Abstract
This study is part of numerical simulations performed on an in-situ heating test conducted by the French National Radioactive Waste Management Agency (Andra) at the Meuse/Haute-Marne Underground Research Laboratory (URL) to study the thermo-hydromechanical behavior of the host Callovo-Oxfordian COx claystone in quasi real conditions, through the international research project DECOVALEX. We present a numerical study of damage and cracking process in saturated claystone subjected to thermo-hydromechanical coupling by considering material heterogeneity distribution. For this purpose, a macroscopic elastic model is first determined by using two steps of homogenization by taking into account the effects of porosity and mineral inclusions. This model is implemented into a finite element code devoted to solving thermo-hydromechanical coupling problems. The nucleation and propagation of cracks are described by using an extended phase-field method, considering the effects of temperature and fluid pressure on the evolution of phase-field. The proposed model is applied to the numerical analysis of cracking process due to excavation and heating around a group of boreholes (CRQ). The numerical results of the 3D simulation are compared with in-situ measurements of temperature and pore pressure distribution. The excavation damage zone and heating fracture is reproduced and analysed according to the structure of the heating position and the heterogeneity of the rock.
Highlights
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A phase-field model is developed with thermo-hydromechanical processes;
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Both tensile and shear cracks are taken into account;
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Crack nucleation is emphasized by spatial heterogeneity of material properties;
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Cracking processes due to thermal-hydraulic interaction are analyzed in three-dimensional conditions.
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Data Availability
The data that support the findings of this study are available from the corresponding author upon reasonable request.
Abbreviations
- \(\alpha _b\) :
-
Scalar of thermal dilation coefficient in drained condition for isotropic material
- \(\alpha _f\) :
-
Thermal dilation coefficient of fluid
- \(\alpha _m\) :
-
Differential thermal dilation of saturated porous medium
- \(\varvec{\sigma }\) :
-
Stress tensor
- \(\varvec{I}\) :
-
Second order unit tensor
- \(\epsilon ^e\) :
-
Elastic strain tensor
- \(\Gamma\) :
-
Set of cracks
- \(\gamma\) :
-
Crack density
- \(\phi\) :
-
Porosity
- \(\rho ^0_f\) :
-
Volumetric density of fluid
- \(\theta\) :
-
Variation of temperature
- \(A_{\Gamma }\) :
-
Crack surface
- b :
-
Biot coefficient for isotropic material
- \(C_\sigma ^b\) :
-
Volumetric specific heat for constant stress under drained condition
- \(d^s\) :
-
Damage variable of shear crack
- \(d^t\) :
-
Damage variable of tensile crack
- E :
-
Total energy
- \(E_c\) :
-
Fracture surface energy
- \(E_e\) :
-
Elastic strain energy of damaged material
- \(K_b\) :
-
Bulk modulus of drained material
- \(K_f\) :
-
Bulk modulus of fluid
- \(K_m\) :
-
Bulk modulus of solid matrix
- \(K_{reuss}\) :
-
Reuss equivalent bulk modulus
- M :
-
Scalar coefficient of Biot modulus
- m :
-
Fluid mass change per unit initial volume
- p :
-
Fluid pressure or pore pressure
- s :
-
Entropy
- T :
-
Temperature
- \(w_c\) :
-
Energy density per unit volume requested to create crack
- \(w_e\) :
-
Elastic strain energy of cracked material
- \(\beta _i\) :
-
Mean value of random variable for mineral inclusions volumetric fraction
- \(\beta _p\) :
-
Mean value of random variable for porosity
- \(\mathbb {C}^{hom}\) :
-
Macroscopic elastic tensor of heterogeneous rocks
- \(\mathbb {C}^{in}\) :
-
Elastic tensor of inclusions
- \(\mathbb {C}^{mp}\) :
-
Effective elastic tensor of porous matrix
- \(\mathbb {C}^{m}\) :
-
Elastic tensor of solid matrix
- \(\mathbb {I}\) :
-
Fourth order unit tensor
- \(\mathbb {P}^i\) :
-
Fourth order Hill tensor for spherical inclusions
- \(\mathbb {P}^p\) :
-
Fourth order Hill tensor for ellipsoidal pores
- \(\mathbb {P}^{\pm }_\sigma\) :
-
Operators for spectral decomposition of stress tensor
- \(\Omega _i\) :
-
Volume of inclusions
- \(\Omega _m\) :
-
Volume of solid clay matrix
- \(\Omega _p\) :
-
Volume of pores
- \(\sigma ^t_1\) :
-
Major Terzaghi effective principal stress
- \(\sigma ^t_3\) :
-
Minor Terzaghi effective principal stress
- \(\sigma _t\) :
-
Average value of uniaxial tensile strength
- \(\varphi\) :
-
Friction angle
- \(\xi _i\) :
-
Probability density for inclusions
- \(\xi _p\) :
-
Probability density for pores
- c :
-
Cohesion
- \(f_i\) :
-
Random distribution of mineral inclusions volumetric fraction
- \(f_p\) :
-
Random distribution of porosity
- G :
-
Shear modulus
- \(g_c^s\) :
-
Toughness parameter for shear crack
- \(g_c^t\) :
-
Toughness parameter for tensile crack
- \(h_s\) :
-
Degradation variable for shear crack
- \(h_t\) :
-
Degradation variable for tensile crack
- k :
-
Small positive value to avoid calculating error
- \(l_d\) :
-
Length scale parameter for width of smeared cracks
- \(m_i\) :
-
Homogeneity index for mineral inclusions
- \(m_p\) :
-
Homogeneity index for pores
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Acknowledgements
This work is jointly supported by the French National Agency for radioactive waste management (ANDRA), the DECOVALEX project, the National Natural Science Foundation of China (No. 12202099) and the China Postdoctoral Science Foundation funded project (No. 2023M730525). DECOVALEX is an international research project comprising participants from industry, government and academia, focusing on development of understanding, models and codes in complex coupled problems in sub-surface geological and engineering applications. The authors appreciate and thank the DECOVALEX-2023 Funding Organizations for their financial and technical support of the work described in this paper. The statements made in the paper are, however, solely those of the authors and do not necessarily reflect those of the Funding Organizations.
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Appendix: Positions of Sensors and Dates of the Heater Boreholes Drilling
Appendix: Positions of Sensors and Dates of the Heater Boreholes Drilling
In order to identify the coordinates of the sensor points, the origin (0,0,0) of the model domain is located at the mid-distance between the heads of borehole CRQ1720 and CRQ1721 (See Tables 5 and 6). In this way, the studied 3D domain of cube with a side length of 50 m vary between x=\(-\) 2.6 m to 47.4 m (parallel to the heater boreholes); y=\(-\) 25.0 m to 25.0 m (parallel to the GCS gallery) and z = – 25 m to 25 m (perpendicular to the heater boreholes and the GCS gallery). In this defined coordinate system, the position of sensor points are shown as follows:
The detail date of the main operations during CRQ test is:
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The drift of GCS gallery: \(15{th}\) September 2010
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The drift of heater boreholes: between \(20{th}\) and \(30^{30}\) October 2017 (see Table)
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The first heating phase: between \(3{rd}\) June and \(31{st}\) July 2019
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The second heating phase: between \(13{th}\) January and \(14{th}\) February 2020
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Yu, Z., Shao, J., Sun, Y. et al. Three-dimensional Modeling of Cracking with Thermo-hydromechanical Process by Considering Rock Heterogeneity. Rock Mech Rock Eng (2023). https://doi.org/10.1007/s00603-023-03536-4
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DOI: https://doi.org/10.1007/s00603-023-03536-4