CHIM0698 Surface tension
2014-2015
Surface tension
On Youtube http://www.youtube.com/watch?v=E6_vXVd_0O4
The surface tension can be thought of as a force
http://www.funsci.com/fun3_en/exper2/exper2.htm
F A
The energy per unit area is γ It can often be thought of as a force
Wilhelmy’s ring (and plate)
http://www.funsci.com/fun3_en/exper2/exper2.htm
Values of γ for some usual liquids
Substance Surface tension (mN/m) Water (10°C) 74.2 Water (25°C) 72.0 Water (50°C) 67.9 Mercury (25°C) 485.5 Acetone (25°C) 23.5 Ethanol (25°C) 23.2 Formamide (25°C) 57.0 Nitrogen (77°K) 8.85
Values from Butt, Graf & Kappl, Physics and Chemistry of Interfaces, Wiley, 2006
There is an extra energy associated with a surface
Molecules on the surface are less bounded than molecules in the bulk.
There is therefore an energy associated with a free surface.
More rigorously: there is a free energy
associated with an interface. This energy is the surface tension γ
A rough estimation of γ from the energy of vaporization
Cyclohexane @ 25°C Uevap = 30.5 kJ/mol ρ=773 kg/m³ M=84.16 g/mol
Assuming a cubic structure (6-coordinated), Uevap converts to 5.08 kJ/mol for each bond. Each molecule on the surface has one missing bond. All is left to determine is the area of each molecule on the surface. This can be estimated as a² with NA a³ ρ = M, i.e. a = 0.565 nm The final estimate is about 26 mJ/m² (the experimental value is ~ 25 mJ/m²)
Stefan’s law
From K.S. Birdi, Surface and Colloid Chemistry, Principles and Applications
2010, CRC Press
Jozef Stefan 1835-1893
Effect of surfactants on surface tension
Critical micellar concentration
Surfactants
Surfactant classification according to the composition of their head: nonionic, anionic,
cationic, amphoteric.
Laplace
Nous devons donc envisager l’état présent de l’univers comme l’effet de son état antérieur et comme la cause de celui qui va suivre. Une intelligence qui, pour un instant donné, connaîtrait toutes les forces dont la nature est animée, et la situation respective des êtres qui la composent, si d’ailleurs elle était assez vaste pour soumettre ces données à l’Analyse, embrasserait dans la même formule les mouvements des plus grands corps de l’univers et ceux du plus léger atome : rien ne serait incertain pour elle et l’avenir, comme le passé serait présent à ses yeux. (Laplace, Essai philosophique sur les probabilités, 1795)
Géomètre de première catégorie, Laplace n’a pas tardé à se montrer un administrateur plus que médiocre ; de son premier travail nous avons immédiatement compris que nous nous étions trompés. Laplace ne traitait aucune question d’un bon point de vue : il cherchait des subtilités de partout, il avait seulement des idées problématiques et enfin il portait l’esprit de l’infiniment petit jusque dans l’administration. (Napoléon Bonaparte, à propos du passage de Laplace au ministère de l’intérieur)
Pierre-Simon de Laplace (1749-1827)
Thomas Young
Thomas Young 1773-1829
• Optics: the double-slit interference experiments • Mechanics: Young’s modulus • Wetting phenomena: Young-Laplace & Young-Dupré relations • Vision and color theory: Young-Helmholtz, 3-dimensional color space • Physiology: pulse speed • Linguistics: he introduced the idea of « Indo-European languages » • Egyptology: he decyphered the hieroglyphs (before Champollion) • Music: Young temperament
Young-Laplace equation
R
Pext
Pin
γ γ
The mechanical equilibrium of a half-droplet requires
For a more complex interface, the relation is
with R1 & R2 being the principal radii of curvature
What is the pressure in a soap bubble ?
« Amusons nous sur la terre comme sur l'onde, Malheureux celui qui se fait un nom
Richesses, Honneurs, Faux éclat de ce monde Tout n’est que boules de savon. »
Taken from the Nobel lecture of P.-G. de Gennes Rev. Modern Phys. 64 (1992) 645
And in an anti-bubble?
http://www.youtube.com/watch?v=6r_8Pp9WkF0
Laplace equation applies to solid particles as well
Lattice Contraction and Surface Stress of fcc Nanocrystals J. Phys. Chem. B, 2001, 105 (27), pp 6275–6277
What happens now?
A small and a large droplets lie on a fiber wetted by a thin liquid film.
How does the system evolve?
Some menisci configurations
Ostwald ripening
Wilhelm Ostwald 1853-1932
http://iopscience.iop.org/1367-2630/7/1/040/media/movie1_SD.mpg
New Journal of Physics Volume 7 2005 D G A L Aarts et al 2005 New J. Phys. 7 40 doi:10.1088/1367-2630/7/1/040
Interfacial dynamics in demixing systems with ultralow interfacial tension
Minimal surfaces
Costa’s minimal surface (1982)
Minimal surfaces in materials sciences
Micron, Volume 38, July 2007, Pages 478–485
Plateau-Rayleigh instability
1 2
Think about the pressure difference between 1 and 2
Plateau-Rayleigh instabilities in materials science
Appl. Phys. Lett. 85, 5337 (2004)
Nano Lett., 2007, 7 (1), pp 183–187
Cu nanowires PMMA in pores
Joseph Plateau
Joseph Plateau 1801-1883
Doctoral thesis at the University of Liège (1829) Professor of experimental physics in Ghent University (1835)
The phenakistiscope (“phenakizein” means “to deceive”)
Plateau’s laws
John Strutt (1842-1919) 3rd baron Rayleigh
Second Cavendish professor of physics at Cambridge (following Maxwell)
• Dynamic soaring (flying of birds) • Rayleigh scattering (why is the sky blue) • Rayleigh waves (acoustics and mechanics) • Rayleigh-Jeans law (blackbody radiation) • Discovery of Argon with Ramsay (Nobel Prize for physics 1904) • Etc.
What can you tell about the pressure in a liquid from the shape of a rising bubble?
http://people.rit.edu/andpph/exhibit-bubbles.html