2020
DOI: 10.1029/2019gc008809
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Gravity, Topography, and Melt Generation Rates From Simple 3‐D Models of Mantle Convection

Abstract: Convection in fluid layers at high Rayleigh number (Ra ∼ 10 6 ) have a spoke pattern planform. Instabilities in the bottom thermal boundary layer develop into hot rising sheets of fluid, with a component of radial flow toward a central upwelling plume. The sheets form the "spokes" of the pattern, and the plumes the "hubs." Such a pattern of flow is expected to occur beneath plate interiors on Earth, but it remains a challenge to use observations to place constraints on the convective planform of the mantle.Her… Show more

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Cited by 13 publications
(12 citation statements)
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“…In fact, the areas of greatest recent uplift and volcanism in Anatolia are those where we infer an introduction of subslab material into the Anatolian asthenosphere, either vertically through the Cyprus slab tear or laterally through the slab gap (Figure 10, Section 5.4). This suggests that any hot material being introduced originates below the African slabs, perhaps part of a regional North African/Mediterranean upwelling (Nikogosian et al., 2018) or simply a background ‘spoke‐pattern’ mantle convection pattern that has been suggested to occur in the region (Lees et al., 2020; McKenzie, 2020).…”
Section: Discussionmentioning
confidence: 99%
“…In fact, the areas of greatest recent uplift and volcanism in Anatolia are those where we infer an introduction of subslab material into the Anatolian asthenosphere, either vertically through the Cyprus slab tear or laterally through the slab gap (Figure 10, Section 5.4). This suggests that any hot material being introduced originates below the African slabs, perhaps part of a regional North African/Mediterranean upwelling (Nikogosian et al., 2018) or simply a background ‘spoke‐pattern’ mantle convection pattern that has been suggested to occur in the region (Lees et al., 2020; McKenzie, 2020).…”
Section: Discussionmentioning
confidence: 99%
“…Low viscosities imply higher temperatures and low convective stresses. For the isoviscous case, the association of low viscosity with low topography can be seen clearly in Table 2 of Lees et al (2020), from which we get a numerical scaling of h ¢ µh rms 0.6 , with interior temperature and lithospheric thickness fixed. If we have two isoviscous layers with a stiffer top layer (i.e., approximating a cool viscous lithosphere), then there is an analytical solution for the surface normal stress induced by a spherical density anomaly at some depth (Equation (34) in Morgan 1965).…”
Section: The Role Of Rheology and Its Uncertaintiesmentioning
confidence: 80%
“…This choice is based on the reasoning that the rms value may be less sensitive to the model geometry-crucial for inferring 3D behavior from 2D models, as we will be doing. As such, we ran preliminary isoviscous convection simulations to confirm that neither Cartesian nor cylindrical 2D geometries show the same peak topographies as the equivalent 3D spherical experiments from Lees et al (2020), whereas, for all three setups, the rms topographies align well. That the same result holds for non-isoviscous simulations is an outstanding caveat of this study.…”
Section: Numerical Convection Modelmentioning
confidence: 95%
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“…It is the presence of hubs that led to Wilson and Morgan's proposals. Recent numerical experiments by Lees et al (2020) in large aspect ratio boxes show that the spokes, as well as the hubs, can deform the surface, generate gravity anomalies and magma, provided the overlying lithosphere is sufficiently thin.…”
Section: Introductionmentioning
confidence: 99%