- Research Article
- Open access
- Published:

# Two-dimensional THM modelling of the large scale natural hydrothermal circulation at Soultz-sous-Forêts

*Geothermal Energy*
**volume 2**, Article number: 17 (2014)

## Abstract

### Background

A two-dimensional numerical model is developed for the Soultz-sous-Forêts reservoir from an idealized cross-section containing six homogeneous horizontal layers. The considered constitutive equations are those of homogenized saturated porous media involving Thermo-Hydro-Mechanical (THM) couplings, and most of materials properties (for brine and rocks) are taken dependent on temperature and pressure.

### Methods

The constitutive equations are solved in transient regime with the finite element software *Code_Aster* to reach a stationary state of the reservoir.

### Results

We show that a large scale natural convection is compatible with present boundary conditions if the permeability of the reservoir is of the order of 1.0×10^{−14}m^{2}. Convection cells are of the order of 1.3 km in width and we analyze several vertical profiles and maps of physical properties.

### Conclusions

A stationary convective solution at large scale is highlighted.

## Background

The interest of obtaining a numerical and coupled model of a given geothermal reservoir is fourfold. First, it allows the physical integration of laboratory measurements (rock physics), such as well logging, well head parameters, geological description, and geophysics field measurements. It shows how data are precious input parameters of the model and gives them an utility of great importance. Furthermore, numerical simulations can not only help to interpret and understand physical processes measured with laboratory and field experiments but also address and quantify the relevant processes occurring in a reservoir. Secondly, it provides a direct model based on geophysical inversion of field measurements: fluid flow, fluid pressure, temperature profile, seismicity monitoring, deformation of the ground surface (INSAR/GPS) related to reservoir modification, and gravity or electromagnetic geophysical measurements. Another advantage of simulating the reservoir behaviour is the possibility to analyse the sensitivities of parameters involved in the hydrothermal circulation (or in other physical processes). This analysis can lead to the identification of relevant processes occurring in the reservoir and material properties having the greatest influence on the model outputs, thus providing useful informations for the planification of new experimental investigations. Finally, the model can also be used as a decision tool for drilling and implacement planning, stimulation and exploitation.

Several models have been developed in literature to reproduce field measurements or to predict the value of physical properties in reservoirs. The most simplified approaches are unidimensional. They couple hydraulic with thermics as in (Pasquale et al. [2011b]), but more complex geometries have been considered in two dimensions as in ([Guillou-Frottier et al. 2013]; [Kohl et al. 2000]; [Cerminara and Fasano 2012]; [Magri et al. 2010]) or in three dimensions ([Bächler et al. 2003]; [Kohl and Mégel 2007]). Most of these models aim at reproducing or predicting the temperature profile measured in wells and/or hydraulic data obtained during injection and production phases (water flow, water pressure and temperature vs. time). Some numerical models have also been developed to account for mechanical, thermal and hydraulic couplings at the same time, with a simplified geometry of the fault network, see, e.g. [Kohl et al. (1995]) or [Gelet et al. (2012]). In addition, other thermodynamical aspects have been addressed like chemical couplings in [Bächler and Kohl (2005]).

The present work is in line with these previous approaches and can be viewed as another thermo-hydro-mechanical (THM) model of the Soultz-sous-Forêts geothermal reservoir. Our geomechanical model aims at solving constitutive equations using poroelastic medium theory, completed by reasonable boundary conditions. The goal is first to show the existence of a convective and stationary solution at large scale, considering only the regional stratigraphy and known rheophysic properties of the rock matrix and the saturating brine. This solution, different from the Elder problem ([Elder 1967]), is the starting point to proceed to a stability analysis of the reservoir when it is submitted to some mechanical, thermal or hydraulic perturbation specific of stimulation or production phases. As it will be shown below, the constitutive equations governing the evolution of the reservoir are strongly nonlinear. Consequently, one expects that the time evolution of the reservoir may be highly sensitive to initial conditions and that it can reach several metastable equilibrium states during the simulation. Given the complexity of the stability analysis, we focus in this paper on the existence of a stationary state of the Soultz-sous-Forêts reservoir. We consider it at large scale (about 10 km in width and 5 km in height). Our specificity is to assume that media are homogenized, i.e. at a scale above the representative elementary volume (REV) of the well-known contribution of [Coussy (2004]), as porous materials saturated with a single-phase fluid but including all major THM couplings. Our work is limited to a two-dimensional modelling, as in the recent contribution from [Guillou-Frottier et al. (2013]). The main geological structures retained here are as follows: (i) the main sedimentary beddings of the Rhine Graben and (ii) major petrographic transitions in the granite, which are supposed to be horizontal. No fault is included in the model at this stage. Despite these strong geometrical assumptions, we aim at accounting for the rich rheologies of rocks and brine, which constitute the main contribution of the present work compared to the above mentioned studies. At last, let us notice that a transient simulation has been chosen to ‘slowly’ evolve towards a stationary state starting from an initial (given) state of the reservoir. Indeed, integrating the constitutive equations governing THM processes is strongly constrained by stability issues due to the non-linearity of these equations.

