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<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" article-type="research-article"><?xmltex \bartext{Development and technical paper}?>
  <front>
    <journal-meta><journal-id journal-id-type="publisher">GMD</journal-id><journal-title-group>
    <journal-title>Geoscientific Model Development</journal-title>
    <abbrev-journal-title abbrev-type="publisher">GMD</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Geosci. Model Dev.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1991-9603</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/gmd-15-7099-2022</article-id><title-group><article-title>Coupling a large-scale hydrological model (CWatM v1.1) with a high-resolution groundwater flow model (MODFLOW 6) to<?xmltex \hack{\break}?> assess the impact of irrigation at regional scale</article-title><alt-title>Coupling CWatM v1.1 with MODFLOW 6​​​​​​​</alt-title>
      </title-group><?xmltex \runningtitle{Coupling CWatM v1.1 with MODFLOW 6​​​​​​​}?><?xmltex \runningauthor{L. Guillaumot et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Guillaumot</surname><given-names>Luca</given-names></name>
          <email>guillaumot@iiasa.ac.at</email>
        <ext-link>https://orcid.org/0000-0002-6579-6287</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Smilovic</surname><given-names>Mikhail</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-9651-8821</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Burek</surname><given-names>Peter</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-6390-8487</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>de Bruijn</surname><given-names>Jens</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Greve</surname><given-names>Peter</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9454-0125</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Kahil</surname><given-names>Taher</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7812-5271</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Wada</surname><given-names>Yoshihide</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4770-2539</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Water Security Research Group, Biodiversity and Natural Resources
Program, International Institute for Applied Systems Analysis (IIASA),
Laxenburg, Austria</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Institute for Environmental Studies, VU University, De Boelelaan
1087, 1081HV, Amsterdam, the Netherlands</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Luca Guillaumot (guillaumot@iiasa.ac.at)</corresp></author-notes><pub-date><day>20</day><month>September</month><year>2022</year></pub-date>
      
