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
The author performed some experiments (_Elect. Eng._, N.Y., Apr. 15,
’96, p. 379) in relation to candle-power of X-rays by looking into a
sciascope and moving it away until the luminosity just disappeared. He
then detached the black paper cover from the phosphorescent screen and
pointed the sciascope toward a candle flame and receded away until the
fluorescence also disappeared. The distances, with different candles,
would, of course, somewhat vary, but it would in the rough be a constant
quantity, while different discharge tubes would cause the vanishing
fluorescence at different distances. Now, assuming that the X-rays vary
inversely as the square of the distance, as believed by Röntgen, their
power to fluoresce could, therefore, always be named as so much of a
candle-power.
105. SIMPLE DEVICE FOR COMPARING AND LOCATING THE SOURCE AND DIRECTION
OF X-RAYS. PHOSPHORESCENCE NOT ESSENTIAL.—In the ordinary sciascope, the
fluorescent screen is located at one end, and the eyehole at the other.
He modified this construction by employing a long straight tube, made of
thick metal, so that X-rays could not enter through the wall. About at
the centre of the tube was a diaphragm of a fluorescent material. Now,
it is evident that if this is directed toward the phosphorescent spot
and placed very close to the same, and the other end be looked into, the
screen will become fluorescent, if X-rays are emitted from the area
expected. Such a result occurred. With this instrument, he was able to
show, in a similar way, that X-rays did not come from the anode, nor
from the cathode directly. In one case, he provided a piece of platinum
within the discharge tube, in such a position as to be struck by the
cathode rays. § § 91 and 116. The instrument showed that X-rays radiated
from the platinum, although the latter was not luminous nor
phosphorescent,—illustrating again that phosphorescence is not a
necessary accompaniment of X-rays, and assisting in upholding the
principle that as the phosphorescence diminishes by increase of vacuum
and increase of E. M. F., the X-rays increase. It should be noticed that
Prof. Thomson emphasizes that the tube should be made of thick metal.
Public-domain text, read in full here on John Shaqi.
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