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
Let us fix our attention on a vertical slice of ice transverse to the
glacier, and to which the pressure is applied perpendicular to its
surfaces. The ice liquefies, and, supposing the means of escape offered
to the compressed water to be equal all round, it is plain that there
will be as great a tendency to squeeze the water upwards as downwards;
for the mere tendency to flow down by its own gravity becomes, in
comparison to the forces here acting on the water, a vanishing quantity.
But the fact is, that the ice above the slice is more permeable than
that below it; for, as we descend a glacier, the ice becomes more
compact. Hence the greater part of the dispersed water will be refrozen
on that side of the slice which is turned towards the origin of the
glacier; and the consequence is, that, according to Mr. Thomson's
principle, the glacier ought to move up hill instead of down.
I would invite Mr. Thomson to imagine himself and me together upon the
ice, desirous of examining this question in a philosophic spirit; and
that we have taken our places beside a stake driven into the ice, and
descending with the glacier. We watch the ice surrounding the stake, and
find that every speck of dirt upon it retains its position; there is no
liquefaction of the ice that bears the dirt, and consequently it rests
on the glacier undisturbed. After twelve hours we find the stake fifteen
inches distant from its first position: I would ask Mr. Thomson how did
it get there? Or let us fix our attention on those six stakes which M.
Agassiz drove into the glacier of the Aar in 1841, and found erect in
1842 at some hundreds of feet from their first position:--how did they
get there? How, in fine, does the end of a glacier become its end? Has
it been liquefied and re-frozen? If not, it must have been _pushed_ down
by the very forces which Mr. Thomson invokes to produce his
liquefaction. Both the liquefaction, as far as it exists, and the
motion, are products of the same cause. In short, this theory, as it
presents itself to my mind, is so powerless to account for the simplest
fact of glacier-motion, that I feel disposed to continue to doubt my own
competence to understand it rather than ascribe to Mr. Thomson an
hypothesis apparently so irrelevant to the facts which it professes to
explain.
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