      <volume>15</volume>
      <issue>18</issue>
      <fpage>7099</fpage><lpage>7120</lpage>
      <history>
        <date date-type="received"><day>16</day><month>June</month><year>2022</year></date>
           <date date-type="rev-request"><day>23</day><month>June</month><year>2022</year></date>
           <date date-type="rev-recd"><day>21</day><month>August</month><year>2022</year></date>
           <date date-type="accepted"><day>24</day><month>August</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Luca Guillaumot et al.</copyright-statement>
        <copyright-year>2022</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://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022.html">This article is available from https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022.html</self-uri><self-uri xlink:href="https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022.pdf">The full text article is available as a PDF file from https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e145">In the context of changing climate and increasing water
demand, large-scale hydrological models are helpful for understanding and
projecting future water resources across scales. Groundwater is a critical
freshwater resource and strongly controls river flow throughout the year. It
is also essential for ecosystems and contributes to evapotranspiration,
resulting in climate feedback. However, groundwater systems worldwide are
quite diverse, including thick multilayer aquifers and thin heterogeneous
aquifers. Recently, efforts have been made to improve the representation of
groundwater systems in large-scale hydrological models. The evaluation of
the accuracy of these model outputs is challenging because (1) they are
applied at much coarser resolutions than hillslope scale, (2) they simplify
geological structures generally known at local scale, and (3) they do not
adequately include local water management practices (mainly groundwater
pumping). Here, we apply a large-scale hydrological model (CWatM), coupled
with the groundwater flow model MODFLOW, in two different climatic,
geological, and socioeconomic regions: the Seewinkel area (Austria) and the
Bhima basin (India). The coupled model enables simulation of the impact of
the water table on groundwater–soil and groundwater–river exchanges,
groundwater recharge through leaking canals, and groundwater pumping. This
regional-scale analysis enables assessment of the model's ability to
simulate water tables at fine spatial resolutions (1 km for CWatM, 100–250 m for MODFLOW) and when groundwater pumping is well estimated. Evaluating
large-scale models remains challenging, but the results show that the
reproduction of (1) average water table fluctuations and (2) water table
depths without bias can be a benchmark objective of such models. We found
that grid resolution is the main factor that affects water table depth bias
because it smooths river incision, while pumping affects time fluctuations.
Finally, we use the model to assess the impact of groundwater-based
irrigation pumping on evapotranspiration, groundwater recharge, and water
table observations from boreholes.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e157">Regional- and large-scale hydrological models are often used to assess water
resource trajectories under different scenarios for climate change,
socioeconomic development, and water management. Despite extensive work, at
least three challenges persist: appropriately representing groundwater
dynamics and flow
(Gleeson
et al., 2021; Kollet and Maxwell, 2008; Reinecke et al., 2020; Sutanudjaja
et al., 2011; Vergnes et al., 2014), including human impact
(Hanasaki
et al., 2018; Wada et al., 2017, 2014), and improving spatial resolution
(Bierkens,
2015; Fan et al., 2019; Wood et al., 2011). The last point can be replaced
in part by “representing water flows driven by small-scale topography” and
is of interest for processes at large scale and locally relevant
applications. Several large-scale hydrological models include
representations of groundwater flow between grid cells and interactions
among groundwater, soils, and surface water bodies, such as CWatM
(Burek et al., 2020), LISFLOOD
(Trichakis et al., 2017), ORCHIDEE
(Verbeke et al., 2019), ParFlow-CLM
(Keune et al.,
2016; Maxwell et al., 2015), PCR-GLOBWB
(de Graaf et al., 2017;
Sutanudjaja et al., 2018), ISBA-CTRIP (Decharme et
al., 2019), VIC (Scheidegger et al., 2021),
LEAFHYDRO (Martínez-de la Torre and
Miguez-Macho, 2019), and WaterGAP
(Reinecke et al., 2019a).
These models differ somewhat in their implementation, including the physical
representation and parametrization of the groundwater. Currently,
developments are oriented towards hyper-resolution models (less than or
around a 1 km grid) and representing water management
(Hanasaki et al., 2022). However,
large-scale model resolutions (<inline-formula><mml:math id="M1" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 10–50 km) remain much
coarser than the hillslope-scale controlling hydrologic processes, as
hypothesized by Fan et al. (2019)
and Swenson et al. (2019). In addition, coarse
resolutions of groundwater representation tend to smooth hydraulic
gradients, leading to unrealistic aquifer properties
(Shrestha et al., 2018), and
potentially to underestimate water table depth drawdowns due to groundwater
pumping because withdrawals are applied to entire grid cells instead of
applied to punctual boreholes.</p>
      <p id="d1e167">A proper representation of groundwater is essential to consider lateral
groundwater exchanges between grid cells; otherwise, they remain connected
only through the river or drainage network. Darcy's law links hydraulic head
gradient, hydraulic conductivity, and aquifer thickness and can describe
this lateral groundwater flow. Some studies have already highlighted the
contribution of lateral groundwater flow to regions and basins
(Krakauer et al.,
2014; Schaller and Fan, 2009). Groundwater flows redistribute water from
hillslope to regional scale, leading to evapotranspiration variability
between upstream and downstream areas
(Condon
et al., 2020; Condon and Maxwell, 2019; Famiglietti and Wood, 1994; Fan and
Miguez-Macho, 2010; Keune et al., 2016; Miguez-Macho and Fan, 2012; Swenson
et al., 2019). These studies highlight the fact that evapotranspiration is impacted
to a greater degree during dry seasons and where the water table is shallow.
Oversimplifying lateral water redistribution and exchanges between soils and
groundwater may also induce non-negligible evapotranspiration biases
(Koirala
et al., 2019; Martínez-de la Torre and Miguez-Macho, 2019;
Rouholahnejad Freund and Kirchner, 2017; Wang et al., 2018). The impact of
the depth of the groundwater level on evapotranspiration and consequently on
net groundwater recharge (recharge minus capillary flux) has also been
demonstrated by Szilagyi et al. (2013) based on observed depth to
groundwater and evapotranspiration estimated from MODIS data and by Koirala
et al. (2017) based on simulated depth to
groundwater and remote sensing data. Finally, reproducing soil moisture
drainage, capillary rise, and baseflow more accurately depends on properly
representing groundwater depth and time fluctuation.</p>
      <p id="d1e170">Recent studies based on different models
(de
Graaf et al., 2017; Fan et al., 2013; Martínez-de la Torre and
Miguez-Macho, 2019; Maxwell et al., 2015; Sutanudjaja et al., 2014, 2011;
Vergnes et al., 2020) have compared simulated and observed water tables at
continental and regional scales; these studies have argued that the main
spatial trends were well reproduced. However, some of these studies have
acknowledged that water table depth is not well reproduced, given the coarse
spatial resolution (including problems of the spatial representativity of
the boreholes and potential bias sampling) and the lack of representation of
water management within the models
(Fan
et al., 2013; Maxwell et al., 2015; Reinecke et al., 2020). This raises the
question of the reliability of such models in terms of parametrization and
application (Gleeson et al., 2021).
For example, regional- and continental-scale models often assume very simple
groundwater pumping schemes or no pumping at all, and they consider
these withdrawals to simply leave the system
(Vergnes
et al., 2020; Surinaidu et al., 2013; Martínez-de la Torre and
Miguez-Macho, 2019). Hanasaki et al. (2022)
demonstrated the difficulty of introducing regional water management schemes
into large-scale hydrological models. Therefore, the interaction between
human water management and water availability is a critical aspect of
large-scale hydrological models. Humans strongly impact natural water
fluxes, affecting available water resources
(Keune et al., 2018; Taylor et al., 2012).
Irrigation sustained by groundwater significantly impacts the water cycle in
several regions
(Cao
et al., 2016; Dalin et al., 2017; Gleeson et al., 2012; Keune et al., 2018;
Siebert et al., 2010; Taylor et al., 2012). To predict future water
resources, it is necessary to decipher climate and human contributions
contained within the space and time variability of hydrological signals.
Large-scale hydrological models have been developed to estimate water
availability and water use from surface water bodies and groundwater at a
global scale
(Döll et
al., 2014; Wada et al., 2014). Recently, Hanasaki et al. (2018) improved the representation of
human interventions in the H08 model and showed more realistic river discharges
and terrestrial water storage anomalies for several huge basins. Sadki et
al. (2022) explored the possibility of improving dam
representation in the ISBA-CTRIP model applied over Spain. Long et al. (2020) studied the impact of the south-to-north
water diversion in China on groundwater pumping using CWatM. Using a global-scale hydrological model coupled with MODFLOW, de Graaf et al. (2019) reproduced the water table drawdown
dynamic caused by pumping and its impact on rivers. They determined that
rivers reach their environmental flow limit (meaning that groundwater
baseflow supporting rivers fails below its 10th percentile as suggested by
Gleeson and Richter, 2018) before substantial groundwater
depletion occurs.</p>
      <p id="d1e173">Studying and simulating regions with significant use of ground and surface
waters requires accounting for the management and linkages between the two
sources of water. Surface water management and groundwater management are fundamentally
connected. Water demand that is satisfied with surface water stored in
reservoirs and delivered through pipes or canals may be supplemented with
groundwater when the timing or volume of delivery does not coincide with the
need. Distribution networks, including urban pipes and agricultural canals,
may encourage groundwater recharge through aging and leaking infrastructure.
Further, it is necessary to understand who has access to surface water to
know where groundwater is the only source that can satisfy the demand. Some
farmers will withdraw river water in the rainy season and otherwise depend
exclusively on groundwater or leave fields fallow in the dry season. In
addition, to understand groundwater's spatial and temporal use it is
necessary to appreciate the spatial and temporal distribution of crop water
needs.</p>
      <p id="d1e177">In this paper, we present refinements on both fronts relative to previous
studies by applying the model at finer resolutions,accounting for water
management, and comparing simulations with observed water table fluctuations
and water table depths. Our new water management representation includes
estimating irrigation demand and automatic supply from canals (with
potential leakage recharging groundwater), reservoirs, and/or groundwater
(Smilovic et al., 2019). To this end, we coupled a
high-resolution version of CWatM (<inline-formula><mml:math id="M2" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 1 km resolution) with
MODFLOW implemented at high resolutions of 100 and 250 m. These model
versions are used in the Seewinkel region (Austria) and the Bhima basin
(India), extending over 573 and 46 000 km<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>, respectively. Studying
groundwater processes at regional scale allows for better calibration and
validation of models at a high resolution based on observed groundwater
levels and estimated groundwater pumping. The Seewinkel area is much smaller
and less complex than the Bhima basin regarding the aquifer and less
anthropic regarding water management. Comparing the two regions is of
interest to evaluate how geological (as well as geomorphological) complexity
constrains the model's ability to reproduce water tables. The comparison
should also help clarify the impact of two levels of water management on the
water cycle.</p>
      <p id="d1e196">The remainder of this paper is organized as follows. We first describe
CWatM (Sect. 2.1 and 2.2). Section 3 describes the two study
regions. Model performance (Sect. 4) is evaluated based on the water table
observed in the monitoring well networks. Then we describe the experiment to
assess the impact of groundwater-based irrigation on water tables and the
water cycle (Sect. 5). The results show the model's ability to reproduce
temporal and spatial variability of water table depth (Sect. 6.1). Then
the experiment shows how different water cycle components are impacted by
irrigation (Sect. 6.2 and 6.3). Finally, we discuss the most critical
factors affecting the model's accuracy (Sect. 7).</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Method</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>CWatM</title>
      <p id="d1e214">CWatM (Community Water Model) is a distributed hydrological model that can
be implemented at regional to global scales
(Burek et al., 2020). The model is developed
with the Python programming language and is open-access (<uri>https://cwatm.iiasa.ac.at/</uri>, last access: 13 June 2022). CWatM aims to reproduce the main hydrological
processes, including water management. In this study, CWatM is applied in
two regions and coupled with a finer-resolution groundwater flow model,
MODFLOW (Harbaugh, 2005). CWatM is used at a spatial
resolution of 1 km in Seewinkel and <inline-formula><mml:math id="M4" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 0.9 km (30 arcsec) in
Bhima. Because the Bhima basin covers a large area, CWatM is applied in a
geographic projection system (WGS84), while square cells are used for
Seewinkel (Lambert azimuthal equal area projection system ETRS89). MODFLOW
is applied at 100 m in Seewinkel and 250 m in Bhima using square cells in
both regions.</p>
      <p id="d1e227">The following sections more extensively describe how groundwater processes
and pumping are modeled. The coupled CWatM–MODFLOW uses a computationally
efficient approach combining MODFLOW 6's Basic Model Interface (BMI)
(Hughes et al., 2017) and Python packages
Flopy (Bakker et al., 2016) and xmipy
(Russcher et al., 2020). The coupling of CWatM and
groundwater is illustrated in Fig. 1. In
particular, it is necessary to use high-resolution groundwater models, as
topography controls the variability in the water table. For example,
Fig. 1 contains an illustration of 1 CWatM cell
containing 100 MODFLOW cells (10 shown within the cross-section), and it
highlights the fact that different land cover types are considered in each CWatM
cell. Soil processes that occur within each land cover part are modeled
independently before being averaged according to their respective coverage
area within the CWatM cell. This approach allows consideration of the
subgrid variability without reducing resolution.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e232">CWatM vertical and lateral sections focusing on coupling with
MODFLOW. The CWatM cells are composed of five land cover types: grasslands,
grasslands experiencing groundwater (GW) capillary rise, irrigated crops,
urban areas, and surface water bodies. The figure illustrates the impact of
aquifer pumping on the water table depth and consequently on baseflow and
groundwater capillary rise toward soils.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022-f01.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Including groundwater within CWatM</title>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>Representation of soil and groundwater flows</title>
      <p id="d1e256">CWatM–MODFLOW simulates subdaily hydrological processes that occur in soil
and surface water bodies. Soils are represented in three layers. Unsaturated
soil moisture redistribution and capillary rise effects are calculated using
the van Genuchten–Mualem equations and soil hydraulic properties
(Wösten and van Genuchten, 1988). At every daily
time step and within each CWatM cell, the upper soil layer receives
infiltration from precipitation and irrigation. If the underlying simulated
water table is below the bottom soil layer, water percolates from the
deepest soil layer as a function of saturation. This water reaches the
groundwater layer of the model as groundwater recharge. If the water table
is above the lower bound of the soil, downward percolation does not occur,
and groundwater feeds the soil (i.e., capillary flux). Finally,
evapotranspiration depletes soil moisture, given the potential
evapotranspiration demand and soil water availability.</p>
      <p id="d1e259">The groundwater model is implemented using MODFLOW 6. Each day, the coupling
is performed based on the following steps (Fig. 2):
(1) CWatM initializes the time step and begins processing the surface
hydrological components, (2) CWatM simulates the groundwater recharge and
extraction, which are converted in memory to MODFLOW inputs, (3) MODFLOW
inputs are passed to the MODFLOW model using the BMI, (4) MODFLOW runs the
time step using CWatM outputs, (5) MODFLOW outputs (baseflow and groundwater
capillary rise) are read into CWatM using the BMI and are converted in
memory into CWatM inputs, and (6) CWatM simulates other surface hydrological
components. The MODFLOW model can be used at different space and time
resolutions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e264">Scheme of the CWatM–MODFLOW coupling. <italic>Conversion</italic> refers to changing spatial
resolution and units as well as passing to the MODFLOW model using BMI (blue case) or
reading MODFLOW output (red case). Note that the MODFLOW model can be used at
different space and time resolutions.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022-f02.png"/>

