Determination of effective charges of negative ions by reference to the lifetime of positrons

1971 ◽  
Vol 11 (6) ◽  
pp. 1051-1052
Author(s):  
V. I. Gol'danskii ◽  
E. P. Prokop'ev ◽  
A. D. Tsyganov

In a previous paper an account has been given of an investigation of the effect of water vapour on the diffusion coefficients and mobilities of ions in air. It was found that as the concentration of water vapour in the air varied, the values of the diffusion coefficients for positive and negative ions showed rather wide oscillations. These oscillations appeared to be of an irregular character, but a long series of experiments showed that the values of the coefficients found for any vapour pressure could be reproduced with a considerable degree of accuracy. In a subsidiary investigation, it was found that the mean mobilities of the ions varied in the same way with vapour pressure, if the fields to which the ions were exposed were less than about 1.4 volts per centimetre. In stronger fields the oscillations were suppressed, the mobility values plotted against vapour pressure lying on a smooth curve. The method used for the determination of the diffusion coefficients was practically the same as that originally used by Townsend. The chief difference was the employment of only one long and one short tube for the capture of the diffusing ions, instead of the sets of 24 tubes in parallel used in Townsend’s apparatus. The ionization was produced by α -particles from polonium. A rather small volume of air, enclosed and kept at a definite humidity, was passed alternately through the long and the short tube, after exposure to the α -radiation, and the diffusion coefficient was calculated from the ratio of the concentrations of the ions in the issuing air by the use of Townsend’s formula.


The following paper contains an account of a series of experiments on the electrical conductivity of a coal-gas flame, the principal object being to determine the velocities of the negative ions in the flame produced either by the ionisation of salt-vapours or by the ionisation of the flame gases. Two methods have been used, and the results arrived at are concordant. The first method depends on a determination of the ratio between the potential gradient in the flame at some distance from the electrodes and the current flowing through it. This method was used to determine the velocity of the ions of the flame gases.


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