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Application of the Gibbs Absorption Isotherm to Mixed Films at Air-Water Interfaces PDF

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Preview Application of the Gibbs Absorption Isotherm to Mixed Films at Air-Water Interfaces

FORDHAM UNIVERSITY G raduate School of A rts and Sciences February 1, _ 1950.. This dissertation prepared under my direction by Robert <J« Conan entitled Application of the Gibbs Absorption Isotherm to Mixed Films at Air-Water Interfaces* has been accepted in partial fulfilment of the requirements for the Degree of. Doctor of Philosophy. Eric Hutchinson {Faculty Adviser) application of the gibbs adsorption isotherm to MIXED FILMS AT AIR-WATER INTERFACES by Robert J. Gonan, Jr. B. Sc. Syracuse University, Syracuse, New York M. S. Syracuse University, Syracuse, New York THESIS Submitted in p a rtia l fulfillm ent of the requirements for the degree of Doctor of Philosophy in Chemistry in the Graduate School of Fordham University September, 1949 ProQuest Number: 10992987 All rights reserved INFORMATION TO ALL USERS The quality of this reproduction is dependent upon the quality of the copy submitted. In the unlikely event that the author did not send a complete manuscript and there are missing pages, these will be noted. Also, if material had to be removed, a note will indicate the deletion. uest ProQuest 10992987 Published by ProQuest LLC(2018). Copyright of the Dissertation is held by the Author. All rights reserved. This work is protected against unauthorized copying under Title 17, United States Code Microform Edition © ProQuest LLC. ProQuest LLC. 789 East Eisenhower Parkway P.O. Box 1346 Ann Arbor, Ml 48106- 1346 ACKNOWLEDGMENT The w riter wishes to express his grateful appreciation for the assistance and encouragement given by Dr. E. Hutchinson in the course of th is work. TABLE OF CONTENTS Page Introduction Theory 13 Method 31 M aterials 37 Experimental Results 40 Discussion and Conclusion 108 References 11? I. INTRODUCTION Adsorption may be defined as an accumulation of matter at or near an interface. In the absence of an interface, and a consequent change of force field , adsorption is not known to occur. Adsorption phenomena are recognized at a ll types of interfaces which may be obtained by a combination of the three states of matter taken either in pairs or in m- trip lic a te . In the case of liquid-gas and liq u id -liq u id interfaces, the thermodynamic basis underlying adsorption has been elegantly outlined by G-ibbs (8); which predicts that the surface concentration or surface excess of a given component in a solution is a function of the rate of change of the surface tension with the activ ity of that component, but in­ dependent of the absolute value of the surface tension of the solution. As w ill be demonstrated, later, the ordinary surface tension-concentration curves are easily explained on the basis of th is theory. Three general types of surface ten slon-activity curves are distinguished at. the present time (see Fig. I), In Type I there is a progressive lowering of the surface tension as the concentration of the s.olute is increased. Type II exhibits a progressive and slight rise of surface tension 0 with increasing concentration. Neither present* complications -1 n_int_erpr et a t-io n—f r-om-a-bhe or etic-al—viewpoint-___However.,_ FIGURE" I M O i S N F T e C A F W S COWCF/VTRATiON TYPES OF SURFACE TFNSIOW-CONCENTRATION CORVES 2 the Type III curves, where the surface tension of the solution f ir s t decreases rapidly, passes through a minimum, and then rises again as the concentration of the solute is increased, are at f ir s t sight incompatible with the theory as it is commonly applied. For th is theory, applied to the horizontal portion of the curve at the position of the minimum, would suggest that there is no adsorption at a ll at th is point, That this interpretation is false is obvious from the fact that the surface tension of the solution, at th is concentration is far below the surface tension of the pure solvent. Such a marked lowering of surface tension must imply the presence of matter other than pure solvent in the surface. The object of th is thesis is a quantitative study of a numbbi* of these “Type III curves“ and the application of a thermodynamic interpretation that w ill account for th is unusual behavior. It is the above mentioned contradiction between theory and experimental observation which is to be resolved. A great many examples of Type III surface tension- concentration curves have been obtained by numerous in v esti­ gators using every experimental method known for the measure­ ment of surface tension of solutions. A minimum was firs t noted by Raleigh (33) in aqueous solutions of sodium oleate using the capillary rise method. Later w riters (11) verified his findings, reporting that the Mdip“ had a depth of about 2 dynes/cm. Other examples of this same effect are shown in 3 aqueous solutions of soaps, paraffin chain salts, some dye- stu ffs, many synthetic detergents and even inorganic salts (25) This minimum generally occurs in very d ilute solutions, and has also been observed at oil~water interfaces. Another effect which is frequently noticed with solutions of these compounds is that of surface ageing, ..e. time effects in the establishment of the equilibrium surface tension of solutions. Salts normally exhibiting both of these effects of special in terest here are the sodium alkyl sulfates, such as sodium octyl, decyl, dodecyl sulfates, which have been studied" by a number of authors (6, 19, 32). Numerous attempts have been made to explain these Type III curves. MeBain and Miles (25) made a special study of the surface tension-concentration curve of lauryl sulfonic acid at the air-w ater interface, and found a minimum in the A dOVCPVT1tAT/<*/ ad curve a t A0 .006 molal with an observed depression of about 10 dynes/cm. Calculations made on the basis of the Gibbs Adsorption Theorem indicated no adsorption at the minimum. However, direct measurements by the microtome method (23) showed positive adsorption of the lauryl sulfonic acid over the entire concentration range studied, including that of the minimum. (Other experiments with the microtome on substances showing Type I and II surface tension curves indicated at least qu alitativ e agreement (28) with the values obtained by theoretical calculations), Moreover, the

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