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Technical Paper by A. Fakher and C.J.F.P. Jones WHEN THE ...

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FAKHER & JONES • When Bending Stiffness of Geosynthetic Reinforcement is Important<br />

G<br />

E<br />

= ------------------- ( = 1.2 × 10<br />

21 ( + ν)<br />

7 Pa)<br />

(1)<br />

E<br />

K = ---------------------- ( = 4.1 × 10 (2)<br />

31 ( – 2ν)<br />

7 Pa)<br />

The elastic properties of super soft clays are difficult to measure; however, experimental<br />

studies have shown that the elastic modulus of the super soft clay is not significant<br />

in the problem (<strong>Fakher</strong> 1997). Based upon experimental findings the shear<br />

modulus <strong>and</strong> bulk modulus of the super soft clay were assumed equal to 42 <strong>and</strong> 20<br />

MPa, respectively. The shear strength of the super soft clay was assumed to be 50 Pa<br />

for the majority of the analysis, but was increased up to a value of 1,000 Pa to illustrate<br />

the influence of stronger <strong>and</strong> stiffer soil. An elastic-perfectly plastic behaviour was<br />

assumed for the soils in order to simplify the analyses.<br />

2.3 Geosynthetic Reinforcement<br />

The reinforcements were modelled in two ways in order to investigate the effects of<br />

reinforcement bending stiffness on the bearing capacity of the super soft clay:<br />

1. As cable elements, with no bending stiffness. This method is frequently used to<br />

model geosynthetic reinforcements when bending is considered unimportant. The<br />

cable elements used in the analyses were one-dimensional axial elements described<br />

in terms of cross-sectional area, elastic modulus, <strong>and</strong> yield strength of the cable.<br />

2. As beam elements with elastic bending stiffness. The beam elements used in the<br />

analyses were two-dimensional elements with three degrees of freedom at each<br />

node providing displacement in two perpendicular directions <strong>and</strong> rotation. The<br />

beam elements were described in terms of cross-sectional area, elastic modulus,<br />

second moment of area (moment of inertia), <strong>and</strong> plastic moment. The moment<br />

capacity was assumed to be infinite.<br />

The reinforcements were fixed to the line of symmetry (Figure 1). However, they<br />

were not fixed to any other vertical boundary so as not to cause an unrealistic pull-out<br />

resistance. The length of the geosynthetic reinforcement was 2 × 7B, where B is the<br />

width of the footing. In view of the low value of the shear strength of super soft clay, it<br />

was assumed that perfect adherence existed between the clay <strong>and</strong> the reinforcement.<br />

The elastic modulus <strong>and</strong> cross-sectional area of the reinforcement were assumed to<br />

be equal to 1 × 10 5 Pa <strong>and</strong> 0.0033 m 2 , respectively. The second moment of area, I, of<br />

the beam elements was assumed to be equal to 7.64 × 10 -7 m 4 . However, this value was<br />

varied from 1 × 10 - 8 to 2.15 × 10 - 6 m 4 in order to study the effect of bending stiffness,<br />

EI. The bond stiffness <strong>and</strong> the bond strength of the element-soil interface <strong>and</strong> the yield<br />

strength of the cable elements were assumed to be 3 × 10 7 N/m/m, 4.5 × 10 4 N/m, <strong>and</strong><br />

6.8 × 10 3 N, respectively for all the analyses. Details of the material properties used in<br />

the different analyses are shown in Table 1.<br />

448 GEOSYN<strong>THE</strong>TICS INTERNATIONAL • 2001, VOL. 8, NO. 5

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