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The impact of splay faults on fluid flow, solute transport, and pore pressure distribution in subduction zones: A case study offshore the N icoya P eninsula, C osta R ica
Author(s) -
Lauer Rachel M.,
Saffer Demian M.
Publication year - 2015
Publication title -
geochemistry, geophysics, geosystems
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.928
H-Index - 136
ISSN - 1525-2027
DOI - 10.1002/2014gc005638
Subject(s) - geology , forearc , trench , subduction , petrology , seafloor spreading , pore water pressure , geomorphology , outcrop , fault (geology) , tectonics , geophysics , seismology , geotechnical engineering , chemistry , organic chemistry , layer (electronics)
Observations of seafloor seeps on the continental slope of many subduction zones illustrate that splay faults represent a primary hydraulic connection to the plate boundary at depth, carry deeply sourced fluids to the seafloor, and are in some cases associated with mud volcanoes. However, the role of these structures in forearc hydrogeology remains poorly quantified. We use a 2‐D numerical model that simulates coupled fluid flow and solute transport driven by fluid sources from tectonically driven compaction and smectite transformation to investigate the effects of permeable splay faults on solute transport and pore pressure distribution. We focus on the Nicoya margin of Costa Rica as a case study, where previous modeling and field studies constrain flow rates, thermal structure, and margin geology. In our simulations, splay faults accommodate up to 33% of the total dewatering flux, primarily along faults that outcrop within 25 km of the trench. The distribution and fate of dehydration‐derived fluids is strongly dependent on thermal structure, which determines the locus of smectite transformation. In simulations of a cold end‐member margin, smectite transformation initiates 30 km from the trench, and 64% of the dehydration‐derived fluids are intercepted by splay faults and carried to the middle and upper slope, rather than exiting at the trench. For a warm end‐member, smectite transformation initiates 7 km from the trench, and the associated fluids are primarily transmitted to the trench via the décollement (50%), and faults intercept only 21% of these fluids. For a wide range of splay fault permeabilities, simulated fluid pressures are near lithostatic where the faults intersect overlying slope sediments, providing a viable mechanism for the formation of mud volcanoes.

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