The outline of the paper is the following: first, we present the constitutive equations considered in the model. We then develop numerical aspects and finally discuss the main results of our simulations.

## Methods

### Governing equations

The constitutive equations used in this work are those of fluid saturated porous media with THM couplings, as described in the reference book of [Coussy (2004]). Three forms of energy are considered: mechanical, thermal and hydraulic energies, each of them being characterized by a generalized displacement, strain (i.e. gradient of the latter) and stress (i.e. thermodynamic dual of the generalized strain, see Table 1). The local thermodynamic equilibrium and small perturbation assumptions are made. In doing so, no confusion between Eulerian and Lagrangian operators is then possible. The balance equations driving the evolution of extensive quantities associated with all forms of energies write the following:

where ** σ** [Pa] is the Cauchy stress tensor,

*r*[kg.m

^{-3}] the total homogenized specific mass, and

*F*^{m}[N.kg

^{-1}] the massic force density (gravity in the present paper). In this work,

*r*is decomposed into two contributions,

*r*=

*r*

_{0}+

*m*

_{ w },

*r*

_{0}[kg.m

^{-3}] being the initial total homogenized specific mass and

*m*

_{ w }[kg.m

^{-3}] the mass content of water, that is the mass of water

*d*

*m*

_{ w }that entered or left an elementary volume

*dV*of the porous medium since the initial state, per unit of volume. The vector

*M*_{ w }[kg.m

^{-2}.s

^{-1}] appearing in Equation (2) is the massic flow of water. Concerning Equation (3), {h}_{w}^{m} [J.kg

^{-1}] is the specific enthalpy of water,

*Q*[J.m

^{-3}] is the ‘non-convective’ heat (see below) and

**[J.m**

*q*^{-2}.s

^{-1}] the heat flow due to conduction. The radioactivity of rocks is taken into account through the heat source term

*Θ*[W.m

^{-3}].

The balance equations must be supplemented with not only relations between generalized stresses and strains but also relations from porous medium theory. First, we use the classical decomposition of the Cauchy stress tensor into the following two contributions:

with *σ*^{′} [Pa], the effective Cauchy stress tensor for the solid grains behaviour and *σ*_{
p
} [Pa], the hydraulic stress. In this work, the behaviour of solid grains is assumed to be thermo-elastic and linear, so that we can introduce the linear total strain ** ε** and the drained elasticity tensor [Pa] with the following incremental law:

in which *α*_{0} [K^{-1}] stands for the linear thermal dilation of the dry material, *T* [K] the absolute temperature and ** 1** the unit tensor. Below, we denote by

*E*[Pa] and

*ν*the drained Young’s modulus and Poisson’s ratio, respectively. The porous behaviour is described by the incremental evolution of the Eulerian porosity

*ϕ*and the hydraulic stress

*σ*

_{ p }[Pa] ([Coussy 2004]) as follows:

where *b* is the Biot coefficient, *ε*_{
v
}=Tr (** ε** ) is the volume total strain,

*p*

_{ w }[Pa] is the water pressure and

*K*

_{ s }[Pa] is the bulk modulus of solid grains. The mass content of water can then be expressed as the variation of water mass per unit of volume between the actual state and the initial state

with {\rho}_{w}^{0} [kg.m^{-3}] the initial specific mass of water and *ϕ*_{0} the initial porosity.

