Determination of Air Negative Ions Level in Shanghai Coastal Shelter Forests

Author(s):  
Jianfeng Zhang
Keyword(s):  

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.


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

We report a precise experimental determination of the Landau critical velocity v L for roton creation in Hen. The technique used was based on measurements of the drift velocity, v , of negative ions through isotopically pure liquid 4 He at ca . 80 m K , under the influence of weak electric fields, E , for pressures, P , within the range 13 < P < 25 bar. It relied on the use of the equation ( v — v L ) oc E 1/3 , which is believed to correspond to the creation of rotons occurring predominantly in pairs and which fitted the experimental data to very high precision for E > 500 V m -1 . At lower values of E , however, small deviations from this equation were observed. These are tentatively attributed, not to the predicted onset of single-roton emission, but to a novel form of ion-vortex scattering. The values of v L ( P ) deduced from the measurements of v ( E ) at various pressures for E > 500 V m -1 agree to within 1.5% with theoretical predictions based on Landau’s excitation model of HeII, incorporating accepted numerical values of the roton parameters. The observed pressure dependence of v L ( P ) is significantly stronger than that predicted ; however, a discrepancy that appears to point towards the decreasing accuracy with which the roton parameters are known at high pressures. The modulus of the matrix element | V k0,k0 | characterizing roton-pair emission has also been deduced and is found to decrease rapidly with falling pressure. A linear extrapolation of the data suggests that | V k0,k0 | falls to zero at P « 3 bar (1 bar = 10 5 Pa).


In a paper on “The Charges on Positive and Negative Ions in Gases,” Prof. Townsend has described a method for the direct determination of the quantity N e , where N is the number of molecules in a cubic centimetre of a gas at standard pressure and temperature and e the charge on an ion. His experiments were carried out on ions produced by the action of secondary Rontgen rays, and he showed that for negative ions the method led with great accuracy to the value 1.23 x 10 10 for N e , the same as that for NE, where E is the charge on a monovalent ion in a liquid electrolyte. For positive ions the value obtained in the first set of experiments was 2.4 x 10 10 , but subsequently with less penetrating secondary rays it was found to be as low as 1.26 x 10 10 . It would therefore appear that the positive ions have in some cases a single and in others a double atomic charge, whereas the charge on the negative ions is always the same. With a view of testing the theory for ions produced by radium, experiments have been made with an apparatus precisely similar to that used by Prof. Townsend, and the results obtained confirm the reliability of the method. After making due allowance for experimental and other known sources of error the positive ion appears to behave at all pressures and under all forces in accordance with the theory, but in the case of the negative ion some considerable deviations were observed, if the gas is very dry, but these disappear as soon as some water vapour is added.


Sign in / Sign up

Export Citation Format

Share Document