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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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84 EXPERIMENTAL METHODS FOR SLOW REACTIONSamplifier. The detector is relatively temperature-insensitive and therefore ideal forPTGC. However, it is also insensitive to a number <strong>of</strong> substances, notably the inertgases, CO, CO, and formic acid. The sensitivity <strong>of</strong> this detector is such that10-2-10-3 pmole may be estimated with a precision <strong>of</strong> 1 % under optimum conditions.(c) Gas density balance (Fig. 55)Column effluent enters the detector at A and splits at B and B', and leaves atC and C . Pure carrier gas splits at F and F' and also leaves at C and C'. Forbalance there is zero flow across the detector element H. Addition <strong>of</strong> vapour at Achanges the density <strong>of</strong> the gas mixture, causing an unbalance and a flow across H.In commercial instruments, the detector elements are usually matched thermistorsor hot wires which can be incorporated into a Wheatstone bridge network. Thedetector is unique in that it measures an accurately defined property <strong>of</strong> the elutedvapour. The peak area, A,, in the chromatogram, is related to the molecularweights <strong>of</strong> the carrier gas M, and the unknown M, by equation (M'). The carrierA, = M,/M,- M, (M')gas is usually nitrogen, unless x is <strong>of</strong> the same mol. wt. as N,, i.e. CO, C2H, etc.,AJ-310'-1Ic---L-G'C'I LJcTI11-Fig. 55. Schematic view <strong>of</strong> the gas density balance detector. See J. H. P~rnell*'~ p. 271.

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