The hydraulic and thermal phenomena are governed by the Darcy’s law and Fourier’s law, respectively, and most rock properties (like the specific heat at constant stress {c}_{0}^{\sigma} or the thermal conductivity *λ*) are assumed to depend on temperature *T* and/or porosity *ϕ* (see the next section for a detailed presentation). More precisely, if we denote by *K*_{int} [m^{2}], the intrinsic permeability, we consider the following well-known relations:

Since measurements of the rock permeability along the wells exhibit several orders of magnitude of variability, we decided to neglect the influence of porosity on permeability to improve the numerical stability, despite the existence of well-known models in the literature (e.g. Van-Genuchten model). In Equation (3), the non-convected heat *Q* can be understood as the ‘variation of heat per unit of volume not coming from convection nor conduction’. It comes not only from the heat produced by the volumic deformation of solid grains and water but also from the internal energy of the homogenized medium. It follows the equality

with *K*_{0} [Pa] the drained bulk modulus, *α*_{
w
} [K^{-1}] the dilation of water, and {c}_{0}^{\epsilon} [J.kg^{-1}.K^{-1}] the specific heat at constant strain. The latter is calculated from the specific heat at constant stress {c}_{0}^{\sigma} by using the following formula ([Coussy 2004]):

### Physical properties of constituents

At this stage, the main constitutive equations have been presented, and this section is devoted to the presentation of relationships governing the evolution of physical properties with temperature, porosity, and pressure. The entire set of properties is extracted from the literature dealing with experimental investigations.

In an attempt to characterize as precisely as possible the convective movement of water and the associated heat flow, the properties of water (specific mass *ρ*_{
w
}(*T*, *p*_{
w
}), specific enthalpy {h}_{m}^{w}(T,{p}_{w}), dynamic viscosity *μ*_{
w
}(*T*), thermal dilation *α*_{
w
}(*T*), and specific heat {c}_{w}^{p}\left(T\right)) are assumed to depend on the pressure and/or temperature. In this first approach, the brine of the reservoir is treated as a pure solution of NaCl, characterized by a mass content of about 100 kg.m^{-3} in accordance with the paper of [Genter et al. (2010]). If we admit a mean specific mass of brine equal to 1,000 kg.m^{-3} - corresponding to the specific mass at temperature of about 150°C and pressure of about 25 MPa, representative values in the reservoir - this mass content is equivalent to a molar content of 1.5 mol.kg^{-1}. The specific mass is here governed by the following incremental relation:

with *K*_{
w
} [Pa] as the (constant) bulk modulus and *α*_{
w
}(*T*) as the thermal dilation assumed quadratic with respect to the temperature *T*

where *T*^{0} is a reference temperature equal to 293 K. Note that Equation (13) was already used in the work of [Segall and Rice (2006]) but with constant thermal dilation *α*_{
w
}(*T*)=*α*_{
w
} describing a linear dependence of the relative variation of density with temperature and pressure. Several other models exist in the literature, see, e.g. the review of [Francke and Thorade (2010]), but Equation (13) has been used because it is the law implemented in *Code_Aster*. Equation (13) can be rewritten in the following integral form:

where {p}_{w}^{0}=0.1\phantom{\rule{0.3em}{0ex}}MPa is a reference water pressure and {\rho}_{w}^{0} is a synthetic notation for {\rho}_{w}\left({T}^{0},{p}_{w}^{0}\right). The bulk modulus *K*_{
w
} and the coefficients {a}_{{\alpha}_{w}}, {b}_{{\alpha}_{w}} and {c}_{{\alpha}_{w}} have been calibrated to make Equation (15) fit the experimental correlation proposed in [Rowe and Chou (1970]) evaluated for a NaCl mass fraction *w*=0.1 (corresponding to 100 kg.m^{-3} assuming a mean density of 1,000 kg.m^{-3}). The result of the fit and the derived evolution of *α*_{
w
} with temperature are plotted in Figures 1 and 2.

Concerning the heat capacity, the quadratic correlation given in [Zaytsev and Aseyev (1992]) for NaCl solutions is used

with *T*^{1}=273.15 K, see Figure 3. The same authors propose a correlation for the thermal conductivity but only valid for a temperature varying between 0°C and 100°C. We decided to extrapolate this correlation over 100°C with a quasi constant value by using the following exponential relation:

which is plotted in Figure 4. The viscosity of the brine is approximated by the Eyring law (Figure 5)

fitted on the data of [Rowe and Chou (1970]). Finally, the specific enthalpy is governed by the following relation:

in which *α*_{
w
}(*T*) and {c}_{w}^{p}\left(T\right) are given by Equations (14) and (16), respectively. In Equations (15), (16), (17), and (18), the quantities

are constant parameters which are given in Table 2.

