Overpressure and fluid flow in the new jersey continental slope: implications for slope failure and cold seeps

Miocene through Pleistocene sediments on the New Jersey continental slope (Ocean Drilling Program Site 1073) are undercompacted (porosity between 40 and 65%) to 640 meters below the sea floor, and this is interpreted to record fluid pressures that reach 95% of the lithostatic stress. A two-dimensional model, where rapid Pleistocene sedimentation loads permeable sandy silt of Miocene age, successfully predicts the observed pressures. The model describes how lateral pressure equilibration in permeable beds produces fluid pressures that approach the lithostatic stress where overburden is thin. This transfer of pressure may cause slope failure and drive cold seeps on passive margins around the world.

[1]  L. Cathles,et al.  Capillary sealing in sedimentary basins: A clear field example , 1998 .

[2]  L. Pratson,et al.  A model for the headward erosion of submarine canyons induced by downslope-eroding sediment flows , 1996 .

[3]  C. Neuzil How permeable are clays and shales , 1994 .

[4]  M. Hubbert,et al.  ROLE OF FLUID PRESSURE IN MECHANICS OF OVERTHRUST FAULTING II. OVERTHRUST BELT IN GEOSYNCLINAL AREA OF WESTERN WYOMING IN LIGHT OF FLUID-PRESSURE HYPOTHESIS , 1959 .

[5]  H. Kooi Insufficiency of compaction disequilibrium as the sole cause of high pore fluid pressures in pre‐Cenozoic sediments , 1997 .

[6]  William W Rubey,et al.  ROLE OF FLUID PRESSURE IN MECHANICS OF OVERTHRUST FAULTING I. MECHANICS OF FLUID-FILLED POROUS SOLIDS AND ITS APPLICATION TO OVERTHRUST FAULTING , 1959 .

[7]  L. F. Athy Density, Porosity, and Compaction of Sedimentary Rocks , 1930 .

[8]  John A. Goff,et al.  Potential for large-scale submarine slope failure and tsunami generation along the U.S. mid-Atlantic coast , 2000 .

[9]  Craig M. Bethke,et al.  Erratum: Correction to ``Inverse hydrologic analysis of the distribution and origin of gulf coast-type geopressured zones'' , 1986 .

[10]  Li Yuan-hui,et al.  Diffusion of ions in sea water and in deep-sea sediments , 1974 .

[11]  C. Paull,et al.  Biological Communities at the Florida Escarpment Resemble Hydrothermal Vent Taxa , 1984, Science.

[12]  Peter B. Flemings,et al.  Generation of overpressure and compaction‐driven fluid flow in a Plio‐Pleistocene growth‐faulted basin, Eugene Island 330, offshore Louisiana , 1998 .

[13]  B. Hart,et al.  Porosity and pressure: Role of compaction disequilibrium in the development of geopressures in a Gulf Coast Pleistocene basin , 1995 .

[14]  J. F. Reilly,et al.  Gulf of Mexico hydrocarbon seep communities: VI. Patterns in community structure and habitat , 1990 .

[15]  Pierre Henry,et al.  Cold seep communities as indicators of fluid expulsion patterns through mud volcanoes seaward of the Barbados accretionary prism , 1997 .

[16]  R. E. Gibson The progress of consolidation in a clay layer increasing in thickness with time , 1958 .

[17]  J. Bredehoeft,et al.  On the Maintenance of Anomalous Fluid Pressures: I. Thick Sedimentary Sequences , 1968 .

[18]  N. R. Morgenstern,et al.  On the consolidation of sedimenting clays , 1982 .

[19]  P. Rona Middle Atlantic Continental Slope of United States: Deposition and Erosion , 1969 .

[20]  P. Rona,et al.  Stratigraphy and structure along a continuous seismic reflection profile from Cape Hatteras, North Carolina, to the Bermuda Rise , 1967 .

[21]  F. P. Shepard Submarine Canyons: Multiple Causes and Long-Time Persistence , 1981 .

[22]  W. Ryan,et al.  Wilmington Submarine Canyon: A marine fluvial-like system , 1982 .

[23]  J. M. Robb,et al.  Geomorphology and Sediment Stability of a Segment of the U.S. Continental Slope off New Jersey. , 1981, Science.