          </fig>

      <p id="d1e277">CWatM provides a recharge rate to each MODFLOW cell for each time step.
However, when the previous simulated water table reaches the top of the
aquifer (equal to the bottom of the soil layer), the aquifer cell is
saturated. In this case, the recharge rate is set to zero. Recharge occurs
once the water table drops below the top of the aquifer. Hydraulic heads,
also referred to as a water table here, are computed in MODFLOW by
numerically solving the groundwater flow equation (combining Darcy's law and
the equation of continuity), considering no anisotropy and with one
unconfined layer on the Dupuit–Forchheimer assumption (Eq. 1):
              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M5" display="block"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mo>∂</mml:mo><mml:mrow><mml:mo>∂</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced close=")" open="("><mml:mrow><mml:mi>T</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>h</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mo>∂</mml:mo><mml:mrow><mml:mo>∂</mml:mo><mml:mi>y</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>T</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>h</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>y</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>h</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:mi>R</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mi>Q</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M6" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> is the transmissivity [<inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msup><mml:mi>L</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>/</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>​​​​​​​] equal to the hydraulic conductivity
(<inline-formula><mml:math id="M8" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>) times the saturated thickness of the aquifer (<inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">sat</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), <inline-formula><mml:math id="M10" display="inline"><mml:mi mathvariant="italic">θ</mml:mi></mml:math></inline-formula> is the
porosity, <inline-formula><mml:math id="M11" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> is the recharge rate [<inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:mi>L</mml:mi><mml:mo>/</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>], and <inline-formula><mml:math id="M13" display="inline"><mml:mi>Q</mml:mi></mml:math></inline-formula> is the pumping rate [<inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:mi>L</mml:mi><mml:mo>/</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>]. Hydraulic
head lateral propagation is controlled by diffusivity ​​​​​​​<inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:mi>D</mml:mi><mml:mo>=</mml:mo><mml:mi>K</mml:mi><mml:mo>⋅</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">sat</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:math></inline-formula>. Upward flow is computed using the DRAIN MODFLOW package when the
simulated water table reaches the top of the aquifer. This flow is equal to
the difference between the hydraulic head in the cell and the top of the
aquifer multiplied by a conductance parameter [<inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:msup><mml:mi>L</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>/</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>]. This upward flow is
partitioned between the baseflow feeding the river's network directly and
the groundwater capillary rise feeding the soils. This ratio depends on the
percentage of rivers attributed to each MODFLOW cell. Suppose a MODFLOW cell
is highly saturated and no river is identified above this cell. In that
case, groundwater can indirectly feed the river network through capillary
rise. In this area, the soil in CWatM becomes oversaturated, reproducing an
area of groundwater overflow.</p>
      <p id="d1e502">Moreover, exchanges between groundwater and surface water bodies (lakes,
rivers, and channels) are implemented within CWatM–MODFLOW. Below the
surface water bodies, if the simulated water table reaches the top of the
aquifer (equal to the bottom of the surface water body), an upward flow is
sent from the aquifer toward the surface water body. On the contrary,
leakage toward the aquifer occurs if the simulated water table drops below
the top of the aquifer. Lakes and reservoirs are identified inside the CWatM
grid using an identifier and the fraction of the “water” land cover type (as
illustrated by the “surface water bodies” fraction receiving baseflow in
Fig. 1).</p>
</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <label>2.2.2</label><title>Groundwater pumping</title>
      <p id="d1e513">CWatM–MODFLOW simulates water management and demand. Irrigation depends on
the fraction of the irrigated crop land cover type on each CWatM cell.
Irrigation need is estimated as a function of potential crop
evapotranspiration and available soil moisture within the land cover type
(Burek et al., 2020). Next, CWatM imposes
pumping to the groundwater model for each day. The water demand from all
sectors (irrigation, livestock, industry, and households) can be attributed
to surface water bodies and to different groundwater model cells depending
on where boreholes have been defined in the groundwater model
(Fig. 1). Pumping in the aquifer is simulated
with the WELL MODFLOW package. Groundwater abstraction can be limited if the
water table in the pumping wells drops below a certain depth. This limit can
correspond to physical or economic constraints and is adapted to the study
areas. Finally, once the water table recovers above this limit, pumping can
begin again.</p>
      <p id="d1e516">Note that here, we benefit from a new CWatM development, including surface
water and agricultural management (discussed further by Smilovic et al.,
2019). To appreciate the impacts of surface water
management on groundwater, more than 40 reservoirs simulated in the Bhima
basin were outfitted with daily reservoir-specific operations and connected
to specific spatial distribution areas (command areas) and canal networks.
Reservoirs in the model distribute water based on daily command area demand
and according to daily maximums with preference given to non-irrigation
requests (domestic, industrial, and livestock). A fraction of this water
leaks through the canal network. Further, rivers and lakes are set to
satisfy some agricultural demands. Water demand may be supplemented with
groundwater when surface water volume does not coincide with the need.</p>
      <p id="d1e519">For irrigation demand, this study includes more than a dozen spatially
distributed crops specific to the given region, each represented by four
crop-specific growth stages affecting water use as well as planting and harvest
dates. Regions within command areas have access to both surface water and
groundwater, while irrigated crops outside command areas only have access to
groundwater. Irrigation is applied depending on crop water needs, soil
moisture deficits, and surface water and groundwater availability. Several
agricultural practices encourage groundwater recharge, such as non-precision
irrigation, bare and freshly seeded fields at the beginning of the rainy
season (low actual evapotranspiration), and leaky surface water distribution
networks.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Two study regions with contrasting groundwater dynamics</title>
      <p id="d1e532">The two study areas offer the possibility to refine CWatM–MODFLOW spatial
resolution and water management, as well as  to examine the ability of the model to
reproduce groundwater tables for decades, due to the existence of monitoring
borehole networks</p>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Seewinkel region, Austria</title>
      <p id="d1e542">The Seewinkel region is a subpart of the Burgenland region in Austria
(Karner et
al., 2019; Hatvani et al., 2014; Mitter and Schmid, 2021). The study area, of
around 573 km<inline-formula><mml:math id="M17" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>, is limited in the west by Lake Neusiedl (Neusiedlersee
in German) and in the south and in the east by the border between Austria
and Hungary. The Seewinkel region has been classified as semi-arid
(Karner et al., 2019; Magyar
et al., 2021), even if the aridity index, defined as the ratio between mean
annual precipitation and potential evapotranspiration, reaches 1.0.
Evapotranspiration shows a strong seasonal pattern, while precipitation is
relatively homogeneous throughout the year (Table 1). The region is an important agricultural area, and around 16 % of it
is allocated to irrigated crops (maize, potatoes, vineyards, vegetables, and
wheat). Only groundwater is used to satisfy irrigation demands. The study
area hosts several natural ponds of environmental interest. These ponds
mainly depend on the water table in the aquifer. To keep the ponds safe,
pumping from irrigation wells is limited when the water table reaches a
threshold depth (Magyar et al., 2021). The Seewinkel region
and associated groundwater are modestly impacted by human water management.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e556">Location of the two study regions. <bold>(a)</bold> The Seewinkel region in
Austria. Blue lines represent canals included in the model. CWatM and
MODFLOW are respectively set up at 1 km and 100 m resolutions. <bold>(b)</bold> The
upper Bhima basin in India. Blue lines represent the main rivers. CWatM and
MODFLOW are set up at <inline-formula><mml:math id="M18" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 0.9 km and 250 m resolutions,
respectively.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022-f03.png"/>

