The Student's Elements of GeologyLyell, Charles, Sir
Science
The Student's Elements of Geology
Lyell, Charles, Sir
Geology
Folding by Lateral Movement.—An experiment was made by Sir James Hall,
with a view of illustrating the manner in which such strata, assuming
them to have been originally horizontal, may have been forced into
their present position. A set of layers of clay were placed under a
weight, and their opposite ends pressed towards each other with such
force as to cause them to approach more nearly together. On the removal
of the weight, the layers of clay were found to be curved and folded,
so as to bear a miniature resemblance to the strata in the cliffs. We
must, however, bear in mind that in the natural section or sea-cliff we
only see the foldings imperfectly, one part being invisible beneath the
sea, and the other, or upper portion, being supposed to have been
carried away by _denudation_, or that action of water which will be
explained in the next chapter. The dark lines in the plan (Fig. 57)
represent what is actually seen of the strata in the line of cliff
alluded to; the fainter lines, that portion which is concealed beneath
the sea-level, as also that which is supposed to have once existed
above the present surface.
Fig. 56: Curved strata of slate near St. Abb’s Head, Berwickshire.
Fig. 57
We may still more easily illustrate the effects which a lateral thrust
might produce on flexible strata, by placing several pieces of
differently coloured cloths upon a table, and when they are spread out
horizontally, cover them with a book. Then apply other books to each
end, and force them towards each other. The folding of the cloths (see
Fig. 58) will imitate those of the bent strata; the incumbent book
being slightly lifted up, and no longer touching the two volumes on
which it rested before, because it is supported by the tops of the
anticlinal ridges formed by the curved cloths. In like manner there can
be no doubt that the squeezed strata, although laterally condensed and
more closely packed, are yet elongated and made to rise upward, in a
direction perpendicular to the pressure.
Fig. 58
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