T64 Folding: Processes, Observations, and Consequences
Sunday, 22 September 2019
1:30 PM - 5:30 PM
Room 231ABC, North Building
AUTOGENIC ORGANIZATION OF SYN-TECTONIC SEDIMENTARY PATTERNS AROUND DEEP-WATER DETACHMENT FOLDS: A SIMPLE DYNAMIC MODEL
Paper number: T64-7
Program: Technical Sessions
Time: 3:10 PM – 3:25 PM
Authors
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Andrea LoteroCentro de Investigación Científica y de Educación Superior de Ensenada (CICESE), Ensenada, BJ
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Juan Contreras Presenting AuthorCentro de Investigación Científica y de Educación Superior de Ensenada (CICESE), Ensenada, BJ
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Ismael YarbuhUniversidad Autónoma de Baja California, Facultad de Ciencias Marinas, Ensenada, BJ
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Raquel Negrete-ArandaCentro de Investigación Científica y de Educación Superior de Ensenada (CICESE), Ensenada
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Ronald SpelzUniversidad Autónoma de Baja California, Facultad de Ciencias Marinas, Campus Ensenada, Ensenada, BJ
Abstract
We represent the stratigraphic response predicted by our model in a two-dimensional parametric space whose axes are given by the Peclet number (Pe), the ratio of the mass transported by tectonic uplift and the mass transferred by diffusive hillslope processes, and the sediment delivery number (Sd), the ratio of sediments transported by density currents to those produced by intrabasinal processes. We identify three well-defined regions of sedimentary behavior in that parametric space. A central domain (Pe>2, Sd>2) of cyclic stratigraphy produced by self-sustained oscillations in the sedimentary system, and two regions near the graph axes of stable sedimentation in which a continuous stratigraphy is produced. In the central domain, all the system mass fluxes are equally important. This creates the conditions for a series of complex interaction between hillslope sediment transport, fold growth, and sedimentation. The other two regions correspond to end-members in which either the or are small. For small values, topographic degradation and sediment dispersal by hillslope transport dominates over tectonic uplift. Thus, any tectonic perturbation appearing in the system dissipates readily. For small values, sediment transport is dominated by creep, and the system rapidly evolves toward a steady state.
Geological Society of America Abstracts with Programs. Vol. 51, No. 5
doi: 10.1130/abs/2019AM-337937
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