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
Mr. Oliver B. Shallenberger, (_Mem. Amer. Inst. Elec. Eng._) whose
laboratory is in Rochester, Pa., gave some important general
instructions concerning the Tesla system § 51, that he employed in the
production of remarkably clear sciagraphs, in conjunction with the focus
tube, § 91, representing the hand at page 68, and showing a rat shown at
this § 137. (_Elec. World_, N.Y., March 17, ’96.) Even the ligaments
were clearly shown in the sciagraph of the rat, and some of them are
dimly reproduced by the half tone process. As to the apparatus and
operation, which are especially important, it may be stated that the
current was taken from an alternator, of a frequency of 133 periods per
second, and passed through a primary coil of a transformer for
increasing the E. M. F. from 100 volts to from 16 to 25 thousand. The
secondary current was then passed through Leyden jars and a double
cascade of slightly separated brass cylinders, whereby it was changed
into an oscillatory current of an extremely high frequency, which was
then conducted through the primary of a second induction coil having
very few turns of wire, and no iron core and having a ratio of 7 to 1.
By this means the E. M. F. was raised to somewhere between 160,000 volts
to 250,000, and was used to energize the discharge tube for the
generation of X-rays. Caution should be taken, because the current
coming from the first transformer, being of large quantity and very high
E. M. F. is exceedingly dangerous, but the current of the second
secondary has been passed through one’s body without danger, as reported
by Mr. Tesla several years ago, and confirmed by Mr. Shallenberger.
138. PHOSPHORESCENT SPOT MAINTAINED COOL.—In testing the power of the
X-rays in connection with the appearance of the phosphorescent spot,
Tesla noticed that they were most powerful when the cathode rays caused
the glass to appear as if it were in a fluid state. § 61. To prevent
actual puncture, he maintained the spot cool by means of jets of cold
air. It became possible thereby to use bulbs of thin glass at the
location of the generation of the X-rays. § 119. He concluded from
certain results that not only was glass a better material for discharge
tubes than aluminum, but because, by other tests, he found that thin
aluminum cast more shadow with X-rays than thicker glass. There are, of
course, many other reasons, based on mechanical construction, why glass
is preferable, and also why a tube with an aluminum window is not to be
desired. Principally, the latter will soon leak.
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