curves of the emanation are determined by exactly the same conditions as the decay and recovery curves of Ur X and Th X. In both cases there is:
(1) A supply of fresh radio-active particles produced at a
constant rate.
(2) A loss of activity of the particles following an exponential law with the time.
In the case of Ur X and Th X, the active matter produced
manifests its activity in the position in which it is formed; in this
new phenomenon, a proportion of the active matter in the form of
the emanation escapes into the surrounding gas. The activity of
the emanation, due to a thorium compound kept in a closed vessel,
thus reaches a maximum when the rate of supply of fresh emanation
particles from the compound is balanced by the rate of change
of those already present. The time for recovery of half the final
activity is about 1 minute, the same as the time taken for the
emanation, when left to itself, to lose half its activity.
If q_{0} is the number of emanation particles escaping into the gas per second, and N_{0} the final number when radio-active equilibrium is reached, then (section 133),
q_{0} = λN_{0}.
Since the activity of the emanation falls to half value in 1 minute
λ = 1/87,
and N_{0} = 87q_{0}, or the number of emanation particles present when a steady state is reached is 87 times the number produced per second. Radium Emanation.
144. Discovery of the emanation. Shortly after the
discovery of the thorium emanation, Dorn[1] repeated the results,
and, in addition, showed that radium compounds also gave off
radio-active emanations, and that the amount given off was much
increased by heating the compound. The radium emanation differs
from the thorium emanation in the rate at which it loses its
activity. It decays far more slowly, but in other respects the
emanations of thorium and radium have much the same properties.
Both emanations ionize the gas with which they are mixed, and
- ↑ Dorn, Abh. der. Naturforsch. Ges. für Halle-a-S., 1900.
