activity produced on a body exposed in the presence of a constant amount of emanation are complementary to the curves of decay for a long exposure. The sum of the ordinates of the rise and decay curves is at any time a constant. This follows necessarily from the theory and can also be deduced simply from à priori considerations. (See section 200.)
The curves of rise and decay of the excited activity for both the α and β rays are shown graphically in Fig. 91. The thick line curves are for the α rays. The difference between the shapes of the decay curves when measured by the α or β rays is clearly brought out in the figure. The equations representing the rise of activity to a maximum are given below.
For the β and γ rays,
I_{t}/I_{max} = 1 - (4·3 e^{-λ_{3}t} - 3·3 e^{-λ_{2}t}).
For the α rays,
I_{t}/I_{max} = 1 - (1/2)e^{-λ_{1}t} - (1/2)(4·3 e^{-λ_{3}t} - 3·3 e^{-λ_{2}t}).
226. Effect of temperature. We have so far not considered
the evidence on which the 28-minute rather than the
21-minute change is supposed to take place in the matter C.
This evidence has been supplied by some recent important
experiments of P. Curie and Danne[1] on the volatilization of
the active matter deposited by the emanation. Miss Gates[2]
showed that this active matter was volatilized from a platinum
wire above a red heat and deposited on the surface of a cold
cylinder surrounding the wire. Curie and Danne extended these
results by subjecting an active platinum wire for a short time
to the action of temperatures varying between 15° C. and 1350° C.,
and then examining at room temperatures the decay curves not
only for the active matter remaining on the wire, but also for
the volatilized part. They found that the activity of the distilled
part always increased after removal, passed through a maximum,
and finally decayed according to an exponential law to half value in
28 minutes. At a temperature of about 630° C. the active matter
left behind on the wire decayed at once according to an exponential