Complementary to water properties, several assumptions need to be made to calculate homogenized thermal properties. The thermal conductivity *λ* is hereby homogenized by using a classical mixing law

where the lower scripts ‘ _{
s
}’ and ‘ _{
w
}’ still refer to solid grains and water, respectively. To estimate the thermal conductivity of solid grains, we rewrite Equation (20) for the dry state

By neglecting the thermal conductivity of air, we obtain the following:

Since several values are available for *λ*_{dry}(*T*) in the literature, we can calculate *λ*_{
s
}(*T*) using Equation (22). From experimental studies (see Tables 3 and 4 for the references), we retain a linear variation of *λ*_{dry}(*T*) with temperature:

A similar method is applied to calculate (i) the specific heat at constant stress of solid grains

from a linear variation of {c}_{\text{dry}}^{\sigma}\left(T\right) (in accordance with experimental data found in the literature):

and (ii) the initial and homogenized specific masses

being the initial density of water. Tables 3 and 4 present a synthetic literature review of sediments and granite properties. It must be noted that these values were obtained on similar rocks to those present in Soultz-sous-Forêts but not on the drilling cores of the reservoir. However, they provide orders of magnitude which are sufficient to reproduce the main mechanisms involved in the reservoir. From this literature review, we took the set of properties given in Tables 2 and 5 as inputs of the numerical model.

### Numerical model

The geological layers considered in this work are slightly adapted from the idealized cross section presented in the paper of [Guillou-Frottier (2011]) and inspired by the contribution of [Genter et al. (1997]) and [Genter and Traineau (1992]). We only consider six layers: the first three layers correspond to the sedimentary cover, i.e. Tertiary to Jurassic marls and clays between 0 and 800 m of depth, Keuper and Muschelkalk formations between 800 and 1,000 m, and Buntsandstein sandstones between 1,000 and 1,400 m. The granitic basement is represented by three other layers corresponding to the different petrographic units of the granite massif. On top, a thin layer between 1,400 and 1,550 m is considered to reproduce the strongly altered granite from the paleo-erosion surface. The second layer, between 1,550 and 3,700 m, corresponds to a more fractured monzonitic granite in which the homogenized permeability is high. The last layer, located between 3,700 and 5,350 m, corresponds to a crystalline unit made of a porphyritic monzogranite and a fine grained granite. The height of the model corresponds to the height of the measured temperature profile obtained in GPK2, see, e.g. [Pribnow and Schellschmidt (2000]).

The constitutive equations presented in the two last sections are solved with the Finite Elements Method. The implicit Euler time scheme is used, and the non-linear system giving the increment of the generalized nodal displacements is solved by the Newton-Raphson algorithm. The six layers are meshed with quad elements (see Figure 6) performing an eight-term polynomial interpolation of mechanical displacements and a four-term polynomial interpolation of pressures and temperatures. Below, we denote by *x* the horizontal direction inside the mesh, *y* the vertical direction, and *z* the out-of-plane direction perpendicular to it. For symmetry reasons and to save CPU time, the mesh represents half the reservoir. The boundary conditions of the problem are the following: normal mechanical displacement is nil, and no friction is considered on the left and lower boundaries of the domain, whilst the upper boundary is stress-free. A normal stress {\sigma}_{\mathit{\text{xx}}}^{\text{reg}} - with no shear - is applied on the right boundary of the reservoir to account for the regional stress (presented in the next section). For thermal aspects, a temperature of 15°C and 208°C is imposed on the upper and lower boundary, respectively. These values are directly taken from the experimental temperature profile shown in Figure 7. The thermal flow vanishes on lateral facets. For hydraulic aspects, the flow vanishes on all boundaries except the upper one for which the water pressure approximately equals the atmospheric pressure, i.e. *p*_{
w
}=0.1 MPa. Figure 8 summarizes the entire set of boundary conditions.

The simulation is carried out with the assumption of plane strains (in the *x*, *y* plane) by using the French finite elements software *Code_Aster* ([EDF 2014]). Some routines of the latter have been overloaded to integrate the constitutive equations presented above. First, the boundary conditions and gravity are progressively applied during a ‘short’ period of 100 years, starting from a temperature and a water pressure field presented hereafter. In a second step, the code iterates with a time increment equal to 1,000 years until a stationary state is reached. A stationary state is here defined by using four convergence indicators *I*_{
n
}(*X*) involving the generalized displacements *X*≡** ξ** ,

*p*

_{ w },

*T*calculated for different time increments

*t*

_{ n }. More precisely, a stationary state is reached if

for *m* consecutive time increments *t*_{
n
}, with *X*_{
n
}≡** ξ** (

*t*

_{ n }),

*p*

_{ w }(

*t*

_{ n }),

*T*(

*t*

_{ n }). The notation ‘ maxnodes[⋆]’ indicates the maximal nodal value of the quantity ‘ ⋆’. In practice, a value of

*m*=15, and the following maximal errors were used:

Once a stationary state is obtained, post-processing operations - such as the calculation of the simulated vertical profiles of temperature and vertical stress - are performed.