        </fig>

      <p id="d1e578">The CWatM–MODFLOW model (shown in black in Fig. 3a) is applied at 1 km resolution, associated with a MODFLOW resolution of
100 m from a 10 m resolution digital elevation model (DEM; Comprehensive
digital field model (DGM) of the state of Burgenland, 2019). To capture the influence of regional groundwater
flow, the modeled area is larger than the study area (marked in red in
Fig. 3a). Therefore, small ponds are included in
the study area, but Neusiedlersee is not. Outside the study area, the
percentage of river within each MODFLOW cell is defined from a river network
computed with the finer 10 m resolution DEM assuming that rivers are created
when the drainage area exceeds 1 km<inline-formula><mml:math id="M19" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>. There is no river inside the
study area, but there are several canals draining groundwater. Note that the
MODFLOW DRAIN boundary condition on these canals is set at 1 m below the
altitude inferred from the 100 m DEM. Groundwater leaving the aquifer below
canals and lakes directly reaches the surface water network (see the
baseflow in Fig. 1). Using field data, the
Seewinkel aquifer is modeled as one aquifer layer with a thickness of 20 m.
Regional characteristics and model properties are synthesized in
Table 1.</p>
      <p id="d1e591">One pumping well is set up every 1 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> at the center of each CWatM
cell. Irrigation demand and associated pumping rates depend on the deficit
between potential evapotranspiration demand and current soil water contents
within the CWatM cell (see the Supplement about the influence of
irrigation efficiency and spatial density of pumping wells). Finally, the
simulated CWatM–MODFLOW pumping rate at the Seewinkel scale for 2015 is
48 % smaller than the abstraction limits imposed for the year 2015 in
Seewinkel. Therefore, the model seems to appropriately represent groundwater
use.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e606">Main characteristics and model properties of Seewinkel and Bhima.
Annual averages are given for 1983–2016 and 2000–2009 periods for
Seewinkel and Bhima, respectively. Aquifer permeability and porosity are
obtained after calibration.</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="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Seewinkel region</oasis:entry>
         <oasis:entry colname="col3">Bhima basin</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Precipitation [mm yr<inline-formula><mml:math id="M21" 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>]</oasis:entry>
         <oasis:entry colname="col2">582</oasis:entry>
         <oasis:entry colname="col3">805</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Potential evapotranspiration [mm yr<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>]</oasis:entry>
         <oasis:entry colname="col2">578</oasis:entry>
         <oasis:entry colname="col3">1077</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Fraction of irrigated area [%]</oasis:entry>
         <oasis:entry colname="col2">16</oasis:entry>
         <oasis:entry colname="col3">30</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">CWatM resolution [m]</oasis:entry>
         <oasis:entry colname="col2">1000</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M23" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 900 (30”)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MODFLOW resolution [m]</oasis:entry>
         <oasis:entry colname="col2">100</oasis:entry>
         <oasis:entry colname="col3">250</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Average soil thickness (three layers) [m]</oasis:entry>
         <oasis:entry colname="col2">0.05, 0.25, 1.70</oasis:entry>
         <oasis:entry colname="col3">0.05, 0.26, 1.16</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Aquifer permeability [m 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>]</oasis:entry>
         <oasis:entry colname="col2">5.0 <inline-formula><mml:math id="M25" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M26" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">1.2 <inline-formula><mml:math id="M27" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M28" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Aquifer porosity</oasis:entry>
         <oasis:entry colname="col2">0.07</oasis:entry>
         <oasis:entry colname="col3">0.018</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Aquifer thickness [m]</oasis:entry>
         <oasis:entry colname="col2">20</oasis:entry>
         <oasis:entry colname="col3">50</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Groundwater pumping simulated with CWatM–MODFLOW [mm yr<inline-formula><mml:math id="M29" 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>]</oasis:entry>
         <oasis:entry colname="col2">31</oasis:entry>
         <oasis:entry colname="col3">107 (<inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">115</mml:mn></mml:mrow></mml:math></inline-formula> from surface water bodies)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Bhima basin, India</title>
      <p id="d1e866">The Bhima basin is located in India and hosts 19 million people. The basin
area is 46 000 km<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>. The average aridity index is 0.75
(Table 1); however, precipitation shows strong
seasonality due to the monsoon. Both surface water and groundwater satisfy
domestic, industrial, and agricultural water demand. Irrigation is by far
the most important groundwater use. Around 30 % of the basin area is
allocated to irrigated crops. The river discharge recorded at the most
downstream gauging stations (Takli) indicates a flow of 120 mm yr<inline-formula><mml:math id="M32" 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> on
average, but this flows for only 2 months on average.</p>
      <p id="d1e890"><?xmltex \hack{\newpage}?>CWatM is applied at 30 arcsec resolution (<inline-formula><mml:math id="M33" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 900 m),
associated with a MODFLOW resolution of 250 m from a 90 m resolution DEM
(Yamazaki et al., 2019). Lakes and
reservoirs are marked using HydroLAKES
(Messager et al., 2016) and are refined and
expanded upon with local data made available by the Pune Irrigation Circle.
The percentage of river within each MODFLOW cell is defined from a river
network computed with a 90 m resolution DEM, assuming that rivers are
created when the draining area exceeds 1 km<inline-formula><mml:math id="M34" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>. In Seewinkel,
the aquifer upper limit under the rivers is set at 1 m below the altitude
inferred from the 250 m DEM. This correction allows us to better take into
account the river incision, which is strongly smoothed when resolution is
upscaled to 100 or 250 m. When the water table reaches the top of the
aquifer, groundwater is sent either to the soil or to the surface water
network (see the groundwater feeding soils and baseflow indicated in
Fig. 1) based on the river percentage map. In
Bhima, canal networks are added to bring water from reservoirs toward
cultivated areas where water is required for irrigation (see Sect. 2.2.3).
Leakage is considered to occur below these canals through a water conveyance
efficiency of 70 %.</p>
      <p id="d1e910">The Bhima basin aquifer was modeled with MODFLOW in Surinaidu et al. (2013) at 1 km resolution, assuming spatially uniform
recharge and pumping, deriving each as a linear relationship with
precipitation, incorporating different data sources. The ranges for
hydraulic conductivity and specific yield used for calibration were also
used for this study, and we refer the reader to Surinaidu et al. (2013) for a more detailed description of the region.
The model presented here expands on this by including surface water
hydrology and management, spatially distributed groundwater recharge and
outflow (pumping, capillary rise, and baseflow), and spatially distributed
non-irrigation demand, as well as by modeling crop-specific irrigation demand and
increasing the spatial resolution. While the Seewinkel alluvial aquifer was
identified, the Bhima basin is much larger and is not composed of one
homogeneous aquifer alone. The area hosts crystalline rocks, where
weathering may potentially enhance permeability and porosity. We considered
one homogenous aquifer layer with a thickness of 50 m
(Surinaidu et al., 2013). We set up one pumping
well in every MODFLOW cell (see the Supplement regarding the
influence of irrigation efficiency and the spatial density of pumping
wells). As for the Seewinkel model, pumping rates depend on the deficit
between potential evapotranspiration demand and soil water content in each
CWatM cell. Finally, the imposed pumping rate depends on the fraction of
irrigated areas above each pumping well. Pumping is prevented when the water
table falls below a depth of 15 m (Surinaidu et
al., 2013).</p>
      <p id="d1e913">Table 1 provides mean simulated water withdrawals.
Annual surface water and groundwater withdrawals within the Bhima basin are
estimated for different sectors for 2013 in the upper Bhima subbasin draft
report. The model simulates these withdrawals closely (5 % higher), with
higher groundwater use and lower surface water use. Through discussions with
local water managers and engineers, including through stakeholder workshops
(Karutz et al., 2022), it was found that groundwater use is
generally underreported and underestimated for both irrigation and
non-irrigation purposes. Further, canal leakage is not included in the
report, producing an underestimation of groundwater availability. In
agreement with the uncertainty of the reported values and following the expert
opinions mentioned above, this model appropriately represents the region's
annual surface water and groundwater use.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Validation of the hydrological models</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Available observed data</title>
      <p id="d1e932">Water table data from 81 and 373 monitoring boreholes were gathered for the
Seewinkel and Bhima areas, respectively. These observed datasets come from
the eHYD (<uri>https://ehyd.gv.at/</uri>, last access: 3 January 2021​​​​​​​) database in Austria
(BMLRT, 2020) and the Central Groundwater Board in India. They
have been preprocessed to make them compatible with the simulated water
table. First, boreholes close to the model's boundary limits were removed,
given that the simplified no-flow boundary condition in the groundwater
model could lead to an unrealistic water table in these parts. Second,
boreholes were removed where time data covered less than 50 % of the
simulation period. Third, we did not consider 5 % of the remaining
boreholes with the greatest discrepancy between simulation and observation
because they are impacted by specific local conditions that are not well
reproduced by the model. This prevents them from influencing the
calibration. Indeed, because of model assumptions such as homogeneous aquifers
or pumping well locations, it can be inferred that some boreholes could not
be well represented by the model due to the vicinity of pumping wells,
rivers, or local heterogeneities. Finally, we kept 62 and 351 boreholes for
the Seewinkel and Bhima areas (Figs. 4a and 5a), respectively. In the Bhima basin, we
also used daily discharge data aggregated at a weekly scale at five gauging
stations from the National Hydrology Project in India.</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Comparison between observed and simulated water table</title>
      <p id="d1e946">To fully benefit from the informative content of the observed water table,
we separately evaluated time-averaged water tables (static part) and water
table time fluctuations (transient part). This was done to better understand
how each parameter is sensitive to both static and transient parts of
observed data. As described above, the calibration relies on 62 and 351
boreholes for  Seewinkel and Bhima, respectively.</p>
      <p id="d1e949">First, we assessed the model's ability to reproduce the mean spatial variability
of the water table driving the lateral groundwater flow. Observed and
simulated water tables were averaged along the calibration period at each
borehole. However, a comparison between observed and simulated water tables
is not relevant and not sensitive to parameters, as the water table mimics
the surface elevation, which extends to several orders of magnitude, as
noted by Gleeson et al. (2021) and
Reinecke et al. (2020). Indeed, the observed
water table varies from 430 to 1000 m in Bhima, while observed water table
depth varies from 1 to 20 m. Moreover, model topography can differ from
actual topography. On the other hand, water table depths contain more
discriminant information and are essential for the interaction between
groundwater, soil, and surface. Therefore, we compared the water table depth
(WTD) instead of the water tables. As a criterion, we used the “normalized
mean water table depth difference” [%], defined by the following equation
(Eq. 2):
            <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M35" display="block"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">mean</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mo>×</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>n</mml:mi></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:munderover><mml:mo>|</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi mathvariant="normal">WTD</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mrow><mml:mi mathvariant="normal">obs</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mover accent="true"><mml:mi mathvariant="normal">WTD</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mrow><mml:mi mathvariant="normal">sim</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi mathvariant="normal">WTD</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mrow><mml:mi mathvariant="normal">obs</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>|</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M36" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> is the number of monitoring boreholes, obs and sim refer to observed and
simulated depths, respectively, and <inline-formula><mml:math id="M37" display="inline"><mml:mover accent="true"><mml:mi mathvariant="normal">WTD</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> refers to the time-averaged
WTD. Note that <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi mathvariant="normal">WTD</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mrow><mml:mi mathvariant="normal">obs</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> ranges from 0.25 to 12 m and from 1 to 20 m for Seewinkel and Bhima, respectively. Thus, shallow water table depths do
not have too much weight on <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">mean</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e1087">The second criterion focuses on time fluctuations in water tables observed
in boreholes, whatever the mismatch value between observed and simulated
time-averaged water table depth. Water table fluctuations correspond to the
initial signal after the time average is removed. To simplify, we averaged
observed and simulated water table fluctuations from all boreholes instead
of comparing the fluctuations at each borehole. This approach smooths local
behaviors and informs the water table fluctuations (WTFs) at the basin scale at
the first order. As a criterion, we used the normalized root mean square
error [%] on average time fluctuations, defined by (Eq. 3):
            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M40" display="block"><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{8.5}{8.5}\selectfont$\displaystyle}?><mml:mi mathvariant="normal">nRMSE</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">100</mml:mn><mml:mrow><mml:mi mathvariant="normal">SD</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">WTF</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:msqrt><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">WTF</mml:mi><mml:mrow><mml:mi mathvariant="normal">obs</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">WTF</mml:mi><mml:mrow><mml:mi mathvariant="normal">sim</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt><mml:mo>,</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> refers to the number of observations in time (<inline-formula><mml:math id="M42" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>). Thus, the
nRMSE corresponds to the root mean square error (RMSE) expressed as a percentage of the standard deviation
(SD) of the observed data.</p>
      <p id="d1e1199">CWatM–MODFLOW simulation starts in 1981 and ends in 2016 for Seewinkel,
while it begins in 1993 and ends in 2009 for Bhima. For both regions, models
are run the first time during the whole period to initialize the water table.
For Bhima, hydraulic conductivity and specific yield variables were included
first in a calibration (Fortin et al., 2012) using five
daily discharge stations (2000–2009), and ranges for calibration were
derived from Surinaidu et al. (2013). The top 20 %
from the discharge calibration was further analyzed for water table
fluctuation and depths. Groundwater parameters hydraulic conductivity and
porosity are further calibrated by comparing the simulated and observed water
table recorded monthly in boreholes from 1983 to 2016 and twice a year from
1997 to 2009, respectively, for Seewinkel and Bhima. Standard CWatM
parameters were used in Seewinkel. Therefore, only groundwater parameters
are calibrated in this study.</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Experiments to infer the impact of irrigation</title>
      <p id="d1e1212">The effects of irrigation are evaluated by comparing simulations with and
without irrigation. To infer the effects of irrigation during the simulation
period, we focus on the annual average of several variables
(Fig. 1): groundwater store, soil water content,
evapotranspiration, groundwater recharge, and the fraction of humid areas
(areas where groundwater often feeds soils). We focus on the impact of
irrigation on actual evapotranspiration rate and groundwater
recharge in two land cover types, namely groundwater-supported grasslands
and irrigated areas. We expect that irrigation will increase
evapotranspiration in irrigation areas and reduce evapotranspiration (and
increase recharge) in non-irrigated areas. In Seewinkel, we also assess the
impact of irrigation during the very dry summer of 2003, as we expect a more
substantial effect of irrigation during that period. We also adjusted the
irrigation efficiency parameter, which also impacts groundwater pumping, as
well as the spatial density of pumping wells to test the sensitivity of the
results to these settings (Supplement).</p>
      <p id="d1e1215">Land cover variability within the CWatM–MODFLOW grid cell is considered
using a subgrid approach. Each CWatM cell includes five land cover
fractions: grasslands (including non-irrigated crops), irrigated crops,
groundwater-supported grasslands (Fig. 1), urban
areas, and water body areas. For each CWatM cell, the sum of each land cover
fraction equals 1. Here, groundwater-supported grasslands have the same
properties as grasslands but correspond to land fractions where groundwater
often feeds soils. Setting up a groundwater-supported grassland fraction
allows the groundwater flow to be concentrated toward the fraction of the
soil that usually receives groundwater instead of distributing this flow
homogeneously over all CWatM grid cells (Fig. 1).
By this means, we can better take advantage of the finer resolution of the
groundwater layer (100 or 250 m). Consequently, soil moisture, surface
runoff, and evapotranspiration are more pronounced in groundwater-supported
grasslands than in regular grasslands. Technically, the
groundwater-supported grassland fractions need to be estimated after an
initialization simulation to infer the groundwater-supported areas. Thus,
the calibrated CWatM–MODFLOW model is run for the first time during the
simulation period to initialize the water table and to define the
groundwater-supported fraction for each CWatM grid cell. From this first
simulation, MODFLOW cells are defined as groundwater-supported areas if
groundwater feeds the soil for more than 4 months out of 12. Then,
groundwater-supported fractions are computed at CWatM resolution and
used during simulations. Because this land cover fraction is constant over
time, the groundwater-saturated land fraction may exceed some grid cells'
predefined fractions during extreme events. In this case, groundwater is
also sent to other land cover types (grasslands and irrigated areas). In
other cases, when the simulated groundwater-saturated area is smaller than
the predefined groundwater-supported area, groundwater is distributed
equally within the groundwater-supported fraction. Therefore, choosing a
threshold of “4 months out of 12” is a compromise allowing us to focus on
areas significantly supported by groundwater. This illustrates the
importance of simulating water table depths well.</p>
</sec>
<sec id="Ch1.S6">
  <label>6</label><title>Results</title>
<sec id="Ch1.S6.SS1">
  <label>6.1</label><title>Groundwater parameters</title>
      <p id="d1e1233">Optimal aquifer permeability and porosity (Table 1)
are compared to different datasets as described below. The permeability and
porosity in Seewinkel are 5 <inline-formula><mml:math id="M43" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M44" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m s<inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 0.07, respectively.
These values are respectively 3.10<inline-formula><mml:math id="M46" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m s<inline-formula><mml:math id="M47" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 0.19 in the global GLHYMPS
database (Gleeson et al., 2014;
Huscroft et al., 2018). The imposed aquifer thickness (20 m) agrees with the
global depth-to-bedrock map (Shangguan et al., 2016), where
the average value for the study area is around 22 m.</p>
      <p id="d1e1291">In Bhima, the permeability and porosity are 1.2 <inline-formula><mml:math id="M48" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M49" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m s<inline-formula><mml:math id="M50" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and
0.018, respectively. These values are respectively 3.16 <inline-formula><mml:math id="M51" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M52" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m s<inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 0.09 in the global GLHYMPS database. The global depth-to-bedrock
values consider thinner aquifers in this region (from zero to a few meters)
compared to the imposed aquifer thickness (50 m). Note that for similar
permeability (1 <inline-formula><mml:math id="M54" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M55" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m s<inline-formula><mml:math id="M56" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) and thickness (50 m), Surinaidu
et al. (2013) calibrated a porosity of 0.01–0.03 in
a regional model. This suggests that permeability is underestimated and
porosity overestimated in GLHYMPS over this basin.</p>
</sec>
<sec id="Ch1.S6.SS2">
  <label>6.2</label><title>Validation</title>
      <p id="d1e1396">The model reproduces the time-averaged water table depths recorded in
boreholes in Seewinkel (Fig. 4b), with a
<inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">mean</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> value of 38 %. Therefore, we can infer that the hydraulic
gradient and water table depth are reasonably well reproduced. The results
for the Bhima basin show more contrast (Fig. 5b),
as the <inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">mean</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is 69 % and simulated water table depth is too shallow on
average. Indeed, the simulated mean water table averaged over all monitoring
wells is 1.7 m higher than the observed mean in Bhima
(Fig. 6b), while the model shows a slight bias of
0.5 m in Seewinkel (Fig. 6a). The reason for this
bias is examined in the Discussion section.</p>
      <p id="d1e1421">In Seewinkel, the observed mean water table lies above a 1 m (2 m) depth for
17 % (47 %) of monitoring wells, while this fraction is 29 % (56 %)
in the model (Fig. 4b). Thus, the model
overestimates very shallow conditions (<inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:mi mathvariant="italic">&lt;</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> m depth). The total land
fraction where the simulated mean water table is shallower than a 1 m (2 m)
depth is 25 % (46 %). Thus, it can be inferred that a non-negligible land
fraction hosts shallow groundwater in Seewinkel.</p>
      <p id="d1e1434">In Bhima, the observed mean water table lies above a 1 m (2 m) depth for
0 % (2 %) of monitoring wells, while this fraction is 17 % (32 %) in
the model (Fig. 5b). Thus, we conclude that the
model overestimates shallow conditions in Bhima. Moreover, the total land
fraction where the simulated mean water table is shallower than a 1 m (2 m)
depth is 6 % (10 %), indicating that monitoring wells are preferentially
located in shallow areas.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e1440"><bold>(a)</bold> Map of the monitoring boreholes in the Seewinkel region. <bold>(b)</bold>
Comparison between observed and simulated time-averaged water table depth.
<bold>(c)</bold> Comparison between monthly observed and simulated water table time
fluctuations averaged across all monitoring boreholes and expressed as
anomalies (relative to the time average).</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022-f04.png"/>

