2014
DOI: 10.1088/0169-5983/46/4/041421
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Structure and dynamics of particle-accumulation in thermocapillary liquid bridges

Abstract: The accumulation of small mono-disperse heavy particles in thermocapillary liquid bridges is investigated experimentally and numerically. We consider particle accumulation near the center of the toroidal vortex, the so-called toroidal core of particles (COP), and the particle-depletion zone near the axis of the liquid bridge. Based on the acceleration and deceleration of the tangential flow along the thermocapillary free surface it is argued that the interaction of the particles with the free surface is of key… Show more

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Cited by 29 publications
(14 citation statements)
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“…These additional conditions concern, in particular, the influence of particle motion on the large-scale flow and the particle-particle interplay (Derksen and Eskin, 2011;Balboa Usabiaga et al, 2013). To fix these issues, like earlier studies Kuhlmann and Muldoon, 2012), our investigation targets the dilute regime, i.e. it is assumed that the effect of the particles onto the fluid, as well as the interaction among particles are negligible (in the presence of vibrations, as shown by several authors, this is permissible if the concentration of the dispersed phase in the flow is small, i.e.…”
Section: The Dispersed Phasementioning
confidence: 99%
“…These additional conditions concern, in particular, the influence of particle motion on the large-scale flow and the particle-particle interplay (Derksen and Eskin, 2011;Balboa Usabiaga et al, 2013). To fix these issues, like earlier studies Kuhlmann and Muldoon, 2012), our investigation targets the dilute regime, i.e. it is assumed that the effect of the particles onto the fluid, as well as the interaction among particles are negligible (in the presence of vibrations, as shown by several authors, this is permissible if the concentration of the dispersed phase in the flow is small, i.e.…”
Section: The Dispersed Phasementioning
confidence: 99%
“…Note that the fundamental azimuthal modal number m 0 is generally described as m in the previous researches. The temperature deviation rotates without any variation of its structure as a rigid body at a constant azimuthal velocity (Muldoon and Kuhlmann, 2013;Kuhlmann et al, 2014). Figure 3 (b) shows the time series as in frame (a) but in the rotating frame of reference against the fundamental period of the convection with 1/ f 0 .…”
Section: Resultsmentioning
confidence: 99%
“…where Gr is Grashof number, Ma is Marangoni number, Pr is Prandtl number, β is the coefficient of cubic expansion, μ is the viscosity, a is thermal diffusivity, v is kinematic viscosity, ρ is density, T σ is the temperature derivative of surface tension coefficient [17] and T ∆ is the gap between initial fuel temperature and flashpoint. Then, the Gr number is related to t h , and the Ma number is related to L. The experimental data is expressed as, By submitting Equation (7) into Equation (3) (4), we can obtain the following Equation (8).…”
Section: The Non-dimensional Numbermentioning
confidence: 99%