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Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

Practice of Kinetics (Comprehensive Chemical Kinetics, Volume 1)

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6 MISCELLANEOUS PHYSICAL TECHNIQUES 325hydrogenzs1, and atomic chlorine in the photochemical decomposition <strong>of</strong> molecularchlorinezs2.6.3 CALORIMETRYBonhoeffer” fist realised the possibility <strong>of</strong> detecting hydrogen atoms by measurement<strong>of</strong> the heat released when they recombine on a catalytic surface. Theatoms are destroyed, so the applications <strong>of</strong> the technique are to systems where thespecies are generated continuously. All the studies to be described refer to dischargeflowexperiments; even in these cases diffusion effects caused by the recombinationprocess can lead to errors unless the flow velocity is sufficiently great”’. The heat<strong>of</strong> recombination is known accurately, so that if the heat losses may be calculatedor measured, the atom concentration can be determined. A few flow experimentshave been described in which atomic hydrogen is measured by a determination <strong>of</strong>the temperature increase <strong>of</strong> a greater or smaller mass; thermocouples are normallyemployed in this kind <strong>of</strong> study to measure the temperature change. However, foratomic hydrogen, the preferred method <strong>of</strong> study is by the use <strong>of</strong> an isothermal hotwire calorimeter. The method, which was developed by Tollefson and LeRoyZS4for quantitative work, uses what is effectively a resistance thermometer in a current-passingarm <strong>of</strong> a balanced bridge circuit. The recombination <strong>of</strong> atoms on thehot wire would lead to an increase in temperature, so that to keep the bridgebalanced, the electrical power dissipated in the catalytic probe must be reduced.It is apparent that the rate <strong>of</strong> flow, @, <strong>of</strong> atomic hydrogen is given bywhere R is the resistance <strong>of</strong> the probe at the constant temperature, io and i thecurrents required to maintain the temperature without and with the atoms present,AH the heat <strong>of</strong> recombination per mole <strong>of</strong> the atoms and J the mechanical equivalent<strong>of</strong> heat. It is assumed in using the above relation that all the atoms recombineon the probe. At room temperature the recombination’efficiency <strong>of</strong> atomic hydrogenon materials such as platinum is low, but increases with temperaturezs5, andcareful design <strong>of</strong> the apparatus is necessary. Larkin and T h r ~ s h describe ~ ~ ~ an * ~ ~ ~experimental arrangement designed to eliminate uncertainties in the fraction <strong>of</strong>atoms recombining on the probe, and their apparatus is shown in Fig. 12. Two calorimeterswere used, each consisting<strong>of</strong> 50 cm <strong>of</strong> 34 swg rhodium-platinum wire.The calorimeters were mounted in tandem about 3 cm apart, and the second, downstream,calorimeter was used to determine the efficiency <strong>of</strong> the first (which wasalways > 80 %). Kinetic measurements were effected by making the pair <strong>of</strong> calorimetersmoveable up- or down-stream in the flow tube.References pp. 336-342

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