Critical wedges in three dimensions: Analytical expressions from Mohr‐Coulomb constrained perturbation analysis

We present simple analytical expressions for evaluating three-dimensional stress fields in critical wedges (Coulomb failure throughout) that are deforming within an oblique convergent zone. We assume that the load and geometry variations in the lateral direction, and the topographic slope, are relatively small. The stress state of a two dimensional critical wedge is perturbed by admitting a small lateral shear, which is accommodated (to maintain criticality) by a reduction in the dominant normal compressive stress. Cohesionless cases are further simplified with Taylor series expansions in the topographic slope. The analytical expressions distinguish the behavior of strong base wedges associated with steep slopes from weak base wedges with more modest slopes, and are reliable for lateral shear values as large as half the lithostatic load. In the weak base case where the vertical shear is small, the orientations of the principal stresses are very sensitive to the perturbation. As the lateral shear increases through relatively small values, the roles of the lateral and vertical coordinate axes are interchanged, with a resultant transition from predominantly thrust failure to strike slip failure. Transition to strike slip in the strong base case is more gradual. The particular value of horizontal shear for which transition occurs also depends on the difference of the minor normal stresses. We produce an analytical expression predicting displacement patterns compatible with those observed in natural and analog orogens. Displacement partitioning is predicted for weak base wedges due to minor changes in lateral boundary conditions associated with variable orogen geometry.

[1]  F. A. Dahlen,et al.  Noncohesive critical Coulomb wedges: An exact solution , 1984 .

[2]  J. Angelier,et al.  Determination of the mean principal directions of stresses for a given fault population , 1979 .

[3]  J. Suppe,et al.  State of stress near the San Andreas fault: Implications for wrench tectonics , 1987 .

[4]  C. Teyssier,et al.  Strain modeling of displacement-field partitioning in transpressional orogens , 1994 .

[5]  S. Khan,et al.  Strike‐slip faulting in a foreland fold‐thrust belt: The Kalabagh Fault and Western Salt Range, Pakistan , 1990 .

[6]  R. Norris,et al.  Anatomy, structural evolution, and slip rate of a plate-boundary thrust: The Alpine fault at Gaunt Creek, Westland, New Zealand , 1994 .

[7]  C. Beaumont,et al.  Three‐dimensional numerical experiments of strain partitioning at oblique plate boundaries: Implications for contrasting tectonic styles in the southern Coast Ranges, California, and central South Island, New Zealand , 1995 .

[8]  J. Suppe,et al.  Mechanics of fold‐and‐thrust belts and accretionary wedges: Cohesive Coulomb Theory , 1984 .

[9]  James R. Rice,et al.  Chapter 20 Fault Stress States, Pore Pressure Distributions, and the Weakness of the San Andreas Fault , 1992 .

[10]  J. Platt MECHANICS OF OBLIQUE CONVERGENCE , 1993 .

[11]  H. Weitzner,et al.  Perturbation Methods in Applied Mathematics , 1969 .

[12]  D. Bamford,et al.  Lithospheric structural contrasts across the Caledonides of northern Britain , 1979 .

[13]  P. Koons,et al.  Geodetic analysis of model oblique collision and comparison to the Southern Alps of New Zealand , 1995 .

[14]  R. J. Lillie,et al.  Changing mechanical response during continental collision: active examples from the foreland thrust belts of Pakistan , 1994 .

[15]  William M. Chapple,et al.  Mechanics of thin-skinned fold-and-thrust belts , 1978 .

[16]  Peter O. Koons,et al.  The obliquely-convergent plate boundary in the South Island of New Zealand: implications for ancient collision zones , 1990 .

[17]  Peter O. Koons,et al.  Three‐dimensional critical wedges: Tectonics and topography in oblique collisional orogens , 1994 .

[18]  Peter O. Koons,et al.  Two-sided orogen: Collision and erosion from the sandbox to the Southern Alps, New Zealand , 1990 .

[19]  M. Zoback,et al.  New Evidence on the State of Stress of the San Andreas Fault System , 1987, Science.

[20]  G. Stockmal Modeling of large-scale accretionary wedge deformation , 1983 .

[21]  Basil Tikoff,et al.  Oblique plate motion and continental tectonics , 1995 .

[22]  M. Beck On the mechanism of tectonic transport in zones of oblique subduction , 1983 .

[23]  F. Lehner Comments on “Noncohesive critical Coulomb wedges: An exact solution” by F. A. Dahlen , 1986 .

[24]  P. Molnar,et al.  Fault plane solutions of earthquakes and active tectonics of the Tibetan Plateau and its margins , 1989 .

[25]  William E. Holt,et al.  Velocity fields in deforming Asia from the inversion of earthquake-released strains , 1993 .

[26]  K. Terzaghi Theoretical Soil Mechanics , 1943 .

[27]  Richard G. Gordon,et al.  Current plate motions , 1990 .

[28]  J. Suppe,et al.  Mechanics of fold-and-thrust belts and accretionary wedges , 1983 .

[29]  R. Mccaffrey Oblique plate convergence, slip vectors, and forearc deformation , 1992 .

[30]  William W Rubey,et al.  ROLE OF FLUID PRESSURE IN MECHANICS OF OVERTHRUST FAULTING I. MECHANICS OF FLUID-FILLED POROUS SOLIDS AND ITS APPLICATION TO OVERTHRUST FAULTING , 1959 .

[31]  F. A. Dahlen,et al.  CRITICAL TAPER MODEL OF FOLD-AND-THRUST BELTS AND ACCRETIONARY WEDGES , 1990 .

[32]  Mark D. Zoback,et al.  The effect of topography on the state of stress in the crust: Application to the site of the Cajon Pass Scientific Drilling Project , 1992 .