2015
DOI: 10.1017/jfm.2014.722
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Dissolution of a vertical solid surface by turbulent compositional convection

Abstract: We examine the dissolution of a vertical solid surface in the case where the heat and mass transfer is driven by turbulent compositional convection. A theoretical model of the turbulent dissolution of a vertical wall is developed, which builds on the scaling analysis presented by Kerr (J. Fluid Mech., vol. 280, 1994, pp. 287–302) for the turbulent dissolution of a horizontal floor or roof. The model has no free parameters and no dependence on height. The analysis is tested by comparing it with laboratory measu… Show more

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Cited by 49 publications
(134 citation statements)
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“…Figure 3 shows the measured interface temperature as a function of the BruntVäisälä frequency, N = (−(g/ρ 0 )(dρ/dz)) 1/2 , where ρ 0 is the density at mid-depth. The theory of Kerr & McConnochie (2015) suggests that, for a far-field temperature of T f = 3.5 • C and a homogeneous far-field salinity of C f = 3.5 wt% NaCl, the interface temperature should be −0.52 • C. This agrees with the low-stratification experiments shown in figure 3.…”
Section: Methodssupporting
confidence: 83%
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“…Figure 3 shows the measured interface temperature as a function of the BruntVäisälä frequency, N = (−(g/ρ 0 )(dρ/dz)) 1/2 , where ρ 0 is the density at mid-depth. The theory of Kerr & McConnochie (2015) suggests that, for a far-field temperature of T f = 3.5 • C and a homogeneous far-field salinity of C f = 3.5 wt% NaCl, the interface temperature should be −0.52 • C. This agrees with the low-stratification experiments shown in figure 3.…”
Section: Methodssupporting
confidence: 83%
“…Table 1 shows the experimental parameters and results for the stratified ambient experiments where an interface temperature was measured. Like the homogeneous ambient experiments of Kerr & McConnochie (2015), we observed no height dependence on interface temperature. Figure 3 shows the measured interface temperature as a function of the BruntVäisälä frequency, N = (−(g/ρ 0 )(dρ/dz)) 1/2 , where ρ 0 is the density at mid-depth.…”
Section: Methodssupporting
confidence: 73%
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