FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2554034429> ?p ?o ?g. }

• W2554034429 abstract "The fundamental physics and dynamics relating to two-layer convection with an infinite Prandtl number and large viscosity contrasts have not yet been quantitatively resolved by previous numerical analyses or simulations and laboratory experiments. Here, a series of high-resolution numerical simulations of Rayleigh-Bénard convection with a highly viscous outer layer (HVL) and a low-viscosity inner layer (LVL) in 2-D spherical-shell geometry were performed to investigate the dynamics of convection between the two layers with large viscosity contrasts of up to 103. To achieve a two-layer thermal convection system considering a thermally and mechanically continuous interface between the two layers without any specified boundary conditions, an “effective thermal expansion coefficient” was introduced to the buoyancy term of the momentum equation, discretized in a finite-volume-based regular grid system. In this study, the heat transport efficiency of two-layer convection was evaluated, and the coupling modes between the two layers were directly analyzed using the temperature anomaly and deviatoric stress fields near the interface. Results show that the mechanical coupling mode is dominant in two-layer convection when the absolute viscosity contrast between the two layers is sufficiently small, and it weakens, becoming closer to the thermal coupling mode, as the LVL viscosity decreases. This transition from the mechanical coupling to the thermal coupling modes is quantitatively detected even when the viscosity contrast between the two layers is 10−3, and results in the stabilizing of the convection speed and the heat transport efficiency of the HVL. Applying the mantle–outer core coupling of the present Earth with an extremely large absolute viscosity contrast, our numerical results imply that thermal convection in the mantle may control the heat transport efficiency of a layered whole solid-earth system and the convective style in the outer core." @default.
• W2554034429 created "2016-11-30" @default.
• W2554034429 creator A5013109536 @default.
• W2554034429 creator A5027910225 @default.
• W2554034429 date "2016-11-01" @default.
• W2554034429 modified "2023-10-14" @default.
• W2554034429 title "Numerical studies on the dynamics of two-layer Rayleigh-Bénard convection with an infinite Prandtl number and large viscosity contrasts" @default.
• W2554034429 cites W1027217899 @default.
• W2554034429 cites W1518740426 @default.
• W2554034429 cites W1526731424 @default.
• W2554034429 cites W1526762037 @default.
• W2554034429 cites W1571345535 @default.
• W2554034429 cites W1689232968 @default.
• W2554034429 cites W1964847811 @default.
• W2554034429 cites W1965327191 @default.
• W2554034429 cites W1967598321 @default.
• W2554034429 cites W1967793970 @default.
• W2554034429 cites W1968433040 @default.
• W2554034429 cites W1974295225 @default.
• W2554034429 cites W1975840213 @default.
• W2554034429 cites W1982925530 @default.
• W2554034429 cites W1983528946 @default.
• W2554034429 cites W1984484729 @default.
• W2554034429 cites W1986671908 @default.
• W2554034429 cites W1990234080 @default.
• W2554034429 cites W1990447481 @default.
• W2554034429 cites W1990985465 @default.
• W2554034429 cites W1991650472 @default.
• W2554034429 cites W1995277550 @default.
• W2554034429 cites W1997512428 @default.
• W2554034429 cites W1997931655 @default.
• W2554034429 cites W1997989802 @default.
• W2554034429 cites W1999741397 @default.
• W2554034429 cites W2002704244 @default.
• W2554034429 cites W2003654260 @default.
• W2554034429 cites W2006214166 @default.
• W2554034429 cites W2008955839 @default.
• W2554034429 cites W2013210818 @default.
• W2554034429 cites W2017954284 @default.
• W2554034429 cites W2018133579 @default.
• W2554034429 cites W2019551697 @default.
• W2554034429 cites W2020187485 @default.
• W2554034429 cites W2023530215 @default.
• W2554034429 cites W2025544010 @default.
• W2554034429 cites W2026096125 @default.
• W2554034429 cites W2031854576 @default.
• W2554034429 cites W2032179986 @default.
• W2554034429 cites W2040310647 @default.
• W2554034429 cites W2042708187 @default.
• W2554034429 cites W2044754098 @default.
• W2554034429 cites W2045044603 @default.
• W2554034429 cites W2048240400 @default.
• W2554034429 cites W2049971373 @default.
• W2554034429 cites W2050933236 @default.
• W2554034429 cites W2051724188 @default.
• W2554034429 cites W2052893725 @default.
• W2554034429 cites W2054943641 @default.
• W2554034429 cites W2056884602 @default.
• W2554034429 cites W2066195054 @default.
• W2554034429 cites W2066870142 @default.
• W2554034429 cites W2067612763 @default.
• W2554034429 cites W2070929261 @default.
• W2554034429 cites W2073804062 @default.
• W2554034429 cites W2077208327 @default.
• W2554034429 cites W2079260131 @default.
• W2554034429 cites W2083269074 @default.
• W2554034429 cites W2084352787 @default.
• W2554034429 cites W2085459043 @default.
• W2554034429 cites W2085581605 @default.
• W2554034429 cites W2085845463 @default.
• W2554034429 cites W2085875759 @default.
• W2554034429 cites W2087077480 @default.
• W2554034429 cites W2091199044 @default.
• W2554034429 cites W2091450224 @default.
• W2554034429 cites W2097596053 @default.
• W2554034429 cites W2098617150 @default.
• W2554034429 cites W2098874977 @default.
• W2554034429 cites W2110713121 @default.
• W2554034429 cites W2111959780 @default.
• W2554034429 cites W2114164194 @default.
• W2554034429 cites W2126388052 @default.
• W2554034429 cites W2130265341 @default.
• W2554034429 cites W2131272233 @default.
• W2554034429 cites W2133675958 @default.
• W2554034429 cites W2134229376 @default.
• W2554034429 cites W2136391139 @default.
• W2554034429 cites W2157813471 @default.
• W2554034429 cites W2170339782 @default.
• W2554034429 cites W2170997682 @default.
• W2554034429 cites W2176624776 @default.
• W2554034429 cites W2411105275 @default.
• W2554034429 cites W2416078785 @default.
• W2554034429 cites W2495087378 @default.
• W2554034429 cites W2963196277 @default.
• W2554034429 cites W3098507781 @default.
• W2554034429 cites W3100829481 @default.
• W2554034429 cites W3101584190 @default.
• W2554034429 cites W3121813492 @default.
• W2554034429 cites W392436494 @default.
• W2554034429 doi "https://doi.org/10.1063/1.4966685" @default.

• next