2020
DOI: 10.1103/physreve.102.033102
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Scaling laws of electroconvective flow with finite vortex height near permselective membranes

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Cited by 11 publications
(8 citation statements)
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“…Recently, Lui et al presented results from scaling analysis and DNS of electroconvection in the absence of an externally imposed shear flow. These results support a linear scaling of both the dimensionless steady-state vortex height and overlimiting current with V . Similarly, studies have also shown that gravitational effects can play an important role in the onset of convective flow especially in systems with large Rayleigh numbers, where Rayleigh–Bernard convection can lead to an unstable overlimiting current and this effect becomes more pronounced as the characteristic length of the system increases. , …”
Section: Introductionsupporting
confidence: 76%
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“…Recently, Lui et al presented results from scaling analysis and DNS of electroconvection in the absence of an externally imposed shear flow. These results support a linear scaling of both the dimensionless steady-state vortex height and overlimiting current with V . Similarly, studies have also shown that gravitational effects can play an important role in the onset of convective flow especially in systems with large Rayleigh numbers, where Rayleigh–Bernard convection can lead to an unstable overlimiting current and this effect becomes more pronounced as the characteristic length of the system increases. , …”
Section: Introductionsupporting
confidence: 76%
“…Meanwhile for 0.1 mM, the extent of convection keeps increasing linearly with voltage, and for voltages higher than 250 V T , the flow occurs even beyond the experimental viewing window. Previous studies have reported a linear scaling for nonsheared electroconvection for steady vortex height, but we find this scaling valid for chaotic electroconvection too. , Figure shows a comparison of the vortex size distribution for different c and highlights the marked effect of electrolyte concentration. For example, at c = 0.1 M, vortices remain small and localized near the permselective interface (Figure a, e).…”
Section: Resultsmentioning
confidence: 45%
“…Using a first-order approximation 1/∂x ∼ 1/∂y ∼ 1/δ 0 , (∂ 2 c + /∂x∂y)/(∂c + /∂y) can be further simplified as∼1/δ 0 , where the depletion layer thickness δ 0 can be identified by a given vortex height d EC . Furthermore, the slip velocity can be estimated by u s ∼ φ 2 (1/δ 0 ) (Kwak et al 2017), which is proven to be valid for analysing the slip velocity of non-shear flows (Liu et al 2020b). However, for the shear shielding case, the slip velocity is dominated by the shear flow velocity.…”
Section: Critical Selection Of Shear Shelteringmentioning
confidence: 99%
“…2017), which is proven to be valid for analysing the slip velocity of non-shear flows (Liu et al. 2020 b ). However, for the shear shielding case, the slip velocity is dominated by the shear flow velocity.…”
Section: Theoretical Analysismentioning
confidence: 99%
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