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Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

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4 SPECTRAL LINE-BROADENING 151This reaction is <strong>of</strong> the second order with rate coefficient k, and it may be shown70that(cf. in the NMR treatment, above), thus k = l/cNzN-. This may be expressed interms <strong>of</strong> the line-width at half height, but it is a much simpler matter experimentallyto measure the difference in field between the points <strong>of</strong> extreme slope (AH, inFig. 17) than the half-height width.Thus k is more simply derived from k = 1.6 x lo7AH&,, where the numerical constant contains the Land6 g-factor, the Bohr mag-neton and Planck’s constant.This is one <strong>of</strong> several reactions <strong>of</strong> this type in which an organic negative radicalionand its parent molecule react in the presence <strong>of</strong> an alkali metal. It is found,rather interestingly, that the rate coefficients depend on the nature <strong>of</strong> the metal.To account for this, it has been postulated that the metal is involved in a bridgingrole in the activated complex, e.g., dipy . . K+ . . dipy- for the case <strong>of</strong> 2,2’-dipyridyl(dipy)”. A more extreme case <strong>of</strong> this association between the radical-ion andthe ion <strong>of</strong> the alkali metal used to form it occurs in the reaction <strong>of</strong> benzophenonewith its negative ion. The spectrum <strong>of</strong> (bemophenone)- in DMB has many hyperhelines caused by the interaction <strong>of</strong> the free electron with the ‘H and, when themetal is sodium, the 23Na nuclei. When benzophenone is added, the structure, dueto the proton interaction, disappears and only the lines associated with the sodiuminteraction remain. To account for this, it has been suggested that the odd electronmoves rapidly over all the proton positions (too fast for the lines characteristic <strong>of</strong>the electron in the different proton environments to be seen), but relatively slowlyfrom one sodium nucleus to another. Seen another way, this means that the transfer<strong>of</strong> an electron from molecule to molecule is associated with the transfer <strong>of</strong> thecation72.Before leaving ESR techniques a couple <strong>of</strong> methods will be mentioned which measurethe rate <strong>of</strong> decay <strong>of</strong> radicals during a matter <strong>of</strong> milliseconds. Normally ESRcannot be used to follow decay rates in this time range because <strong>of</strong> the largeoutput time constants <strong>of</strong> the spectrometer. In what was effectively a combination<strong>of</strong> pulse radiolysis and ESR, ethyl radicals were produced in liquid ethane by pulses<strong>of</strong> electrons and two techniques were used to follow their rate <strong>of</strong> di~appearance~~.The first <strong>of</strong> these was a rotating sector <strong>of</strong> the type which has been used in photosynthesisexperiments (cf. Section 1); the average radical concentration was measureddirectly from the height <strong>of</strong> the recorded ESR signal at a fixed field, correspondingto maximum absorption. The time function was varied by altering the speed <strong>of</strong>rotation <strong>of</strong> the disc. The second technique used sampling. As discussed in Section 1,the signal/noise ratio <strong>of</strong> a signal can be increased by averaging many measurements<strong>of</strong> the same quantity. The intensity <strong>of</strong> maximum absorption was measured manytimes at a fixed time-interval after irradiation and averaged; this procedure wasReferences pp. 176-1 79

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