History of the inductive sciences, from the earliest to the present timeWhewell, William
History
History of the inductive sciences, from the earliest to the present time
Whewell, William
Science -- History
[Note 72\3: _Paradise Lost_, viii.]
[Note 73\3: A. D. 1252.]
We must endeavor to correct or remove these prejudices, not only in
order that we may do justice to the Hipparchian, or, as it is
usually called, Ptolemaic system of astronomy, and to its founder;
but for another reason, much more important to the purpose of this
work; {152} namely, that we may see how theories may be highly
estimable, though they contain false representations of the real
state of things, and may be extremely useful, though they involve
unnecessary complexity. In the advance of knowledge, the value of
the true part of a theory may much outweigh the accompanying error,
and the use of a rule may be little impaired by its want of
simplicity. The first steps of our progress do not lose their
importance because they are not the last; and the outset of the
journey may require no less vigor and activity than its close.
That which is true in the Hipparchian theory, and which no
succeeding discoveries have deprived of its value, is the
_Resolution_ of the apparent motions of the heavenly bodies into an
assemblage of circular motions. The test of the truth and reality of
this Resolution is, that it leads to the construction of theoretical
Tables of the motions of the luminaries, by which their places are
given at any time, agreeing nearly with their places as actually
observed. The assumption that these circular motions, thus
introduced, are all exactly uniform, is the fundamental principle of
the whole process. This assumption is, it may be said, false; and we
have seen how fantastic some of the arguments were, which were
originally urged in its favor. But _some_ assumption is necessary,
in order that the motions, at different points of a revolution, may
be somehow connected, that is, in order that we may have any theory
of the motions; and no assumption more simple than the one now
mentioned can be selected. The merit of the theory is this;--that
obtaining the amount of the eccentricity, the place of the apogee,
and, it may be, other elements, from _few_ observations, it deduces
from these, results agreeing with _all_ observations, however
numerous and distant. To express an inequality by means of an
epicycle, implies, not only that there is an inequality, but
further,--that the inequality is at its greatest value at a certain
known place,--diminishes in proceeding from that place by a known
law,--continues its diminution for a known portion of the revolution
of the luminary,--then increases again; and so on: that is, the
introduction of the epicycle represents the inequality of motion, as
completely as it can be represented with respect to its _quantity_.
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