2017
DOI: 10.1021/acs.jpcc.7b06124
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Viscous Force Retards Initial Droplet Spreading

Abstract: A droplet could spread on a solid substrate within several milliseconds, and be divided into two stages, a fast inertial stage and a subsequent slow viscous stage. The effects of inertia and viscosity on spreading are presented with Ohnesorge number. A small Ohnesorge number corresponds to an initial inertial spreading. In this study, spreading experiments were carried out with a time resolution of 1 μs. Results disclose that the viscous force could retard droplet spreading at the beginning of liquid/solid sur… Show more

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Cited by 15 publications
(4 citation statements)
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“…While the spreading of spherical droplets has been extensively investigated via experiments, ,, theory, and computational methods, , the spreading of filaments has received little attention. One exception is the work by Starov et al, which developed a theoretical model for the spreading of a 2D symmetric cylindrical filament in the capillary and gravitational spreading limits.…”
Section: Introductionmentioning
confidence: 99%
“…While the spreading of spherical droplets has been extensively investigated via experiments, ,, theory, and computational methods, , the spreading of filaments has received little attention. One exception is the work by Starov et al, which developed a theoretical model for the spreading of a 2D symmetric cylindrical filament in the capillary and gravitational spreading limits.…”
Section: Introductionmentioning
confidence: 99%
“…Figure 5b shows the droplet shape and the droplet resistance at different times. A high-speed camera (NAC HX-6) with a frame rate of 10 000 frames/s was used to capture the spreading of the droplet (initial radius R ≈ 1.12 mm) 37 and to obtain the spreading radius. As the spreading radius increased, the droplet began to deform at the top and propagated rapidly to the bottom.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…In general, the larger the value of , the longer it takes to reach the equilibrium state of spreading, and vice versa. These indicated that the early spreading stage, t < 10 ms, of oil droplets was quite short, which was dominated by the inertial force [ 26 , 43 , 47 , 48 ]. In the intermediate stage of spreading (10 ms ≤ t < 100 ms), the temporal evolution of dynamic contact angle could be well described by a simple scaling law of , and the spreading exponent (−0.28) was close to −0.3 ( ) obtained based on the HD model, which suggested that the spreading of the oleic acid droplet on the Teflon in air during the intermediate spreading process was dominated by the viscous dissipation due to viscous flow in the core of the droplet [ 27 , 30 ].…”
Section: Resultsmentioning
confidence: 99%
“…Starov et al [ 24 ] and Lee et al [ 25 ] considered the spreading behavior of surfactant solution droplets over various substrates from both theoretical and experimental points of view, and suggested that the transfer of surfactant molecules from the water droplet onto the hydrophobic surface changed the wetting characteristics in front of the droplet on the TPCL. Shi et al [ 26 ] performed an interesting experiment to study the spreading behavior of a conducted droplet on two glass plates coated with a conductive indium tin oxide (ITO) thin film within several milliseconds, and found that the spreading process in this time scale could be separated into two stages: a fast-inertial stage and a subsequent slow-viscous stage.…”
Section: Introductionmentioning
confidence: 99%