### Initial state

To initiate the simulation, several fields like generalized displacements, internal variables and generalized stress have to be prescribed. First, we start the simulation with

a temperature field rather close of the observed temperature profile in the vertical direction *y* for *x*=0. A sinusoidal evolution in the horizontal direction *x* and satisfying the boundary conditions are taken into account as an initial perturbation (see Figure 9). The water pressure field is simply initialized by a linear profile

and no mechanical displacements are considered, *ξ*^{ini}=** 0** .

The two internal variables used in *Code_Aster* for the simulation of saturated porous media are the variations of water density {\rho}_{w}-{\rho}_{w}^{0} and porosity *ϕ*−*ϕ*_{0}. In the present model, these variables are respectively initialized with Equation (15) and the integral form of Equation (6) computed for *ε*_{
v
}=0

Obviously, both formula are evaluated for *T*≡*T*^{ini}(*x*, *y*) and {p}_{w}\equiv {p}_{w}^{\text{ini}}(x,y).

For the initial stress field {\sigma}_{\mathit{\text{ij}}}^{\text{ini}}, the linear correlation of ([Heineman 1994]) giving the experimental regional stress has been used and linearly extrapolated to the top of the reservoir

with *y*_{0}=−1,400 m. The values of the *a*_{
ij
} and *b*_{
ij
} coefficients are given in Table 6. Note that, as previously written, the horizontal initial stress {\sigma}_{\mathit{\text{xx}}}^{\text{reg}} is used as a stress boundary condition, see Figure 8. Finally, the hydraulic stress is initialized as follows:

## Results and discussion

First, the numerical dependence of the results to mesh refinement and element types has been investigated. Figure 10 shows vertical profiles of calculated quantities at *x*=0 for two kinds of finite elements (triangles and quads) and mesh sizes starting from 330 to 2,070 quad elements. The meshes using triangle elements have been obtained by splitting the quad elements along a diagonal, symbolically:

where the blue nodes are the nodes of the linear mesh (used for water pressure and temperature degrees of freedom) and the red ones are the supplementary nodes of the quadratic mesh (used for mechanical displacements). Based on the results of the most refined meshes, it can be concluded that a suitable mesh refinement was reached and that element type have no significant effect on the simulation. Subsequently, we decided to work arbitrarily with quad elements.

The temperature map of the obtained stationary state (see Figure 11) clearly shows convection loops having a size of about 1.3 km. Two other simulations with a model of 20 and 30 km in width proved that the cell width is quasi constant independently of the model width. Furthermore, the value of permeability of the five upper geological layers that trigger the convection seems to be approximately between 1.0×10^{−14} and 1.0×10^{−15} m^{2}, see Figure 12.

The temperature map of Figure 11 illustrates the fact that the vertical profile of temperature depends on the horizontal coordinate *x*. To quantify the lateral variation of temperature and other calculated quantities with the horizontal coordinate *x*, different vertical profiles have been plotted in Figure 7a every 500 m between 0 and 2,500 m. We recall that the value *x*=0 corresponds to the left of the mesh. A lateral variation of about 50°C is observed in the interval of depth corresponding to the zone of convective flow. At this stage, the numerical profile reproduces the main tendency of the experimental profile, whilst not fitting exactly the data in particular in the upper part of the convective cell (Buntsandstein layer) where the large scale permeability is possibly underestimated. This difference can also be explained by the fact that we used values of input parameters extracted from the literature without any back analysis to refine them.

The vertical profiles of Figure 7b and the section of Figure 13 show that the variation of porosity *ϕ*−*ϕ*_{0} ranges between 0.1% and 20% of the initial porosity *ϕ*_{0}. These rather low values could be explained by a competition between two mechanisms: (i) a decrease of the porosity due to the lithostatic stress (gravity is applied during the whole simulation) and (ii) an increase due to the dilation of water filling the pores.

