Water table maps are key tools for water resources and flood risk management.
A way to characterize a water table distribution is to describe it using piezometric maps. Although this seems an obvious statement, some methodological aspects require further development, such as the way to take into account uncertainty about surface water (SW) and groundwater (GW) connectivity.</p>
      <p id="d1e159"><?xmltex \hack{\newpage}?>This connectivity status can be either connected, transitional or disconnected <xref ref-type="bibr" rid="bib1.bibx20 bib1.bibx25 bib1.bibx8 bib1.bibx56" id="paren.1"/>. For the connected case, the surface water elevation corresponds to the water table and should be counted as an observation sample <xref ref-type="bibr" rid="bib1.bibx12 bib1.bibx69" id="paren.2"/>, whereas surface water level should not be considered when mapping in the disconnected case <xref ref-type="bibr" rid="bib1.bibx34" id="paren.3"/>.</p>
      <?pagebreak page4836?><p id="d1e172">The river–aquifer connectivity status depends on hydrological and geological parameters such as the surface water level, water table, riverbed geometry and hydrogeological parameters of the substratum  <xref ref-type="bibr" rid="bib1.bibx8 bib1.bibx52 bib1.bibx56" id="paren.4"/>. Water table and surface water level distribution results from precipitation, recharge of aquifers, topography, riverbed and aquifer geometries, and hydrodynamic parameters <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx6" id="paren.5"/>.
Urban GW is seriously affected by the development of urban areas in several ways. Besides the barrier effect induced by the occurrence of underground structures across groundwater flow, some modification of the water budget may be caused by the interaction between groundwater and these underground structures <xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx4" id="paren.6"/>. For instance, leaky sewer and water supply plumbing networks may act as recharge <xref ref-type="bibr" rid="bib1.bibx1" id="paren.7"/> or drain (in the case of sewers), limiting the water table rising above the structure <xref ref-type="bibr" rid="bib1.bibx17" id="paren.8"/>.
Generally speaking, human settlement nearby fluvial environments results in significant SW and GW decline due to pumping wells for domestic and industrial usages, as well as for underground structure protection and the construction of underground infrastructures  <xref ref-type="bibr" rid="bib1.bibx42 bib1.bibx61" id="paren.9"/>.
Moreover, the development of levees along the river and riverbed dredging generate major modifications of the stream–aquifer status. So far, all those aspects have not been taken into account in water table mapping methodologies.</p>
      <p id="d1e194">The most commonly used methods for the estimation of a continuous variable are linear estimators, neural networks and kriging <xref ref-type="bibr" rid="bib1.bibx66" id="paren.10"/>. The main linear estimators are inverse distance weighting (<xref ref-type="bibr" rid="bib1.bibx27" id="altparen.11"/>; <xref ref-type="bibr" rid="bib1.bibx53" id="altparen.12"/>; <xref ref-type="bibr" rid="bib1.bibx57" id="altparen.13"/>; <xref ref-type="bibr" rid="bib1.bibx9" id="altparen.14"/>; <xref ref-type="bibr" rid="bib1.bibx62" id="altparen.15"/>) and influence polygon or moving average <xref ref-type="bibr" rid="bib1.bibx67" id="paren.16"/>. These different methodologies were compared in several studies and kriging was found to be a better estimator in terms of cross-validation and performance than the other linear interpolators <xref ref-type="bibr" rid="bib1.bibx66 bib1.bibx21 bib1.bibx2 bib1.bibx50" id="paren.17"/> .
Although the linear estimation methods provide unbiased results, they do not account for the spatial heterogeneity of the sample distribution. The estimated value depends either on the nearest sampled value (influence polygon), or on every sampled value surrounding the estimation point (moving average) regardless of the distance between the estimation point and each individual sampling point. Inverse distance weighting involves the arbitrary choice of the distance degree. The distance degree is a conditioning setting for the variability of estimated fields whereas kriging involves a weighting of observation that is consistent with the spatial distribution of the variable.</p>
      <p id="d1e223">Recently, interpolations based on fuzzy logic or neural-network-derived methods have been tested <xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx62" id="paren.18"/>. These methods are still suffering a main drawback, which is that they produce results without coherent spatial error structures <xref ref-type="bibr" rid="bib1.bibx22" id="paren.19"/>.
The diffusion kernel interpolation method used in <xref ref-type="bibr" rid="bib1.bibx7" id="text.20"/> showed good results for large datasets. This method is based on geographically weighted regression which aims to map the trend of a variable <xref ref-type="bibr" rid="bib1.bibx31" id="paren.21"/>. Depending on the parameter used in the application of this methodology, the map produced can be very smoothed or noisy. This method allows for the spatial representation of estimation error; nevertheless there is no guarantee that the resulting map honors the input data.</p>
      <p id="d1e238">A widely accepted solution that provides information on estimation errors is kriging <xref ref-type="bibr" rid="bib1.bibx11 bib1.bibx43" id="paren.22"/>. It can be applied on different types of variables <xref ref-type="bibr" rid="bib1.bibx14" id="paren.23"/> including the water table <xref ref-type="bibr" rid="bib1.bibx35" id="paren.24"/>. Many studies produced water table maps resulting  from kriging in order to describe water table distributions <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx5 bib1.bibx9 bib1.bibx12 bib1.bibx34 bib1.bibx35 bib1.bibx40 bib1.bibx47 bib1.bibx71" id="paren.25"/>. <xref ref-type="bibr" rid="bib1.bibx58" id="text.26"/> noticed that water table data display spatial nonstationarities, which are due to the directional trends in hydraulic head gradients. Such nonstationarities cause problems in the determination of the experimental variogram and also generate large standard deviations of the estimation errors. A way to overcome the issues linked to nonstationarities was proposed by <xref ref-type="bibr" rid="bib1.bibx19" id="text.27"/>. Their methodology also based on kriging was developed for an unconfined aquifer. It relies on the spatial correlation between the water table and the topographic surface <xref ref-type="bibr" rid="bib1.bibx39 bib1.bibx63" id="paren.28"/>. This assumption was established by <xref ref-type="bibr" rid="bib1.bibx19" id="text.29"/> at large scales considering several watersheds. <xref ref-type="bibr" rid="bib1.bibx33" id="text.30"><named-content content-type="post">p. 786</named-content></xref> proposed that “shallow aquifers in flat or gently rolling terrain may exhibit a relatively low <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>/</mml:mo><mml:mi>k</mml:mi></mml:mrow></mml:math></inline-formula> ratio and still exhibit a water table that seems a subdued replica of the terrain surface”, where <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>[</mml:mo><mml:mi>m</mml:mi><mml:mo>/</mml:mo><mml:mi>d</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> is the areal recharge rate, and <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mi>k</mml:mi><mml:mo>[</mml:mo><mml:mi>m</mml:mi><mml:mo>/</mml:mo><mml:mi>d</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> is the aquifer hydraulic conductivity. This methodology, which targets the unsaturated zone depth (UZD) instead of the hydraulic head, leads to lower values of the standard deviation of the estimation error for unconfined aquifers in non-urbanized areas <xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx47 bib1.bibx55 bib1.bibx59" id="paren.31"/>.</p>
      <p id="d1e323">In urbanized areas, the pumping of GW implies the decline of the water table, which could lead to the drying out of a few piezometers. The knowledge of a dry well can be added to a dataset in the form of an inequality (i.e., UZD larger than the well depth) <xref ref-type="bibr" rid="bib1.bibx45" id="paren.32"/>. The use of such information translated into a mathematical inequality is not compatible with kriging itself. Therefore another methodology has to be used for water table mapping in such environments.</p>
      <p id="d1e329">A solution is the usage of multiple conditional simulations that provides a conditional expectancy map of the variable.
