The physics of moving wetting lines.
By T. Blake. Journal of Colloid and Interface Science, 2006
887 citations recorded by the source corpus.
Subfields: Computational Mechanics, Mechanical Engineering, Surfaces, Coatings and Films
View Paper: https://www.semanticscholar.org/paper/7c599a9168a77975d6bb18755adb9e89764e2938
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Computational Mechanics
- Martin J. Blunt
- Branko Bijeljic
- Chunfeng Zhou
- James J. Feng
- Ali Q. Raeini
- Pengtao Yue
- D. Daniel
- J. Snoeijer
In Mechanical Engineering
- Branko Bijeljic
- Ali Q. Raeini
- D. Daniel
- J. Snoeijer
- Hussam Jouhara
- Ruoping Li
- Joanna Aizenberg
- Bruno Andreotti
In Surfaces, Coatings and Films
- D. Daniel
- J. Snoeijer
- Hussam Jouhara
- Pengtao Yue
- Chunfeng Zhou
- Jeremey A Miller
- Ruoping Li
- Joanna Aizenberg
Citations in the corpus
- Sharp-interface limit of the Cahn–Hilliard model for moving contact lines (2010, background): “More in-depth discussion of the outstanding issues can be found in recent reviews (Pismen 2002; Blake 2006; Qian, Wang & Sheng 2006b).”
- Hydrophilic and hydrophobic materials and their applications (2018, background): “The rate of liquid movement also influences contact angle hysteresis (Blake 2006).”
- Oleoplaning droplets on lubricated surfaces (2017, methodology): “[5] Terence D Blake, “The physics of moving wetting lines,” J.”
- Contact angle of micro- and nanoparticles at fluid interfaces (2014, background): “negligible role in contrast to the macroscopic wetting where the opposite behaviour is true [67].”
- Modelling two-phase flow in porous media at the pore scale using the volume-of-fluid method (2012, background): “Therefore, the dynamics of the contact line can be predicted only in simulation methods where the heterogeneities are resolved down to the molecular scale [42].”
- Moving Contact Lines: Scales, Regimes, and Dynamical Transitions (2013, background): “However, MKT provides a phenomenological description that treats contact line motion as a single mode of propagation, characterized by a length scale ξ and by an energy barrier for the activated process E∗ (Blake 2006).”