To support the last argument, we return to the definition of the Eulerian porosity as the ratio between the actual void volume and the total actual volume of an elementary representative piece of saturated porous medium. Since the dilation of solid grains (≈1.4×10^{−5}, quasi independent of temperature) is about ten times smaller than the dilation of water (≥1.5×10^{−4} at 50°C), and since the system is globally unconfined and drained because of the upper stress-free and drained boundary, one may surmise that an increase of temperature will greatly increase the volume of water whilst keeping the volume of solid grains quasi constant, thus explaining a possible increase of porosity due to thermal effects. The vertical profiles presented in Figure 7b indicate that the two mentioned contradictory effects seem to globally balance. Finally, one should keep in mind that no dependences of the bulk moduli (solid framework and water) with temperature and pressure have been taken into account, and that these dependences may significantly affect the variation of porosity.

For hydraulic aspects, we note from the vertical profiles plotted in Figure 7 that the field of water pressure keeps globally linear with depth. The order of magnitude of the vertical Darcy velocity *V*_{
y
}=*M*_{
w
}.*e*_{
y
}/*ρ*_{
w
} in the fractured granite is 20 cm.year^{-1}, which is in accordance with the value 15 cm.year^{-1} obtained by ([Guillou-Frottier et al. 2013]) using slightly different permeability profiles. The change of sign of *V*_{
y
} inside the convective loop (Figure 7f) is obviously the consequence of ascending and descending movements of water triggered by the variation of its density (see Figure 14). Globally, the impact of hydraulics on mechanics seem to be rather low. Indeed, if we consider the vertical profiles of total stress pictured in Figure 15, calculated for different values of *x*, one can see that the hydraulic stress *σ*_{
p
} keeps relatively small (less than 25%) relative to total stresses whatever the position of the vertical profile. We conclude that effective stress and total stress are approximately the same in this model. Furthermore, the shear stress *σ*_{
hv
} corresponding to the shear associated with the horizontal and vertical directions is negligible. It is then possible to claim that the total Cauchy stress tensor keeps diagonal. In addition, the vertical stress *σ*_{
v
} remains close to the initial lithostatic stress *σ*_{litho}=*r*_{0}*g* *z*, showing that thermo-hydraulic phenomena do not have a great impact on the vertical stress state in the reservoir. Of course, this conclusion obtained in two dimensions and with the assumption of plane strains could be different with a three-dimensional model including the main faults present in the reservoir.

## Conclusions

The two-dimensional numerical model developed in this work lead us to the following main conclusions:

A stationary convective solution at large scale is highlighted. The order of magnitude of the convective cell size in the reservoir is about 1.3 km, a value being independent of the model width. A periodic pair of cells is then 2.6 km wide. We insist on the fact that the unicity of this solution is not guaranteed. Furthermore, the way the initial conditions influence the final result is a difficult task accounting for the strong non-linearity of the constitutive equations. The unicity of this solution, its stability, and the way initial conditions may influence the final results will be analysed in a future work.

The order of magnitude of the maximal vertical Darcy velocity is 20 cm.year^{-1}, a value confirmed by previous works found in the literature.

The field of water pressure keeps globally linear with depth, and the influence of thermo-hydraulic coupling on the vertical stress state of the reservoir is rather low.

The large scale convection is triggered with a permeability in the five upper geological layers of about 1.0×10 to 1.0×10^{−15} m^{2}.

One should keep in mind that these first conclusions have been obtained with a two-dimensional model under the assumption of plane strains. They should consequently be confirmed or infirmed by a three-dimensional model, accounting for the presence of main faults in the reservoir. Works are currently in progress to follow this route and to make our model more realistic.

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## Acknowledgements

The author are grateful to the reviewers for their constructive expertise and the useful hints aimed at improving the content of our manuscript. They also gratefully acknowledge Dr. François Cornet for very helpful discussions. This work has been published under the framework of the LABEX ANR-11-LABX-0050-G-EAU-THERMIE-PROFONDE and benefits from a funding from the state managed by the French National Research Agency as part of the ‘Investments for the Future’ program.

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VM carried out the numerical study and wrote the first version of the paper. The three other authors conducted the final version of the manuscript. All authors read and approved the final manuscript.

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Magnenet, V., Fond, C., Genter, A. *et al.* Two-dimensional THM modelling of the large scale natural hydrothermal circulation at Soultz-sous-Forêts.
*Geotherm Energy* **2**, 17 (2014). https://doi.org/10.1186/s40517-014-0017-x

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DOI: https://doi.org/10.1186/s40517-014-0017-x