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Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

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2 CLASSICAL SPECTROSCOPY 29 1emerged. Garton and Broida6’ have made vacuum ultraviolet studies <strong>of</strong> flamesburning in a nitrogen atmosphere, but without definite result.One <strong>of</strong> the first radicals to be investigated by absorption spectroscopy was thehydroxyl radical. Bonhoeffer and Reichardt6’ detected the absorption <strong>of</strong> theA’Z-X’ZI transition <strong>of</strong> OH in water heated to 1600” C. Oldenburg and his collaboratorsmade an exhaustive study <strong>of</strong> the absorption by OH resulting from electricalor thermal dissociation <strong>of</strong> water vapour and hydrogen peroxide. An absolutevalue for the oscillator strength <strong>of</strong> the transition is derived in the paper by Dwyerand OldenburgZ6, and the paper gives references to Oldenburg’s earlier work.Direct calculation <strong>of</strong> extinction coefficients (and hence oscillator strengths) requiresa knowledge <strong>of</strong> both intensity <strong>of</strong> absorption and concentration <strong>of</strong> absorbingspecies. For the transition described above, concentrations <strong>of</strong> OH were calculatedfrom the known fractional dissociation <strong>of</strong> water at elevated temperatures. In a fewother instances, it may be possible to estimate the concentration <strong>of</strong> the intermediatefrom chemical considerations. Thus, Lipscomb et ~ 1.’~ were able to calculate theextinction coefficient at L = 2577 A <strong>of</strong> the radical C10 from flash photolysis studies<strong>of</strong> chlorine dioxide. It was shown that the disappearance <strong>of</strong> C10 obeyed a secondorder rate law, so that---- +-1 1 ktD Do Ewhere D is the optical density (= ~[Clo]) at time t and Do the optical density att = 0. The optical density <strong>of</strong> the reaction mixture was determined by plate photometryat a number <strong>of</strong> delay times, and the value <strong>of</strong> Do obtained by extrapolation<strong>of</strong> the results. The assumption was made that, apart from some C10, (for whichcorrections were applied), there was material balance between ClO and ClO,, andthat [ClO], could be calculated from the amount <strong>of</strong> C102 destroyed. The values<strong>of</strong> Do and [ClO], lead immediately to an estimate <strong>of</strong> E.Extinction coefficients obviously may be determined for suitable absorptions <strong>of</strong>species whose concentration is already known from non-spectroscopic investigations.The results obtained in this way are limited by the accuracy and availability<strong>of</strong> other methods for the estimation <strong>of</strong> the species in question. For many reactionintermediates, direct calculation <strong>of</strong> Concentration is not possible, and until recentlyonly theoretical estimates were available for the oscillator strengths <strong>of</strong> absorptionsinvolving such species.Dalby and Bennett have now calculated oscillator strengths from spontaneousradiative lifetimes <strong>of</strong> several excited species. Excited unstable species are producedby electron bombardment <strong>of</strong> suitable parent molecules. After the electron beam isturned <strong>of</strong>f the intensity <strong>of</strong> radiation decays, and from observations <strong>of</strong> the decayrate the absolute lifetime for the radiative transition may be calculated. The experimentalmethod and theory are given in the first paper6’. Among the oscillatorReferences pp. 336-342

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