In the earlier experiments made on this point no such deflection was observed. If the rays are charged with negative electricity they ought to be deflected by an electrified body as well as by a magnet. This experiment was made conclusive by placing the catching vessel out of the path of the rays, and bending them into it by means of a magnet, when the vessel became negatively charged. The next step in the proof that cathode rays are negatively charged particles was to show that when they are caught in a metal vessel they give up to it a charge of negative electricity. When the magnet is placed so that the magnetic force is along the direction in which the particle is moving, the latter will not be affected by the magnet. Thus, if the particles are moving horizontally from east to west, and the magnetic force is horizontal from north to south, the force acting on the negatively electrified particles will be vertical and downwards. We know that such particles, when a magnet is placed near them, are acted upon by a force whose direction is at right angles to the magnetic force, and also at right angles to the direction in which the particles are moving. The arguments in favour of the rays being negatively charged particles are primarily that they are deflected by a magnet in just the same way as moving, negatively electrified particles. Two views were prevalent: one, which was chiefly supported by English physicists, was that the rays are negatively electrified bodies shot off from the cathode with great velocity the other view, which was held by the great majority of German physicists, was that the rays are some kind of ethereal vibration or waves. The green phosphorescence is caused by cathode rays and at one time there was a keen controversy as to the nature of these rays. There is now a well-defined cross in the phosphorescence at the end of the tube the mica cross has thrown a shadow and the shape of the shadow proves that the phosphorescence is due to something travelling from the cathode in straight lines, which is stopped by a thin plate of mica. When the discharge is past, the green phosphorescence no longer extends all over the end of the tube, as it did when the cross was absent. That this is due to something proceeding in straight lines from the cathode-the electrode where the negative electricity enters the tube-can be shown in the following way (the experiment is one made many years ago by Sir William Crookes ): A Maltese cross made of thin mica is placed between the cathode and the walls of the tube. When an electric discharge is sent through a highly exhausted tube, the sides of the tube glow with a vivid green phosphorescence. The first place in which corpuscles were detected was a highly exhausted tube through which an electric discharge was passing. In this lecture I wish to give an account of some investigations which have led to the conclusion that the carriers of negative electricity are bodies, which I have called corpuscles, having a mass very much smaller than that of the atom of any known element, and are of the same character from whatever source the negative electricity may be derived. Nobel Lecture, Decemin Nobel Lectures: Physics, 1901-1921 (Amsterdam: Elsevier, 1967), pp. (See Pais 1986.) But Thomson did carry out this measurement and (later) the measurement of the particles's charge, and he recognized its importance as a constituent of ordinary matter. Thomson was not the only physicist to measure the charge-to-mass ratio of cathode rays in 1897, nor the first to announce his results. The credited discoverer makes crucial contributions to be sure, but often after fundamental observations have been made and tools invented by others. In what sense, then, can Thomson be said to have discovered the electron? After all, he did not invent the vacuum tube or discover cathode rays. Clearly, the characterization of cathode rays was a process begun long before Thomson's work, and several scientists made important contributions. The case of the electron raises several interesting points about the discovery process. He was awarded the Nobel Prize for physics in 1906 for this work, and in 1908 he was knighted. In 1899, he measured the charge of the particles, and speculated on how they were assembled into atoms. In 1897 he reported that "cathode rays" were actually negatively charged particles in motion he argued that the charged particles weighed much less than the lightest atom and were in fact constituents of atoms. For much of his career, Thomson worked on various aspects of the conduction of electricity through gases. Thomson was the Cavendish professor of Experimental Physics at Cambridge University and director of its Cavendish Laboratory from 1884 until 1919. Thomson, 1856-1940 see photo at American Institute of Physics) is widely recognized as the discoverer of the electron.
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