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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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2 THE SOLIPGAS INTERFACE 205or an evaporated metal film'28 on the wall <strong>of</strong> the cell. The electrode arrangementused in these experiments is shown diagrammatically in Fig. 13.(e) The contact potentialIf two metals <strong>of</strong> differing work function are connected electrically, at the sametemperature and without a source <strong>of</strong> emf, the electrostatic potentials just outsidethe two surfaces are different. This potential difference V,, is known as the contactpotential difference and is equal to the difference in the work functions <strong>of</strong> the twometals 4, and 4,. If a compensating potential, equal and opposite, is appliedacross the plates, the field becomes zero.The two metals act as the plates <strong>of</strong> a condenser, one <strong>of</strong> the plates being usedfor adsorption <strong>of</strong> the gas and the other being a reference electrode. Adsorption<strong>of</strong> gas causes a change in contact potential equal to the change in work function.Disappearance <strong>of</strong> the electrical field between the two plates may be detected eitherby the steady condenser methodx3' or the vibrating condenser method'3'*'32.A glass adsorption cell used for the static condenser method is shown in Fig. 14.The condenser is formed from two concentric cylinders separated by a 2 mm gap.IFig. 14. Cell for the measurement <strong>of</strong> contact potential difference by the static condenser method.From ref. 130.References pp. 270-278

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