Page:Radio-activity.djvu/463

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pointed out that a large store of energy would be released by a contraction of the atom.

Sir William Crookes[1], in 1899, proposed the theory that the radio-active elements possess the property of abstracting energy from the gas. If the moving molecules, impinging more swiftly on the substance, were released from the active substance at a much lower velocity, the energy released from the radio-elements might be derived from the atmosphere. This theory was advanced again later on to account for the large heat emission of radium, discovered by P. Curie and Laborde.

F. Re[2] recently advanced a very general theory of matter with a special application to radio-active bodies. He supposes that the parts of the atom were originally free, constituting a nebula of extreme tenuity. These parts have gradually become united round centres of condensation, and have thus formed the atoms of the elements. On this view an atom may be likened to an extinct sun. The radio-active atoms occupy a transitional stage between the original nebula and the more stable chemical atoms, and in the course of their contraction give rise to the heat emission observed.

Lord Kelvin in a paper to the British Association meeting, 1903, has suggested that radium may obtain its energy from external sources. If a piece of white paper is put into one vessel and a piece of black paper into an exactly similar vessel, on exposure of both vessels to the light the vessel containing the black paper is found to be at a higher temperature. He suggests that radium in a similar manner may keep its temperature above the surrounding air by its power of absorption of unknown radiations.

Richarz and Schenck[3] have suggested that radio-activity may be due to the production and breaking up of ozone which is known to be produced by radium salts.


255. Discussion of Theories. From the survey of the general hypotheses advanced as possible explanations of radio-*

  1. Crookes, C. R. 128, p. 176, 1899.
  2. F. Re, C. R. p. 136, p. 1393, 1903.
  3. Richarz and Schenck, Berl. Ber. p. 1102, 1903. Schenck, Berl. Ber. p. 37, 1904.