FREE BOOKS

Author's List




PREV.   NEXT  
|<   144   145   146   147   148   149   150   151   152   153   154   155   156   157   158   159   160   161   162   163   164   165   166   167   168  
169   170   171   172   173   174   175   176   177   178   179   180   181   182   183   184   185   186   187   188   189   190   191   192   193   >>   >|  
er something as to the past history of our Globe. Nothing is, on the other hand, known respecting the origin of uranium or thorium--the parent radioactive bodies. And while not questioning the law 239 and regularity which undoubtedly prevail in the periods of the members of the radioactive families, it appears to me that it is allowable to ask if the change rate of uranium has been always what we now believe it to be. This comes to much the same thing as supposing that atoms possessing a faster change rate once were associated with it which were capable of yielding both helium and lead to the rocks. Such atoms might have been collateral in origin with uranium from some antecedent element. Like helium, lead may be a derivative from more than one sequence of radioactive changes. In the present state of our knowledge the possibilities are many. The rate of change is known to be connected with the range of the alpha ray expelled by the transforming element; and the conformity of the halo with our existing knowledge of the ranges is reason for assuming that, whatever the origin of the more active associate of uranium, this passed through similar elemental changes in the progress of its disintegration. There may, however, have been differences in the ranges which the halo would not reveal. It is remarkable that uranium at the present time is apparently responsible for two alpha rays of very different ranges. If these proceed from different elements, one should be faster in its change rate than the other. Some guidance may yet be forthcoming from the study of the more obscure problems of radioactivity. Now it is not improbable that the halo may contribute directly to this discussion. We can evidently attack 240 the biotite with a known number of alpha rays and determine how many are required to produce a certain intensity of darkening, corresponding to that of a halo with a nucleus of measurable dimensions. On certain assumptions, which are correct within defined limits, we can calculate, as I have done above, the number of rays concerned in forming the halo. In doing so we assume some value for the age of the halo. Let us take the maximum radioactive value. A halo originating in Devonian times may attain a certain central blackening from the effects of, say, rob rays. But now suppose we find that we cannot produce the same degree of blackening with this number of rays applied in the laboratory. What are we to c
PREV.   NEXT  
|<   144   145   146   147   148   149   150   151   152   153   154   155   156   157   158   159   160   161   162   163   164   165   166   167   168  
169   170   171   172   173   174   175   176   177   178   179   180   181   182   183   184   185   186   187   188   189   190   191   192   193   >>   >|  



Top keywords:
uranium
 
radioactive
 
change
 

number

 
origin
 

ranges

 
helium
 
present
 

knowledge

 

element


produce

 
faster
 

blackening

 

improbable

 

contribute

 
radioactivity
 

degree

 

directly

 

attack

 

evidently


problems

 

suppose

 

discussion

 

obscure

 

apparently

 

responsible

 

proceed

 

laboratory

 
applied
 
forthcoming

guidance

 
elements
 

effects

 

forming

 

dimensions

 

nucleus

 

measurable

 

concerned

 

assumptions

 

defined


limits

 
calculate
 

correct

 

assume

 

originating

 
determine
 
Devonian
 

central

 

attain

 
maximum