About This Item
- Full text of this item is not available.
- Abstract PDFAbstract PDF(no subscription required)
Share This Item
The AAPG/Datapages Combined Publications Database
Houston Geological Society Bulletin
Abstract
Abstract: The Great Pliocene Salt Squirt–Mechanics of Folding along the Down-dip Limit of Salt, Gulf of Mexico
ENI Petroleum
From Perdido Canyon to Atwater Valley, the frontal fold-thrust
belt along the down-dip limit of salt in
the deepwater Gulf of Mexico has become a
very active structural play. Salt has played an
active role in forming these structures and
influencing the deposition of reservoirs
of Paleogene, Miocene and Pliocene age. A
key to better predictive geologic
models
for
successful hydrocarbon exploitation lies
in understanding the mechanisms of salt
involvement.
Seismic interpretation across the frontal fold belt was used to sequentially reconstruct 14 horizons from the present through end of the Cretaceous. The top, base and pinchout of both shallow and deep allochthonous salt were well imaged. Paleobathymetry was reconstructed to seafloor gradients representative of present conditions. Cover shortening and deep-salt area, recorded for each time step, show salt flow into the frontal anticline exceeded shortening during Miocene folding. During Pliocene folding, expulsion of deep salt exceeded shortening. Similar effects are observed in other analogues.
The geometry of buckle folding above a mobile substrate requires
that material initially moved into the fold core is expelled during
continued shortening. This can be explained by two mechanically
distinct drivers: 1)
horizontal
buckling of cover sediments forces
salt into the fold core or 2) excess halostatic fluid pressure forces
vertical flexures of the cover. Geodynamic
models
for a stiff
isostatically-supported layer predict a large difference in flexural
wavelength for vertical or
horizontal
loading.
The observed short-wavelength folds (~10 km) can be modeled
as
horizontal
buckles that nucleated in early Paleogene time and
were controlled by the elastic thickness of Cretaceous strata. The
observed long-wavelength Miocene fold
(~50 km) cannot be similarly modeled.
However, a simple model of continuous plate
flexure resulting from excess halostatic
pressure effectively predicts the observed
wavelength. The halostatic pressure model
further predicts that deep salt will rise to an
isostatically compensated elevation well
above the regional datum when released
t h r o u g h e m e r g e n t s a l t d i a p i r s .
Reconstruction shows more than a kilometer
increase in bathymetric relief associated with
the emplacement of shallow salt. Extensive,
nearly concordant contacts observed below
shallow salt imply that an almost catastrophic release of excess
halostatic pressure occurred in the Pliocene.
End_of_Record - Last_Page 21---------------