apparatus). In dissolving these chlorides in water and in precipitating a part with
alcohol, the part precipitated is much more active than the part remaining in solution.
Based on this fact, one ought to be able to effect a series of fractionations, securing an
activity nine hundred times greater than that of uranium. We have been stopped by the
lack of material but, from the progress of the work, it is anticipated that the activity
would have increased much more if we had been able to continue. These facts may be
understood in terms of the presence of a radioactive element whose chloride is less
soluble in a water solution of alcohol than that of barium.
3. M. Demarçay has examined the spectrum of our material so obligingly that we
cannot thank him enough. These results of his examination are set forth in a special
note following ours. M. Demarçay has found in the spectrum a line which does not
appear to belong to any known element. This line, hardly visible with the chloride sixty
times more active than uranium, is considerably stronger when the chloride is enriched
by fractionation to nine hundred times that of uranium. The intensity of this line thus
increases at the same time as the radioactivity and this we think is a very weighty
reason for attributing the radioactive part of our substance to it.
The various reasons which we have just enumerated lead us to believe that the new
radioactive substance contains a new element to which we propose to give the name
radium.
We have determined the atomic weight of our active barium by titrating chlorine in the
anhydrous chloride. We have found values which differ very slightly from those
obtained in a parallel manner with inactive barium chloride; however, the values for
the active barium are always a little greater but the difference is of the order of
magnitude of the experimental errors. The new radioactive substance certainly
contains a large proportion of barium, despite the fact that the radioactivity is
considerable. The radioactivity of radium ought therefore to be enormous.
Uranium, thorium, polonium, radium, and their compounds make the air a conductor of
electricity and expose photographic plates. From these two points of view, polonium
and radium are considerably more active than uranium and thorium. On photographic
plates one obtains good images with radium and polonium in a half-minute exposure; it
takes several hours to obtain the same results with uranium or thorium.
The rays emitted by the compounds of polonium and radium make barium
platinocyanide fluorescent. Their action from this point of view is analogous to that of
Roentgen rays, but considerably weaker.[4] To make the experiment, one places on the
active substance a very thin leaf of aluminum, upon which a thin film of barium
platinocyanide is spread; in the dark, the platinocyanide appears weakly luminous in
front of the active substance.
Thus one contructs a source of light, a very weak one to tell the truth, but one that
functions without a source of energy. There is a contradiction, or an apparent one at
the very least, with Carnot's principle.