Al. Merlani et al., ON THE THEORY OF PRESSURE AND TEMPERATURE NONLINEAR-WAVES IN COMPRESSIBLE FLUID-SATURATED POROUS ROCKS, Geophysical and astrophysical fluid dynamics, 85(1-2), 1997, pp. 97-128
Thermo-pore-elastic equations describing fluid migration through fluid
-saturated porous media at depth in the crust are analyzed theoretical
ly following recent formulations of Rice and Cleary (1976), McTigue (1
986) and Bonafede (1991). In this study these ideas are applied to a r
ather general model, namely to a deep hot and pressurized reservoir of
fluid, which suddenly enters into contact with an overlaying large co
lder fluid-saturated layer. In a one-dimensional idealization this sys
tem can be described by two nonlinear differential heat-like equations
on the matrix-fluid temperature and on the fluid overpressure over th
e hydrostatic value. The nonlinear couplings are due to Darcy thermal
advection and to the mechanical work rate. Here we first sketch nonlin
ear solutions corresponding to Burgers' ''solitary shock waves'', whic
h have recently been found valid for rocks with very low fluid diffusi
vity. Subsequently other nonlinear transient waves are discussed, such
as ''thermal'' and ''compensated'' waves, which are found to exist fo
r every value of the parameters present in the equations involved. One
interesting aspect of these mechanisms is that the resulting time-sca
les are particularly small. Moreover, in order to figure out the syste
m time-evolution and the role played by the fluid diffusivity/thermal
diffusivity ratio, a mechanical similitude is proposed, which we treat
both analytically and numerically. Although for realistic systems the
se solutions are somewhat idealized, they allow one to gain fundamenta
l insight into fluid migration mechanisms in volcanic areas and in fau
lt regions under strong frictional heating. As already discussed by Mc
Tigue, the theory is also of interest in studying areas of nuclear was
te disposal. Furthermore such a theoretical study allows one to invest
igate the site at depth at which such nonlinear waves are generated.