Faraday, Michael, 1791-1867; Physicists -- Great Britain -- Biography
manifest relation to the crystalline structure of bismuth and other
bodies, and therefore to the power by which their molecules are able to
build up the crystalline masses.'
And here follows one of those expressions which characterize the
conceptions of Faraday in regard to force generally:--'It appears to me
impossible to conceive of the results in any other way than by a mutual
reaction of the magnetic force, and the force of the particles of the
crystals upon each other.' He proves that the action of the force,
though thus molecular, is an action at a distance; he shows that a
bismuth crystal can cause a freely suspended magnetic needle to set
parallel to its magne-crystallic axis. Few living men are aware of the
difficulty of obtaining results like this, or of the delicacy necessary
to their attainment. 'But though it thus takes up the character of
a force acting at a distance, still it is due to that power of the
particles which makes them cohere in regular order and gives the mass
its crystalline aggregation, which we call at other times the
attraction of aggregation, and so often speak of as acting at insensible
distances.' Thus he broods over this new force, and looks at it from all
possible points of inspection. Experiment follows experiment, as thought
follows thought. He will not relinquish the subject as long as a hope
exists of throwing more light upon it. He knows full well the anomalous
nature of the conclusion to which his experiments lead him. But
experiment to him is final, and he will not shrink from the conclusion.
'This force,' he says, 'appears to me to be very strange and striking
in its character. It is not polar, for there is no attraction
or repulsion.' And then, as if startled by his own utterance, he
asks--'What is the nature of the mechanical force which turns the
crystal round, and makes it affect a magnet?'... 'I do not remember,' he
continues 'heretofore such a case of force as the present one, where a
body is brought into position only, without attraction or repulsion.'
Plucker, the celebrated geometer already mentioned, who pursued
experimental physics for many years of his life with singular devotion
and success, visited Faraday in those days, and repeated before him
his beautiful experiments on magneto-optic action. Faraday repeated and
verified Plucker's observations, and concluded, what he at first seemed
to doubt, that Plucker's results and magne-crystallic action had the
same origin.
Public-domain text, read in full here on John Shaqi.
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