2006
DOI: 10.1016/j.jcis.2006.03.027
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Kinetics of polyelectrolyte adsorption onto polystyrene latex particle studied using electrophoresis: Effects of molecular weight and ionic strength

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Cited by 48 publications
(45 citation statements)
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“…With respect to polymer molecular weight, the shift in bubble zeta potential to less positive values was surprising as Aoki and Adachi (2006) had observed that the electrophoretic mobility of polystyrene latex particles with adsorbed fully quaternised polyDMAEMA was constant, regardless of the polymer molecular weight. However, the adsorption of polymers onto bubbles may be inhibited not only by steric interferences in the case of high molecular weight polymers, but also by electrostatic repulsion in areas where cationic unimers have adsorbed to form areas of high charge concentration.…”
Section: Bubble Coating With Hydrophobically Functionalised Polymersmentioning
confidence: 99%
“…With respect to polymer molecular weight, the shift in bubble zeta potential to less positive values was surprising as Aoki and Adachi (2006) had observed that the electrophoretic mobility of polystyrene latex particles with adsorbed fully quaternised polyDMAEMA was constant, regardless of the polymer molecular weight. However, the adsorption of polymers onto bubbles may be inhibited not only by steric interferences in the case of high molecular weight polymers, but also by electrostatic repulsion in areas where cationic unimers have adsorbed to form areas of high charge concentration.…”
Section: Bubble Coating With Hydrophobically Functionalised Polymersmentioning
confidence: 99%
“…These rules of the flocculation model are based on some known facts such as: 1) a colloidal suspension is sometimes stabilized by the hydrophilic nature of polymer flocculant which excessively adheres to the particle surface (Fleer and Lyklema, 1974;Napper, 1977;Gregory and Barany, 2011); and 2) appearance of a lump of polymer flocculant leads to a decrease in bridging ability. However, this model does not consider the following phenomena which are encountered in practice: 1) breakage of flocs; 2) changes in flocculation rate due to the growth of the flocs (Higashitani et al, 1978;Tambo and Watanabe, 1984);, 3) changes in flocculation ability due to a combination of physical and chemical properties of particle and polymer; 4) changes in adsorption rate and adsorbed amount of polymer due to change of the flocculant morphology and its concentration (Black et al, 1966;Van de Ven, 1994;Aoki and Adachi, 2006;Gregory and Barany, 2011); and 5) flocculation by polymer flocculant other than bridging mechanism (Gregory, 1973;Gregory and Barany, 2011;Feng et al, 2015). Therefore, this model is restricted to systems where bridging is the predominant mechanism of flocculation.…”
Section: Model Simulation Of Bridging Flocculationmentioning
confidence: 99%
“…The explanation for the aforementioned results is given as follows. Under lower ionic strengths, polymer chains are rigidly adsorbed on the oppositely charged particles while they repel each other with strong electrostatic repulsion among charged segments, making both polymers and particles difficult to move as illustrated in Figure 27 [39][40][41]. In contrast, under the high ionic strength, that is, when polymer-particle electrostatic attraction and polymerpolymer repulsion are screened, adsorbed polyelectrolytes smoothly undergo reconformation and subsequently produced flocs easily rearrange their structures to have increased contact points.…”
Section: Monitoring Rearrangement Of Floc Structuresmentioning
confidence: 99%