Open AccessA differential scheme for elastic properties of rocks with dry or saturated cracks
Author(s) -
Berryman James G.,
Pride Steven R.,
Wang Herbert F.
Publication year - 2002
Publication title -
geophysical journal international
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.302
H-Index - 168
eISSN - 1365-246X
pISSN - 0956-540X
DOI - 10.1046/j.1365-246x.2002.01801.x
Subject(s) - poisson distribution , poisson's ratio , porosity , spheres , porous medium , mathematics , shear modulus , mathematical analysis , aspect ratio (aeronautics) , elastic modulus , materials science , differential equation , modulus , mechanics , thermodynamics , geometry , physics , composite material , statistics , astronomy
Summary Differential effective medium (DEM) theory is applied to the problem of estimating the physical properties of elastic media with penny‐shaped cracks, filled either with gas or liquid. These cracks are assumed to be randomly oriented. It is known that such a model captures many of the essential physical features of fluid‐saturated or partially saturated rocks. By making an assumption that the changes in certain factors depending only on Poisson's ratio do not strongly affect the results, it is possible to decouple the equations for bulk ( K ) and shear ( G ) modulus, and then integrate them analytically. The validity of this assumption is then tested by integrating the full DEM equations numerically. The analytical and numerical curves for both K and G are in very good agreement over the whole porosity range. Justification of the Poisson ratio approximation is also provided directly by the theory, which shows that as porosity tends to unity, Poisson's ratio tends towards small positive values for dry, cracked porous media and tends to one‐half for liquid‐saturated samples. A rigorous stable fixed‐point is obtained for Poisson's ratio, ν c , of dry porous media, where the location of this fixed‐point depends only on the shape of the voids being added. Fixed‐points occur at for spheres and ν c ≃πα/18 for cracks, where α is the aspect ratio of penny‐shaped cracks. These theoretical results for the elastic constants are then compared and contrasted with results predicted by Gassmann's equations and with results of Mavko and Jizba, for both granite‐like and sandstone‐like examples. Gassmann's equations do not predict the observed liquid dependence of the shear modulus G at all. Mavko and Jizba predict the observed dependence of the shear modulus on the liquid bulk modulus for a small crack porosity and a very small aspect ratio, but fail to predict the observed behaviour at higher porosities. In contrast, the analytical approximations derived here give very satisfactory agreement in all cases for both K and G . For practical applications of this work, it appears that the ratio of compliance differences is approximately independent of the crack porosity for a given rock, but the constant is usually greater than for granites, while general statements concerning sandstones are more difficult to make.