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Pile Design and Construction Practice, Fifth edition

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400 Piling for marine structures<br />

(7) Compressive <strong>and</strong> uplift forces induced by overturning movements due to loads 1 to 5 above<br />

(8) In some parts of the world piles may also have to carry vertical <strong>and</strong> lateral loads from<br />

floating ice, <strong>and</strong> loading from earthquakes.<br />

The above forces are not necessarily cumulative. Whereas wind, wave, <strong>and</strong> current forces<br />

can occur simultaneously <strong>and</strong> in the same direction, the forces due to berthing impact <strong>and</strong><br />

mooring rope pull occur in opposite directions. Berthing would not take place at times of<br />

maximum wave height, nor would the thrust from ice sheets coincide with the most severe<br />

wave action. Where containers are stored on the deck slab the possibility of stacking them<br />

in tiers above a nominal permitted height must be considered.<br />

8.1.1 Loading on piles from berthing impact forces<br />

The basic equation used in calculating the force on a jetty or independent berthing structure<br />

due to the impact of a ship as it is brought to rest by the structure is<br />

kinetic energy Ek � msV 2<br />

2g<br />

(8.1)<br />

where m s is the displacement of the ship <strong>and</strong> the mass of water moving with the ship, <strong>and</strong><br />

V is the velocity of approach to the structure.<br />

The whole of the energy as represented by equation 8.1 is not imparted directly to the jetty<br />

piles. Kinetic energy is also absorbed by the deformation of the hull of the ship <strong>and</strong> by the<br />

compression of the fenders <strong>and</strong> of the cushioning between the fenders <strong>and</strong> their supporting<br />

structure. Ships normally approach the jetty at a narrow angle to the berthing line <strong>and</strong> the<br />

kinetic energy in the direction parallel to this line is generally retained in kinetic form but<br />

a part may be lost in overcoming the resistance of the water ahead of the ship’s bows, in friction<br />

against the fenders, <strong>and</strong> in the pull on the mooring ropes if these are used to restrain<br />

longitudinal movement. A full consideration of the complexities involved in calculating the<br />

magnitude <strong>and</strong> direction of berthing forces cannot be dealt with adequately in this book, <strong>and</strong><br />

the reader is referred to Part 4 of the British St<strong>and</strong>ards Code of <strong>Practice</strong> (BS 6349-1: 2000)<br />

for maritime structures (8.1) for guidance on these problems.<br />

On the assumption that the kinetic energy of the ship transverse <strong>and</strong> parallel to the<br />

berthing line has been correctly calculated the problem is then to assess the manner in which<br />

the energy is absorbed by the fenders <strong>and</strong> their supporting piles. Taking the case of a vertical<br />

pile acting as a simple cantilever from the point of virtual fixity below the sea bed, <strong>and</strong><br />

receiving a blow from the ship with a force H applied at a point A (Figure 8.3a), the distance<br />

moved by the point A can then be calculated by the simple method shown in equation 6.20<br />

<strong>and</strong> repeated here for convenience, namely:<br />

distance moved y � H(e � z f) 3<br />

3EI<br />

(8.2)<br />

If the ship is brought to rest by the vertical pile as it moves the pile head over the distance<br />

y, then the work done by the force H over this distance is given by<br />

work done � 1<br />

2 Hy � H 2 (e � zf) 3<br />

6EI<br />

(8.3)

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