396 Conduction in Solutions and Gases, The alternative to the molecular-torrent theory is to suppose that the cathode radiation is a disturbance of the aether. This view was maintained by several physicists,[1] and notably by Hertz,[2] who rejected Varley's hypothesis when he found experimentally that the rays did not appear to produce any external electric or magnetic force, and were apparently not affected by an electrostatic field. It was, however, pointed out by FitzGerald[3] that external space is probably screened from the effects of the rays by other electric actions which take place in the discharge tube.
It was further urged against the charged-particle theory that cathode rays are capable of passing through films of metal which are so thick as to be quite opaque to ordinary light;[4] it seemed inconceivable that particles of matter should not be stopped by even the thinnest gold-leaf. At the time of Hertz's experiments on the subject, an attempt to obviate this difficulty was made by J.-J. Thomson,[5] who suggested that the metallic film when bombarded by the rays might itself acquire the property of emitting charged particles, so that the rays which were observed on the further side need not have passed through the film. It was Thomson who ultimately found the true explanation; but this depended in part on another order of ideas, whose introduction and development must now be traced.
The tendency, which was now general, to abandon the electron-theory of Weber in favour of Maxwell's theory involved certain changes in the conceptions of electric charge.
- ↑ E.g. E. Wiedemann, Ann. d. Phys. x (1880), p. 202: translated, Phil. Mag. x (1880), p. 357. E. Goldstein, Ann. d. Phys. xii (1881), p. 249.
- ↑ Ann. d. Phys. xix (1883), p. 782.
- ↑ Nature, November 5, 1896; Fitz Gerald's Scientific Writings, p. 433.
- ↑ The penetrating power of the rays had been noticed by Hittorf, and by E. Wiedemann and Ebert, Sitzber, d. phys.-med. Soc. zu Erlangen, 11th December, 1891. It was investigated more thoroughly by Hertz, Ann. d. Phys. xlv (1892), p. 28, and by Philipp Lenard, of Bonn, Ann. d. Phys. li (1894), p. 225; lii (1894), p. 23, who conducted a series of experiments on cathode rays which had passed out of the discharge tube through a thin window of aluminium.
- ↑ J.J. Thomson, Recent Researches, p. 126.
