Linking stress-dependent effective porosity and hydraulic conductivity fields to RMR

Abstract Relations are developed to define changes in effective porosity and hydraulic conductivity that result from the redistribution of stresses and strains in disturbed rock masses. In each instance, changes in porosity and directional conductivities are determined from pre-disturbance porosities and conductivities, knowledge of the number of joint sets, and the indices of Rock Quality Designation (RQD) and Rock Mass Rating (RMR), defining the rock mass structure. Measured magnitudes, or estimates, of the applied strain distribution are the final required parameter. These parameters allow porosity and conductivity changes to be straightforwardly evaluated for a broad spectrum of rock mass qualities, including the representation of granular media. The model is applied to an effective stress analysis of conductivity changes that develop around a unlined circular drift in a biaxial stress field. Large increases in tangential conductivity, and reductions in radial conductivity are shown to result. These results are corroborated against the drift macropermeability test at Stripa where increases in hydraulic conductivity of the order of 1000–10000 times were measured in a 0.5–1.0 m wide zone adjacent to the excavation.

[1]  O. Richmond,et al.  Interaction of compaction near mine openings and drainage of pore fluids from coal seams , 1984 .

[2]  Z. T. Bieniawski,et al.  The Geomechanics Classification In Rock Engineering Applications , 1979 .

[3]  F. Skoczylas,et al.  A study of the intrinsic permeability of granite to gas , 1995 .

[4]  J. S. Y. Wang,et al.  Validity of cubic law for fluid flow in a deformable rock fracture. Technical information report No. 23 , 1979 .

[5]  F. Descoeudres,et al.  Permeability predictions for jointed rock masses , 1995 .

[6]  J. Franklin,et al.  Prediction of water flow into rock tunnels: an analytical solution assuming an hydraulic conductivity gradient , 1993 .

[7]  John A. Hudson,et al.  Discontinuity spacings in rock , 1976 .

[8]  R. Pusch,et al.  Alteration of the hydraulic conductivity of rock by tunnel excavation , 1989 .

[9]  D. Elsworth,et al.  Transient poroelastic response of equivalent porous media over a mining panel , 1993 .

[10]  Derek Elsworth,et al.  Evaluation of groundwater flow into mined panels , 1993 .

[11]  Z. Şen Theoretical RQD-porosity-conductivity-aperture charts , 1996 .

[12]  Derek Elsworth,et al.  Modeling of subsidence and stress-dependent hydraulic conductivity for intact and fractured porous media , 1994 .

[13]  P. C. Kelsall,et al.  Evaluation of excavation-induced changes in rock permeability , 1984 .

[14]  D. Elsworth,et al.  Modeling the effects of longwall mining on the ground water system. Report of investigations/1995 , 1995 .

[15]  D. T. Snow,et al.  Anisotropie Permeability of Fractured Media , 1969 .

[16]  A. T. Jakubick,et al.  Vacuum testing of the permeability of the excavation damaged zone , 1993 .

[17]  S. S. Peng,et al.  Workshop on surface subsidence due to underground mining , 1982 .

[18]  Somasundaram Valliappan,et al.  Numerical modelling of methane gas migration in dry coal seams , 1996 .

[19]  Derek Elsworth,et al.  Three-dimensional effects of hydraulic conductivity enhancement and desaturation around mined panels , 1997 .

[20]  Z. Bieniawski,et al.  A nonlinear deformation modulus based on rock mass classification , 1990 .