Scientific American Supplement, No. 711, August 17, 1889Various
History
Scientific American Supplement, No. 711, August 17, 1889
Various
Science -- Periodicals
The ring had been polarized, or retained its magnetic energy, and we
are now taking out one set of lines and putting in reversely polarized
lines of force. This done, we break the reversed current without much
effect of self-induction. The ring remains polarized and inert until
an opposite flow of current be sent through. Iron is then a different
medium from the ether.
The ring once magnetized must, in losing its magnetism, permit a
closure of the lines by shortening. This involves their passage from
the iron across the space in the center of the ring, notwithstanding
its great resistance to the lines of force. As passage from iron to
air is equivalent to lengthening of the lines, it is readily seen that
such lengthening may oppose more effect than a slight shortening due
to leaving iron, for air or space may give in provoking a closure and
disappearance of the lines. Looked at from another standpoint, the
lines on the iron may actually require a small amount of initial
energy to dislodge them therefrom, so that after being dislodged they
may collapse and yield whatever energy they represent.
I must reserve for the future further consideration of the iron ring,
but in thinking upon this matter I am led to think that the production
of a magnetic line in an iron ring around a conductor may represent a
sort of wave of energy, an absorption of energy on the evolution of
the line from the conductor, and a slight giving out of energy on the
line reaching that position of proximity to the iron ring, that its
passage thereto may be said to be a shortening process or a lessening
of its resistance.
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