rheological controls on strain partioning during continental extension (when does e=mc 2 ?)

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Rheological Controls Rheological Controls on Strain Partioning on Strain Partioning during Continental during Continental Extension Extension (When does E=MC (When does E=MC 2 2 ?) ?) Chris Wijns , Klaus Gessner, Roberto Weinberg, Louis Moresi

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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 Presentation

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Page 1: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

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

Page 2: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

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.

Page 3: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

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 !

Page 4: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

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

Page 5: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

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)

Page 6: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

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

Page 7: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Crustal strength profileCrustal strength profile

Byerlee coeff = 0.44

maximum shear stress = 250 Mpa

crustal thickness = 60 km

Page 8: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

End-member: distributed faultingEnd-member: distributed faulting

• strong lower crust• many closely-spaced faults; limited slip;

contiguous upper crust

QuickTime™ and aYUV420 codec decompressorare needed to see this picture.

Page 9: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

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

QuickTime™ and aYUV420 codec decompressorare needed to see this picture.

Page 10: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Two basic modesTwo basic modes

Page 11: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Two basic modesTwo basic modes

Page 12: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Continuum of behaviourContinuum of behaviour

• r = ratio of integrated maximum shear stress of upper to lower crust

Page 13: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Continuum of behaviour: rContinuum of behaviour: r

Page 14: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Continuum of behaviour: rContinuum of behaviour: rhh

Page 15: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Continuum of behaviour: fault spacingContinuum of behaviour: fault spacing

• empirical relationship predicts mode of extension

Page 16: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Secondary factors: fault weakeningSecondary factors: fault weakening

• crustal necking instead of planar fault zones

QuickTime™ and aYUV420 codec decompressorare needed to see this picture.

Page 17: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Secondary factorsSecondary factors

• fault weakening

• buoyancy

Page 18: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Validation testValidation test

Central Menderes mcc

Page 19: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

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

Page 20: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

II. Field Examples and II. Field Examples and Conceptual ModelsConceptual Models

Numerical models explain some field observations or suggest new observations

Page 21: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Western Turkey: Central MenderesWestern Turkey: Central Menderes

Page 22: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

from Gessner et al. (2001) [Wernicke, 1981; Spencer, 1984; Buck, 1988]

Conceptual models: rolling hingeConceptual models: rolling hinge

vs.

Page 23: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Initial low angle detachmentInitial low angle detachment

from Davis, Lister, and Reynolds (1986)

Page 24: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

from Koyi and Skelton (2001)

Analogue modellingAnalogue modelling

Page 25: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

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

Page 26: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Single fault: “rolling hinge”Single fault: “rolling hinge”

• in mcc mode

QuickTime™ and aYUV420 codec decompressorare needed to see this picture.

Page 27: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Temperature evolutionTemperature evolution

uniform T contours, i.e., single T “top” as in Snake Range

Page 28: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Low-angle “detachment fault”Low-angle “detachment fault”

• very low friction coefficient (yield strength) for lower crust near lithostatic pore pressure

QuickTime™ and aYUV420 codec decompressorare needed to see this picture.

Page 29: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Reproducible field observationsReproducible field observations

Page 30: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

Not modelledNot modelled

Page 31: Rheological Controls on Strain Partioning during Continental Extension (When does E=MC 2  ?)

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