Its application in hydrogeology was demonstrated for hydrofacies determination <xref ref-type="bibr" rid="bib1.bibx16" id="paren.33"/>, converting lithofacies into hydrofacies to constrain groundwater flow models. This study proved that the use of
conditional probability reduces the variance of possible values of the targeted variable, for instance here hydrofacies properties. This methodology was applied in different geological contexts  <xref ref-type="bibr" rid="bib1.bibx65 bib1.bibx15" id="paren.34"/> proving its robustness and has not been applied to the UZD so far.</p>
      <p id="d1e338">The mapping methodology presented in this paper  relies on the assumption that the UZD variable is related to the topographic elevation and the river water level. The second assumption is that UZD is not related to the stream water level in the case of a disconnected hyporheic zone. Therefore, it can be applied to superficial aquifer units submitted to human pressures and other locations where the SW-GW connectivity is uncertain.
The following questions are addressed: (i) which methodological steps are required for water table mapping in alluvial plains? (ii) How do we account for human practices such as pumping in the mapping methodology? (iii) How do we determine the SW-GW connection status? (iv) Finally, what are the consequences of such<?pagebreak page4837?> methodological refinements on maps of the water table linked to hydrological events?</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Mapping methodology</title>
      <p id="d1e349">Water table mapping was initially developed for the description of regional aquifers into natural or pristine environments. The usual way of mapping a water table is to use synchronous UZD measurements resulting from snapshot campaigns. The synchronization of measurements is crucial to avoid experimental bias <xref ref-type="bibr" rid="bib1.bibx64" id="paren.35"/>. This section describes a methodology that combines conditional simulations of UZD, with an assessment of SW-GW connectivity and a final ordinary kriging of the UZD. Geostatistical processings are performed using the RGeostats R package <xref ref-type="bibr" rid="bib1.bibx54" id="paren.36"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><label>Figure 1</label><caption><p id="d1e360">Flow chart for the mapping of the water table. Steps 1 to 4 for the first-guess map. Step 5 for the final map. UZD: unsaturated zone depth. Diamonds display raw data, ellipses display input data after pre-processing and squares display intermediary products.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/23/4835/2019/hess-23-4835-2019-f01.png"/>

      </fig>

      <p id="d1e369">Figure <xref ref-type="fig" rid="Ch1.F1"/> describes the methodology. Firstly, the raw dataset is composed of each measured UZD for the corresponding measurement campaign. The raw dataset is then transformed into a Gaussian score dataset using an anamorphosis function fitting in order to obtain a Gaussian probability density function <xref ref-type="bibr" rid="bib1.bibx11" id="paren.37"/>. Inequality constrained samples (dry wells) are estimated using a Gibbs sampling of the Gaussian score subset <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx26" id="paren.38"/>. Thereafter, one hundred turning band simulations <xref ref-type="bibr" rid="bib1.bibx44" id="paren.39"/> are performed and averaged before their back-transformation into the real data. A first-guess map of the water table is obtained by averaging all back-transformed simulations. The SW-GW connectivity status is deduced from the first-guess map following a new connectivity criteria that permits the final UZD dataset to be constituted. The final water table map is finally produced by performing an ordinary kriging of the final UZD dataset. It is in this step that the UZD map is converted into a water table map, subtracting the UZD from a reference digital elevation model (DEM) of the ground.</p>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>First guess – simulations without considering the river water level</title>
      <p id="d1e391">The initial dataset is made of hard data and soft data. The hard data consist of UZD values measured during snapshot campaigns. The soft data are dry well depths.
The dataset is characterized in terms of spatial statistics in order to justify the use of an appropriate geostatistical tool.
UZD is defined in terms of a non-Gaussian probability density function conditioned with a non-negativity constraint.</p>
      <p id="d1e394">Water table and UZD variables may show some directional non-stationarities at the local scale, especially looking in the same direction as the directional gradients. Nevertheless, the directional gradients in UZD are much less pronounced than the water table gradients, making it more amenable to treatment with stationary geostatistics.
In the cases where a significant trend in the data is identified, the interpolation must be carried out using other geostatistical approaches, such as universal kriging, which deal with the non-stationarity of the variable <xref ref-type="bibr" rid="bib1.bibx30" id="paren.40"/>.</p>
<sec id="Ch1.S2.SS1.SSS1">
  <label>2.1.1</label><title>Input data pre-processing and DEM smoothing</title>
      <p id="d1e407">The use of UZD as a variable for mapping the water table requires the water table to be computed referring to the ground elevation.
