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
11. GLOW BY DISCHARGE. GLOW CHANGED TO SPARK. MOTION OF AIR. CONTINUOUS
DISCHARGE DURING GLOW. The glow was most easily obtained in rarefied
air. The electrodes were of metal rods about .2 of an inch in diameter.
He also obtained a glow in the open air by means of one or both of the
small rods. He noticed some peculiarities of the glow. In the first
place, it occurred in all gases and slightly in oil of turpentine. It
was accompanied by a motion of the gas, either directly from the light
or towards it. He was unable to analyze the glow into visible elementary
intermittent discharges, nor could he obtain any evidence of such an
intermittent action, § 8_a_. No sound was produced even in open air. §
9. He was able to change the brush into a glow by aiding the formation
of a current of air at the extremity of the rod. He also changed the
glow into a brush by a current of air, or by influencing the inductive
action near the glow. The presentation of a sharp point assisted in
sustaining or sometimes even in producing the glow; so also did
rarefaction of the air. The condensation of the air, or the approach of
a large surface tended to change the glow into a brush, and sometimes
into a spark. Greasing the end of the wire caused the glow to change
into a brush.
12. LULLIN’S EXPERIMENT. SPARK. PENETRATING POWER. PASSAGE THROUGH
SOLIDS. _Encyclo. Brit._ Article Electricity. He placed a piece of
cardboard between two electrodes and discovered that a spark penetrated
the material and left a hole with burnt edges. When the electrodes were
not exactly opposite each other, the perforation occurred in the
neighborhood of the negative pole. Later experiments have shown that a
glass plate, 5 or 6 cm. in thickness, can be punctured by the spark of a
large induction coil. The plate should be large enough to prevent the
spark from going around the edges. The spark is inclined, also, to
spread over the surface of the glass instead of piercing it, § 24. Glass
has been cracked by the spark in some experiments.
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