STRENGTH CHARACTERISTICS AND SHEAR ACOUSTIC ANISOTROPY OF ROCK CORE SUBJECTED TO TRUE TRIAXIAL COMPRESSION

Abstract Results are presented from an initial experimental programme aimed towards evaluating the capabilities of a new true triaxial cell, designed to apply independent and unequal principal stresses to the curved surfaces of cylindrical core plugs. A series of discrete failure tests on dry specimens from two sandstone lithologies exhibiting different deformation, strength and poroperm characteristics, were conducted under azimuthal stress anisotropy ( σ 2 > σ 3 ) with σ 1 being applied axially. The true triaxial cell consistently orientates induced brittle shear fractures so that they strike parallel to the direction of σ 2 , and slip against the direction of least confinement, σ 3 . Both peak (fracture) and residual (friction) strengths are shown to be strongly dependent on the magnitude of the applied σ 2 , as well as on that of σ 3 . Results from multi-failure state testing using the conventional “triaxial” compression configuration are contrasted with discrete failure tests conducted in the true triaxial cell, by means of the familiar von Mises and extended 3-D Griffith criteria. Digitised records of shear-waves obtained at 40, 60 and 80% of peak failure strength during true triaxial testing, show clear evidence of progressively increasing stress-induced “splitting” or birefringence between the arrival of the faster S1(∥ σ 2 ) and the slower S2(∥ σ 3 ) shear-wave. Microseismic data and macroscopic observations from discrete failure tests performed within the true triaxial cell, are thus supportive of a brittle deformation mechanism involving stress-induced dilatant microcracks extending parallel to σ 2 and opening against σ 3 , progressively coalescing with increasing σ 1 to form a pervasive fault also oriented by the applied 3-D stress field.

[1]  M. Paterson Experimental Rock Deformation: The Brittle Field , 1978 .

[2]  Kiyoo Mogi,et al.  Fracture and flow of rocks under high triaxial compression , 1971 .

[3]  W. Brace,et al.  Electrical resistivity changes in saturated rocks during fracture and frictional sliding , 1968 .

[4]  C. H. Scholz,et al.  Experimental study of the fracturing process in brittle rock , 1968 .

[5]  John A. Franklin,et al.  Developments in triaxial testing technique , 1970 .

[6]  John A. Hudson,et al.  In Situ rock stresses and their measurement in the U.K.—Part I. The current state of knowledge , 1988 .

[7]  W. F. Brace A note on permeability changes in geologic material due to stress , 1978 .

[8]  T. Harper,et al.  The nature and determination of stress in the accessible lithosphere , 1991, Philosophical Transactions of the Royal Society of London. Series A: Physical and Engineering Sciences.

[9]  Gene Simmons,et al.  Stress‐induced velocity anisotropy in rock: An experimental study , 1969 .

[10]  Chandrakant S. Desai,et al.  FLUID CUSHION TRULY TRIAXIAL OR MULTIAXIAL TESTING DEVICE , 1979 .

[11]  N. Hast The state of stresses in the upper part of the earth's crust , 1967 .

[12]  Stuart Crampin,et al.  Seismic-wave propagation through a cracked solid: polarization as a possible dilatancy diagnostic , 1978 .

[13]  J. Hudson Overall properties of a cracked solid , 1980, Mathematical Proceedings of the Cambridge Philosophical Society.

[14]  B. T. Brady,et al.  A statistical theory of brittle fracture for rock materials Part II—Brittle failure under homogeneous triaxial states of stress , 1969 .

[15]  I. Gupta Seismic velocities in rock subjected to axial loading up to shear fracture , 1973 .

[16]  B. Smart,et al.  Microseismic properties of a homogeneous sandstone during fault nucleation and frictional sliding , 1994 .

[17]  H. C. Heard,et al.  EFFECTS OF THE INTERMEDIATE PRINCIPAL STRESS ON THE FAILURE OF LIMESTONE, DOLOMITE, AND GLASS AT DIFFERENT TEMPERATURES AND STRAIN RATES , 1967 .

[18]  G. Reik,et al.  STRENGTH AND DEFORMATION CHARACTERISTICS OF JOINTED MEDIA IN TRUE TRIAXIAL COMPRESSION , 1978 .

[19]  C. Froidevaux,et al.  Tectonic stresses in the lithosphere , 1983 .

[20]  J. B. Walsh,et al.  Changes in seismic velocity and attenuation during deformation of granite , 1977 .

[21]  Brian George Davidson Smart,et al.  A true triaxial cell for testing cylindrical rock specimens , 1995 .

[22]  S. Murrell,et al.  The Effect of Triaxial Stress Systems on the Strength of Rocks at Atmospheric Temperatures , 1965 .

[23]  Kiyoo Mogi,et al.  Effect of the intermediate principal stress on rock failure , 1967 .

[24]  Kiyoo Mogi,et al.  Effect of the triaxial stress system on fracture and flow of rocks , 1972 .

[25]  S. J. Green,et al.  Triaxial stress behavior of Solenhofen limestone and westerly granite at high strain rates , 1972 .

[26]  M. Wyss,et al.  Magnetism of rocks and volumetric strain in uniaxial failure tests , 1975 .

[27]  John A. Hudson,et al.  Optimizing the control of rock failure in servo-controlled laboratory tests , 1971 .