        </fig>

      <p id="d1e1457">Both models successfully reproduce water table fluctuations averaged across
all monitoring boreholes (Figs. 4c and 5c). The nRMSE reaches 52 % and 41 % for the
Seewinkel and Bhima models, respectively. While the primary seasonal and
interannual behavior is well reproduced in both areas, some events or
periods are not well captured. For example, the Seewinkel model
underestimates simulated fluctuations from 1986 to 1988. In addition,
fluctuations are overestimated from 2000 to 2005, but the seasonal amplitude
is slightly underestimated. In the Bhima basin, it also appears difficult to
reproduce several interannual fluctuations and seasonal behavior at the
same time. For example, changing the hydraulic parameters to increase
seasonal amplitudes from 2003 to 2005 would decrease the base level even
more during this period (Fig. 5c). Likewise,
increasing or decreasing pumping rates would improve the mean water table
bias but would increase the nRMSE focused on water table fluctuations
(Supplement).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e1462"><bold>(a)</bold> Map of the monitoring boreholes on the Bhima basin. <bold>(b)</bold>
Comparison between observed and simulated time-averaged water table depth.
<bold>(c)</bold> Comparison between observed and simulated water table time fluctuations
averaged across all monitoring boreholes and expressed as anomalies
(relative to the time average). Based on the daily simulation, the simulated
water table is compared on the same days as the observed water table twice a
year, before and after the monsoon.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022-f05.png"/>

