Popular lectures on scientific subjects : $b Second series, with an autobiography of the authorHelmholtz, Hermann von
Science
Popular lectures on scientific subjects : $b Second series, with an autobiography of the author
Helmholtz, Hermann von
Science; Universities and colleges -- Germany
In reference to atoms in molecular physics, Sir W. Thomson says, with
much weight, that their assumption can explain no property of the
body which has not previously been attributed to the atoms. Whilst
assenting to this opinion, I would in no way express myself against
the existence of atoms, but only against the endeavour to deduce the
principles of theoretical physics from purely hypothetical assumptions
as to the atomic structure of bodies. We now know that many of these
hypotheses, which found favour in their day, far overshot the mark.
Mathematical physics has acquired an entirely different character
under the hands of Gauss, of F. E. Neumann and their pupils, among the
Germans; as well as from those mathematicians who in England followed
Faraday’s lead, Stokes, W. Thomson, and Clerk-Maxwell. It is now
understood that mathematical physics is a purely experimental science;
that it has no other principles to follow than those of experimental
physics. In our immediate experience we find bodies variously formed
and constituted; only with such can we make our observations and
experiments. Their actions are made up of the actions which each of
their parts contributes to the sum of the whole; and hence, if we wish
to know the simplest and most general law of the action of masses and
substances found in nature upon one another, and if we wish to divest
these laws of the accidents of form, magnitude, and position of the
bodies concerned, we must go back to the laws of action of the smallest
particles, or, as mathematicians designate it, the elementary volume.
But these are not, like the atoms, disparate and heterogeneous, but
continuous and homogeneous.
The characteristic properties of the elementary volumes of different
bodies are to be found experimentally, either directly, where the
knowledge of the sum is sufficient to discover the constituents, or
hypothetically, where the calculated sum of effects in the greatest
possible number of different cases must be compared with actual fact by
observation and by experiment. It is thus admitted that mathematical
physics only investigates the laws of action of the elements of a body
independently of the accidents of form, in a purely empirical manner,
and is therefore just as much under the control of experience as what
are called experimental physics. In principle they are not at all
different, and the former only continues the function of the latter,
in order to arrive at still simpler and still more general laws of
phenomena.
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