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Announcements Field trip this Saturday to Cottonwood Canyon area 7:30 AM at loading dock. We will map some really cool stuff! Please review map symbols. We may return after sunset.
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Outline for Today 1. More about geometry and kinematics of thrust systems 2. Forced folds 3. Mechanical "paradox" of moving large thrust sheets 4. Thrust belt evolution: Critical Taper theory 5. Foreland basins 6. Two examples 7. Economic applications
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the architecture of many fold-thrust belts "thin-skinned" deformation
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development of duplexes
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Summary Thrust systems: 1. Accommodate significant crustal shortening 2. Basal detachment/decollement; decoupling within the crust 3. Faults have ramp and flat geometries 4. Thrusts place older/higher grade rocks over younger/lower grade rocks 5. Faults cut up-section 6. Faults generally propagate (get younger) toward the foreland 7. Younger and structurally deeper faults rotate older faults to steeper angles
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Mt Kidd Fold and thrust belts! Forced folds (D&R 413-423)
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Free folds: fold profiles are based entirely on physical- mechanical properties of the layers Forced folds: geometry related to movement over fault ramps- "they just go along for the ride, and some of the beds happen to fined themselves in awkward places and are required to stretch or bend" 2-main types of forced folds: fault-bend folds fault-propagation folds
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Fault-bend folds
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Fault-propagation folds
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monoclines as "drape" folds
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"thick-skinned" basement-involved shortening
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Colorado Plateau monoclines may be related to thick-skinned deformation
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Major issues “mechanical paradox” of thrusting - why such thin sheets (e.g. 100 km long/2-3 km thick) can remain intact during faulting? What happened to the missing basement?
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“mechanical paradox” of thrusting - why such thin sheets (e.g. 100 km long/2-3 km thick) can remain intact during faulting?
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Recall Byerlee's Law Question: How much shear stress is needed to cause movement along a preexisting fracture surface, subjected to a certain normal stress? c = tan ( N ), where tan is the coefficient of sliding friction
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c = tan ( N ), where tan is the coefficient of sliding friction
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Possible explanation- water pressure plays a big role c = tan (* N ), where tan is the coefficient of sliding friction and * N = N – fluid pressure
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What drives a thrust belt?? Old timers thought that decollements beneath thrust belts dipped away from the elevated hinterland- and therefore gravity "sliding" was the main mechanism
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But now we know that decollements to thrust belts dip toward the hinterland. Thrust belts move uphill!
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Elevated fluid pressure certainly decreases the stress required to move a thrust belt. Gravitational stresses due to elevated topography also aids sliding. BUT, a push from the rear is still necessary
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Critical Taper Thrusts belts are wedge shaped- characterized by a topographic slope ( ) and a decollement dip ( ) Only at some critical angle ( + ), will the thrust belt propagate
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The critical taper angle is controlled by the coefficient of friction along the decollement and the frictional sliding strength of the rock EPISODIC propagation
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Thrust belts create topographic loads that flex the lithosphere like a person on a diving board- foreland basins!
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Important terminology/concepts role of elevated pore fluid pressure in movement of thrust sheets Critical taper theory / wedge theory foreland basin development
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Example 1: Tibet Geographic Setting
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Regional Geologic Setting
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Geometry
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Footwall rocks include high-pressure blueschists that formed at depths of >35 km!
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Tectonic significance
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Example 2: Canadian Cordillera
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Roche Ronde
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Boulle Range
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Roche Ronde Boulle Range
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Cross-sections Thrust faults cut up-section only! (or section-parallel) Every flat or ramp in the FW should correspond to an equivalent flat or ramp in the WH Bed thickness is preserved (conservation of volume and mass) Other than that - it’s all interpretation!
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Roche Ronde Boulle Range
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Relevance to oil exploration
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On Thursday: Normal faults
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