The Forms of Water in Clouds and Rivers, Ice and GlaciersTyndall, John
Science
The Forms of Water in Clouds and Rivers, Ice and Glaciers
Tyndall, John
Clouds; Glaciers; Ice; Rivers; Water
269. Dropping down from the village to the bottom of the valley, we
should breast the opposite mountain, and with the great limestone
precipices of the Wetterhorn to our left, we should get upon a path
which commands a view of the glacier. Here we should see beautiful
examples of the opening of crevasses at the summit of a brow, and
their closing at the bottom. But the chief point of interest would
be the crevasses formed at the _side_ of this glacier--the _marginal
crevasses_, as they may be called.
270. We should find the side copiously fissured, even at those places
where the centre is compact; and we should particularly notice that
the fissures would neither run in the direction of the glacier, nor
straight across it, but that they would be _oblique_ to it, enclosing
an angle of about 45 degrees with the sides. Starting from the side
of the glacier the crevasses would be seen to point _upwards_; that
is to say, the ends of the fissures abutting against the bounding
mountain would appear to be _dragged down_. Were you less instructed
than you now are, I might lay a wager that the aspect of these
fissures would cause you to conclude that the centre of the glacier
is left behind by the quicker motion of the sides.
271. This indeed was the conclusion drawn by M. Agassiz from this
very appearance, before he had measured the motion of the sides and
centre of the glacier of the Unteraar. Intimately versed with the
treatment of mechanical problems, Mr. Hopkins immediately deduced
the obliquity of the lateral crevasses from the quicker flow of the
centre. Standing beside the glacier with pencil and note-book in
hand, I would at once make the matter clear to you thus.
[Illustration]
272. Let A C, in the annexed figure, be one side of the glacier, and
B D the other; and let the direction of motion be that indicated
by the arrow. Let S T be a transverse slice of the glacier, taken
straight across it, say to-day. A few days or weeks hence this
slice will have been carried down, and because the centre moves more
quickly than the sides it will not remain straight, but will bend
into the form S' T'.
273. Supposing T _i_ to be a small square of the original slice near
the side of the glacier. In its new position the square will be
distorted to the lozenge-shaped figure T' _i'_. Fix your attention
upon the diagonal T _i_ of the square; in the lowest position this
diagonal, _if the ice could stretch_, would be lengthened to T' _i'_.
But the ice does not stretch; it breaks, and we have a crevasse
formed at right angles to T' _i'_. The mere inspection of the diagram
will assure you that the crevasse will point obliquely _upwards_.
274. Along the whole side of the glacier the quicker movement of the
centre produces a similar state of strain; and the consequence is
that the sides are copiously cut by those oblique crevasses, even at
places where the centre is free from them.
Public-domain text, read in full here on John Shaqi.
Reviews
Reviews
No reviews yet
Be the first to share your thoughts on this work.
Elsewhere in the archive
Join the Discussion
Join the discussion
Sign in to leave a comment or review.
Sign InorCreate an account