In our approach the elevation of the ground is approximated using a smoothed DEM, called a reference DEM. It is obtained by merging a DEM and river water levels. This merged DEM is smoothed (Fig. <xref ref-type="fig" rid="Ch1.F1"/>, step 1) using the SAGA GIS algorithm <xref ref-type="bibr" rid="bib1.bibx13" id="paren.41"/> for moving-average filtering, this methodology was already proposed by <xref ref-type="bibr" rid="bib1.bibx47" id="text.42"/>. The smoothing of the DEM is required to avoid the occurrence of high-frequency topography signals that would not be relevant with the water table signal. The search radius is defined regarding two conditions: (i) the DEM has to be smoothed enough to remove its high-resolution noise and (ii) the information of river water level must be conserved in the final product.  We tested several radii to fit these conditions and found out an appropriate value of 325 m.</p>
      <p id="d1e418">The difference between rough DEM and smoothed DEM may be important in locations where the topographic slope is the most important. These locations include crucial areas near the riverbanks.
Therefore, this difference is calculated at each sampling point. Due to the use of UZD, this generates a biased estimation of the water table at these locations, given that this difference is not yet accounted for in the UZD measured value.
The way to tackle the DEM smoothing effect is to constitute a first data subset, deducting the difference between smoothed DEM data and true wellhead elevation from the raw UZD data before proceeding with the next steps of our procedure (Fig. <xref ref-type="fig" rid="Ch1.F1"/>).
For the sake of readability, this first data subset will still be called the UZD raw dataset in the rest of the paper.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS2">
  <label>2.1.2</label><title>Hard data selection and variograms</title>
      <p id="d1e431">The variographic analysis of the UZD raw dataset is achieved in order to describe the variability of UZD in a 2-D domain. In urbanized areas, anthropic pressure such as permanent pumping affects the natural correlation between DEM and UZD with the occurrence of local piezometric depletions. In terms of an experimental variogram, the use of samples affected by anthropic pressure induces a drastic increase in the semi-variogram value.
This cannot be considered as a representative variability of the UZD variable.
To prevent this effect on the experimental variogram calculation, the original dataset is divided  into  two categories (Fig. <xref ref-type="fig" rid="Ch1.F1"/>, step 2). The first category regroups all samples where the UZD value is affected by the pumping wells. The second category is composed of the other samples. Information about the locations of pumping wells is required to identify these samples.
In this study, the locations and pumping flow rates are not available. The affected and unaffected piezometers are differentiated regarding the correlation between the topography and the water table. <xref ref-type="bibr" rid="bib1.bibx32" id="text.43"/> stated that the water table within the capture zone of a pumping well is not hydrostatic; then it is assumed that topography and water table are not correlated within this capture zone. The samples where there is no correlation between the topography and the water table are identified as the affected samples. In this study, samples with a UZD value exceeding 10 m were found in that category. Note that this value may vary according to the case study.
This differentiation is required to elaborate a geostatistical tool (i.e., variogram model) that only depends on natural variability. Therefore, all the variographic studies are performed on this second category, called the unaffected UZD dataset. While the above procedure was used to roughly approximate which wells are affected by pumping, any future applications<?pagebreak page4839?> of the method outlined in this technical note should identify the wells impacted by pumping using actual data on pumping rates and locations.</p>
      <p id="d1e439">The experimental variograms are calculated on two types of variables: the Gaussian score used in the Gibbs sampling and conditional simulations, and the unaffected UZD dataset for the final ordinary kriging procedure. The Gaussian score variable used for Gibbs sampling-conditional simulation steps is described in the next subsections. UZD is the variable ultimately used for ordinary kriging.
Each calculated experimental variogram is a representation of the spatial variability of the dataset. A variogram model is fitted to each experimental variogram with a composition of spherical, exponential and cubic functions. The variogram fitting is achieved using an automated procedure <xref ref-type="bibr" rid="bib1.bibx18" id="paren.44"/>.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS3">
  <label>2.1.3</label><title>Anamorphosis function fitting</title>
      <p id="d1e454">In order to handle the non-Gaussian behavior of the UZD, one possibility is to transform a random function into a Gaussian function using an anamorphosis function fitting such that <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mi mathvariant="italic">φ</mml:mi><mml:mo>=</mml:mo><mml:msup><mml:mi>F</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>∘</mml:mo><mml:mi>G</mml:mi></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math id="M5" display="inline"><mml:mi mathvariant="italic">φ</mml:mi></mml:math></inline-formula> is the anamorphosis function, <inline-formula><mml:math id="M6" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> the continuous marginal distribution function of unaffected UZD and <inline-formula><mml:math id="M7" display="inline"><mml:mi>G</mml:mi></mml:math></inline-formula> the cumulative density function of the Gaussian score (<xref ref-type="bibr" rid="bib1.bibx11" id="altparen.45"/>). First, the cumulative histogram of the unaffected UZD dataset is established. Therefore, the corresponding Gaussian score is empirically obtained using the frequency inversion of unaffected UZD. The unaffected UZD dataset is transformed into a Gaussian score dataset using an anamorphosis function (Fig. <xref ref-type="fig" rid="Ch1.F1"/> step 3). This transformation was already used by <xref ref-type="bibr" rid="bib1.bibx23" id="text.46"/> to study aquifer contamination by nitrates.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS4">
  <label>2.1.4</label><title>Gibbs sampling – including soft data</title>
      <p id="d1e517">A dry well corresponds to soft data that can be formulated as constrained by an inequality. One way to deal with these data is to use Gibbs sampling in order to propose a realistic UZD value in accordance with the inequality. The Gibbs sampling method is a way to produce a realization of a Markov random field at a given location (<xref ref-type="bibr" rid="bib1.bibx28" id="altparen.47"/>; <xref ref-type="bibr" rid="bib1.bibx26" id="altparen.48"/>). This methodology can be directly applied to UZD data <xref ref-type="bibr" rid="bib1.bibx45" id="paren.49"/> in order to provide a value at each dry well. In this study, Gibbs sampling is applied to the Gaussian score dataset in order to obtain a re-sampled Gaussian score value at each dry well (Fig. <xref ref-type="fig" rid="Ch1.F1"/>, step 3).
