The Glaciers of the Alps: Being a narrative of excursions and ascents, an account of the origin and phenomena of glaciers and an exposition of the physical principles to which they are relatedTyndall, John
Science
The Glaciers of the Alps: Being a narrative of excursions and ascents, an account of the origin and phenomena of glaciers and an exposition of the physical principles to which they are related
Tyndall, John
Alps -- Description and travel; Glaciers -- Alps
[Sidenote: ICE MOULDED TO CUPS AND RINGS.]
[Illustration: Fig. 33. Moulds used in experiments with ice.]
To make these results more applicable to the bending of glacier-ice, the
following experiments were made:--A block of box-wood, M, Fig. 33, 4
inches long, 3 wide, and 3 deep, had its upper surface slightly curved,
and a groove an inch wide, and about an inch deep, worked into it. A
corresponding plate was prepared, having its under surface part of a
convex cylinder, of the same curvature as the concave surface of the
former piece. When the one slab was placed upon the other, they
presented the appearance represented in section at N. A straight prism
of ice 4 inches long, an inch wide, and a little more than an inch in
depth, was placed in the groove; the upper slab was placed upon it, and
the whole was subjected to the hydraulic press. The prism broke, but,
the quantity of ice being rather more than sufficient to fill the
groove, the pressure soon brought the fragments together and
re-established the continuity of the ice. After a few seconds it was
taken from the mould a bent bar of ice. This bar was afterwards passed
through three other moulds of gradually augmenting curvature, and was
taken from the last of them a _semi-ring_ of compact ice.
The ice, in changing its form from that of one mould to that of another,
was in every instance broken and crushed by the pressure; but suppose
that instead of three moulds three thousand had been used; or, better
still, suppose the curvature of a single mould to change by extremely
slow degrees; the ice would then so gradually change its form that no
rude rupture would be apparent. Practically the ice would behave as a
_plastic_ substance; and indeed this plasticity has been contended for
by M. Agassiz, in opposition to the idea of viscosity. As already
stated, the ice, bruised, and flattened, and bent in the above
experiments, was incapable of being sensibly stretched; it was plastic
to pressure but not to tension.
A quantity of water was always squeezed out of the crushed ice in the
above experiments, and the bruised fragments were intermixed with this
and with air. Minute quantities of both remained in the moulded ice, and
thus rendered it in some degree turbid. Its character, however, as to
continuity may be inferred from the fact that the ice-cup, moulded as
described, held water without the slightest visible leakage.
[Sidenote: SOFTNESS OF ICE DEFINED.]
[Sidenote: PRESSURE AND TENSION.]
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