Fragments of Science: A Series of Detached Essays, Addresses, and Reviews. V. 1-2Tyndall, John
Science
Fragments of Science: A Series of Detached Essays, Addresses, and Reviews. V. 1-2
Tyndall, John
Chemistry; Physics; Science
Conversant as you now are with the theory of magnetic fluids, you have
already, I doubt not, anticipated me in imagining the exact condition
of an iron nail under the influence of the magnet. You picture the
iron as possessing the neutral fluid in abundance; you picture the
magnetic pole, when brought near, decomposing the fluid; repelling the
fluid of a like kind with itself, and attracting the unlike fluid;
thus exciting in the parts of the iron nearest to itself the opposite
polarity. But the iron is incapable of becoming a permanent magnet.
It only shows its virtue as long as the magnet acts upon it. What,
then, does the iron lack which the steel possesses? It lacks coercive
force. Its fluids are separated with ease; but, once the separating
cause is removed, they flow together again, and neutrality is
restored. Imagination must be quite nimble in picturing these
changes--able to see the fluids dividing and reuniting, according as
the magnet is brought near or withdrawn. Fixing a definite pole in
your mind, you must picture the precise arrangement of the two fluids
with reference to this pole, and be able to arouse similar pictures in
the minds of your pupils. You will cause them to place magnets and
iron in various positions, and describe the exact magnetic state of
the iron in each particular case. The mere facts of magnetism will
have their interest immensely augmented by an acquaintance with the
principles whereon the facts depend. Still, while you use this theory
of magnetic fluids to track out the phenomena and link them together,
you will not forget to tell your pupils that it is to be regarded as a
symbol merely,--a symbol, moreover, which is incompetent to cover all
the facts, but which does good practical service whilst we are waiting
for the actual truth. [Footnote: This theory breaks down when applied
to diamagnetic bodies which are repelled by magnets. Like soft iron,
such bodies are thrown into a state of temporary excitement, in virtue
of which they are repelled; but any attempt to explain such a
repulsion by the decomposition of a fluid will demonstrate its own
futility.]
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