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Antonello, S.; Gennaro, A.; Maran, F.; Venzo, A. To be published.
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note
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The two limiting values arise by either neglecting or by taking into account in the calculation a different solvation of the halide relative to the corresponding radical. For details, see refs 3 and 4b.
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52
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17344364918
-
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note
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12 In the hypothesis that the double-layer effects of glassy carbon and mercury are similar, we applied the same correction to the results obtained with 4 (the uncorrected E° is -1.13 V). We believe, however, that the error estimated for E°(±0.1 V) takes into account also possible double-layer differences.
-
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53
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17344367412
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note
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3,4b
-
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54
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17344366613
-
-
note
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p(4) > 0.2 V proved to be adequate.
-
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-
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55
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0021458374
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27a Since it is not completely clear how these decays take place (Wagenknecht, J. H.; Goodin, R. D.; Kinlen, P. J.; Woodard, F. E. J. Electrochem. Soc. 1984, 131, 1559), the above radical anions were discarded as candidate electron donors.
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note
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(c) By acting as a proton donor, part of the starting material is transformed into a species that is not reducible at the working potentials. Accordingly, the number of exchanged electrons is less than expected. An increase of v tends to outrun the effect of self-protonation reactions. We are currently investigating the relevance of this reaction and of radical coupling reactions in the overall process.
-
-
-
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67
-
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17344362933
-
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note
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p/∂log v varies form 29.6 mV/log v to 59.1 mV/log v (25 °C, α = 0.5) when the system passes from the former to the latter kinetic control. In the intermediate situation (ca. 6 orders of magnitude in v), a nonlinear peak potential shift connects the two limiting zones.
-
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68
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17344367645
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note
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4 both derivatives being calculated at the midpoint of the explored ΔG° range.
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Interesting improvements of the adiabatic dissociative ET are underway
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