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Micellization of Anionic Sulfonate Gemini Surfactants and Their Interactions With Anionic Polyacrylamide
Author(s) -
Wang Ruijuan,
Yan Haitao,
Hu Wenmin,
Li Yanhong,
Mei Zikun
Publication year - 2018
Publication title -
journal of surfactants and detergents
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.349
H-Index - 48
eISSN - 1558-9293
pISSN - 1097-3958
DOI - 10.1002/jsde.12003
Subject(s) - chemistry , surface tension , critical micelle concentration , pulmonary surfactant , sulfonate , aqueous solution , polyacrylamide , viscosity , micelle , thermodynamics of micellization , rheology , analytical chemistry (journal) , polymer chemistry , chromatography , organic chemistry , sodium , thermodynamics , biochemistry , physics
Anionic sulfonate gemini surfactants 8‐ s ‐8(SO 3 ) 2 and 12‐ s ‐12(SO 3 ) 2 ( s = 3, 6) were synthesized, and their micellization in aqueous solution at 25.0 °C and pH 9 was investigated. The results show that the critical micelle concentrations (CMC) of 8‐ s ‐8(SO 3 ) 2 are more than 2 orders of magnitude larger than those of 12‐ s ‐12(SO 3 ) 2 , but the spacer length has a relatively small impact on the CMC. Moreover, the interactions of n ‐ s ‐ n (SO 3 ) 2 ( n = 8, 12; s = 3, 6) with anionic polyacrylamide (PAM) at 25.0 °C and pH 9 were investigated using surface tensiometry, rheolgy, and scanning electron microscopy (SEM). The results indicate that the surface tension and rheological properties of PAM depend on the concentration of n ‐ s ‐ n (SO 3 ) 2 . Below the critical aggregation concentration of C 1 , surface tension is sharply reduced, the surface tension of n ‐ s ‐ n (SO 3 ) 2 /PAM is lower than n ‐ s ‐ n (SO 3 ) 2 alone, but viscosity is almost unchanged with increasing C n ‐ s ‐ n (SO3)2 . Above C 1 , surface tension reduces very slowly until the saturated concentration of C 2 is reached. Above C 2 , surface tension rapidly reduces until C M is attained, suggesting free n ‐ s ‐ n (SO 3 ) 2 micelles begin to form. In the region of C 1 – C M , the viscosity significantly increases. Above C M , surface tension is basically unchanged and these curves coincide with those of the single surfactant system. Moreover, the viscosity is almost constant. The SEM images indicate that fibrous aggregates are formed below C 1 , then transformed into multilayer fibrous aggregates above C 1 , and further into fiber‐braided‐structured and spider‐web‐structured aggregates above C M . The variation of viscosity is closely associated with the transformation of aggregates.