rheological controls on strain partioning during continental extension (when does e=mc 2 ?)
DESCRIPTION
Chris Wijns , Klaus Gessner, Roberto Weinberg, Louis Moresi. Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2 ?). Dynamical modelers’ joke. There are only 10 types of people in this world those that understand binary and those that don’t - PowerPoint PPT PresentationTRANSCRIPT
Rheological Controls on Rheological Controls on Strain Partioning during Strain Partioning during Continental ExtensionContinental Extension(When does E=MC(When does E=MC22 ?) ?)
Chris Wijns, Klaus Gessner,
Roberto Weinberg, Louis Moresi
Dynamical modelers’ jokeDynamical modelers’ joke
There are only 10 types of people in this world • those that understand binary • and those that don’t
If you don’t think this is funny you’ll realize that modelers don’t necessarily think like other people.
A Meta-benchmark …A Meta-benchmark …
• How do you know to trust dynamic models ?• If you trust a black box model, then what ?• Why would you want a dynamic model and
not a kinematic one ?– When the kinematics is ambiguous– When you want to predict general behaviours
• Example - what happens when geologists get hold of a modeling code !
OutlineOutline
I. Generic crustal extension models physical and numerical model end-member modes: distributed faulting vs. mcc continuum of behaviour and secondary factors
II. Field Examples western Turkey conceptual models of mcc and rolling hinges related numerical modelling results
I. Generic Extension ModelsI. Generic Extension Models
Conclusion: the vertical rheological contrast between upper and lower crust is the key to fault spacing and the mode of extension(in the absence of heterogeneities)
Physical and numerical modelPhysical and numerical model
T=0 oC
T=1200 oC
T=400 oC
d/dt = 6.3x10-15 s-1 = 3.1 mm/yr = 100% extension in 5 Ma
Crustal strength profileCrustal strength profile
Byerlee coeff = 0.44
maximum shear stress = 250 Mpa
crustal thickness = 60 km
End-member: distributed faultingEnd-member: distributed faulting
• strong lower crust• many closely-spaced faults; limited slip;
contiguous upper crust
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End-member: metamorphic core End-member: metamorphic core complexescomplexes
● weak lower crust● few, widely-spaced faults; large strain; block
and fault rotation; exhumed lower crust
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Two basic modesTwo basic modes
Two basic modesTwo basic modes
Continuum of behaviourContinuum of behaviour
• r = ratio of integrated maximum shear stress of upper to lower crust
Continuum of behaviour: rContinuum of behaviour: r
Continuum of behaviour: rContinuum of behaviour: rhh
Continuum of behaviour: fault spacingContinuum of behaviour: fault spacing
• empirical relationship predicts mode of extension
Secondary factors: fault weakeningSecondary factors: fault weakening
• crustal necking instead of planar fault zones
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Secondary factorsSecondary factors
• fault weakening
• buoyancy
Validation testValidation test
Central Menderes mcc
Conclusions part IConclusions part I
• ratio of upper to lower crust “strength” controls fault spacing and mode of extension– strong lower crust = distributed faulting– weak lower crust = mcc– note: pre-existing weaknesses may change the
mode
• secondary controls: ratio of upper to lower crust thickness, fault weakening, lower crust buoyancy
II. Field Examples and II. Field Examples and Conceptual ModelsConceptual Models
Numerical models explain some field observations or suggest new observations
Western Turkey: Central MenderesWestern Turkey: Central Menderes
from Gessner et al. (2001) [Wernicke, 1981; Spencer, 1984; Buck, 1988]
Conceptual models: rolling hingeConceptual models: rolling hinge
vs.
Initial low angle detachmentInitial low angle detachment
from Davis, Lister, and Reynolds (1986)
from Koyi and Skelton (2001)
Analogue modellingAnalogue modelling
upper crust: 12.5 km lower crust: 25 km upper mantle: 9.375 km
ß =1.7 velocity: 1.25 cm / yr each side d/dt = 6.3x10-15
time: 3.52 Ma
More modelling reultsMore modelling reults
Single fault: “rolling hinge”Single fault: “rolling hinge”
• in mcc mode
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Temperature evolutionTemperature evolution
uniform T contours, i.e., single T “top” as in Snake Range
Low-angle “detachment fault”Low-angle “detachment fault”
• very low friction coefficient (yield strength) for lower crust near lithostatic pore pressure
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Reproducible field observationsReproducible field observations
Not modelledNot modelled
Conclusions part IIConclusions part II
• current-like lateral flow of lower crust relative to upper crust segments
• thermal structure of metamorphic domes• ductile shear zone operates continuously from
surface to mid-crustal levels• flow patterns of exhumed footwall match
kinematics of exhumed mylonitic fronts in mcc• mylonites may be a secondary feature, not an
exhumed part of a primary, lithospheric scale shear zone