        </fig>

      <p id="d1e1479">A comparison between observed and simulated weekly discharge in the Bhima
basin is provided in the Supplement. The Kling–Gupta efficiency
(KGE) (Gupta et al., 2009) values are
0.75, 0.68, 0.54, 0.76, and 0.66 from upstream to downstream stations. These
results and the associated good criterion on water table fluctuations
(nRMSE) make us confident that the model simulates rainfall partitioning between
discharges and evapotranspiration wells.</p>
</sec>
<sec id="Ch1.S6.SS3">
  <label>6.3</label><title>Impact of pumping on the water table</title>
      <p id="d1e1490">The impact of pumping on the water table is a function of mean pumping rate
and aquifer properties (permeability, saturated thickness, and porosity).
Groundwater pumping theoretically decreases the water table within and
around irrigated areas. The results show that groundwater pumping enhances
the seasonal water table fluctuations by intensifying water table recession
during the dry season in both regions (Fig. 6).
It is also shown in Fig. 6 that irrigation
accentuates water table depletion during the driest years. Interestingly,
during the recharge seasons, the water table within the borehole network is
not strongly influenced by pumping in the two study regions, as the water
tables with and without pumping are very close
(Fig. 6). Because the water table is a proxy for
groundwater storage, this result indicates that groundwater storage recovers
rapidly and/or irrigation enhances net groundwater inputs. However, this is
not the case for the driest periods (i.e., 2004–2005 in Seewinkel and
2003–2005 in Bhima).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e1495">Comparison between absolute water table depth fluctuations
obtained from CWatM with (red lines) and without (gray lines) irrigation in
the Seewinkel <bold>(a)</bold> and Bhima <bold>(b)</bold> areas. Black lines
represent observed data. Water table depth fluctuations are aggregated from
62 and 351 boreholes for Seewinkel and Bhima, respectively.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022-f06.png"/>

        </fig>

      <p id="d1e1510">Comparing models with and without irrigation allows us to infer the impact
of pumping on the water table. However, groundwater recharge is impacted by
irrigation, as we elaborate in the next section. Pumping reduces the average
water table at boreholes from 0 during the wet season to around 30 cm and
1–2 m during the growing season in Seewinkel and Bhima, respectively
(Fig. 6). The impact of pumping also varies
spatially, depending on whether the monitoring borehole is located near the
irrigation areas where pumping occurs. Drawdown due to pumping obtained on
the time-averaged water table in monitoring boreholes varies between 0 and
50 cm and between zero and a few meters for Seewinkel and Bhima,
respectively.</p>
      <p id="d1e1514">The impact of pumping on the water table is more pronounced in Bhima than in
Seewinkel (Fig. 6). This can be explained in two
ways. First, aquifer permeability, thickness, and porosity are higher in
Seewinkel (5 <inline-formula><mml:math id="M60" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M61" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m s<inline-formula><mml:math id="M62" 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>, 20 m, and 0.07, respectively) than in
Bhima (1.2 <inline-formula><mml:math id="M63" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M64" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m s<inline-formula><mml:math id="M65" 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>, 50 m, and 0.018). Therefore, water table
drawdowns around pumping wells are less pronounced in Seewinkel. Second, the
mean pumping rate is smaller in Seewinkel (31 mm yr<inline-formula><mml:math id="M66" 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>) than in Bhima (107 mm yr<inline-formula><mml:math id="M67" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>).</p>
</sec>
<sec id="Ch1.S6.SS4">
  <label>6.4</label><title>Impact of irrigation</title>
      <p id="d1e1612">As expected, irrigation increases the total actual evapotranspiration in the
two study regions. In Seewinkel, evapotranspiration in irrigated areas
increases from 77 to 87 mm yr<inline-formula><mml:math id="M68" 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>. In Bhima, evapotranspiration in irrigated
areas increases significantly from 102 to 209 mm yr<inline-formula><mml:math id="M69" 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>. However, these changes
in evapotranspiration are substantially smaller than the allocated
irrigation withdrawals due to conveyance and application losses and the fact
that some of the irrigated water reaching the soil percolates toward the
groundwater without being used by crops. Indeed, groundwater pumping amounts
to an annual average of 31 mm yr<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in Seewinkel, while annual groundwater and
surface water withdrawal amounts to 107 and 115 mm yr<inline-formula><mml:math id="M71" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in Bhima,
respectively. The increase in evapotranspiration is associated with a
decrease in river discharge. In Seewinkel, irrigation reduces streamflow
from 158 to 152 mm yr<inline-formula><mml:math id="M72" 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>. However, pumping increases the net lateral
groundwater inflow to the study area by around 2 mm yr<inline-formula><mml:math id="M73" 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>. In Bhima, irrigation
reduces streamflow from 257 to 167 mm yr<inline-formula><mml:math id="M74" 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>. In all, 3 and 14 mm yr<inline-formula><mml:math id="M75" 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> from
groundwater pumping reach the river network due to irrigation losses in
Seewinkel and Bhima, respectively.</p>
      <p id="d1e1712">Irrigation also significantly increases groundwater recharge in both areas.
Recharge increases by 24 % and 50 % in Seewinkel and Bhima,
respectively. This is counterbalanced by groundwater pumping such that
irrigation causes a reduction of net groundwater input of 12 and 5 mm yr<inline-formula><mml:math id="M76" 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> in
Seewinkel and Bhima, respectively. However, the net recharge reduction is
more pronounced without irrigation from the surface water bodies in Bhima.
Indeed, around 40 mm yr<inline-formula><mml:math id="M77" 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> of the recharge rise is attributed to irrigation
from surface water bodies in Bhima. Note that in both models, irrigation
increases recharge in irrigated lands, not only during the irrigation season but
also during the wet season (Appendix A1).</p>
      <p id="d1e1739">Recharge increases not only in irrigated areas (92 % and 94 % for
Seewinkel and Bhima, respectively) but also in grasslands (6 % and 5 %)
and in groundwater-supported grasslands (2 % and 1 %). These results can
be explained by the influence of groundwater pumping, which reduces the
water table outside the irrigated areas. When irrigation is not applied,
recharge is limited in some periods due to the high water table in
groundwater-supported grasslands and episodically in other land cover types. The
water table is deeper when irrigation pumping is used, thus enhancing water
percolation from the soils to the aquifer. Consequently, soil humidity and
evapotranspiration rates decrease in groundwater-supported areas due to
irrigation, while recharge increases. This mechanism is illustrated by
Fig. 1, which shows a 1D section of a water table
with and without irrigation.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e1745">Comparison of some indicators obtained from CWatM–MODFLOW
simulation with and without irrigation in annual average values in
1983–2016 for Seewinkel <bold>(a)</bold> and in 1997–2009 for Bhima <bold>(b)</bold>. Note that the
units are different for each variable. Areas were considered humid when the
groundwater supported soils for at least 4 months of 12.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022-f07.png"/>

