The electron, its isolation and measurement and the determination of some of its properties — John Stuart Mill — John Shaqi
The electron, its isolation and measurement and the determination of some of its properties
John Stuart Mill · en
Next consider the apparent variation in when it is
computed from the law of fall. Zerner computes from my law of
fall in the case of the nine drops published by Fletcher, in which
came out as in electrolysis, and finds that one of them yields
, one , one
, one , while
the other five yield about the right value, namely, .
In other words (as stated on p. 165 above), five of these
drops fall exactly on my curve (Fig. 5), one falls somewhat above
it, one somewhat below, while two are entirely off and very much too
low. These two, therefore, I concluded were not oil at all, but dust
particles. Since Zerner computes the radius from the rate of fall,
these two dust particles which fall much too slowly, and therefore
yield too low values of , must, of course, yield correspondingly
low values of . Since they are found to do so, Zerner concludes
that our oil drops, as well as Ehrenhaft’s mercury particles, yield
decreasing values of with decreasing radius. His own tabulation
does not show this. It merely shows three erratic values of ,
two of which are very low and one rather high. But a glance at all
the other data which I have published on oil drops shows the complete
falsity of this position,[119] for these data show that after I had
eliminated dust all of my particles yielded exactly the same value of
“” whatever their size[120]. The only possible interpretation
[Pg 170]
then which could be put on these two particles which yielded correct
values of , but too slow rates of fall, was that which I put upon
them, namely, that they were not spheres of oil.