Cosmos: A Sketch of the Physical Description of the Universe, Vol. 1Humboldt, Alexander von
History
Cosmos: A Sketch of the Physical Description of the Universe, Vol. 1
Humboldt, Alexander von
Astronomy; Cosmography; Physical geography; Science -- History
[footnote] *Plato, 'Phaedo', p. 97. (Arist., 'Metaph.', p. 985.) compare
Hegel, 'Philosophie der Geschichte', 1840, s. 16.
The delineation of the principal characteristics of telluric phenomena must
begin with the form of our planet and its relations in space. Here too, we
may say that it is not only the mineralogical character of rocks, whether
they are crystalline, granular, or densely fossiliferous, but the
geometrical form of the Earth itself, which indicates the mode of its
origin, and is, in fact, its history. An elliptical spheroid of revolution
gives evidence of having once been a soft or fluid mass. Thus the Earth's
compression constitutes one of the most ancient geognostic events, as every
attentive reader of the book of nature can easily discern; and an analogous
fact is presented in the case of the Moon, the perpetual direction of whose
axes toward the Earth, that is to say, the increased accumulation of matter
on that half of the Moon which is turned toward us, determines the relations
of the periods of rotation and revolution, and is probably contemporaneous
with the earliest epoch in the formative history of this satellite. The
mathematical figure of the Earth is that which it would have were its
surface covered entirely by water in a state of rest; and it is this assumed
form to which all geodesical measurements of degrees refer. This
mathematical surface is different from that true physical surface which is
affected by all the accidents and inequalities of the solid parts.*
[footnote] *Bessel, 'Allgemeine Betrachtungen uber Gradmessungen nach
astronomisch-geodätischen Arbeiten', at the conclusion of Bessel and
Baeyer, 'Gradmessung in Ostpreussen', s. 427. Regarding the accumulation of
matter on the side of the Moon turned toward us (a subject noticed in an
earlier part of the text), see Laplace, 'Expos. du Syst. du Monde', p. 308.
The whole figure of the Earth is determined when we know the amount of the
p 164
compression at the poles and the equatorial diameter; in order, however, to
obtain a perfect representation of its form it is necessary to have
measurements in two directions, perpendicular to one another.
Eleven measurements of degrees (or determinations of the curvature of the
Earth's surface in different parts), of which nine only belong to the
present century, have made us acquainted with the size of our globe, which
Pliny names "a point in the immeasurable universe."*
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