Assessing the role of oceanic, continental, and cratonic lithosphere in mantle circulation
Abigail Plimmer1 , J. Huw Davies1, James Panton1
1Cardiff University, UK
Supercontinent cycling is a pervasive process which has endured in its current Wilson tectonics style for at least 1 Ga (Stern, 2008; Ernst, 2017). Despite this, the degree of feedback between the surface and CMB boundary layers during the supercontinent cycle remains elusive.
Historically, mantle models have treated the lithosphere as a homogenous rigid layer, which deforms in response to the imposed plate velocities or thermal instabilities. However, to properly assess the degree of coupling between the surface and the mantle it is crucial to represent the complexity of the Earth’s lithosphere since the intrinsic properties of different lithospheric domains may affect the dynamics of the upper mantle.
We use the plate motion reconstructions of Merdith et al., (2021), Cao et al., (2021), and Müller et al (2022) to define regions of oceanic, continental, and cratonic lithosphere which can then be implemented into our models with variable buoyancies, viscosities, and depths. We assess upper mantle thermal perturbations in each simulation and consider the implications of this on slab sinking and plume upwelling. We suggest that where the upper mantle is shielded by thicker, viscous cratons, we may observe slab and plume dynamics reminiscent of those proposed in the mantle insulation model proposed by Anderson (1982).
We utilise the 3D mantle convection code, TERRA (Baumgardner 1983), to model the interaction between slabs subducted around the edges of supercontinents and deep mantle structures. Our initial models track and measure the sinking times of slabs with varying physical properties and geometries throughout the mantle. Slab buoyancies and viscosity profiles within the mantle are varied to constrain the implications of each parameter. We find that thermal processes are critical factors controlling the slab sinking times since the thermal and density structure of the slab, as well as the upper mantle viscosity ultimately control the slab velocity. We show the effects of composition are secondary and relatively minor.
As such, the lithospheric complexities at the surface may be considered alongside plate density and strength as significant controls on slab dynamics and as one of many possible explanations of global slab heterogeneity.
References
Anderson, D.L., 1982. Hotspots, polar wander, Mesozoic convection and the geoid. Nature, 297(5865), pp.391-393.
Cao, X., Flament, N. and Müller, R.D., 2021. Coupled evolution of plate tectonics and basal mantle structure. Geochemistry, Geophysics, Geosystems, 22(1), p.e2020GC009244.
Ernst, W.G., 2017. Earth’s thermal evolution, mantle convection, and Hadean onset of plate tectonics. Journal of Asian Earth Sciences, 145, pp.334-348.
Merdith, A.S., Williams, S.E., Collins, A.S., Tetley, M.G., Mulder, J.A., Blades, M.L., Young, A., Armistead, S.E., Cannon, J., Zahirovic, S. and Müller, R.D., 2021. Extending full-plate tectonic models into deep time: Linking the Neoproterozoic and the Phanerozoic. Earth-Science Reviews, 214, p.103477.
Müller, R.D., Flament, N., Cannon, J., Tetley, M.G., Williams, S.E., Cao, X., Bodur, Ö.F., Zahirovic, S. and Merdith, A., 2022. A tectonic-rules-based mantle reference frame since 1 billion years ago–implications for supercontinent cycles and plate–mantle system evolution. Solid Earth, 13(7), pp.1127-1159.
Stern, R.J., 2008. Modern-style plate tectonics began in Neoproterozoic time: An alternative interpretation of Earth’s tectonic history. When did plate tectonics begin on planet Earth, 440, pp.265-280.
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