        </fig>

      <p id="d1e1760">In Seewinkel, the mean soil water content in groundwater-supported areas
decreases from 85 to 79 cm due to pumping (Fig. 7a). The associated evapotranspiration rate diminishes from 595 to 573 mm yr<inline-formula><mml:math id="M78" 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> per unit area of groundwater-supported areas. In Bhima, the mean soil
water content in groundwater-supported areas decreases from 48 to 46 cm when
pumping is applied, leading to a drop in the associated evapotranspiration
rate from 920 to 752 mm yr<inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> per unit area of groundwater-supported areas
(Fig. 7b).</p>
      <p id="d1e1787">The water cycle is slightly impacted by irrigation at an annual scale in
Seewinkel, and we can expect a more significant impact through the dry
season when irrigation withdrawals occur. Focusing on the dry summer of
2003, the soil water content in groundwater-supported areas decreased from
70 to 65 cm due to pumping (Supplement). Consequently, the
evapotranspiration rate in groundwater-supported areas decreased from 292 to
274 mm m<inline-formula><mml:math id="M80" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and increased by 40 % in irrigated areas.</p>
</sec>
</sec>
<sec id="Ch1.S7">
  <label>7</label><title>Discussion</title>
<sec id="Ch1.S7.SS1">
  <label>7.1</label><title>Impact of irrigation on the hydrological cycle</title>
      <p id="d1e1818">Here, we tested the implication of irrigation using the coupled
CWatM–MODFLOW model at very high resolutions and including a fine
representation of water management practices. In Seewinkel, groundwater is
the only source of irrigation, while surface water in Bhima satisfies half
of the irrigation demand. Our experiment to infer the impact of the
irrigation highlights the fact that irrigation does not significantly impact the
average annual water balance in Seewinkel. However, the impact of irrigation
is more pronounced during dry periods (e.g., the dry summer of 2003). The
low average pumping rate can explain the small effect of pumping in
Seewinkel (31 mm yr<inline-formula><mml:math id="M81" 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>) compared to the recharge rate (80 mm yr<inline-formula><mml:math id="M82" 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>). Moreover, the
net water balance of the aquifer only drops by 12 mm yr<inline-formula><mml:math id="M83" 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> because recharge
increases by 19 mm yr<inline-formula><mml:math id="M84" 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> due to irrigation. In addition, permeability and
porosity in Seewinkel are high enough to limit the water table drawdowns
induced by pumping. Finally, the soil storage is larger in Seewinkel than in
Bhima (average soil water content in groundwater-supported areas is 85 and
48 cm, respectively), involving less dependence on groundwater (less
irrigation and less groundwater recharge).</p>
      <p id="d1e1869">In Bhima, the experiment reveals that irrigation strongly increases
evapotranspiration from irrigated areas and slightly reduces available water
in groundwater-supported areas. Consequently, river discharge is strongly
diminished. Like Seewinkel, groundwater recharge increases in both irrigated
and non-irrigated lands. The inclusion of water transfer within the
unsaturated zone, thickened due to pumping, could reduce effective recharge,
as pointed out by Cao et al. (2016).
However, due to the pumping rate and the thickness of the aquifer, the water
table drawdown was much more significant in their study.</p>
      <p id="d1e1872">Assuming negligible groundwater interaction within irrigated lands, 70 %
and 47 % of applied irrigation (without accounting for evaporation and
runoff losses) percolates below soils and increases groundwater recharge in
Seewinkel and Bhima, respectively. Similar values are identified in several
other studies. Estimates of recharge from excess irrigation are variable,
range from 0 % to 80 %
(Groundwater
Resource Committe, 2009; Le Coz et al., 2013; Meixner et al., 2016; Ochoa et
al., 2013; Roark and Healy, 1998; Scanlon et al., 2005; Willis and Black,
1996), and depend on the efficiency of irrigation techniques
(Grafton et al., 2018;
Meredith and Blais, 2019).</p>
      <p id="d1e1875">In Seewinkel and Bhima, we find that groundwater storage is replenished each
year during the wet season in spite of pumping during dry seasons because
water tables with and without pumping are very similar during wet seasons
(Fig. 6). We infer that this result depends on
the studied regions, as explained below. Indeed, the Seewinkel and Bhima
aquifers are shallow, and pumping is limited by water table depth
thresholds. Consequently, groundwater resources can be replenished during
wet seasons. In Seewinkel, pumping is limited to protect the natural ponds
sustained by groundwater. In Bhima, pumping is limited due to economic
constraints and decreases in aquifer permeability with depth.</p>
      <p id="d1e1879">Recharge is enhanced where the water table is deep, while soil water content
and evapotranspiration increase where it is shallow
(Fig. 1)
(Martínez-de la Torre
and Miguez-Macho, 2019; Swenson et al., 2019). Therefore, the spatial
distribution of the water table depth is critical when focusing on the
interaction between groundwater and soils. Our results suggest that
simulated water tables are overestimated. This point is discussed in the
next section. In addition, the model could be improved by allowing crops to
draw water directly from groundwater systems where their roots exceed the
soil depth and where the water table is shallow. Finally, water table depth
representation is also relevant from an irrigation perspective. First,
pumping redistributes groundwater, potentially impacting baseflow or
neighboring areas. Second, water table depth is a proxy for available
groundwater resources. Finally, it affects pumping costs
(Turner et al., 2019).</p>
</sec>
<sec id="Ch1.S7.SS2">
  <label>7.2</label><title>Difficulty of reproducing water table variability</title>
      <p id="d1e1890">The primary result of this study is that the coupled CWatM–MODFLOW model
managed to reproduce the average water table time fluctuations
(Figs. 4c and 5c)
very well. This result is in line with other large-scale models
(de
Graaf et al., 2017; Martínez-de la Torre and Miguez-Macho, 2019;
Sutanudjaja et al., 2014, 2011; Vergnes et al., 2020). Groundwater pumping
appears to be necessary to reproduce time fluctuation anomalies in the water
table (fluctuations are amplified by pumping in
Fig. 6). We infer that, by calibrating water
table fluctuations separately, we simulated a good combination between
groundwater recharge, pumping, and aquifer lateral flow (driven by hydraulic
diffusivity). Therefore, water table time fluctuations contain important
information (Houben et al., 2022), even when reproducing the
absolute water table depth remains challenging, particularly in Bhima, as
also noted by Vergnes et al. (2020).
Note that here, we initially averaged water table time fluctuations from all
boreholes located within the basins, similarly to Long et al. (2020).</p>
      <p id="d1e1893">By contrast, the spatial distribution of water table depth can be
challenging to reproduce and may be less informative because it is subject
to spatial resolution and geological heterogeneity. The comparison between
observed and simulated water table depth is satisfactory in Seewinkel
(Fig. 4b) but only provides first-order
satisfaction in Bhima (Fig. 5b). A first
explanation for this may be that the Seewinkel aquifer is more homogenous
and well known. Consequently, the model can better describe its properties,
such as thickness, permeability, and porosity. In contrast, the Bhima basin
is much larger and hosts mainly crystalline rocks with potentially variable
weathering and fracture density, making its aquifer properties
heterogeneous. Beyond the aquifer parameters, the ability to reproduce
time-averaged water table depth is constrained by two critical factors in
both areas: the pumping rates and the spatial resolution of the groundwater
model. These two factors are more acute in Bhima, where pumping is more
pronounced and the resolution is coarser (250 m). In both study areas,
simulated mean annual pumping rates at the basin scale were validated.
However, we acknowledge that pumping estimates could remain uncertain
regarding annual averages, seasonal behavior, and pumping well locations.</p>
      <p id="d1e1896">Groundwater model resolution is critical because degrading resolution
smoothens topographical variability. The altitude of local low points in
valleys due to river incision, often corresponding to aquifer resurgences,
is increased more than it is in neighboring cells when degrading resolution.
Consequently, the water table is shallower than expected because the low
points locally controlling the water table are higher than expected (see
topography and water table comparisons at 100 and 250 m resolution in
Appendix A2). This explains why very shallow conditions (<inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mi mathvariant="italic">&lt;</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> m
depth) close to rivers are overestimated in Seewinkel despite the 100 m
resolution employed. A similar bias was obtained by Maxwell et al. (2015), who used a spatial resolution of 1 km
over the continental US.</p>
      <p id="d1e1909">The weakness of large-scale models for reproducing the spatial distribution
of water table depths has been mentioned but not adequately explained in
several previous studies
(Fan
et al., 2013; Maxwell et al., 2015; Reinecke et al., 2020). These studies
indicate that mismatch between models and observed data could be due to (i)
well representativity within a mesh that is too coarse (see also Martínez-de la
Torre and Miguez-Macho, 2019), (ii) well
sampling bias, or (iii) groundwater pumping. However, the ability of
large-scale models to reproduce water tables remains primordial, and the
means of evaluating them should be improved
(Gleeson et al., 2021). Here, for the
first time, we used a large-scale hydrological model, including groundwater
flow and pumping, at a very fine resolution. We note that, as expected,
regional models show a better aptitude to reproduce water table depth. For
instance, Vergnes et al. (2020)
reproduced a mean water table depth on 639 piezometers across several French
regions with a median bias of around 3 m. Similarly, Soltani et al. (2021) simulated water
tables with an RMSE of 3.8 m based on around 28 000 groundwater head stations in
Denmark. Jing et al. (2018)
reproduced water table depths with an RMSE of 6.3 m. In this study, we simulated
mean water table depths with RMSEs of 1.0 and 5.0 m in Seewinkel and Bhima,
respectively. Surinaidu et al. (2013) obtained a
similar RMSE in Bhima with a simpler model at a coarser resolution as well as uniform
recharge and discharge. However, a comparison with water table fluctuations,
depth bias, and surface water flows, including discharge and reservoir
levels, was not performed.</p>
      <p id="d1e1913">We argue that simulated water tables tend to be shallower than the observed
water table due to the coarse spatial resolution, as explained above.
However, increasing the groundwater model resolution would significantly
increase computing time, which makes it challenging to perform sensitivity
analysis. Indeed, the same simulation performed in the Bhima basin at a 100 m resolution lasts around 2 d versus 9 h at a 250 m resolution.
Figure 8 illustrates how increasing the resolution
from 250 to 100 m slightly reduces water table depth bias. While the nRMSE
criterion is not significantly better, highlighting the role of
heterogeneity rather than spatial resolution, the mean water table depth is
now overestimated by 0.5 m instead of 1.7 m (Fig. 8). Reinecke et al. (2019b) focused on the reason
for water table depth mismatch and its sensitivity. They highlighted the
importance of hydraulic conductivity, recharge, and surface water body
elevation. The surface water body elevation can be assimilated to the top of
the aquifer in the two CWatM–MODFLOW models described here. Therefore, this
critical factor is linked to spatial resolution. By comparison, Reinecke et
al. (2019a) improved their
RMSE from 54 to 27 m using a resolution of <inline-formula><mml:math id="M86" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 9 km and 900 m,
respectively. Note that their experiment was located in a steep domain (New
Zealand).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e1925">Comparison between simulated water table depth using a groundwater
model resolution of 250 and 100 m in the Bhima basin. Black lines represent
observed data. Water table depth fluctuations are aggregated from 351
boreholes. Note how improving the resolution reduces the water table.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022-f08.png"/>

