Dynamic poroelasticity: A unified model with the squirt and the Biot mechanisms
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Amos Nur | Jack Dvorkin | A. Nur | J. Dvorkin
[1] James G. Berryman,et al. Confirmation of Biot’s theory , 1980 .
[2] R. Kleinberg,et al. Acoustic relaxation in sedimentary rocks; dependence on grain contacts and fluid saturation , 1986 .
[3] Theodoros Klimentos,et al. Relationships among compressional wave attenuation, porosity, clay content, and permeability in sandstones , 1990 .
[4] G. Gardner. Extensional Waves in Fluid‐Saturated Porous Cylinders , 1962 .
[5] A. Nur,et al. Relating P-wave attenuation to permeability , 1993 .
[6] M. Miksis. Effects of contact line movement on the dissipation of waves in partially saturated rocks , 1988 .
[7] J. Keller,et al. Poroelasticity equations derived from microstructure , 1981 .
[8] Robert D. Stoll,et al. Acoustic Waves in Saturated Sediments , 1974 .
[9] M. Biot. General Theory of Three‐Dimensional Consolidation , 1941 .
[10] I. Palmer,et al. Attenuation by squirt flow in undersaturated gas sands , 1980 .
[11] N. Christensen,et al. Compressional wave attenuation in oceanic basalts , 1990 .
[12] J. Rice,et al. Some basic stress diffusion solutions for fluid‐saturated elastic porous media with compressible constituents , 1976 .
[13] A. Nur,et al. Compressional and shear waves in saturated rock during water-steam transition , 1979 .
[14] A. Nur,et al. Dispersion analysis of acoustic velocities in rocks , 1990 .