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
Before leaving the subject of sea waves there are two or three
interesting matters which must be considered. In the first place,
the breaking of a wave on the shore or on shallow water calls for an
explanation. If we watch a sea wave rolling in towards the beach, we
shall notice that, as it nears the shore, it gets steeper on the shore
side, and gradually curls over until it falls and breaks into spray.
The reason is because, as the wave gets into the shallow water, the top
part of the wave advances more rapidly than the bottom portion. It has
already been explained that the path of the water-particle is a circle,
with its plane vertical and perpendicular to the wave-front or line.
Accordingly, if the wave is moving in shallow water, the friction of
the water against the bottom retards the backward movement at the
lowest position of the water, but no such obstacle exists to the
forward movement of the water at its highest position. An additional
reason for the deformation of the wave on a gently sloping shore may be
found in the fact that the front part of the wave is then in shallower
water, and hence moves more slowly than the rearward portion in deeper
water. From both causes, however, the wave continually gets steeper and
steeper on its landward side until it curls over and tumbles down like
a house which leans too much on one side. The act of curling over in
a breaking wave is a beautiful thing to watch, and one which attracts
the eye of every artist who paints seascapes and storm waves, or of any
lover of Nature who lingers by the shore.
Public-domain text, read in full here on John Shaqi.
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