FREE BOOKS

Author's List




PREV.   NEXT  
|<   51   52   53   54   55   56   57   58   59   60   61   62   63   64   65   66   67   68   69   70   71   72   73   74   75  
76   77   78   79   80   81   82   83   84   85   86   87   88   89   90   91   92   93   94   95   96   97   98   99   100   >>   >|  
. The preceding tables show that the negative ions diffuse more rapidly than the positive, especially in dry gases. The superior mobility of the negative ions was observed first by Zeleny (_Phil. Mag._, 1898 [5], 46, p. 120), who showed that the velocity of the negative ions under an electric force is greater than that of the positive. It will be noticed that the difference between the mobility of the negative and the positive ions is much more pronounced in dry gases than in moist. The difference in the rates of diffusion of the positive and negative ions is the reason why ionized gas, in which, to begin with, the positive and negative charges were of equal amounts, sometimes becomes electrified even although the gas is not acted upon by electric forces. Thus, for example, if such gas be blown through narrow tubes, it will be positively electrified when it comes out, for since the negative ions diffuse more rapidly than the positive, the gas in its passage through the tubes will lose by diffusion more negative than positive ions and hence will emerge positively electrified. Zeleny snowed that this effect does not occur when, as in carbonic acid gas, the positive and negative ions diffuse at the same rates. Townsend (loc. cit.) showed that the coefficient of diffusion of the ions is the same whether the ionization is produced by Rontgen rays, radioactive substances, ultra-violet light, or electric sparks. The ions produced by chemical reactions and in flames are much less mobile; thus, for example, Bloch (_Ann. chim. phys._, 1905 [8], 4, p. 25) found that for the ions produced by drawing air over phosphorus the value of [alpha]/e was between 1 and 6 instead of over 3000, the value when the air was ionized by Rontgen rays. _Velocity of Ions in an Electric Field._--The velocity of ions in an electric field, which is of fundamental importance in conduction, is very closely related to the coefficient of diffusion. Measurements of this velocity for ions produced by Rontgen rays have been made by Rutherford (_Phil. Mag._ [5], 44, p. 422), Zeleny (_Phil. Mag._ [5], 46, p. 120), Langevin (_Ann. Chim. Phys._, 1903, 28, p. 289), Phillips (_Proc. Roy. Soc._ 78, A, p. 167), and Wellisch (_Phil. Trans._, 1909, 209, p. 249). The ions produced by radioactive substance have been investigated by Rutherford (_Phil. Mag._ [5], 47, p. 109) and by Franck and Pohl (_Verh. deutsch. phys.
PREV.   NEXT  
|<   51   52   53   54   55   56   57   58   59   60   61   62   63   64   65   66   67   68   69   70   71   72   73   74   75  
76   77   78   79   80   81   82   83   84   85   86   87   88   89   90   91   92   93   94   95   96   97   98   99   100   >>   >|  



Top keywords:

negative

 

positive

 

produced

 
diffusion
 
electric
 

Rontgen

 

diffuse

 
velocity
 

electrified

 

Zeleny


coefficient

 

ionized

 

difference

 
mobility
 

positively

 

radioactive

 

showed

 
Rutherford
 

rapidly

 
mobile

Velocity

 
Electric
 

drawing

 

fundamental

 
phosphorus
 

Phillips

 

Wellisch

 

substance

 

deutsch

 

Franck


investigated

 

Measurements

 

related

 

closely

 
conduction
 

Langevin

 
importance
 
snowed
 
amounts
 

charges


forces

 

reason

 

superior

 
observed
 

preceding

 

tables

 

noticed

 
pronounced
 

greater

 
ionization