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Pile Design and Construction Practice, Fifth edition

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(a) (b)<br />

y y<br />

e<br />

z f<br />

A<br />

The bending moment M on the pile is equal to H(e � z f) therefore<br />

work done � M 2 (e � z f)<br />

6EI<br />

(8.4)<br />

If required the more-rigorous methods described in Sections 6.3.3 <strong>and</strong> 6.3.4 can be used to<br />

calculate the deflection of the pile head <strong>and</strong> hence the work done in bringing the ship to rest.<br />

The bending moment which can be applied to a pile is limited by the allowable working<br />

stress on the extreme fibres of the material forming the pile for normal berthing impacts, or<br />

by the yield stress with abnormal berthing velocities. Thus if the allowable resistance<br />

moment M a is used in equation 8.4 the capacity of the pile to absorb kinetic energy can be<br />

calculated <strong>and</strong> compared to the kinetic energy of the moving ship which must be brought to<br />

rest. If the capacity of the pile is inadequate the blow from the ship must be absorbed by<br />

more than a single pile. In practice, vertical piles are grouped together <strong>and</strong> linked at the head<br />

<strong>and</strong> at some intermediate point (Figure 8.1a) to form a single berthing dolphin, or are spaced<br />

in rows or ‘bents’ in the berthing head of a jetty structure. In the latter case the kinetic energy<br />

of the ship may be absorbed by a large number of piles. In the case of a pile fixed against<br />

rotation by the deck slab of a structure (Figure 8.3b) it was shown in equation 6.21 that<br />

distance y moved point A � H(e � zf) 3<br />

12EI<br />

H<br />

Point of fixity<br />

Piling for marine structures 401<br />

Figure 8.3 Lateral movement of fender piles due to impact force from berthing ship (a) Single<br />

free-headed pile (b) Group of fixed-headed piles.<br />

(8.5)<br />

1<br />

The bending moment caused by a load at the fixed head of a pile is equal to 2H(e � zf) , <strong>and</strong><br />

thus the work done is the same as shown in equation 8.4.<br />

BS 6349 points out that in the case of a piled wharf erected parallel to a sloping shore line,<br />

the piles supporting the rear of the deck, being more deeply embedded than those at the front<br />

will resist a much higher proportion of the horizontal forces imposed on the fendering. It<br />

may be necessary to consider sleeving the rearward piles to equalize the flexural resistance.<br />

A<br />

e<br />

z f<br />

H

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