{"title":"Depletion flocculation of concentrated latex suspensions by surfactant micelles","authors":"M.K. Packman, Th.F. Tadros","doi":"10.1016/0166-6622(92)80304-K","DOIUrl":null,"url":null,"abstract":"<div><p>The influence of addition of a high concentration of non-ionic surfactants on the rheology of a concentrated (volume fraction φ<sub>p</sub> = 0.4) polystyrene latex suspension was investigated. Four different surfactants containing the same hydrophobic group (C<sub>9</sub>H<sub>19</sub>C<sub>6</sub>H<sub>5</sub>(CH<sub>2</sub>CH(CH<sub>3</sub>)O)<sub>13</sub>) and increasingly large hydrophilic chains (poly(ethylene oxide) with 27, 48, 79 and 174 ethylene oxide (EO) units) were used. The rheology was studied using steady-state shear stress (τ)—shear rate (γ) measurements as well as oscillatory measurements. From the τ—γ curves, the extrapolated yield stress τ<sub>β</sub> and plastic viscosity η<sub>pl</sub> were obtained as a function of surfactant concentration. From oscillatory measurements, the complex modulus <em>G</em>*, the storage modulus <em>G</em>′ and loss modulus <em>G</em>″ were obtained as a function of frequency at different surfactant concentrations. All results showed a rapid increase in the rheological parameters with increase of surfactant concentration, once the latter reached a critical concentration. This rapid increase (non-Newtonian flow) was considered to be due to depletion flocculation. The latter was thought to occur at a surfactant concentration in excess of that required for maximum random packing of surfactant micelles, which were assumed to be spherical. A simple calculation (using a value of 0.63 for random packing) predicted the surfactant concentration at the onset of depletion flocculation, using the aggregation number of surfactant molecules in the micelle (obtained from surface-tension or light-scattering measurements).</p><p>The extrapolated yield value was used to calculate the energy of separation <em>E</em><sub>sep</sub> between contact points in a floc. <em>E</em><sub>sep</sub> was compared with the theoretical free energy of depletion attraction <em>G</em><sub>dep</sub> that was calculated using the Asakura and Oosawa theory. Agreement between the calculated <em>G</em><sub>dep</sub> and experimental <em>E</em><sub>sep</sub> values was fair.</p></div>","PeriodicalId":10488,"journal":{"name":"Colloids and Surfaces","volume":"67 ","pages":"Pages 265-272"},"PeriodicalIF":0.0000,"publicationDate":"1992-11-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0166-6622(92)80304-K","citationCount":"7","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Colloids and Surfaces","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/016666229280304K","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 7
Abstract
The influence of addition of a high concentration of non-ionic surfactants on the rheology of a concentrated (volume fraction φp = 0.4) polystyrene latex suspension was investigated. Four different surfactants containing the same hydrophobic group (C9H19C6H5(CH2CH(CH3)O)13) and increasingly large hydrophilic chains (poly(ethylene oxide) with 27, 48, 79 and 174 ethylene oxide (EO) units) were used. The rheology was studied using steady-state shear stress (τ)—shear rate (γ) measurements as well as oscillatory measurements. From the τ—γ curves, the extrapolated yield stress τβ and plastic viscosity ηpl were obtained as a function of surfactant concentration. From oscillatory measurements, the complex modulus G*, the storage modulus G′ and loss modulus G″ were obtained as a function of frequency at different surfactant concentrations. All results showed a rapid increase in the rheological parameters with increase of surfactant concentration, once the latter reached a critical concentration. This rapid increase (non-Newtonian flow) was considered to be due to depletion flocculation. The latter was thought to occur at a surfactant concentration in excess of that required for maximum random packing of surfactant micelles, which were assumed to be spherical. A simple calculation (using a value of 0.63 for random packing) predicted the surfactant concentration at the onset of depletion flocculation, using the aggregation number of surfactant molecules in the micelle (obtained from surface-tension or light-scattering measurements).
The extrapolated yield value was used to calculate the energy of separation Esep between contact points in a floc. Esep was compared with the theoretical free energy of depletion attraction Gdep that was calculated using the Asakura and Oosawa theory. Agreement between the calculated Gdep and experimental Esep values was fair.