against
or
. We then get
from the intercept of an experimentally determined straight line on the
-axis of our diagram. This whole procedure amounts simply to reducing our drop-velocities to what they would be if the pressure were so large or
against
or
. We then get
from the intercept of an experimentally determined straight line on the
-axis of our diagram. This whole procedure amounts simply to reducing our drop-velocities to what they would be if the pressure were so large or