The electron, its isolation and measurement and the determination of some of its propertiesMillikan, Robert Andrews
Philosophy
The electron, its isolation and measurement and the determination of some of its properties
Millikan, Robert Andrews
Electrons
The idea has at various times been put forth in connection with
attempts to explain chemical and cohesive forces from the standpoint
of electrostatic attractions that the positive and negative charges
in a so-called neutral atom may not after all be exactly equal, in
other words, that there is really no such thing as an entirely
[Pg 83]
neutral atom or molecule. As a matter of fact, it is difficult to find
decisive tests of this hypothesis. The present experiments, however,
make possible the following sort of test. I loaded a given drop first
with negative electrons and took ten or twelve observations of rise
and fall, then with the aid of X-rays, by the method indicated in the
last section, I reversed the sign of the charge on the drop and took a
corresponding number of observations of rise and fall, and so continued
observing first the value of the negative electron and then that of
the positive. Table VIII shows a set of such observations taken in air
with a view to subjecting this point to as rigorous a test as possible.
Similar, though not quite so elaborate, observations have been made
in hydrogen with the same result. The table shows in the first column
the sign of the charge; in the second the successive values of the
time of fall under gravity; in the third the successive times of rise
in the field ; in the fourth the number of electrons carried by
the drop for each value of ; and in the fifth the number,
characteristic of this drop, which is proportional to the charge of one
electron. This number is obtained precisely as in the two preceding
tables by finding the greatest common divisor of the successive values
of () and then multiplying this by an arbitrary
constant which has nothing to do with the present experiment and hence
need not concern us here (see chap. V).
It will be seen that though the times of fall and of rise, even when
the same number of electrons is carried by the drop, change a trifle
because of a very slight evaporation and also because of the fall
in the potential of the battery, yet the mean value of the positive
electron, namely, 6.697, agrees with the mean value of the negative
electron, namely, 6.700, to within less than 1 part in 2,000.
[Pg 84]
TABLE VIII
Sign of Drop
Sec.
Sec.
63.050
}
63.186
41.728}
8
63.332
41.590}
-
63.328
62.728
25.740}
62.926
25.798
11
62.900
25.510
63.214
25.806}
}
Mean = 62.976
}
63.538
22.694}
12}
63.244
22.830}
63.114
25.870}
63.242
25.876
11
+
63.362
25.484}
63.136
10.830}
63.226
10.682
63.764
10.756
22
63.280
10.778
63.530
10.672
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