2012
DOI: 10.1016/j.colsurfa.2012.04.009
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Energy-based model for capillary spreading of power-law liquids on a horizontal plane

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Cited by 34 publications
(62 citation statements)
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“…For constant-temperature or non-reactive wetting, the driving force or energy for spreading is Young's force or energy, the energy input to the droplet is dissipated mainly by bulk viscous dissipation, local dissipation in the vicinity of the contact line, and viscous dissipation in the precursor film [44,47] , with the last one being excluded in the present system.…”
Section: Discussionmentioning
confidence: 99%
“…For constant-temperature or non-reactive wetting, the driving force or energy for spreading is Young's force or energy, the energy input to the droplet is dissipated mainly by bulk viscous dissipation, local dissipation in the vicinity of the contact line, and viscous dissipation in the precursor film [44,47] , with the last one being excluded in the present system.…”
Section: Discussionmentioning
confidence: 99%
“…Many experimental studies had revealed that free surface evaporation greatly affected the contact line motion and the dynamic contact angle [4][5][6][7][8][9]. The spreading of nonevaporating droplets has been widely studied theoretically using macroscopic hydrodynamic models [10][11][12] and numerically using the mesoscopic lattice Boltzmann method (LBM) [13][14][15] and microscopic MD simulations [16][17][18][19][20]. There were some studies of droplet spreading-evaporating using macroscopic computational fluid dynamics (CFD) models [21][22][23].…”
Section: Introductionmentioning
confidence: 99%
“…If n<1, a liquid can be called shear-thinning or pseudoplastic. On the other hand, n>1 corresponds to a shear-thickening or dilatant fluid, while n=1 corresponds to a Newtonian fluid with K as the constant viscosity (Liang et al 2012).…”
Section: Determination Of Rheological Properties Of Wsp Csp and Daspmentioning
confidence: 99%