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Pile Design and Construction Practice, Fifth edition

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344 <strong>Pile</strong>s to resist uplift <strong>and</strong> lateral loading<br />

where y c is the deflection corresponding to the strain ‡ c at a stress equal to the maximum<br />

stress resulting from the laboratory stress/strain curve. The strain ‡ c can also be obtained<br />

from the established relationship between c u <strong>and</strong> the deformation modulus E u (see<br />

Section 5.2.2). Matlock (6.17) quotes values of ‡ c of 0.005 for ‘brittle <strong>and</strong> sensitive clays’ <strong>and</strong><br />

0.020 for ‘disturbed or remoulded clays or unconsolidated sediments’. These values of ‡ c<br />

have been based on the established range of E u/c u of 50 to 200 for most clays, <strong>and</strong> they can<br />

be applied to stiff over-consolidated clays, for example the value of E u/c u for stiff London<br />

Clay is 400. Matlock (6.17) recommends an average value of 0.010 for normally consolidated<br />

clays for use in the equation:<br />

y c � 2.5ε cB<br />

(6.39)<br />

The effect of cyclic loading at depths equal to or greater than x r can be allowed for by cutting<br />

off the p–y curve by a horizontal line representing the ultimate resistance p b of the clay under<br />

cyclically applied loads. From the experimental work of Matlock (6.17) , the point of intersection<br />

of this line with the p–y curve (shown in Figure 6.32 as point b) is given by<br />

p b�p u � 0.72<br />

(6.40)<br />

The p–y curves for cyclic loading with values of y/y c from 3 to 15 <strong>and</strong> for depths of less than<br />

x r, at x � 0 are shown in Figure 6.32.<br />

There are little published data on values of p b for various types of clay. The application of<br />

a static horizontal load after a period of cyclic loading, say in a deep-sea structure where a<br />

berthing ship strikes a dolphin after a period of wave loading, produces a more complex<br />

shape in the p–y curve <strong>and</strong> a method of establishing the curve for this loading condition has<br />

been described by Matlock (6.17) .<br />

The shape of a p–y curve for a pile in s<strong>and</strong> as established by Reese et al. is shown in<br />

Figure 6.33. It is in the form of a three-part curve up to the stage of the ultimate failure p u.<br />

p<br />

p u 5Ap c<br />

p m 5Bp c<br />

k<br />

yk5<br />

c<br />

n x<br />

h<br />

m<br />

n<br />

n–1<br />

l<br />

m<br />

Curve defined by<br />

p5Cy 1 n<br />

ym5 B 60<br />

Figure 6.33 Determining shape of p–y curve in s<strong>and</strong> (after Reese et al. (6.10) ).<br />

u<br />

x5x 1<br />

3B<br />

yu 5<br />

8O<br />

Y

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