ForsideBøgerA Treatise On The Princip… Of Harbour Engineering

A Treatise On The Principles And Practice Of Harbour Engineering

Forfatter: Brysson Cunningham

År: 1908

Forlag: Charles Griffin & Company

Sted: London

Sider: 410

UDK: Vandbygningssamlingen 134.16

With18 Plates And 220 Illustrations In The Text

Søgning i bogen

Den bedste måde at søge i bogen er ved at downloade PDF'en og søge i den.

Derved får du fremhævet ordene visuelt direkte på billedet af siden.

Download PDF

Digitaliseret bog

Bogens tekst er maskinlæst, så der kan være en del fejl og mangler.

Side af 416 Forrige Næste
BREAKWATER DESIGN. 119 the period of the wave, calling this period P and the length of the wave in feet L,—we have or, fairly approximately, T _ P2?. L” 27’ L=5 P2. The length of the wave in conjunetion with the depth of water détermines the speed of movement of the wave and, conjointly, the velocity of the particles of which it is composed. The relationship existing between these elements will be discussed a little later. Breaking ’ Waves.—We have now to consider the manner in which a wave acts upon any fixed obstacle in its path, whether it be the beach upon which it is spent or an artificial barrier which causes its abrupt collapse. Dealing first with the oscillatory wave, and assuming that it reaches a wall or other obstruction having an abrupt, vertical face, we find that it is reflected in the manner indicated by fig. 99. The particles of water in contact with the wall (A) move up and down <;^ through a height which is twice the height of >^\ b the original wave, as also do the particles in the trough (C) half a wave-length distant. At ____________________________ a point (B) midway between the trough and 'Z^^^^^^g the wall, that is, one quarter of a wave-length_____________________Fio. 99. from either, the particles move horizontally backwards and forwards, while at intermediate points the path of the particles is inclined at varions angles. The whole motion, in fact, is the inverse of that which occurs in the unobstructed wave. When, on the other hand, without meeting with any abrupt obstacle, the wave advances into rapidly shoaling water, its energy is communicated to smaller and successively decreasing masses. Consequently there is a tendency to produce in those masses an agitation of inereasing violence. But this effect is generally diminished, and sometimes entirely counteracted, by the loss of energy due to friction along the bottom, and to surging. On the other hand, the influence of concentration arising from funnel- shaped inlets is clearly to intensify the agitation, and the same effect is producible by submerged rocks with deep narrow gorges between, in passing through which the water is heaped up into masses of considérable volume. When, however, the bottom friction has produced the necessary retarda- tion, the crest of the wave falls forward, as has already been explained, and impact takes place at the precise stage at which the forward motion of the particles has become equal to the velocity of the wave, so that the stroke of the latter is delivered with maximum effect. Taking all these diverse phenomena into considération, it is evident that breaking waves result in the generation of four separate and distinct forces