This is made through the distinction between dry well bottom levels (soft data) and UZD measurements (hard data). The UZD measurements are accounted as equality constrained samples and dry well bottom levels are accounted as inequality constrained samples, constituting a lower limit for UZD value, or in other words a minimum value of UZD at the well location. For each dry well a potential value is calculated from successive simulations that reproduce a conditioned value of UZD matching the data distribution and the inequality constraint.</p>
      <p id="d1e531">At the end of the Gibbs sampling, the dry well bottom levels are replaced by a probable UZD value at dry well locations. This procedure leads to the constitution of a re-sampled Gaussian score dataset.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS5">
  <label>2.1.5</label><title>Conditional simulations</title>
      <p id="d1e542">The next step is the spatialization of the Gaussian score dataset using geostatistical simulations. The simulation of a random function is the calculation of a possible distribution that matches the variogram and the histogram and that honors the data <xref ref-type="bibr" rid="bib1.bibx38" id="paren.50"/>. In this study, the simulation is conditioned by the Gaussian score dataset and is performed on a grid covering the study area using the turning bands method <xref ref-type="bibr" rid="bib1.bibx44" id="paren.51"/>. The variogram model used is the same as the one used for Gibbs sampling. Once the simulation is calculated, the resulting Gaussian score map is back-transformed into a UZD map.</p>
      <p id="d1e551">A total of 100 conditional simulations are performed for the calculation of the first guess of the water table map.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS6">
  <label>2.1.6</label><title>First guess of the water table distribution</title>
      <p id="d1e562">Each Gaussian spatial distribution is back-transformed into a UZD spatial distribution. A preliminary map is obtained by averaging the 100 conditional UZD distributions. The first-guess map of the water table is obtained by deducing this preliminary UZD map from the reference DEM (Fig. <xref ref-type="fig" rid="Ch1.F1"/>, step 4).</p>
</sec>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Water table mapping accounting for uncertain SW-GW connectivity</title>
      <p id="d1e576">The second part of the mapping methodology is the final mapping of the water table, with the consideration of the SW-GW connection status: the connection status is evaluated for each cell located below the river network using a new disconnection criteria.</p>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>Defining a disconnection criteria at the reach scale</title>
      <?pagebreak page4840?><p id="d1e586">Stream–aquifer systems fluctuate from a hydraulically connected to a disconnected state due to the development of an unsaturated zone below the stream bed. During the switching between connection status, the SW-GW connection status is considered as a transitional state; this condition can occur when the capillary zone intersects the riverbed <xref ref-type="bibr" rid="bib1.bibx8" id="paren.52"/>. The disconnected SW-GW condition can occur under different settings such as in the case of high hydraulic conductivity contrast between the clogging layer and the aquifer <xref ref-type="bibr" rid="bib1.bibx8 bib1.bibx52" id="paren.53"/>, the lowering of the water table <xref ref-type="bibr" rid="bib1.bibx20 bib1.bibx25 bib1.bibx51 bib1.bibx56 bib1.bibx68" id="paren.54"/>, or the biological clogging of the riverbed <xref ref-type="bibr" rid="bib1.bibx48 bib1.bibx49 bib1.bibx70" id="paren.55"/>.
Considering a constant river water level and river width, the disconnection occurs when any further increase of the hydraulic head difference between the water table and the river water level does not affect the infiltration rate from the stream to the underlying aquifer, which remains constant. <xref ref-type="bibr" rid="bib1.bibx68" id="text.56"/> and <xref ref-type="bibr" rid="bib1.bibx56" id="text.57"/> proved that the disconnected state is reached when the saturation profile between the riverbed and the water table is stabilized. The saturation profile fills the space between an inverted area below the riverbed and a capillary fringe above the water table <xref ref-type="bibr" rid="bib1.bibx56 bib1.bibx68" id="paren.58"/>.
In the methodology, we assume that the disconnection state is reached when these two capillary fringes are separated without the occurrence of a clogging layer.
The thickness of these two areas is controlled by the capillary effect, which mainly depends on the lithology of both the riverbed and the aquifer.  <xref ref-type="bibr" rid="bib1.bibx29" id="text.59"/> proposed values for capillary fringe heights for several lithologies resulting from experimental measurements (Table <xref ref-type="table" rid="Ch1.T1"/>). The disconnection criteria is defined as the distance between the riverbed and water table above which the river water and the groundwater are disconnected. It means that for higher distances, a saturation profile develops between the inverted area below the riverbed and the capillary fringe overlying the water table. Accordingly, the disconnection state is identified for a given lithology at each river cell of the estimation grid, when the difference between the first-guess water table and the riverbed elevation equals or exceeds an empirical disconnection criteria. The methodology therefore requires either an explicit bathymetric description of the river or an estimation of the riverbed elevation.</p>
      <p id="d1e616">Starting from the knowledge of the riverbed lithology, the disconnection criteria can be estimated from <xref ref-type="bibr" rid="bib1.bibx29" id="text.60"/>, and this first guess is uncertain given that the distribution of sedimentary heterogeneities into the alluvial plain induces important lithological contrasts (<xref ref-type="bibr" rid="bib1.bibx37 bib1.bibx24" id="altparen.61"/>), and characterizing such heterogeneities requires important geophysical surveys that are out of reach for the development of our methodology.
At a station, the lithology is hence uncertain and a fortiori even more uncertain along a river reach. However, the disconnection criteria is defined as a threshold difference value between measured UZD and river water level from which the SW-GW connection status switches.
