Abstract
This article presents an investigation into the effects of pneumatic pressure of trapped air on the dynamics of capillary filling. Controlled experiments were carried out in horizontal closed-end capillaries with diameters of 200–700 μm. Glycerol–DI water mixture solutions having viscosities ranging from 8 to 80 mPa s were used as the filling liquids. The pneumatic air backpressure is built up as a result of the air compressed at the closed end of the capillary. A model is presented based on the conventional theory of capillary filling (i.e., Washburn’s equation) with consideration of the effect of air backpressure force on the advancing meniscus. The molecular kinetics theory of Blake and De Coninck’s model (Adv Colloid Interface Sci 96:21–36, 2002) is also incorporated in the model to account for the dependence of dynamic contact angle on wetting velocity. The model predictions agree reasonably well with the experimental data. It is observed that due to the presence of air backpressure, the smaller the capillary diameter, the longer the length that the liquid fills the capillary, regardless of the liquid viscosity. It is also shown that the increased pneumatic air backpressure reduces the equilibrium contact angle (θ 0). A relation is then proposed among liquid penetration, capillary length and radius, and contact angle. In addition, a dimensionless analysis is performed on experimental data, and the power law dependence of dimensionless meniscus position on dimensionless time is obtained.
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Abbreviations
- AV:
-
Attached volume (m3)
- D :
-
Capillary diameter (m)
- g :
-
Gravitational acceleration (m/s2)
- \( g_{\text{W}}^{*} \) :
-
Specific activation free energy of wetting (J/m2)
- h :
-
Planck constant (J s)
- H :
-
Liquid column height (m)
- \( K_{\text{W}}^{0} \) :
-
Equilibrium frequency of displacement of a liquid molecule between adjacent adsorption sites on solid surface (s−1)
- k B :
-
Boltzmann constant (J/K)
- L :
-
Effective total length of the capillary tube (m)
- n :
-
Number of adsorption sites per unit area of solid surface (m−2)
- P air :
-
Air backpressure (Pa)
- P air at equilibrium :
-
Equilibrium air backpressure (Pa)
- P atm :
-
Ambient pressure (Pa)
- P C :
-
Capillary pressure (Pa)
- R :
-
Radius of curvature at liquid–air interface (m)
- r :
-
Capillary radius (m)
- T :
-
Absolute temperature (K)
- t :
-
Time (s)
- x :
-
Meniscus position (m)
- \( \dot{x} \) :
-
Meniscus velocity (m/s)
- \( \ddot{x} \) :
-
Meniscus acceleration (m/s2)
- \( Ca = {{\eta \dot{x}} \mathord{\left/ {\vphantom {{\eta \dot{x}} \gamma }} \right. \kern-\nulldelimiterspace} \gamma } \) :
-
Capillary number
- \( \text{Re} = {{\rho \dot{x}D} \mathord{\left/ {\vphantom {{\rho \dot{x}D} \eta }} \right. \kern-\nulldelimiterspace} \eta } \) :
-
Reynolds number
- \( We = {{\rho \dot{x}^{2} D} \mathord{\left/ {\vphantom {{\rho \dot{x}^{2} D} \gamma }} \right. \kern-\nulldelimiterspace} \gamma } \) :
-
Weber number
- α:
-
Slope of lines curve fitted to data of log x* versus log t*
- β :
-
A constant parameter, logarithm of which is equal to the log x*-intercept of lines curve fitted to data of log x* versus log t*
- γ :
-
Surface tension (N/m)
- θ :
-
Contact angle
- θ D :
-
Dynamic contact angle
- θ 0 :
-
Equilibrium contact angle
- η :
-
Viscosity (Pa s)
- υ :
-
Unit of flow (m3)
- λ :
-
Average distance between adjacent adsorption sites on solid surface (m)
- ζ :
-
Coefficient of friction at the three-phase contact line (Pa s)
- ρ :
-
Density (kg/m3)
- τ :
-
Characteristic time (s)
- ∆:
-
Gradient
- i, j:
-
Any arbitrary experiment
- ∞:
-
Equilibrium position
- *:
-
Dimensionless parameter
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Acknowledgements
The authors gratefully acknowledge the financial support from the Ministry of Education of Singapore to CY (RG17/05) and the A*STAR scholarship to MR.
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Radiom, M., Chan, W.K. & Yang, C. Capillary filling with the effect of pneumatic pressure of trapped air. Microfluid Nanofluid 9, 65–75 (2010). https://doi.org/10.1007/s10404-009-0527-1
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DOI: https://doi.org/10.1007/s10404-009-0527-1