Roentgen Rays and Phenomena of the Anode and Cathode.Thompson, Edward P. (Edward Pruden)
History
Roentgen Rays and Phenomena of the Anode and Cathode.
Thompson, Edward P. (Edward Pruden)
X-rays
139. EXPULSION OF MATERIAL PARTICLES THROUGH THE WALLS OF A DISCHARGE
TUBE.—At quite a low vacuum, and after sealing off the lamp, he attached
its terminal to that of the disruptive coil. After a while, the vacuum
became enormously higher, as indicated by the following steps: First, a
turbid and whitish light existed throughout the bulb. This was the first
principal characteristic. Next, the color changed to red, and the
electrode became very hot, in that case where powerful apparatus was
employed. The precaution should be taken to regulate the E. M. F., to
prevent destruction of the electrode. Gradually, the reddish light
subsided, and white cathode rays, which had begun, grew dimmer and
dimmer until invisible. At the same time, the phosphorescent spot became
brighter and brighter and hotter and hotter, while the electrode cooled,
until the glass adjacent thereto was uncomfortably cold to the touch. At
this stage, the required degree of exhaustion was reached, and yet
without any kind of a pump. He was enabled to hasten the process by
alternate heating and cooling, and by the use of a small electrode. This
whole phenomenon was exhibited with external electrodes as well. He
acknowledged that instead of the disruptive coil, a static machine could
be used, or, in fact, any generator or combination of devices adapted to
produce a very high E. M. F.
The reduction of temperature of the electrode he attributed to its
volatilization. Without actually testing the rays with a fluorescent
screen or photographic plate, he could always know their presence by the
relative temperatures of the phosphorescent spot and the electrode, for
when the latter was at a low temperature and the former at a high
temperature, X-rays were sure to be strong.
Public-domain text, read in full here on John Shaqi.
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