In the absence of such criteria in the literature, an optimization procedure is proposed along the Seine River network given that piezometers are available in the vicinity of the river and that both in-river water level and water table in the piezometers are recorded synchronously. The optimization procedure is described in the application section since it is based on the use of temporal data that are not directly required for the mapping methodology.</p>
      <p id="d1e625">If the two signals are correlated it indicates that the river and the aquifer are connected. Contrarily, a very low correlation indicates a disconnection. At the reach scale, many piezometers are available. The standardized and normalized hydraulic head and river water level are compared to assess the local connection status of SW-GW. On a scatter plot, the disconnection appears below a given slope of the regression line.</p>
      <p id="d1e628">At a reach scale it is therefore possible to inform the connection status locally (at a limited amount of stations). Along the river, the distance between the riverbed and the water table is evaluated from the first-guess map. The disconnection criteria is evaluated within a range defined by <xref ref-type="bibr" rid="bib1.bibx29" id="text.62"/> as the one that reproduces the most of the locally assessed connection status. In the absence of data, the disconnection criteria defined in our study can be used as a first guess.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e638">Values for the capillary fringe height, regarding the lithology, after <xref ref-type="bibr" rid="bib1.bibx29" id="text.63"/>.</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"/>
         <oasis:entry colname="col2">Sand</oasis:entry>
         <oasis:entry colname="col3">Silt</oasis:entry>
         <oasis:entry colname="col4">Clay</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Height of capillary fringe (m)</oasis:entry>
         <oasis:entry colname="col2">0.1–1</oasis:entry>
         <oasis:entry colname="col3">1–10</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <label>2.2.2</label><title>Final step of the mapping methodology</title>
      <p id="d1e709">Disconnected portions of river are deduced from the preliminary water table map with the application of the disconnection criteria.
A final dataset of UZD is then created from the UZD first guess at each sampling location, to which connected river sections are added with a nil UZD value.
An ordinary kriging is performed with this final UZD dataset (Fig. <xref ref-type="fig" rid="Ch1.F1"/>, step 5) for which a variogram model is fitted using the UZD data that are not affected by permanent pumping, as it is described in Sect. <xref ref-type="sec" rid="Ch1.S2.SS1.SSS2"/> (Fig. <xref ref-type="fig" rid="Ch1.F2"/>b and d). The kriging methodology consists of solving the following equation system:
              <disp-formula id="Ch1.Ex1"><mml:math id="M9" display="block"><mml:mfenced open="{" close=""><mml:mtable columnspacing="1em" class="cases" rowspacing="0.2ex" columnalign="left" framespacing="0em"><mml:mtr><mml:mtd><mml:mrow><mml:msup><mml:mi>Z</mml:mi><mml:mo>∗</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi mathvariant="italic">α</mml:mi></mml:munder><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mi>m</mml:mi><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mi mathvariant="normal">Var</mml:mi><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">00</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi mathvariant="italic">α</mml:mi></mml:munder><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced></mml:math></disp-formula>
            where <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:msup><mml:mi>Z</mml:mi><mml:mo>∗</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> is the estimation, <inline-formula><mml:math id="M11" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> is the observation point, <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the weights for observation point and mean value, <inline-formula><mml:math id="M14" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> is the residual value (i.e., absolute error), and <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">00</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mi mathvariant="italic">α</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> are the covariance function values for the origin and  the <inline-formula><mml:math id="M17" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> point. Therefore, the value of <inline-formula><mml:math id="M18" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> is not determined by solving this system, only the variance of <inline-formula><mml:math id="M19" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> is calculated.</p>
      <p id="d1e892">The final water table map is obtained using the reference DEM, from which the UZD kriged map is deduced.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><label>Figure 2</label><caption><p id="d1e897">Experimental variogram and fitted variogram model of unaffected UZD data and Gaussian score, for the LWC dataset <bold>(a, b)</bold> and HWC dataset <bold>(c, d)</bold>.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://hess.copernicus.org/articles/23/4835/2019/hess-23-4835-2019-f02.png"/>

          </fig>

</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results – water table mapping of Paris urban area</title>
      <p id="d1e922">The methodology is demonstrated on the Paris urban area. This urban area covers 900 km<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> and includes Paris city and its closest peripheral suburbs.</p><?xmltex \hack{\newpage}?>
<?pagebreak page4841?><sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Paris urban area</title>
      <p id="d1e942">The Seine and Marne rivers constitute a meandering fluvial system flowing from the southeast to the northwest (Fig. <xref ref-type="fig" rid="Ch1.F3"/>). The confluence between the Marne and the Seine River is located in the southeast of the study area.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><label>Figure 3</label><caption><p id="d1e949">Alluvial plain and regional substratum of the Paris urban area. Piezometers location for the two campaigns: low water campaign (LWC) and high water campaign (HWC).</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://hess.copernicus.org/articles/23/4835/2019/hess-23-4835-2019-f03.png"/>

        </fig>

      <p id="d1e958">The alluvial plain of the Seine and Marne rivers is overlying incised valleys of Eocene to Oligocene sedimentary series, exposing late Lutetian limestones in the south of the study area and early Bartonian limestones in the north (Fig. <xref ref-type="fig" rid="Ch1.F3"/>). Alluvial sediments constitute the alluvial aquifer and substratum of the Seine and Marne rivers. Lutetian and Bartonian limestones are underlying aquifers which are separated by thin heterogeneous and discontinuous formations with low hydraulic conductivity. The high proportion of soil sealed areas and the proliferation of pumping wells due to the urbanization reduce the infiltration of rainfall, making the anthropogenic pressure the main controlling factor of the water table and SW-GW connection status.</p>
      <p id="d1e964">Water tables have been monitored by water managers since the 1970s in central Paris area and since the 2000s in suburban areas. Water managers noticed that the water table of alluvial aquifer in the central area is usually stable at very low levels such that drying out of superficial aquifers may occur. The water table of peripheral areas remains unaffected by such water table drawdown.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><label>Figure 4</label><caption><p id="d1e969">Temporal analysis charts for SW-GW connection status determination: <bold>(a)</bold> recorded time series for river, disconnected piezometer and connected piezometer; <bold>(b)</bold> relationship between standardized river level and UZD for the disconnected piezometer and connected piezometer.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/23/4835/2019/hess-23-4835-2019-f04.png"/>

        </fig>

      <p id="d1e984">Regardless of the groundwater context, the Seine River is fully embanked, and the river bottom is periodically dredged for navigation purposes along the Paris city crossing. Given those anthropogenic forcings, water managers suspect that the Seine River may be disconnected from its underlying alluvial aquifer in some parts of the Paris central area. The interpretations of the joint response of the alluvial aquifer to hydrological events during the 1990–2018 period described further are supported by monthly records for UZD at monitored piezometers located near the Seine River. Seine River water levels vary under two different hydrological regimes (Fig. <xref ref-type="fig" rid="Ch1.F4"/>a): one nominal hydrological regime, corresponding to the low-flow periods during which the river flow and water level are artificially regulated for navigation and water management purposes, and one flood regime during which the river water level reaches the flood peak (eventually causing flood damages). The UZD can vary in relation with the Seine River water level or not. In the case of no variation of UZD, it is assumed that UZD is regulated by the GW pumpings, inducing a disconnection between the water table and river water level.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>UZD datasets: low- and high-flow campaigns</title>
      <p id="d1e997">This study is based on two UZD snapshot campaigns (Table <xref ref-type="table" rid="Ch1.T2"/>) involving measurements in piezometers that are not periodically monitored (Fig. <xref ref-type="fig" rid="Ch1.F3"/>): the low water campaign (LWC), which gathered 314 measurements during the low-flow period of October 2015, and the high water campaign (HWC), gathering 202 measurements during the June 2016 flood event.
