Waves and ripples in water, air, and æther : $b Being a course of Christmas lectures delivered at the Royal Institution of Great BritainFleming, J. A. (John Ambrose), Sir
Science
Waves and ripples in water, air, and æther : $b Being a course of Christmas lectures delivered at the Royal Institution of Great Britain
Fleming, J. A. (John Ambrose), Sir
Electric waves; Sound; Waves
any kind are therefore: (1) that the medium must elastically resist
some sort of deformation; and (2) when it is deformed at any place, and
returns to its original state, it must overshoot the mark or persist in
movement, in consequence of _inertia_, or something equivalent to it.
Briefly speaking, any material or medium in or on which a true
self-propagating wave-motion can be made must _resist_ and _persist_.
It must have an elastic resistance to some change or deformation, and
it must have an inertia which causes it to persist in movement when
once set in motion. These two qualities, or others equivalent to them,
must invariably be present if we are to have a true wave produced in a
medium.
These things may be best understood by considering, for example, the
production of surface waves on water. Let us ask ourselves, in the
first place, what alteration or change it is that a water-surface
_resists_. The answer is, that, for one thing, it resists being made
unlevel. A still water surface is everywhere a level surface. If we
attempt to make it unlevel by pouring water on to it at one point, or
by heaping it up, the water surface would resist this process. We can
dig a hole in sand, or heap up sand to form a hillock, but we know
full well we cannot do the same thing with water. If, for instance,
some water is placed in a glass tube shaped like the letter ⋃,
then it stands at the same level in both limbs. Again, if water is
set in motion, being a heavy substance, it cannot be brought to rest
instantly. Like every other body, it possesses inertia. Accordingly, if
we do succeed by any means in making a depression in a water-surface
for an instant, the water would immediately press in to fill up the
hole; but more, it would, so to speak, overshoot the mark, and, in
consequence of its inertia, it would create a momentary hump, or
elevation, in the place on the surface where an instant ago there was a
depression.
Public-domain text, read in full here on John Shaqi.
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