TY - JOUR
T1 - Dynamic Effects during the Capillary Rise of Fluids in Cylindrical Tubes
AU - Lunowa, Stephan B.
AU - Mascini, Arjen
AU - Bringedal, Carina
AU - Bultreys, Tom
AU - Cnudde, Veerle
AU - Pop, Iuliu Sorin
N1 - Funding Information:
The authors are grateful to Mohammad Heshmati and Mohammad Piri for providing their experimental data. The authors thank the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) for supporting this work by funding the Collaborative Research Center on Interface-Driven Multi-Field Processes in Porous Media (SFB 1313, grant number 327154368) and by funding EXC 2075-390740016 under Germany’s Excellence Strategy. We acknowledge support by the Stuttgart Centre for Simulation Science (SimTech). This work was supported by Hasselt University (project number BOF17NI01) and the Research Foundation Flanders (FWO) [grant numbers G051418N, G0G1316N, and 12X0919N]; Tom Bultreys is a postdoctoral fellow of the Research Foundation Flanders.
Publisher Copyright:
© 2022 American Chemical Society.
PY - 2022/2/8
Y1 - 2022/2/8
N2 - The mathematical models for the capillary-driven flow of fluids in tubes typically assume a static contact angle at the fluid-air contact line on the tube walls. However, the dynamic evolution of the fluid-air interface is an important feature during capillary rise. Furthermore, inertial effects are relevant at early times and may lead to oscillations. To incorporate and quantify the different effects, a fundamental description of the physical processes within the tube is used to derive an upscaled model of capillary-driven flow in circular cylindrical tubes. The upscaled model extends the classical Lucas-Washburn model by incorporating a dynamic contact angle and slip. It is then further extended to account for inertial effects. Finally, the solutions of the different models are compared to experimental data. In contrast to the Lucas-Washburn model, the models with dynamic contact angle match well the experimental data, both the rise height and the contact angle, even at early times. The models have a free parameter through the dynamic contact angle description, which is fitted using the experimental data. The findings here suggest that this parameter depends only on the properties of the fluid but is independent of geometrical features, such as the tube radius. Therefore, the presented models can predict the capillary-driven flow in tubular systems upon knowledge of the underlying dynamic contact-angle relation.
AB - The mathematical models for the capillary-driven flow of fluids in tubes typically assume a static contact angle at the fluid-air contact line on the tube walls. However, the dynamic evolution of the fluid-air interface is an important feature during capillary rise. Furthermore, inertial effects are relevant at early times and may lead to oscillations. To incorporate and quantify the different effects, a fundamental description of the physical processes within the tube is used to derive an upscaled model of capillary-driven flow in circular cylindrical tubes. The upscaled model extends the classical Lucas-Washburn model by incorporating a dynamic contact angle and slip. It is then further extended to account for inertial effects. Finally, the solutions of the different models are compared to experimental data. In contrast to the Lucas-Washburn model, the models with dynamic contact angle match well the experimental data, both the rise height and the contact angle, even at early times. The models have a free parameter through the dynamic contact angle description, which is fitted using the experimental data. The findings here suggest that this parameter depends only on the properties of the fluid but is independent of geometrical features, such as the tube radius. Therefore, the presented models can predict the capillary-driven flow in tubular systems upon knowledge of the underlying dynamic contact-angle relation.
UR - http://www.scopus.com/inward/record.url?scp=85124136634&partnerID=8YFLogxK
U2 - 10.1021/acs.langmuir.1c02680
DO - 10.1021/acs.langmuir.1c02680
M3 - Article
SN - 0743-7463
VL - 38
SP - 1680
EP - 1688
JO - Langmuir
JF - Langmuir
IS - 5
ER -