Both campaigns lasted about a week. HWC took place a few days after the flood peak (1750 m<inline-formula><mml:math id="M21" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M22" 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>) was reached at the Parisian Austerlitz gauging station. The two datasets include around 22 % of samples affected by anthropic pressure (pumping wells and underground structures)  (Table <xref ref-type="table" rid="Ch1.T2"/>). Most of these samples are located in the Paris central area where the water table is affected by  permanent pumping.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e1030">Overview of the samples used for the application of water table mapping.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.93}[.93]?><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Total number</oasis:entry>
         <oasis:entry colname="col3">Number of wells</oasis:entry>
         <oasis:entry colname="col4">Number</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">of wells</oasis:entry>
         <oasis:entry colname="col3">affected by pumping wells</oasis:entry>
         <oasis:entry colname="col4">of dry wells</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">LWC</oasis:entry>
         <oasis:entry colname="col2">314</oasis:entry>
         <oasis:entry colname="col3">25</oasis:entry>
         <oasis:entry colname="col4">47</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">HWC</oasis:entry>
         <oasis:entry colname="col2">202</oasis:entry>
         <oasis:entry colname="col3">33</oasis:entry>
         <oasis:entry colname="col4">11</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Reference DEM for each campaign</title>
      <p id="d1e1120">The used DEM is the IGN scan 25 <xref ref-type="bibr" rid="bib1.bibx36" id="paren.64"/>. As previously mentioned, the DEM is first merged with hydrological data specific for each campaign. Then it is smoothed using a 325 m research radius for moving-average filtering.</p>
      <p id="d1e1126">River water levels are deduced from the recorded data of six discharge gauging stations. The distribution of river water levels is interpolated using a constant gradient between each gauging station. During low-flow periods, the average gradient value is 0.01 ‰. The Seine River discharge is regulated<?pagebreak page4842?> through a series of locks and dams for navigation purposes. At each lock station, water levels are maintained at a given elevation below a threshold water flow of 600 m<inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> s<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> at the Paris Austerlitz station. When a flood occurs as in June 2016, the lock stations are opened, and the water surface returns to its natural 0.2 ‰ gradient.
During the LWC, the Seine River discharge was 160 m<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M26" 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>, so that all locks were up, while they were open during the HWC, when the average discharge still reached 1000 m<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M28" 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> a week after the flood peak.</p>
</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Variograms</title>
      <p id="d1e1201">The experimental variograms and the associated fitted variogram models are depicted in Fig. <xref ref-type="fig" rid="Ch1.F2"/>.
For both datasets, the shape of the variograms is similar, with a sharp increase in the semi-variance near the origin, followed by a smooth evolution until it reaches the sill value. The range is higher for the LWC than for the HWC. The range of the Gaussian score is 12 km for LWC and 5 km for HWC (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a and b). The range of the raw data is 2 km for HWC while it is 6 km for the LWC. It can be noted that the variographic models for unaffected UZD data differ between LWC and HWC datasets in terms of sill value (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a and b). The sill value for the variogram model of the unaffected UZD HWC dataset is 8 m<inline-formula><mml:math id="M29" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> while it is 5 m<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> for the unaffected UZD LWC dataset.   This can be due to either the lower number of samples collected during the HWC, or to variations in the inner structure of the flow propagation process <xref ref-type="bibr" rid="bib1.bibx10 bib1.bibx60" id="paren.65"/>. For both campaigns (LWC and HWC), the variogram models of Gaussian scores have a range larger than the one of unaffected UZD datasets. This is due to the increase in the spatial correlation of the variable once the unaffected UZD data are transformed into Gaussian data.</p>
</sec>
<sec id="Ch1.S3.SS5">
  <label>3.5</label><title>Assessing the disconnection criteria</title>
      <p id="d1e1240">The Gaussian simulations are run on a 25 m <inline-formula><mml:math id="M31" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 25 m grid that matches the DEM resolution. The average of the hundred UZD values is subtracted to the smoothed DEM that includes river water levels evaluated for each hydrological context (LWC and HWC).
The streambed of the Seine River consists of mixed fine sand and silt. The a priori capillary fringe height is within 0.1 and 1.0 m (Table <xref ref-type="table" rid="Ch1.T1"/>). Therefore, the a priori value for the disconnection criteria is between 0.2  and 2 m.
