The electron, its isolation and measurement and the determination of some of its properties
John Stuart Mill · en
63.268
10.646}
}
Mean = 63.325
}
63.642
}
63.020
71.664}
6
62.820
71.248}
63.514
52.668}
+
63.312
52.800
7
63.776
52.496
63.300
52.860}
63.156
71.708
6
63.126
Mean = 63.407
}
63.228
42.006}
}
63.294
41.920
8
63.184
42.108}
63.260
53.210}
63.478
52.922
7
-
63.074
53.034
63.306
53.438}
63.414
12.888}
63.450
12.812
19
63.446
12.748
63.556
12.824}
Mean = 63.335
}
Duration of experiment 1 hr. 40 min.
Mean = 6.697
Initial volts = 1723.5
Mean = 6.700
Final volts = 1702.1
Pressure = 53.48 cm.
[Pg 85]
[Pg 86]
Since this is about the limit of the experimental error (the probable
error by least squares is 1 part in 1,500), we may with certainty
conclude that there are no differences of more than this amount between
the values of the positive and negative electrons. This is the
best evidence I am aware of for the exact neutrality of the ordinary
molecules of gases. Such neutrality, if it is actually exact, would
seem to preclude the possibility of explaining gravitation as a result
of electrostatic forces of any kind. The electromagnetic effect of
moving charges might, however, still be called upon for this purpose.
VI. RESISTANCE OF MEDIUM TO MOTION OF DROP THROUGH
IT THE SAME WHEN DROP IS CHARGED AS WHEN
UNCHARGED
A second and equally important conclusion can be drawn from Table VIII.
It will be seen from the column headed “” that during the whole of
the time corresponding to the observations in the third group from the
top the drop carried either 6 or 7 electrons, while, during the last
half of the time corresponding to the observations in the second group
from the top, it carried three times as many, namely, 22 electrons.
Yet the mean times of fall under gravity in the two groups agree to
within about one part in one thousand. The time of fall corresponding
to the heavier charge happens in this case to be the smaller of the
two. We may conclude, therefore, that in these experiments the
resistance which the medium offers to the motion of a body through it
is not sensibly increased when the body becomes electrically charged.
This demonstrates experimentally the exact validity for this work of
the assumption made on p. 70 that the velocity of the drop is strictly
proportional to the force acting upon it, whether it is charged or
uncharged.