        </fig>

</sec>
<sec id="Ch1.S7.SS3">
  <label>7.3</label><title>Importance of implementing a subgrid approach in large-scale models</title>
      <p id="d1e1942">CWatM uses a mosaic approach to represent the subgrid variability of the
land cover type. In addition, we developed a subgrid approach to improve
model efficiency, specifically for groundwater exchanges, to benefit from
the finer MODFLOW resolution. Indeed, each CWatM grid cell (1 <inline-formula><mml:math id="M87" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1 km) contains a land cover fraction where soil is supported by groundwater.
Therefore, we found that the impact of pumping on soil–groundwater exchanges
was more significant when groundwater capillary rise focused on a fraction
of each grid cell instead of distributing the flow homogenously over the
whole cell. This approach enables better simulation of the link between the
water table, evapotranspiration, and recharge without refining the CWatM
grid.</p>
      <p id="d1e1952">As pointed out previously, surface water body elevation, linked to the
spatial resolution here, is important for simulating absolute water table
depth (Reinecke et al., 2019b). This is
important, as the river network elevation strongly controls water table
depth. Moreover, rivers represent groundwater outlets, as CWatM–MODFLOW
generates baseflow based on the simulated water table below rivers. However,
a whole cell cannot be entirely assimilated to a river due to the coarse
resolution of large-scale models; thus, two critical issues can be noted.
First, large-scale modellers never have a map of the actual river network, including the finest low-order and intermittent rivers.
They usually generate a river network based on a digital elevation model
(Yamazaki et al., 2019), so
partitioning between baseflow and groundwater capillary rise is predefined
before the simulation. Second, groundwater reaching the top of the aquifer
can feed either rivers (as baseflow) or soils (as capillary rise). Our
modeling approach relies on a finer digital elevation model used to compute
a river network at a resolution finer than the groundwater model (Sects. 2.2.1 and 3). However, we acknowledge that small natural or artificial
drains are not included in the model. Then, partitioning between baseflow
and capillary rise is defined at the resolution of the groundwater model.
This partitioning impacts the depth of the water table. Indeed, increasing
the baseflow fraction decreases the water table depth and reduces the soil
water availability. Our approach partly deals with this issue as the
resolution is very fine (100 and 250 m) and because cells where groundwater
oversaturates soils generate overland runoff, feeding rivers.</p>
      <p id="d1e1955">Other subgrid approaches exist. The TOPMODEL approach
(Beven and Kirkby, 1979), for instance, is
used in many regional-scale models. It infers subsurface flow convergence
based on a finer digital elevation model. Vergnes et al. (2014) also proposed an alternative
approach, in which a groundwater flow equation simulates the water table
dynamic but capillary rise only occurs in a fraction of the cells based on
the distribution of the topography at the subgrid level. Similar approaches
are used within CWatM and PCR-GLOBWB when no lateral groundwater flow is
considered. Another option is to represent coarse cells or basins with
equivalent (representative) hillslopes
(Fan
et al., 2019; Loritz et al., 2017; Troch et al., 2003). Recently, new
hillslope models have been developed for use at a large scale
(Hazenberg et al., 2015; Swenson et
al., 2019). However, this conceptual modeling approach cannot include
regional lateral flow convergences or groundwater pumping. Finally, another
approach would be to aim for hyper-resolution in each compartment (surface,
soil, and groundwater). However, this would require huge computing capacity
to be achievable at a continental scale.</p>
</sec>
</sec>
<sec id="Ch1.S8" sec-type="conclusions">
  <label>8</label><title>Conclusion</title>
      <p id="d1e1967">Parametrization, spatial resolution, and human water management are
significant challenges for implementing physically based large-scale
hydrological models. As in Hanasaki et al. (2022), wherein resolution was
<inline-formula><mml:math id="M88" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 2 km, we applied a large-scale model to two regions,
including water management practices with a hyper-resolution of 1 km for
CWatM and of 100–250 m for the groundwater model. Benedict et al. (2019) also recently addressed the
resolution issue in large-scale models. They found no significant
improvement in discharge predictions even after improving the spatial
resolution. However, their hydrological model did not include groundwater
lateral flow, and resolution was still coarse (<inline-formula><mml:math id="M89" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 5 km).
Reinecke et al. (2020) found that improving
resolution alone is not enough to reproduce water table depth distribution.
Their finest resolution was <inline-formula><mml:math id="M90" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 900 m. After all, we found that
improving resolution and model parameters as well as including pumping data are
necessary to improve large-scale models. At the same time, calibrating the
model at a regional scale with a resolution finer than 100 m appears to be
challenging.</p>
      <p id="d1e1991">Supporting the results of several previous studies, we found that relative
water table fluctuations can be sufficiently simulated to infer
groundwater model parameters at the aquifer scale (Houben et
al., 2022) and to simulate discharge well
(Soltani
et al., 2021; Sutanudjaja et al., 2014). Calibrating large-scale
hydrological models with discharge data and the water table would ensure that
the main water cycle is reproduced (evapotranspiration and discharge), in addition to inner processes such as groundwater recharge, baseflow, and
groundwater support to vegetation. The evaluation of large-scale
hydrological models remains a challenge
(Gleeson et al., 2021), as water
table depth patterns are difficult to reproduce at large scales. This
pattern is only acceptable at the first order in the Bhima basin, even at
100–250 m resolution. This result is explained by the difficulty of
including the heterogeneity of groundwater bodies and pumping within the
model. After all, improving resolution to 100 m reduced the bias of the
depth distribution of the water table. We argue that reproducing mean water
table fluctuations and depth distributions without bias constitutes a
significant improvement in large-scale hydrological models. Finally,
validated models can be used to predict responses to climate and human
interventions such as land cover changes and irrigation management.</p>
</sec>

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

<app id="App1.Ch1.S1">
  <?xmltex \currentcnt{A}?><label>Appendix A</label><title/>
<sec id="App1.Ch1.S1.SS1">
  <label>A1</label><title>Impact of irrigation on groundwater recharge</title>
      <p id="d1e2011">Irrigation increases groundwater recharge in Burgenland and Bhima. Figure A1
shows that irrigation increases recharge during irrigation periods but also
during humid seasons when there is no irrigation. During dry seasons, note
that recharge is equal or close to 0 mm yr<inline-formula><mml:math id="M91" 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> when no irrigation is applied
(red lines). During wet seasons, recharge peaks due to rainfall events are
amplified because of water applied during the dry season (orange line).</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="App1.Ch1.S1.SS2">
  <label>A2</label><title>Impact of the spatial resolution on topography and simulated water table</title>
      <p id="d1e2035">The​​​​​​​ spatial resolution of the groundwater flow model MODFLOW implemented in
CWatM–MODFLOW affects absolute water table depths. This is due to the fact
that degrading the spatial resolution smooths topography, as highlighted by
a 1D section of CWatM–MODFLOW in Bhima (Fig. A2). The resulting simulated
water table is affected by the smoothing of the topography, as low points,
representing groundwater resurgences, are higher at 250 than at 100 m
resolution.</p>

      <?xmltex \floatpos{h!}?><fig id="App1.Ch1.S1.F9"><?xmltex \currentcnt{A1}?><?xmltex \def\figurename{Figure}?><label>Figure A1</label><caption><p id="d1e2040">Comparison between average monthly recharge with and without
irrigation in irrigated areas in Seewinkel <bold>(a)</bold> and Bhima <bold>(b)</bold>. Irrigation withdrawal is also represented in blue.</p></caption>
          <?xmltex \hack{\hsize\textwidth}?>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022-f09.png"/>

        </fig>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{h!}?><fig id="App1.Ch1.S1.F10"><?xmltex \currentcnt{A2}?><?xmltex \def\figurename{Figure}?><label>Figure A2</label><caption><p id="d1e2061">1D section of topography and the simulated water table in Bhima.
Comparison between a groundwater model resolution of 100 and 250 m. Note how
topography at 100 m resolution is below topography at 250 m resolution in
valleys. The resulting water table appears lower at 100 than at 250 m
resolution over the whole domain.</p></caption>
          <?xmltex \hack{\hsize\textwidth}?>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/7099/2022/gmd-15-7099-2022-f10.png"/>

        </fig>

</sec>
</app>
  </app-group><notes notes-type="codedataavailability"><title>Code and data availability</title>

      <p id="d1e2077">The CWatM–MODFLOW model and data used in this study are available on Zenodo
(<ext-link xlink:href="https://doi.org/10.5281/zenodo.6609072" ext-link-type="DOI">10.5281/zenodo.6609072</ext-link>​​​​​​​, Guillaumot et al., 2022). CWatM codes, tutorials, and
documentation are available at <uri>https://cwatm.iiasa.ac.at/</uri> (last access: 1 March 2022​​​​​​​) and
<uri>https://github.com/iiasa/CWatM</uri> (last access: 1 March 2022​​​​​​​). Groundwater level measurements in the Seewinkel area (Austria) are available at <uri>https://ehyd.gv.at/</uri> (Bundesministerium für Land- und Forstwirtschaft, Regionen und Wasserwirtschaft, 2021).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e2092">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/gmd-15-7099-2022-supplement" xlink:title="pdf">https://doi.org/10.5194/gmd-15-7099-2022-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e2102">LG, PB, MS, and JdB developed the model code (CWatM–MODFLOW coupling). YW and TK contributed to conceptualization and methodology. MS, PB, and LG prepared model input and observation datasets. LG performed the simulations and associated post-processing. LG prepared the paper with contributions from MS, PB, JdB, PG, TK, and YW. YW and TK acquired the funding and were in charge of project administration and supervision.​​​​​​​</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e2108">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><?xmltex \hack{\newpage}?><?xmltex \hack{\vspace*{8.2cm}}?><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e2116">Any opinions, findings, and conclusions or recommendations expressed in this material do not necessarily reflect the views of the funding organizations.
<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e2125">We thank Christian Wawra for his feedback concerning the groundwater model in Seewinkel.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e2130">This study was partially supported by the WaterstressAT project (grant no. KR19AC0K17504), funded by the Austrian Climate and Energy Fund as part of the Austrian Climate Research Programme 12th call (2019). This work was also conducted as part of the Belmont Forum Sustainable Urbanisation Global Initiative (SUGI) Food–Water–Energy Nexus theme for which coordination was supported by the US National Science Foundation under grant ICER/EAR-1829999 to Stanford University. The Austrian partners ÖFSE and IIASA are funded by the Austrian Research Promotion Agency (FFG). UFZ receives funding from the Federal Ministry of Education and Research (BMBF).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e2136">This paper was edited by Charles Onyutha and reviewed by two anonymous referees.</p>
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