3-d finite element modeling of the rise and fall of the himalayan-tibetan plateau mian liu and...

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inite Element Modeling of the Rise and of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of Missouri-Colu

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Page 1: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau

Mian Liu and Youqing Yang

Dept. of Geological Sciences, University of Missouri-Columbia

Page 2: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

Some of the fundamental questions of the Tibetan tectonics

• What causes the E-W extension in Tibet? When did the “collapse” start?

• When did the Tibetan plateau uplift? What are the temporal and spatial evolution of the mountain building in Tibet?

• How was the >2000 km crustal shortening accommodated? What controlled the strain partitioning between crustal thickening and lateral extrusion?

Page 3: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

GPS velocity relative to stable Siberia

Data from Larson et al., 1999; Chen et al., 2000; Wang et al., 2001

Earthquake focal mechanismshowing E-W extension

Data from Harvard Catalog

Page 4: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

Active crustal deformation in Tibet:3-D finite element model & rheology

Page 5: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

Crustal StressIndicated byEarthquake Data

Predicted Stress State in the upper crust

Page 6: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

Elevation reduced to 50% of present values

No E-W extension predicted

Basal shear = 30 MPa under Himalayas and south Tibet

A narrow zone of nearly N-SExtension – South Tibetan Detachment Fault system?

Page 7: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

Long-term history of the Himalayan-Tibetan orogen

Viscous thin-sheet model

(England & Houseman, 1986)

Plasticine analog model

(Tapponnier et al., 1986)

Page 8: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

3-D finite strain model

x10 vertical exaggeration

Indian plate

Tarim

Sich

uan

BasinAsia

Page 9: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of
Page 10: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

40 Ma

20 Ma Present

10 Ma

Page 11: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

Near surface velocity

Because of the depth-variable lithospheric rheology, the surface velocity can be significantly different from that in the lower crust.

Page 12: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

The predicted plateau formation is sensitive to the lower crustal rheology

Lower crustal viscosity 2.5 times higher than the base model

Lower crustal viscosity 0.5 times the base model value

Page 13: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

Predicted uplift history of the different parts of the Tibetan Plateau

Accelerated uplift but different history at various parts of Tibet; Most parts reached >3 km ~10-20 Myr ago.

Page 14: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

Predicted Crustal Mass Distribution

Page 15: 3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of

Conclusions• The E-W extension in Tibet can be explained by gravitational

collapse of the plateau. Major E-W extension started only when the plateau reached ~75% of its present values.

• Assuming a flat Asian continent before the Indo-Asian collision, the plateau would have grown from S to N, and from W to E; most part of the plateau probably reached >3 km 10-20 million years ago.

• The lower crust flow largely controls the topographic evolution; the motion of the upper crust may be significantly different from that in the lower crust.

• Partitioning of the shortened crustal mass between thickening and lateral extrusion/erosion changed with time. Mass accommodated by mountain building may have peaked ~10 Myr ago; extrusion and erosion become increasingly important.