By K. L. Mittal (Eds.)
content material: Thermodynamics of adsorption and interparticle forces / D.H. Everett and C.J. Radke --
Configurational habit of remoted chain molecules adsorbed from athermal options / M. Lal, M.A. Turpin, K.A. Richardson, and D. Spencer --
Equilibrium movie strain on a flat, low-energy strong / Robert J. strong --
Binding of solute and solvent on the interface and the gibbs floor extra / D.K. Chattoraj and S.P. Moulik --
Mechanism of sulfonate adsorption on the silver iodide-solution interface / okay. Osseo-Asare, D.W. Fuerstenau, and R.H. Ottewill --
Adsorption of dyes on water-swollen and non-swelling good substrates / S.R. Sivaraja Iyer, A.S. Chanekar, and G. Srinivasan --
Adsorption of polystyrene on graphon from toluene / Victor ok. Dunn and Robert D. Vold --
Adsorption of ionic surfactants to porous glass : the exclusion of micelles and different solutes from adsorbed layers and the matter of adsorption maxima / Pasupati Mukerjee and Aroonsri Anavil --
DTA examine of water in porous glass / Chaur-Sun Ling and W. Drost-Hansen --
Monolayer experiences. five, Styrene-acrylic acid movies on aqueous substrates / Erwin Sheppard and Noubar Tcheurekdjian --
interplay of calcium ions with the combined monolayers of stearic acid and stearyl alcohol at pH 8.8 / D.O. Shah --
touch angles in Newton-Black cleaning soap motion pictures drawn from options containing sodium dodecyl sulphate and electrolyte / J.A. De Feijter and A. Vrij --
Stratification in unfastened liquid motion pictures / J.W. Keuskamp and J. Lyklema --
floor chemical homes of hugely fluorinated polymers / Marianne ok. Bernett and W.A. Zisman --
impact of floor oxygen complexes on floor habit of carbons / Balwant Rai Puri --
floor houses of nickel hydroxide ahead of and after dehydration to nickel oxide / M. subject, F.J. Micale, C.L. Cronan, H. Leidheiser, Jr., and A.C. Zettlemoyer --
The size of low interfacial stress through the spinning drop approach / J.L. Cayias, R.S. Schechter, and W.H. Wade --
Adhesion of ice frozen from dilute electrolyte ideas / H.H.G. Jellinek --
Mechanism of olfaction defined utilizing interfacial pressure measurements / D.V. Rathnamma --
function of double interactions and spreading strain in particulate soil removing / Hermann Lange.
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Additional info for Adsorption at Interfaces, Edition: 1ST
22. W. Czanderna, E d . , v. 8, p. 121, Plenum Press, 1971. 23. , (personal communication, 24. , i n "Contact Angle, Wettability and Adhesion," Advan. Chem. , No. 43, pp. , 1964. 1974). ; ACS Symposium Series; American Chemical Society: Washington, DC, 1975. 4 Binding of Solute and Solvent at the Interface and the Gibbs Surface Excess D. K. C H A T T O R A J and S. P. M O U L I K Department of Food Technology and Biochemical Engineering and Department of Chemistry, Jadavpur University, Calcutta-32, India Introduction With the help of an imaginary mathematical plane placed at the interfacial region, a liquid-gas system, according to the Gibbs concept, may be divided into two phases.
C o n f i g u r a t i o n i n v o l v e s m u l t i p l e o c c u p a n c y of any s i t e , go t o 14. 7. C a l c u l a t e Δϋ, the d i f f e r e n c e between the p r e v i o u s and t h e new configuration. 8. I f Δυ 9. Calculate r = 10. Generate a 11. I f r > x, 12. Go 13. Calculate to i s p o s i t i v e or a Z plane such t h a t zero, go to y = x+ constant. energies I f the lattice of the 13. exp(AU/KT). random number go segment i . to ( x ) b e t w e e n 0 and 1. 13. 14. the desired q u a n t i t i e s f o r the new configuration.
For symmetrical ad sorbate molecules, the l a s t term i n the brackets i s omitted. Volume changes are small, i n transfer from l i q u i d to adsorbed state, so we may estimate the enthalpy change as follows: The p a r t i a l molal energy change, i n transfer from the pure l i q u i d to the adsorbed state, i s : AS = - Δϋ « AU V - ÂÏÏ V Here, AU i s the molar energy of vaporization, and AU the p a r t i a l molal energy of adsorption from the vapor. For the purpose of a s t r i c t l y Langmuir-type computation, we assume A U to be constant.