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Efficient exhumation of (ultra) high-pressure rocks by slab extraction Zhao, Z., P.D. Bons, Eberhard Karls University Tübingen, Germany E. Gomez-Rivas,

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Presentation on theme: "Efficient exhumation of (ultra) high-pressure rocks by slab extraction Zhao, Z., P.D. Bons, Eberhard Karls University Tübingen, Germany E. Gomez-Rivas,"— Presentation transcript:

1 Efficient exhumation of (ultra) high-pressure rocks by slab extraction Zhao, Z., P.D. Bons, Eberhard Karls University Tübingen, Germany E. Gomez-Rivas, University of Aberdeen, Scotland, UK A. Soesoo, Tallinn University of Technology, Tallinn, Estonia E. Burov, Université P. & M. Curie (Paris VI), Paris, France

2 Outline Introduction to slab extraction Definition Divergent double subduction zone setting Numerical simulations with FLAMAR Cases in geological records Paleotethys in Qiangtang Suture, Tibet D'Entrecasteaux eclogites, Papua New Guinea Conclusion

3 "Normally" suture between plates has reverse movement When plates diverge – rollback, or – slab extraction Slab extraction

4 Opposing slab pulls: F 2 > F 1 F resistance shear force at base and overlying oceanic lithosphere When F 2 > F 1 + F resistance Short slab may be pulled up by long slab Related to L 1 -L 2, temperature-density relationships, x,  1,2, rheology of slab and mantle, etc. Slab extraction is likely to happen when x becomes small x L1L1  L2L2  F1F1 F2F2 Divergent double subduction zone (DDSZ)

5 It solves simultaneously Newtonian dynamic equations of motion, in a Lagrangian formulation, coupled with visco-elasto-plastic constitutive equations, heat transport equations and state equation (Burov et al., 2001; 2003; Burov and Yamato, 2008)  C p (  T/  t + u  T) –  (k  ) - H r - H a - frac  II  II /  t = 0  = f(P,T) The parameters A, n, Q are experimentally determined material properties Numerical simulations: FLAMAR

6 40km 110km Length differences170km (variable) 10km 80km Geometry: divergent double subduction zone Material properties from Angiboust et al. (2012) Parameters varied: V x, ∆L and rheology of slab ∆L VxVx Starting model and settings

7 Simulations V x =0

8 Simulations The-Depth of passive markers Exhumation rate of passive markers

9 Simulations V x =-2cm/y

10 Simulations The-Depth of passive markers Exhumation rate of passive markers

11 Slab gets extracted when – x is short – ∆L large – subducted lithosphere strong – Lubricate layer is necessary (serpentinite) High-pressure rocks exhumed rapidly – brought in contact with sediments/LP rocks – in locally strong extensional setting in case of plate divergence – rapid exhumation of HP rocks on both sides – opening of pull-apart basin Results

12 HP rocks in direct contact with non-metamorphic sedimentary mélange Consistent top-to-south shear Sedimentation and volcanism – no extensive erosion to exhume HP rocks Case 1: Qiangtang suture, Central Tibet (Zhao et al., 2015).

13 Young eclogites 4.6-5.6 Ma Exhumation rate ~2 cm/yr NW movement of Solomon sea plate New pull-apart basin (Baldwin et al., 2004; DesOrmeau et al., 2014; Korchinski et al., 2014). Case 2: D'Entrecasteaux eclogites

14 Extraction is an efficient mechanism for rapid exhumation of (U)HP rocks – Brings (U)HP rocks in contact with LP rocks – No need for erosion Close to eduction 1 and extension model 2 – Extracted slab can be negatively buoyant (ocean) Requires divergence of subducted slab and overriding plate – Single suture (Western Gneiss, Norway) – DDSZ (Qiangtang, d'Entrecasteaux Islands) Conclusion Refs.: (1) Duretz et al., 2012; (2) Brueckner et al., 2013

15 Thank you Zhao, Z., Bons, P., Wang, G., Soesoo, A., and Liu, Y.: Tectonic evolution and high- pressure rock exhumation in the Qiangtang Terrane, Central Tibet, Solid Earth, 2015.


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