Permeability (k) was measured on synthetic, monomineralic aggregates of qua
rtz and calcite, which serve as analogs for texturally equilibrated, fluid-
and melt-bearings rocks such as those in the deep crust and mantle. Porous
quartzites were synthesized in the presence of silica-saturated H2O and H2
O + NaCl, at 850 degrees C and 1.4 GPa. Permeabilities, measured at near-at
mospheric conditions on the quenched samples and scaled to a common grain-d
iameter (d), increase systematically by about four orders of magnitude as f
luid fraction (phi) increases from 0.006 to 0.170. In this range, the k-phi
relation can be approximated by the equation k = d(2)phi(3)/200. We were n
ot able to determine permeabilities at fluid fractions lower than 0.006 (du
e to microfractures that formed during depressurization), but we expect the
same relation - possibly with a slightly lower exponent on phi - to apply.
Permeabilities measured on porous marbles, synthesized at 800 degrees C an
d 1.0 GPa in the presence of H2O, are lower than values measured on quartzi
tes for a given fluid fraction. At phi > 0.027, an equation similar to that
which applies to quartzites can be used to describe the k-phi relation, bu
t using (phi - 0.015) in place of phi. The lower permeability of the calcit
e aggregates reflects the fact that not all grain edges are 'wetted', and t
hus some fraction of fluid is present in isolated pores. The 'critical' flu
id fraction below which all pores are isolated and k is zero lies somewhere
between 0.005 and 0.027. Our measured permeabilities closely approximate v
alues predicted by numerical modeling of fluid how in texturally equilibrat
ed rocks. This correspondence is somewhat surprising, considering that flui
d distribution in our samples, and in real rocks, is much more complex than
assumed in the numerical models. Assumptions implicit in numerical models
- simple grain shape, a single grain size, non-rational crystal faces, and
isotropic surface energies - do not apply to natural or synthetic texturall
y equilibrated rocks. Despite differences in fluid distribution, the simila
rity of k-phi relations indicates that average length and cross-sectional a
rea of grain-edge channels is the same in a texturally equilibrated rock as
it is in a hypothetical rock with uniform pore geometry. (C) 1998 Elsevier
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