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Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

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3 APPARATUS 51-TlmeFig. 39. Variation <strong>of</strong> radical concentration under quasi-stationary state conditions in the singlepulse-trainmethod. From ref. 133b.<strong>of</strong> the life-time <strong>of</strong> the intermediates. The theory may be developed from here toobtain a value for these life-times'.A very similar technique is that <strong>of</strong> pulsed illumination' 3b, which correspondsvery closely to flash photolysis except that the intensities <strong>of</strong> the flashes are lo-*times those in the latter technique. The method has been used to determine therate coefficients for reactions (14) and (15).Me. +Me. + CZH,Me- + AcMe -, CH, + AcCH,.A block diagram <strong>of</strong> the lamp circuit is shown in Fig. 38. Each pulse produced10-5-10-6 % decomposition. They were fired at the rate <strong>of</strong> 30-40 pulses per second,sufficient to produce a quasi-stationary state. The radical concentration followingeach pulse falls to the same value [R],, prior to the pulse (Fig. 39). A consideration<strong>of</strong> the rate <strong>of</strong> formation <strong>of</strong> CzH6 and CH, leads to an expression from which k,,and k,, may be determined by varying the length <strong>of</strong> the dark period t'. Pairedpulses with a varying t' should lead to direct evidence for the participation <strong>of</strong> hotradical reactions.(b) Vacuum ultra-violetThe 1849A resonance line from the low-pressure mercury lamp has already beenreferred to (p. 41). Suprasil'orsapphire windowsallowthe transmission<strong>of</strong> thisline1I6or alternatively the lamp may be placed inside the RV13,. The intensity <strong>of</strong> thet For a detailed discussion see ref. 133a, p. 1113.References pp. 104-1 I I

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