Page:Cathode Rays.pdf/11

Rh {|style="margin: 1em auto 1em auto" Thus, if we know the values of Q, W, and I, we can deduce the values of v and m/e.
 * align="right"|$$\frac{1}{2}\frac{m}{e}v^2$$||$$=\frac{W}{Q}.$$
 * align="right"|$$v$$||$$=\frac{2W}{QI},$$
 * - valign="bottom"
 * align="right"|$$\frac{m}{e}$$||$$=\frac{I^2Q}{2W}.$$
 * }
 * align="right"|$$\frac{m}{e}$$||$$=\frac{I^2Q}{2W}.$$
 * }

To measure these quantities, I have used tubes of three different types. The first I tried is like that represented in fig. 2, except that the plates E and D are absent, and two coaxial cylinders are fastened to the end of the tube. The rays from the cathode C fall on the metal plug B, which is connected with the earth, and serves for the anode; a horizontal slit is cut in this plug. The cathode rays pass through this slit, and then strike against the two coaxial cylinders at the end of the tube; slits are cut in these cylinders, so that the cathode rays pass into the inside of the inner cylinder. The outer cylinder is connected with the earth, the inner cylinder, which is insulated from the outer one, is connected with an electrometer, the deflexion of which measures Q, the quantity of electricity brought into the inner cylinder by the rays. A thermo-electric couple is placed behind the slit in the inner cylinder; this couple is made of very thin strips of iron and copper fastened to very fine iron and copper wires. These wires passed through the cylinders, being insulated from them, and through the glass to the outside of the tube, where they were connected with a low-resistance galvanometer, the deflexion of which gave data for calculating the rise of temperature of the junction produced by the impact against it of the cathode rays. The strips of iron and copper were large enough to ensure that every cathode ray which entered the inner cylinder struck against the junction. In some of the tubes the strips of iron and copper were placed end to end, so that some of the rays struck against the iron, and others against the copper; in others, the strip of one metal was placed in front of the other; no difference, however, could be detected between the results got with those two arrangements. The strips of iron and copper were weighed, and the thermal capacity of the junction calculated. In one set of junctions this capacity was 5x10-3, in another 3x10-3. If we assume that the cathode rays which strike against the junction give their energy up to it, the deflexion of the galvanometer gives us W or ½Nmv2.