Viscous deformation of unconsolidated reservoir sands—Part 1: Time‐dependent deformation, frequency dispersion, and attenuation

Laboratory experiments on dry, unconsolidated reservoir sands from the Wilmington field, California, reveal significant viscous creep strain under a variety of loading conditions. In hydrostatic compression tests, following initial loading to 10 MPa, the creep strain that accompanies 5‐MPa loading steps to 15, 20, 25, and 30 MPa exceeds the magnitude of the instantaneous strain (∼3 × 10−3). We observed a two‐fold increase in bulk modulus with frequency over the range of frequencies tested (10−6 to 10−2 Hz), which is consistent with a viscoelastic rheology of unconsolidated sand. The data demonstrate that the effective static bulk modulus is approximately one‐third of that at seismic frequencies. By measuring the phase lag between stress and strain during the loading cycles, we were also able to show that inelastic attenuation is nearly constant (Q ≈ 5) over the four‐decade range of frequencies tested at a strain amplitude of 10−3. Interestingly, the viscous effects only appear when loading a sample beyond...

[1]  W. Worrall Clays: their nature, origin and general properties, , 1968 .

[2]  Amos Nur,et al.  Dynamic poroelasticity: A unified model with the squirt and the Biot mechanisms , 1993 .

[3]  M. Zoback,et al.  Anelasticity and dispersion in dry unconsolidated sands , 1997 .

[4]  Mukul M. Sharma,et al.  THE INFLUENCE OF FLUIDS ON GRAIN CONTACT STIFFNESS AND FRAME MODULI IN SEDIMENTARY ROCKS , 1992 .

[5]  D. Wood Soil Behaviour and Critical State Soil Mechanics , 1991 .

[6]  Mukul M. Sharma,et al.  Nonlinear viscoelastic behavior of sedimentary rocks, Part I: Effect of frequency and strain amplitude , 1998 .

[7]  R. Lakes,et al.  Apparatus for measuring viscoelastic properties over ten decades: Refinements , 1995 .

[8]  G. W. Nabor,et al.  Application of Variable Formation Compressibility for Improved Reservoir Analysis , 1993 .

[9]  M. Zoback,et al.  Stress, pore pressure, and dynamically constrained hydrocarbon columns in the South Eugene Island 330 field, northern Gulf of Mexico , 2001 .

[10]  M. Biot MECHANICS OF DEFORMATION AND ACOUSTIC PROPAGATION IN POROUS MEDIA , 1962 .

[11]  J. Pinkston,et al.  Basal slip and mechanical anisotropy of biotite , 1990 .

[12]  R. M. Ostermeier Deepwater Gulf of Mexico Turbidites - Compaction Effects on Porosity and Permeability , 1995 .

[13]  Nick Barton,et al.  Numerical simulation of fiber reinforced shotcrete in a tunnel using the discrete element method , 1997 .

[14]  J. Dieterich Time-dependent friction and the mechanics of stick-slip , 1978 .

[15]  James K. Mitchell,et al.  SOIL CREEP AS A RATE PROCESS , 1968 .

[16]  G. Mavko,et al.  Estimating grain-scale fluid effects on velocity dispersion in rocks , 1991 .

[17]  Serge Leroueil,et al.  Stress–strain–strain rate relation for the compressibility of sensitive natural clays , 1985 .

[18]  R. F. Scott,et al.  Finite element simulation of Wilmington oil field subsidence: I. Linear modelling , 1980 .

[19]  T. Mukerji,et al.  The Rock Physics Handbook , 1998 .