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
We see here the vision of the intellect prolonged beyond the boundaries
of sense into the region of what might be considered mere imagination.
But, unlike other imaginations, we can bring ours to the test of
experiment; indeed, so great a mastery have we obtained over these
waves, which eye has not seen, nor ear heard, that we can with
mathematical certainty cause them to coincide or to interfere, to help
each other or to destroy each other, at pleasure. It is perhaps possible
to be a little more precise here. Let two stones--with a small distance
between them--be dropped into water at the same moment; a system of
circular waves will be formed round each stone. Let the distance from
one little crest to the next following one be called _the length of the
wave_, and now let us inquire what will take place at a point equally
distant from the places where the two stones were dropped in. Fixing our
attention upon the ridge of the first wave in each case, it is manifest
that, as the water propagates both systems with the same velocity, the
two foremost ridges will reach the point in question at the same
moment; the ridge of one would therefore coincide with the ridge of the
other, and the water at this point would be lifted to a height greater
than that of either of the previous ridges.
[Sidenote: COINCIDENCE AND INTERFERENCE.]
Again, supposing that by any means we had it in our power to retard one
system of waves so as to cause the first ridge of the one to be exactly
one wave length behind the first ridge of the other, when they arrive at
the point referred to. It is plain that the first ridge of the retarded
system now falls in with the second ridge of the unretarded system, and
we have another case of coincidence. A little reflection will show the
same to be true when one system is retarded any number of _whole
wave-lengths_; the first ridge of the retarded system will always, at
the point referred to, coincide with a _ridge_ of the unretarded system.
Public-domain text, read in full here on John Shaqi.
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