{"title":"The effect of surface heterogeneity on pseudo-line tension and the flotation limit of fine particles","authors":"Jaroslaw Drelich, Jan D. Miller","doi":"10.1016/0166-6622(92)80236-U","DOIUrl":null,"url":null,"abstract":"<div><p>The contact angles θ for water at methylated quartz surfaces were measured using the sessile-drop technique to determine the advancing contact angle, and using a captive-bubble technique to examine the effect of bubble size on contact angle. No linearity between cos θ and <span><math><mtext>1</mtext><mtext>r</mtext></math></span> where <em>r</em> is the drop base radius, was observed for these systems as would be expected for an ideal system. In fact the pseudo-line tension decreased with decreasing bubble size. Also, the degree of quartz methylation effected a change in the pseudo-line tension. The pseudo-line tension increased from 0.4·10<sup>−6</sup> N to 3.3·10<sup>−6</sup> N with an increase in the fractional coverage of trimethylsilyl groups from 0.14 to 0.51 for large bubbles (bubble base diameter <em>d</em> > 0.34 mm), whereas the pseudo-line tension decreased from 2.2·10<sup>−7</sup> N to 0.8·10<sup>−7</sup> N with an increase in fractional coverage for small bubbles (bubble base diameter <em>d</em> = 0.06–0.2 mm).</p><p>The flotation limit of fine particles has been re-examined based on the effect of bubble size on contact angle, and a new surface chemistry-limited relationship describing the minimum particle size which can be floated is proposed: <figure><img></figure> where <em>r</em><sub>c</sub> is the critical bubble (drop) radius for which there is no effective attachment between solid surface and dispersed phase, 7<sub>LV</sub> is the interfacial tension at the liquid-vapor interface, Δ<em>p</em> is the density difference between the particle and the liquid and <em>V</em> is the bubble ascent velocity.</p></div>","PeriodicalId":10488,"journal":{"name":"Colloids and Surfaces","volume":"69 1","pages":"Pages 35-43"},"PeriodicalIF":0.0000,"publicationDate":"1992-11-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0166-6622(92)80236-U","citationCount":"52","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Colloids and Surfaces","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/016666229280236U","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 52
Abstract
The contact angles θ for water at methylated quartz surfaces were measured using the sessile-drop technique to determine the advancing contact angle, and using a captive-bubble technique to examine the effect of bubble size on contact angle. No linearity between cos θ and where r is the drop base radius, was observed for these systems as would be expected for an ideal system. In fact the pseudo-line tension decreased with decreasing bubble size. Also, the degree of quartz methylation effected a change in the pseudo-line tension. The pseudo-line tension increased from 0.4·10−6 N to 3.3·10−6 N with an increase in the fractional coverage of trimethylsilyl groups from 0.14 to 0.51 for large bubbles (bubble base diameter d > 0.34 mm), whereas the pseudo-line tension decreased from 2.2·10−7 N to 0.8·10−7 N with an increase in fractional coverage for small bubbles (bubble base diameter d = 0.06–0.2 mm).
The flotation limit of fine particles has been re-examined based on the effect of bubble size on contact angle, and a new surface chemistry-limited relationship describing the minimum particle size which can be floated is proposed: where rc is the critical bubble (drop) radius for which there is no effective attachment between solid surface and dispersed phase, 7LV is the interfacial tension at the liquid-vapor interface, Δp is the density difference between the particle and the liquid and V is the bubble ascent velocity.