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. 2014 Jun 20;4:5376. doi: 10.1038/srep05376

Figure 3. Capillary tube rise of low viscosity liquid27.

Figure 3

r, z, ρ, γ, η, and Vcare the radius of a capillary tube, height of meniscus, liquid density, surface tension, viscosity, and meniscus rising velocity, respectively. The liquid-air interface of the liquid pool is located at z = 0 and the liquid starts to intrude into the capillary at t = 0. If the liquid is more viscous than 3/2r5/2γ1/2, the capillary tube imbibition process can be divided into three stages28: acceleration, linear, and Washburn regimes (see Supplementary Information for the description of the capillary rise). Accordingly, Σ for a given system can be calculated (Table S5).