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Title: | Transition State Treatment of the Relative Viscosity of Electrolytic Solutions: Applications to Aqueous, Non-aqueous and Methanol + Water Systems |
Authors: | Feakins, David Freemantle, David J. Lawrence, Kenneth G. |
Keywords: | Chemistry Relative Viscosity Electrolytic Solutions Journal of the Chemical Society : Faraday Transaction - I |
Issue Date: | 1974 |
Publisher: | Journal of the Chemical Society : Faraday Transaction - I. The Chemical Society, London. 1974, 70 (1-6) |
Abstract: | A transition-state treatment of the relative viscosity of electrolyte solutions is described. The following expression is found for the viscosity B-coefficient: B=(V°1–V°2)/1000 +V°1[(Δµ°[graphic omitted]2–Δµ°[graphic omitted]1)/1000 RT]. V°1 and V°2 are the partial molal volumes of the solvent and solute respectively; Δµ°[graphic omitted]1 is the activation energy for viscous flow of the solvent, and Δµ°[graphic omitted]2 the “ionic activation energy” at infinite dilution. For aqueous solutions, at 25°C, the term (V°1–V°2)/1000 accounts completely, in the case of ammonium chloride, and partially in the case of potassium, rubidium and caesium chlorides, for the negative sign of the B-coefficient. When solutions in different solvents are compared, the well-known tendency for B to increase with V°1 is at least partly explained by the form of the above expression; changes in µ°[graphic omitted]2 from water to methanol, for example, are less dramatic than changes in B. B-coefficients in the methanol + water system are consistent with a maximum in solvent structure around 20% methanol (w/w) at 25°C; whilst the µ°[graphic omitted]2-values support this interpretation, it is noted that solvent structure can influence B twice over, in µ°[graphic omitted]2 and (trivially) in µ°[graphic omitted]1. |
URI: | http://dspace.bits-pilani.ac.in:8080/jspui/handle/123456789/17711 |
Appears in Collections: | Journal Articles (before-1995) |
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