2018
DOI: 10.1016/j.tecto.2017.10.019
|View full text |Cite
|
Sign up to set email alerts
|

Impact of an interbedded viscous décollement on the structural and kinematic coupling in fold-and-thrust belts: Insights from analogue modeling

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

2
22
0

Year Published

2018
2018
2023
2023

Publication Types

Select...
6
2
1

Relationship

1
8

Authors

Journals

citations
Cited by 50 publications
(24 citation statements)
references
References 88 publications
2
22
0
Order By: Relevance
“…The variability of the different parameters, in particular the viscosity range of the natural case, introduces a significant uncertainty in the calculation of the shortening velocity of the models, which varies from 0.6 × 10 −6 to 1.7 × 10 −3 m s −1 , that is, 0.2 to 612 cm h −1 . However, as we had to ensure that the silicone employed in our analog models behaves as a Newtonian material, we restricted the shortening velocity to 0.7-0.9 cm h −1 (Luján et al, 2006b;Borderie et al, 2018). With these values of shortening velocity, we calculated the strain rate of our analog models as ε = v M /w, where w is the width of the deformable zone measured in the apex parallel to the shortening direction (between 51 and 65 cm).…”
Section: Scalingmentioning
confidence: 99%
See 1 more Smart Citation
“…The variability of the different parameters, in particular the viscosity range of the natural case, introduces a significant uncertainty in the calculation of the shortening velocity of the models, which varies from 0.6 × 10 −6 to 1.7 × 10 −3 m s −1 , that is, 0.2 to 612 cm h −1 . However, as we had to ensure that the silicone employed in our analog models behaves as a Newtonian material, we restricted the shortening velocity to 0.7-0.9 cm h −1 (Luján et al, 2006b;Borderie et al, 2018). With these values of shortening velocity, we calculated the strain rate of our analog models as ε = v M /w, where w is the width of the deformable zone measured in the apex parallel to the shortening direction (between 51 and 65 cm).…”
Section: Scalingmentioning
confidence: 99%
“…Finally, it must be stressed that in our models, the buoyancy of the ductile layer is higher than in the natural cases (Table 1), which should have some influence on the experiment dynamics. Nevertheless, this behavior is assumed in most of the analog modeling set for the simulation of deformation in upper crustal levels (see models of Ferrer et al, 2016;Li and Mitra, 2017;Borderie et al, 2018;Roma et al, 2018 who used the same analog materials as in this paper). Moreover, at the beginning of our experiments, the lateral flow of the silicone was limited, as it was confined by sand.…”
Section: Initial Sand-silicone Packmentioning
confidence: 99%
“…In general, disharmonic structures develop, with the degree of decoupling of the two levels depending on several factors. The most common are the strain rate, the viscosity and thickness of each décollement, and the thickness of the overburden above each décollement (Borderie et al, 2018;Couzens-Schultz et al, 2003;Gestain et al, 2004;Hudec & Jackson, 2011;Sherkati et al, 2006), being the last factor different in each model of our experimental program.…”
Section: Suprasalt/subsalt Structural Relationshipsmentioning
confidence: 99%
“…This, in turns allows for the vertical stacking of basement thrusts behind the hinterland salt pinch out. In another article (Borderie et al, 2018), we illustrate what would be the further evolution of such a system, a system where deformation in the hinterland progresses much longer, then all new basal thrusts are shorter and stack vertically one above the other, leading to a geometry similar to that of an asymmetric anticlinal stack. Simple mechanical considerations can help explain this change in behavior.…”
Section: Discussion / Conclusionmentioning
confidence: 99%