The available observed data are composed of monthly measurements of UZD among 26 piezometers during the 1990–2018 period. These piezometers are distributed along 18 cross sections of the Seine River. For each piezometer, standardized UZD and river water level values are calculated.
As described in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2.SSS1"/>, the SW-GW connection status can be deduced from the relation between UZD and river water level. Two classes of piezometers are identified given the linear regression between standardized UZD and standardized river water level: disconnected piezometers and connected piezometers. Please note that during disconnection, the flow rate is still related to the hydraulic head<?pagebreak page4843?> difference. The transition cases are therefore included in the connected piezometer group.
In the case of a significant slope of the regression line (<inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.57</mml:mn></mml:mrow></mml:math></inline-formula>), the piezometer is considered connected. It is disconnected otherwise.
A total of 15 piezometers are considered as connected and 11 piezometers are considered as disconnected. Therefore, 9 cross sections along the Seine River are connected and 9 sections are disconnected (Fig. <xref ref-type="fig" rid="Ch1.F5"/>a).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><label>Figure 5</label><caption><p id="d1e1268">Graphical representation for disconnection criteria adjustment: <bold>(a)</bold> map of observed SW-GW status related to estimated SW-GW connection status using the optimal 0.75 m value for disconnection criteria; <bold>(b)</bold> relative number of valid SW-GW connection status out of nine disconnected cross sections and nine connected cross sections.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://hess.copernicus.org/articles/23/4835/2019/hess-23-4835-2019-f05.png"/>

        </fig>

      <p id="d1e1283">As an example, two contrasted situations among the 26 piezometers are displayed (Fig. <xref ref-type="fig" rid="Ch1.F4"/>a).
The UZD measured in the blue piezometer is linearly related to the river water level, while the UZD measured in the red piezometer remains roughly constant. There is a linear regression between UZD measured in the blue piezometer (Fig. <xref ref-type="fig" rid="Ch1.F4"/>b) which confirms that the blue piezometer is connected. In the case of disconnected piezometers, a constant UZD value is measured for most samples. It indicates that UZD is regulated artificially (Fig. <xref ref-type="fig" rid="Ch1.F4"/>a).</p>
</sec>
<sec id="Ch1.S3.SS6">
  <label>3.6</label><title>Sensitivity analysis of the disconnection criteria</title>
      <p id="d1e1300">The distribution of SW-GW connection status is constrained by the disconnection criteria. To estimate this criteria, a sensitivity analysis is achieved. The tested values range from 3  to 0.5 m with a 0.1 m step. This analysis shows that it is not possible to validate the connection status for all cross sections. Therefore, we compare the relative numbers of matched connected cross sections and disconnected cross sections. When the relative numbers are equal, the optimal value is reached, maximizing the total number of sections for which the connectivity status is correctly predicted. Different methods to evaluate the best criteria can be used (e.g., only valid disconnected cross sections or valid connected cross sections). In this study the maximization of relative number of connected and disconnected sections is used in order to obtain an average value of the disconnection criteria that does not favor either disconnection or connection. A way to obtain a better validation of cross section would be to spatialize the disconnection criteria. However, the spatialization of the<?pagebreak page4844?> disconnection criteria must be supported by geological arguments.
This optimal value is 0.75 m (Fig. <xref ref-type="fig" rid="Ch1.F5"/>b). This value is used to obtain the final water table maps.
The value of the disconnection criteria impacts the length of disconnected reaches. When the value for disconnection criteria is overestimated, the length of disconnected reach is underestimated. Contrarily, when the value is underestimated, the length of disconnected reaches is overestimated. In the application presented here for LWC, the length of disconnected reach for a 3 m disconnection criteria value is 150 m in the central area, while it reaches a 6 km length when the disconnection occurs for a 0.25 m disconnection criteria. When the optimal value of 0.75 m is applied for disconnection criteria, the length of disconnect reach is 5 km.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><label>Figure 6</label><caption><p id="d1e1307">Final water table maps obtained using ordinary kriging of UZD deduced from the reference DEM for <bold>(a)</bold> LWC and <bold>(b)</bold> HWC. The disconnected reaches of the river network are indicated in red for a disconnection criteria of 0.75 m.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://hess.copernicus.org/articles/23/4835/2019/hess-23-4835-2019-f06.png"/>

        </fig>

      <?pagebreak page4846?><p id="d1e1322">Further investigation could be carried out to evaluate the reliability of the estimated disconnection criteria, comparing it with the application of other methodologies such as those described in <xref ref-type="bibr" rid="bib1.bibx41" id="text.66"/>. Though this would allow for the determination of the SW-GW flow rate and hydrogeological dynamics, it cannot be applied in our case study context given that there are no data about the riverbed hydraulic conductivity. Such development would constitute a supplementary step after the water table mapping toward the description of the hydrological functioning of the study area.</p>
</sec>
<sec id="Ch1.S3.SS7">
  <label>3.7</label><title>Final mapping integrating SW-GW connectivity</title>
      <p id="d1e1336">The most important GW hydraulic gradients (1 %) are located close to the Seine and Marne rivers and the areas with an important topographic gradient (Fig. <xref ref-type="fig" rid="Ch1.F6"/>). The lowest values of hydraulic gradient are between 0.1 ‰  and 1 ‰  with an average 0.6 ‰ value in rather flat alluvial plains in the north area and the southeast area. The global flow pattern is therefore driven by SW-GW connection status and topography, with the exception of the central area where permanent pumping generates significant water drawdown and a subsequent SW-GW disconnection. In this area, the difference between riverbed elevation and estimated water table is 4 m. The implementation of disconnected reach during final mapping is a key element to reflect the specificity of urban groundwater such as water drawdown caused by pumping wells. The mapped water table near the disconnected reach is only affected by the observed depletion of the water table in wells and dry wells.
