Ion pairing in solutions of sodium tetraphenylborate |
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Authors: | Silvia Schiavo Raymond M. Fuoss Giancarlo Marrosu |
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Affiliation: | 1. Istituto di Chimica Fisica dell'Univerità di Roma, 00185, Rome, Italy 2. Sterling Chemistry Laboratory, Yale University, 06520, New Haven, Connecticut
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Abstract: | Conductance data are presented for sodium tetraphenylborate (NaBPh4) in three solvent systems: water-dimethyl sulfoxide, water-acetone, and acetone-dimethyl sulfoxide. These and other data from the literature were first analyzed by the three-parameter equation Λ′=Λ0+Aτ2+Bτ3, where $$Lambda prime = [Lambda (obs.) + beta _0 c^{1/2} (1 + 0.5tau ln 2tau )]/[1 - alpha _0 c^{1/2} + (tau ^2 /3) ln 2tau ]$$ Here, β0 is the Onsager electrophoresis coefficient, αoc1/2 the limiting relaxation term, τ=e2κ/2DkT, κ?1 is the Debye-Hückel distance, andA andB are empirical constants. The fact that three parameters are necessary to reproduce the data shows that ion pairing is not negligible for NaBPh4 solutions despite the fact that the conductance curve lies above the limiting tangent even in ethanol (D=24.30). The quantity Λo is the limit of Λ′ at zero concentration; the sum Aτ2+Bτ3 represents the part of the observed conductance from which the pairing constantK Λ and the distance parameterR are derived. Conductance experiments should therefore be designed so that this sum is as large as possible, subject to the restriction that the highest concentration should not exceed 10?7D3 (where the effects of short-range three-ion interactions are no longer negligible). Pairing constants for NaBPh4 in the various solvents range from 4.6 in water to 70 in a mixture of Me2SO and Me2CO with dielectric constantD=23.80. The dependence ofE s (the difference in free energy between solvent-separated pairs and contact pairs) on solvent composition is different for aprotic solvents and for mixtures containing water; for the latter, theE s/kT vs. l/D plot shows a maximum while for the former the curve is monotone descending. The Walden produces (Λoη=limiting conductance times viscosity) plotted againstD ?1 follow the same pattern. |
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