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Quantifying the energy dissipation of overriding plate deformation in three‐dimensional subduction models
Author(s) -
Chen Zhihao,
Schellart Wouter P.,
Duarte João C.
Publication year - 2015
Publication title -
journal of geophysical research: solid earth
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.983
H-Index - 232
eISSN - 2169-9356
pISSN - 2169-9313
DOI - 10.1002/2014jb011419
Subject(s) - subduction , slab , slab window , buoyancy , geology , dissipation , deformation (meteorology) , potential energy , seismology , mechanics , geophysics , physics , oceanic crust , thermodynamics , classical mechanics , tectonics , oceanography
In a subduction system the force and the energy required to deform the overriding plate are generally thought to come from the negative buoyancy of the subducted slab and its potential energy, respectively. Such deformation might involve extension and back‐arc basin formation or shortening and mountain building. How much of the slab's potential energy is consumed during overriding plate deformation remains unknown. In this work, we present dynamic three‐dimensional laboratory experiments of progressive subduction with an overriding plate to quantify the force ( F OPD ) that drives overriding plate deformation and the associated energy dissipation rate (Φ OPD ), and we compare them with the negative buoyancy ( F BU ) of the subducted slab and its total potential energy release rate (Φ BU ), respectively. We varied the viscosity ratio between the plates and the sublithospheric upper mantle with η SP / η UM = 157–560 and the thickness of the overriding plate with T OP = 0.5–2.5 cm (scaling to 25–125 km in nature). The results show that F OPD / F BU has average values of 0.5–2.0%, with a maximum of 5.3%, and Φ OPD /Φ BU has average values of 0.05–0.30%, with a maximum of 0.41%. The results indicate that only a small portion of the negative buoyancy of the slab and its potential energy are used to deform the overriding plate. Our models also suggest that the force required to deform the overriding plate is of comparable magnitude as the ridge push force. Furthermore, we show that in subduction models with an overriding plate bending dissipation at the subduction zone hinge remains low (3–15% during steady state subduction).