Field-scale acoustic investigation of a damaged anisotropic shale during a gallery excavation

In the Opalinus Clay formation at the Mont Terri Underground Rock Laboratory, the gallery Ga08 was excavated in August 2008 to join the end-face of the pre-existing gallery Ga04. The aim of the present work was to perform in situ acoustic experiments to monitor the evolution of the Excavation Damaged Zone (EDZ) induced during the gallery construction. The end-face of Ga04 was instrumented with two arrays of acoustic transducers allowing for the active and passive seismic monitoring, i.e. acoustic survey and micro-seismicity. From the acoustic survey data, which required a high energy acoustic source to emit high frequency signals (21, 25, 31 and 38 kHz), the rock mass was observed to be anisotropic and heterogeneous at the scale of the experiment. P-wave velocities were determined to be, in average, between 3300 m/s along a structural bedding plane, and 2700 m/s at θ≃70° incidence relative to that. Assuming a transversely isotropic shale formation, the P-wave velocity dependence versus θ was modeled using Thomsen's Weak Transverse Isotropy model (Thomsen, 1986) [36]. Thomsen's P-wave anisotropy parameter was found to be ϵ≃0.15, and the fifth Thomsen's parameter controlling the deviation of the wave front from an ellipsoidal geometry was found to be δ≃0.16. The S-wave velocity was estimated along a single direction of aligned receivers and turned out to be around 1560 m/s at θ≃30°. We also show that the rock mass acts as a frequency filter for acoustic waves, related to the rock mass heterogeneities, i.e. the inter-bedding structure, which induces wave scattering and refraction. From the micro-seismicity data, we identified a large number of micro-seismic events (MSEs) detected on the acoustic arrays during and following the excavation. Most of the MSEs were induced on the excavated face but we also located some MSEs inside the rock mass itself. We show that these events are located close to a major fault, which seems to be reactivated by the excavation process.

[1]  N. Hoteit,et al.  Electrical tomography monitoring of the excavation damaged zone of the Gallery 04 in the Mont Terri rock laboratory : Field experiments, modelling, and relationship with structural geology , 2006 .

[2]  Yves Guéguen,et al.  Dispersion and anisotropy of elastic waves in cracked rocks , 2003 .

[3]  Christophe Nussbaum,et al.  Analysis of tectonic structures and excavation induced fractures in the Opalinus Clay, Mont Terri underground rock laboratory (Switzerland) , 2011 .

[4]  Patrick N. J. Rasolofosaon,et al.  Comparison between permeability anisotropy and elasticity anisotropy of reservoir rocks , 2002 .

[5]  N. Chandler,et al.  Excavation-induced damage studies at the Underground Research Laboratory , 2004 .

[6]  Y. Guéguen,et al.  A simplified model of effective elasticity for anisotropic shales , 2009 .

[7]  Dominique Gibert,et al.  Nonlinear synthesis of input signals in ultrasonic experimental setups. , 2004, The Journal of the Acoustical Society of America.

[8]  Paul Bossart,et al.  Geological and hydraulic characterisation of the excavation disturbed zone in the Opalinus Clay of the Mont Terri Rock Laboratory , 2002 .

[9]  Dominique Gibert,et al.  Multiscale analysis of waves reflected by complex interfaces: Basic principles and experiments , 2002 .

[10]  D. Dewhurst,et al.  Estimation of anisotropy parameters using the P-wave velocities on a cylindrical shale sample , 2011 .

[11]  D. Gibert,et al.  Seismic tomography of the Excavation Damaged Zone of the Gallery 04 in the Mont Terri Rock Laboratory , 2008 .

[12]  Paul Bossart,et al.  Research in the Mont Terri Rock laboratory: Quo vadis? , 2007 .

[13]  Jung-Ho Kim,et al.  Resistivity and offset error estimations for the small-loop electromagnetic method , 2008 .

