James Clerk Maxwell and Modern PhysicsGlazebrook, Richard
History
James Clerk Maxwell and Modern Physics
Glazebrook, Richard
Maxwell, James Clerk, 1831-1879; Physics -- History
“It is by the use of analogies of this kind that I have
attempted to bring before the mind, in a convenient and
manageable form, those mathematical ideas which are necessary
to the study of the phenomena of electricity. The methods are
generally those suggested by the processes of reasoning which
are found in the researches of Faraday, and which, though they
have been interpreted mathematically by Professor Thomson and
others, are very generally supposed to be of an indefinite and
unmathematical character, when compared with those employed by
the professed mathematicians. By the method which I adopt, I
hope to render it evident that I am not attempting to establish
any physical theory of a science in which I have hardly made
a single experiment, and that the limit of my design is to
show how, by a strict application of the ideas and methods
of Faraday, the connection of the very different orders of
phenomena which he has discovered may be clearly placed before
the mathematical mind. I shall therefore avoid as much as I can
the introduction of anything which does not serve as a direct
illustration of Faraday’s methods, or of the mathematical
deductions which may be made from them. In treating the simpler
parts of the subject I shall use Faraday’s mathematical methods
as well as his ideas. When the complexity of the subject
requires it, I shall use analytical notation, still confining
myself to the development of ideas originated by the same
philosopher.
“I have in the first place to explain and illustrate the idea
of ‘lines of force.’
“When a body is electrified in any manner, a small body
charged with positive electricity, and placed in any given
position, will experience a force urging it in a certain
direction. If the small body be now negatively electrified, it
will be urged by an equal force in a direction exactly opposite.
“The same relations hold between a magnetic body and the north
or south poles of a small magnet. If the north pole is urged
in one direction, the south pole is urged in the opposite
direction.
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