Upscaling
Fault
Flow Properties for Evaluation of Cross-
Fault
Flow
Abstract
An ongoing concern in flow modeling across faults is upscaling the fault
-rock flow properties measured in the lab on cm-scale to the meter and tens of meter scale suitable for evaluating within-reservoir flow and exploration-scale sealing. It is proposed that upscaling is best accomplished by stochastic modeling of cross-
fault
flow guided by the geometries of
fault
-generated rock bodies (“geobodies”) as observed on outcrop. Preliminary models demonstrate that most resistance to flow transverse to the
fault
is in the low permeability
fault
rocks the
fault
core as opposed to the damage zone of deformation in the
fault
zone. Published and proprietary outcrop studies have demonstrated that the
fault
core is heterogeneous normal to the
fault
. Spatial correlation of lithology transverse to the
fault
core is on the order of mm to a cm, much too small to improve estimates of upscaled flow properties. Length of constituent bodies in the
fault
core can be traced along the
fault
on the scale of cm to meters in different settings. The
fault
core is best described as a composite of plate-shaped or equant geobodies with different permeabilities and seal capacities. Upscaling by numerical simulations of flow in composite rocks with these geometries can be compared to mathematical upscaling averages. Equant geobodies result in upscaled permeabilities very close to the geometric mean of the constituent geobody permeabilities and their volumes. Sealing depends on the relative size of the geobody relative to the width of the
fault
core. Plate-shaped geobody constituents lead to upscaled permeability between the harmonic and geometric means of the constituent geobody permeabilities, with upscale permeability approaching the geometric mean as the shape of the constituent geobody approaches equant. The thinner the geobody relative to the
fault
core width, the greater the seal capacity of the composite medium. Realistic upscaling of lab-measured permeability to real faults therefore depends on both the fractions of geobodies with different interpreted permeability and the likely geometry of the geobodies. Settings with smear and shearing of ductile rocks lead towards platy
fault
core geometries, whereas settings where lenses or protolith is mixed into the
fault
core lead towards a more equant geobody shape.
AAPG Datapages/Search and Discovery Article #90189 © 2014 AAPG Annual Convention and Exhibition, Houston, Texas, USA, April 6–9, 2014