Wetting transition

Wetting transitions

The macroscopic parameter characterizing wetting of a solid (or liquid) surface with a liquid is the contact angle.[1] Various contact angles can co-exist on the same solid substrate. A wetting transition corresponds to a certain change in contact angle. Wetting transitions occurring on either flat or rough surfaces should be distinguished.

  1. Flat surfaces. When a liquid drop is put onto a surface, two situations may result. If the contact angle is zero, the situation is referred to as complete wetting. If the contact angle is between 0 and 180°, the situation is called partial wetting. A wetting transition is a surface phase transition from partial wetting to complete wetting.[2]
  2. Rough surfaces.

The situation on rough surfaces is much more complicated. The main characteristic of the wetting properties of rough surfaces is the so-called apparent contact angle (APCA). It is well known that the APCA usually measured are different from those predicted by the Young equation. Two main hypotheses were proposed in order to explain this discrepancy, namely the Wenzel and Cassie wetting models.[3][4][5] According to the traditional Cassie model, air can remain trapped below the drop, forming "air pockets". Thus, the hydrophobicity of the surface is strengthened because the drop sits partially on air. On the other hand, according to the Wenzel model the roughness increases the area of a solid surface, which also geometrically modifies the wetting properties of this surface.[1][3][4][5] Transition from Cassie to Wenzel regime is also called wetting transition.[6][7][8] Under certain external stimuli, such as pressure or vibration, the Cassie air trapping wetting state could be converted into the Wenzel state.[6][9][10][11] It is well accepted that the Cassie air trapping wetting regime corresponds to a higher energetic state, and the Cassie–Wenzel transition is irreversible.[12] However, the mechanism of the transition remains unclear. It was suggested that the Cassie–Wenzel transition occurs via a nucleation mechanism starting from the drop center.[13] On the other hand, recent experiments showed that the Cassie–Wenzel transition is more likely to be due to the displacement of a triple line under an external stimulus.[9][10][11] The existence of so-called impregnating Cassie wetting state also has to be considered.[11] Understanding wetting transitions is of a primary importance for design of superhydrophobic surfaces.[14][15]

See also

References

  1. ↑ 1.0 1.1 P.G. de Gennes, F. Brochard-Wyart, D. Quéré, Capillarity and Wetting Phenomena, Springer, Berlin, 2003.
  2. ↑ D. Bonn, D. Ross, Rep. Prog. Phys. 2001, 64, 1085-1183.
  3. ↑ 3.0 3.1 A. B. D. Cassie and S. Baxter, Trans. Faraday Soc., 1944, 40, 546–551.
  4. ↑ 4.0 4.1 A. B. D. Cassie, Discuss. Faraday Soc., 1948, 3, 11–16.
  5. ↑ 5.0 5.1 R. N. Wenzel, Ind. Eng. Chem., 1936, 28, 988–994.
  6. ↑ 6.0 6.1 A. Lafuma, D. Quéré, Nat. Mater., 2003, 2, 457–460.
  7. ↑ L. Barbieri, E. Wagner, P. Hoffmann, Langmuir, 2007, 23, 1723-1734.
  8. ↑ J. Wang, D. Chen, Langmuir, 2008, 24, 10174-10180.
  9. ↑ 9.0 9.1 E. Bormashenko, R. Pogreb, G. Whyman, Ye. Bormashenko, M. Erlich, Langmuir, 2007, 23, 6501–6503.
  10. ↑ 10.0 10.1 E. Bormashenko, R. Pogreb, G. Whyman, Ye. Bormashenko, M. Erlich, Langmuir, 2007, 23, 12217–12221.
  11. ↑ 11.0 11.1 11.2 E. Bormashenko, R. Pogreb, T. Stein, G. Whyman, M. Erlich, A. Musin, V. Machavariani, D. Aurbach, Phys. Chem. Chem. Phys., 2008, 10, 4056–4061.
  12. ↑ A. Marmur, Soft Matter, 2006, 2, 12–17.
  13. ↑ C. Ishino, K. Okumura, Europhys. Lett., 2006, 76(3), 464–470.
  14. ↑ D. Quéré, M. Reyssat, Philos. Trans. R. Soc. London, A 2008, 366, 1539–1556.
  15. ↑ M. Nosonovsky, B. Bhushan, Adv. Funct. Mater. 2008, 18, 843–855.