Matches in SemOpenAlex for { <https://semopenalex.org/work/W1963840949> ?p ?o ?g. }
- W1963840949 endingPage "169" @default.
- W1963840949 startingPage "157" @default.
- W1963840949 abstract "The standard theory of the sedimentation velocity and potential of a concentrated suspension of charged spherical colloidal particles, developed by H. Ohshima on the basis of the Kuwabara cell model (J. Colloid Interf. Sci. 208 (1998) 295), has been numerically solved for the case of non-overlapping double layers and different conditions concerning volume fraction, and ζ-potential of the particles. The Onsager relation between the sedimentation potential and the electrophoretic mobility of spherical colloidal particles in concentrated suspensions, derived by Ohshima for low ζ-potentials, is also analyzed as well as its appropriate range of validity. On the other hand, the above-mentioned Ohshima's theory has also been modified to include the presence of a dynamic Stern layer (DSL) on the particles’ surface. The starting point has been the theory that Mangelsdorf and White (J. Chem. Soc. Faraday Trans. 86 (1990) 2859) developed to calculate the electrophoretic mobility of a colloidal particle, allowing for the lateral motion of ions in the inner region of the double layer (DSL). The role of different Stern layer parameters on the sedimentation velocity and potential are discussed and compared with the case of no Stern layer present. For every volume fraction, the results show that the sedimentation velocity is lower when a Stern layer is present than that of Ohshima's prediction. Likewise, it is worth pointing out that the sedimentation field always decreases when a Stern layer is present, undergoing large changes in magnitude upon varying the different Stern layer parameters. In conclusion, the presence of a DSL causes the sedimentation velocity to increase and the sedimentation potential to decrease, in comparison with the standard case, for every volume fraction. Reasons for these behaviors are given in terms of the decrease in the magnitude of the induced electric dipole moment on the particles, and therefore on the relaxation effect, when a DSL is present. Finally, we have modified Ohshima's model of electrophoresis in concentrated suspensions, to fulfill the requirements of Shilov–Zharkhik's cell model. In doing so, the well-known Onsager reciprocal relation between sedimentation and electrophoresis previously obtained for the dilute case is again recovered but now for concentrated suspensions, being valid for every ζ-potential and volume fraction." @default.
- W1963840949 created "2016-06-24" @default.
- W1963840949 creator A5021399517 @default.
- W1963840949 creator A5024496433 @default.
- W1963840949 creator A5043767639 @default.
- W1963840949 date "2001-12-01" @default.
- W1963840949 modified "2023-10-16" @default.
- W1963840949 title "Sedimentation velocity and potential in a concentrated colloidal suspension" @default.
- W1963840949 cites W1480333395 @default.
- W1963840949 cites W149549641 @default.
- W1963840949 cites W1515073283 @default.
- W1963840949 cites W1555217699 @default.
- W1963840949 cites W1586011584 @default.
- W1963840949 cites W1592180782 @default.
- W1963840949 cites W1951604893 @default.
- W1963840949 cites W1975041550 @default.
- W1963840949 cites W1977750923 @default.
- W1963840949 cites W1980644069 @default.
- W1963840949 cites W1981484450 @default.
- W1963840949 cites W1991497489 @default.
- W1963840949 cites W1995577272 @default.
- W1963840949 cites W2000754396 @default.
- W1963840949 cites W2001930895 @default.
- W1963840949 cites W2010750921 @default.
- W1963840949 cites W2014036111 @default.
- W1963840949 cites W2039866490 @default.
- W1963840949 cites W2042402386 @default.
- W1963840949 cites W2048641594 @default.
- W1963840949 cites W2057919802 @default.
- W1963840949 cites W2063275739 @default.
- W1963840949 cites W2063562656 @default.
- W1963840949 cites W2066095761 @default.
- W1963840949 cites W2066944054 @default.
- W1963840949 cites W2079909901 @default.
- W1963840949 cites W2086800960 @default.
- W1963840949 cites W2101778058 @default.
- W1963840949 cites W2130225212 @default.
- W1963840949 cites W2132241910 @default.
- W1963840949 cites W2138396414 @default.
- W1963840949 cites W2157597506 @default.
- W1963840949 doi "https://doi.org/10.1016/s0927-7757(01)00839-1" @default.
- W1963840949 hasPublicationYear "2001" @default.
- W1963840949 type Work @default.
- W1963840949 sameAs 1963840949 @default.
- W1963840949 citedByCount "40" @default.
- W1963840949 countsByYear W19638409492013 @default.
- W1963840949 countsByYear W19638409492014 @default.
- W1963840949 countsByYear W19638409492015 @default.
- W1963840949 countsByYear W19638409492016 @default.
- W1963840949 countsByYear W19638409492018 @default.
- W1963840949 countsByYear W19638409492019 @default.
- W1963840949 countsByYear W19638409492020 @default.
- W1963840949 countsByYear W19638409492022 @default.
- W1963840949 crossrefType "journal-article" @default.
- W1963840949 hasAuthorship W1963840949A5021399517 @default.
- W1963840949 hasAuthorship W1963840949A5024496433 @default.
- W1963840949 hasAuthorship W1963840949A5043767639 @default.
- W1963840949 hasConcept C105341887 @default.
- W1963840949 hasConcept C111368507 @default.
- W1963840949 hasConcept C121332964 @default.
- W1963840949 hasConcept C127313418 @default.
- W1963840949 hasConcept C147789679 @default.
- W1963840949 hasConcept C151730666 @default.
- W1963840949 hasConcept C159985019 @default.
- W1963840949 hasConcept C171250308 @default.
- W1963840949 hasConcept C185592680 @default.
- W1963840949 hasConcept C192562407 @default.
- W1963840949 hasConcept C202444582 @default.
- W1963840949 hasConcept C2778517922 @default.
- W1963840949 hasConcept C2778913293 @default.
- W1963840949 hasConcept C2779227376 @default.
- W1963840949 hasConcept C2816523 @default.
- W1963840949 hasConcept C29941650 @default.
- W1963840949 hasConcept C33923547 @default.
- W1963840949 hasConcept C57879066 @default.
- W1963840949 hasConcept C5961521 @default.
- W1963840949 hasConcept C59789625 @default.
- W1963840949 hasConcept C65590680 @default.
- W1963840949 hasConceptScore W1963840949C105341887 @default.
- W1963840949 hasConceptScore W1963840949C111368507 @default.
- W1963840949 hasConceptScore W1963840949C121332964 @default.
- W1963840949 hasConceptScore W1963840949C127313418 @default.
- W1963840949 hasConceptScore W1963840949C147789679 @default.
- W1963840949 hasConceptScore W1963840949C151730666 @default.
- W1963840949 hasConceptScore W1963840949C159985019 @default.
- W1963840949 hasConceptScore W1963840949C171250308 @default.
- W1963840949 hasConceptScore W1963840949C185592680 @default.
- W1963840949 hasConceptScore W1963840949C192562407 @default.
- W1963840949 hasConceptScore W1963840949C202444582 @default.
- W1963840949 hasConceptScore W1963840949C2778517922 @default.
- W1963840949 hasConceptScore W1963840949C2778913293 @default.
- W1963840949 hasConceptScore W1963840949C2779227376 @default.
- W1963840949 hasConceptScore W1963840949C2816523 @default.
- W1963840949 hasConceptScore W1963840949C29941650 @default.
- W1963840949 hasConceptScore W1963840949C33923547 @default.
- W1963840949 hasConceptScore W1963840949C57879066 @default.
- W1963840949 hasConceptScore W1963840949C5961521 @default.
- W1963840949 hasConceptScore W1963840949C59789625 @default.