[14]  François Forney Caractérisation par méthodes ultrasoniques de la zone endommagée induite par le creusement d'un tunnel en milieu argileux : cas d'étude au tunnel du Mont Terri, Suisse , 1999 .

[15]  A. Bona,et al.  Thomsen's parameters from p‐wave measurements in a spherical sample ‡ , 2012 .

[16]  T. Sato,et al.  In-situ experiments on an excavation disturbed zone induced by mechanical excavation in Neogene sedi , 2000 .

[17]  T. Mukerji,et al.  The Rock Physics Handbook: Contents , 2009 .

[18]  Valentin Gischig,et al.  Experimental Study of the Brittle Behavior of Clay shale in Rapid Unconfined Compression , 2011 .

[19]  Y. Guéguen,et al.  Characteristics of anisotropy and dispersion in cracked medium , 2011 .

[20]  D. Gibert,et al.  Anisotropy of electrical conductivity of the excavation damaged zone in the Mont Terri Underground Rock Laboratory , 2010 .

[21]  L. Thomsen Weak elastic anisotropy , 1986 .

[22]  S. Rahman,et al.  Borehole collapse analysis incorporating time-dependent pore pressure due to mud penetration in shales , 2000 .

[23]  The Assessment of Damage Around Critical Engineering Structures Using Induced Seismicity and Ultrasonic Techniques , 2002 .

[24]  Mark Kachanov,et al.  Microcrack‐induced elastic wave anisotropy of brittle rocks , 1995 .

[25]  J. B. Walsh The effect of cracks on the compressibility of rock , 1965 .

[26]  Bd Thompson,et al.  Quantifying Damage, Saturation and Anisotropy in Cracked Rocks by Inverting Elastic Wave Velocities , 2006 .

[27]  J. Henry,et al.  Characterization of the moduli of elasticity of an anisotropic rock using dynamic and static methods , 1993 .

[28]  M. Toksöz,et al.  Ultrasonic P and S wave attenuation in dry and saturated rocks under pressure , 1980 .

[29]  Y. Guéguen,et al.  Crack-induced anisotropy in crustal rocks: Predicted dry and fluid-saturated Thomsen’s parameters , 2009 .

[30]  D. S. Collins,et al.  Quantification and interpretation of seismicity , 2004 .

[31]  Bin Liu,et al.  Relationship between anisotropy of P and S wave velocities and anisotropy of attenuation in serpentinite and amphibolite , 1997 .

[32]  J. C. Jaeger,et al.  Fundamentals of rock mechanics , 1969 .

[33]  D. Gibert,et al.  The wavelet response as a multiscale characterization of scattering processes at granular interfaces. , 2006, Ultrasonics.

[34]  Paul Bossart,et al.  Structural and hydrogeological characterisation of the excavation-disturbed zone in the Opalinus Clay (Mont Terri Project, Switzerland) , 2004 .

[35]  D. S. Collins,et al.  Seismic studies of rock fracture at the Underground Research Laboratory, Canada , 2001 .

[36]  Tsuyoshi Ishida,et al.  Strain monitoring of borehole diameter changes in heterogeneous jointed wall rock with chamber excav , 2000 .

[37]  Yves Guéguen,et al.  Anisotropy of elastic wave velocities in deformed shales: Part 2 — Modeling results , 2008 .

[38]  Laurent Molez,et al.  Shale dynamic properties and anisotropy under triaxial loading: experimental and theoretical investigations , 2007 .

[39]  Y. Guéguen,et al.  Anisotropy of elastic wave velocities in deformed shales: Part 1 — Experimental results , 2008 .

[40]  D. Gibert,et al.  Anomalies of noble gases and self-potential associated with fractures and fluid dynamics in a horizontal borehole, Mont Terri Underground Rock Laboratory , 2013 .

[41]  S. Shapiro,et al.  Stress sensitivity of elastic moduli and electrical resistivity in porous rocks , 2004 .