2016
DOI: 10.1080/03091929.2016.1146264
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Convection of a fluid with strongly temperature and pressure dependent viscosity

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Cited by 6 publications
(3 citation statements)
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“…Previous studies have shown that convection is active in the top part of the convecting system (e.g., Christensen, 1984;Fleitout and Yuen, 1984;Christensen, 1985;Stemmer et al, 2006). At high viscosity contrasts the convective system divides to smaller sub-cells (Khaleque et al, 2015;Fowler et al, 2016), which can be interpreted as a reduction in the effective convective depth as we assume in this paper. Thus, it is important to consider pressure-dependent viscosity in the future studies of lithospheric failure.…”
Section: Discussionmentioning
confidence: 95%
“…Previous studies have shown that convection is active in the top part of the convecting system (e.g., Christensen, 1984;Fleitout and Yuen, 1984;Christensen, 1985;Stemmer et al, 2006). At high viscosity contrasts the convective system divides to smaller sub-cells (Khaleque et al, 2015;Fowler et al, 2016), which can be interpreted as a reduction in the effective convective depth as we assume in this paper. Thus, it is important to consider pressure-dependent viscosity in the future studies of lithospheric failure.…”
Section: Discussionmentioning
confidence: 95%
“…In an infinite horizontal layer, the convective cell is defined as part of a periodic structure. Applying Cartesian coordinates (x, z), the Boussinesq approximation is inferred, implying that density variation may be ignored in the buoyancy term, and therefore equation of continuity takes the form of the incompressibility requirement [21]. The mechanical work produced by thermal convection typically balances the viscous dissipation in the mantle layer, and if the viscosity change is significant enough, the dissipation in the cold boundary layer can be compared to that in the interior region.…”
Section: Governing Equationmentioning
confidence: 99%
“…Both studies find the Nusselt number to be N u ∼ (∆T /∆T r ) −1 Ra 1/5 r , where Ra r = αg∆T r d 3 /ν 0 κ is the Rayleigh number based on the rheological temperature scale ∆T r and the viscosity ν 0 at the hot bottom boundary. Fowler et al (2016) extended the asymptotic analysis of Fowler (1985a) to the case of strongly temperature-and pressure-dependent viscosity. Solomatov (1995) presented a scaling analysis for convection in fluids with temperature-and stress-dependent viscosity, using arguments based on the balance between dissipation and the rate of mechanical work.…”
Section: Convection With Temperature-dependent Viscositymentioning
confidence: 99%