Presentation is loading. Please wait.

Presentation is loading. Please wait.

Physically-based Kinematic Model: from sandbox experiment Nina Lin Ge 277, Nov 7 2008 Readings: Bernard et al. (2007) Kinematics of fault-related folding.

Similar presentations


Presentation on theme: "Physically-based Kinematic Model: from sandbox experiment Nina Lin Ge 277, Nov 7 2008 Readings: Bernard et al. (2007) Kinematics of fault-related folding."— Presentation transcript:

1 Physically-based Kinematic Model: from sandbox experiment Nina Lin Ge 277, Nov 7 2008 Readings: Bernard et al. (2007) Kinematics of fault-related folding derived from a sandbox experiment, JGR Daëron et al. (2007) Modeling the shortening history of a fault tip fold using structural and geomorphic records of deformation, JGR

2 Q: How is the geologic deformation related to seismic cycles? Planar Fault Scenario

3 Q: How is the geologic deformation related to seismic cycles? Listric Fault Scenario

4 Q: How do we determine the right kinematics of a fold?

5 Traditional Kinematic Models: FBF dZ x

6 Traditional Kinematic Models: FTF → Need understanding of structural type → Complicated to derive velocity-deformation relationship

7 Physically-based Kinematic Model: Analogous Experiment

8 Phase I: Distributed Strain Detachment-tip Folding

9 Phase II: Strain Localization Ramp Overthrusting

10 Insights of experiment: 1. Maximum Uplift Much higher internal deformation during FTF Phase IPhase II

11 Insights of experiment: 2. Velocity Field of FTF (Phase I)

12 Insights of experiment: 3. Comparison with Elastic Model Fault-Tip Fold: → Fault depth is too shallow → Slip is overestimated Phase I

13 Insights of experiment: 3. Comparison with Elastic Model Fault-Bend Fold: → Fault depth is too shallow → Slip is overestimated Phase II

14 Example I: Yakeng Anticline, S Tien Shan

15

16

17 dZ x Example I: Yakeng Anticline, S Tien Shan Excess Area  Finite Shortening  Shortening Rate: 0.14 mm/yr for 2.1-5.8 Ma

18 Example I: Yakeng Anticline, S Tien Shan

19  No age control  Age determined by constant sedimentation rate  Shortening rate could be 2.1 mm/yr for 150 ka  Much faster than 0.14 mm/yr for 2.1-5.8 Ma

20 Implications  Physically-based kinematic model offers an approach to model geologic deformation in terms of seismic cycles  Combining with coseismic deformations, one can determine the inelastic deformation in the medium and possibly folding mechanism

21 Example II: Anjihai Anticline, N Tien Shan

22

23 Pretectonic

24 Example II: Anjihai Anticline, N Tien Shan

25

26 Mismatch of Tn:  Change of tectonic pattern  Different age of Ts and Tn


Download ppt "Physically-based Kinematic Model: from sandbox experiment Nina Lin Ge 277, Nov 7 2008 Readings: Bernard et al. (2007) Kinematics of fault-related folding."

Similar presentations


Ads by Google