Detailed internal architecture of a fluvial channel sandstone determined from outcrop, cores, and 3-D ground-penetrating radar: Example from the middle Cretaceous Ferron Sandstone, east-central Utah
Rm. Corbeanu et al., Detailed internal architecture of a fluvial channel sandstone determined from outcrop, cores, and 3-D ground-penetrating radar: Example from the middle Cretaceous Ferron Sandstone, east-central Utah, AAPG BULL, 85(9), 2001, pp. 1583-1608
Ideally, characterization of hydrocarbon reservoirs requires information ab
out heterogeneity at a submeter scale in three dimensions. Detailed geologi
c information and permeability data from surface and cliff face outcrops an
d boreholes in the alluvial part of the Ferron Sandstone are integrated her
e with three-dimensional (3-D) ground-penetrating radar (GPR) data for anal
ysis of a near-surface sandstone reservoir analog in fluvial channel deposi
ts. The GPR survey covers a volume with a surface area of 40 x 16.5 m and a
depth of 12 m. Five architectural elements are identified and described in
outcrop and well cores, using a sixfold hierarchy of bounding surfaces. In
ternally, the lower four units consist of fine-grained, parallel-laminated
sandstone, and the upper unit consists of medium-grained, trough cross-bedd
ed sandstone. The same sedimentary architectural elements and associated bo
unding surfaces are distinguished in the GPR data by making use of principl
es developed in seismic stratigraphic analysis.
To facilitate comparison of geologic features in the depth domain and radar
reflectors in the time domain, the radar data are depth migrated. The GPR
interpretation is carried out mainly on migrated 100 MHz data with a vertic
al resolution of about 0.5 m. Measures of the spatial continuity and variat
ion of the first- and second-order bounding surfaces are obtained by comput
ing 3-D experimental variograms for each architectural element (each radar
facies). The maximum correlation length of the dominant internal features r
anges between 4 and 6 m, and the anisotropy factor ranges between 0.6 and 0
.95.