All disconnected sections are located in the central area during both campaigns. The rise in river water levels during HWC modifies the water table map significantly, especially in the vicinity of the river.</p>
      <p id="d1e1341">The SW-GW relation type for connected sections (gaining, losing and asymmetrical) is established regarding the head difference between the river water level and water table at a 50 m distance (two pixels of the map) from the river center-line. In cases where the river water level is higher than the water table for both river banks, the river is losing water to the aquifer. In the opposite case, the river is gaining groundwater. The sections where the river is gaining on one bank and losing on the other were also identified.</p>
      <p id="d1e1344">The main effect of flood events is to increase the river water level. In connected sections, the increase in hydraulic gradient between river and water table favors the river infiltration toward the aquifer. Comparing Fig. <xref ref-type="fig" rid="Ch1.F6"/>a with Fig. <xref ref-type="fig" rid="Ch1.F6"/>b, it appears that this infiltration causes the switching from losing to gaining SW-GW relation type during flood events. This is supported by the reduction of the total length of losing sections during LWC (Table <xref ref-type="table" rid="Ch1.T3"/>).
The hydrogeologic flow associated with the increase in infiltration induces the reconnection process propagating from the losing sections toward the disconnected sections.</p>
      <p id="d1e1353">As a consequence, almost the whole river network is reconnected to the GW, leading to a rise of the mapped water table. As pumping is increased during a flood to avoid damages against the buildings and underground infrastructures, a small portion of the Seine River remains disconnected in central Paris (0.75 km; see Fig. <xref ref-type="fig" rid="Ch1.F6"/>b).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3"><?xmltex \currentcnt{3}?><label>Table 3</label><caption><p id="d1e1362">Length of disconnected sections, connected gaining sections and connected losing sections, and head difference between the water table and riverbed calculated from preliminary mapping, for LWC and HWC.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">LWC</oasis:entry>
         <oasis:entry colname="col3">HWC</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Disconnected length (km)</oasis:entry>
         <oasis:entry colname="col2">4.9</oasis:entry>
         <oasis:entry colname="col3">0.8</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Losing sections length (km)</oasis:entry>
         <oasis:entry colname="col2">30.3</oasis:entry>
         <oasis:entry colname="col3">20.0</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Both gaining and losing (km)</oasis:entry>
         <oasis:entry colname="col2">38.3</oasis:entry>
         <oasis:entry colname="col3">39.3</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Gaining sections length (km)</oasis:entry>
         <oasis:entry colname="col2">11.5.4</oasis:entry>
         <oasis:entry colname="col3">25.0</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \hack{\newpage}?>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Conclusions</title>
      <p id="d1e1452">This study demonstrates an application for an innovative and generic mapping methodology of the water table in an urbanized alluvial environment.
Besides accounting for information brought by the knowledge of dry well locations and depth, the methodology introduces a SW-GW disconnection criteria for the first time in water table mapping.</p>
      <p id="d1e1455">The methodology is demonstrated for the case of the Paris urban area, for which it confirms GW managers' suspicion of a disconnection between SW and GW downtown Paris. Indeed, the water table appears to be locally depleted causing SW-GW disconnection with the alluvial aquifer.
Water table maps lead to the identification of spatialized SW-GW disconnected portions in the central area of the city. In the case of connected SW-GW, an important hydraulic gradient is observed in the vicinity of the river. In the case of a disconnected state, the water table remains unaffected by the hydrographic network and follows the natural slope of the DEM. Such a methodology offers the opportunity of an automated water table mapping connected with a GW monitoring network in urbanized areas exposed to flood risk.</p>
</sec>

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

      <p id="d1e1463">The dataset used for water table mapping was not acquired by the authors of this study and was kindly provided by the partners mentioned in the Acknowledgements section. These data are protected by a confidentiality agreement mentioning that it can not be widely broadcast by the authors.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e1469">All authors conceived the study and cowrote the paper. MM, NF and AR performed analyses.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e1475">The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e1481">This study has been carried with the support of the Programme d'Actions de Prévention des Inondations de la Seine et de la Marne franciliennes (PAPI SMF) steered by the Etablissement Public Territorial de Bassin Seine Grands Lacs (EPTB SGL, the Seine basin institution for river water flow regulation).<?pagebreak page4847?> The used synchronous datasets were produced and kindly provided by the Inspection Générale des Carrières (IGC, Mairie de Paris) and the other stakeholders involved in that program (Société du Grand Paris, Conseil départementaux de Seine Saint-Denis et du Val de Marne, RATP, CEREMA). We want to address special thanks to Anne-Marie Prunier-Leparmentier and Stéphanie Ventura-Mostacchi (IGC, Mairie de Paris) for their constant commitment and advice on water table monitoring in Paris city. This monitoring is a key point for the analysis of piezometric head time series. Their technical expertise about Paris city groundwater was also a major contribution to this publication. This work is also a contribution to the PIREN Seine research program on the Seine basin, part of the Long-Term Socio-Ecological Research (LTSER), French infrastructure Zones Atelier Seine. Finally, we kindly thank Graham E. Fogg for supervising the review process, as well as the two anonymous reviewers for their accurate comments, which helped improve the paper significantly.</p></ack><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e1486">This paper was edited by Graham Fogg and reviewed by two anonymous referees.</p>
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    <!--<article-title-html>Technical note: Water table mapping accounting for river–aquifer connectivity and human pressure</article-title-html>
<abstract-html><p>A water table mapping method that accounts for surface-water–groundwater (SW-GW) connectivity and human pressure, such as pumping and underground structures occurrence, has been elaborated and tested in the heavily urbanized Parisian area. The method developed here consists of two steps. First, hard data (hydraulic head) and soft data (dry wells) are used as conditioning points for the estimation of the SW-GW connection status. A disconnection criteria of 0.75&thinsp;m is adjusted on observed unsaturated zone depth (UZD). It is a default value in areas where such data are missing. The second step consists of the final mapping of the water table. Given the knowledge of the disconnection criteria, the final map is achieved with an ordinary kriging of the UZD that integrates the surface water elevation without unsaturated zone where it is relevant. The methodology is demonstrated on two datasets of UZD observations that were collected under low- and high-flow conditions.</p></abstract-html>
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