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138 Antonio J. Gil<br />

Total Potential Energy<br />

1<br />

0<br />

−1<br />

−2<br />

−3<br />

x 104<br />

2<br />

−4<br />

1 2 3 4 5 6<br />

Iterations<br />

Infinite Norm on Residual Forces<br />

10 2<br />

10 0<br />

10 −2<br />

10 −4<br />

10 −6<br />

10 −8<br />

10 −10<br />

10<br />

1 2 3 4 5 6<br />

−12<br />

Iterations<br />

Fig. 11. Numerical example: Convergence curves.<br />

Fig. 12. Numerical example: Displacements OX & OZ.<br />

Levy & Spillers Present work<br />

Node u v w u v w<br />

1 0.015 -0.015 -1.431 0.014 -0.014 -1.423<br />

2 0.000 -0.017 -2.605 0.000 -0.017 -2.600<br />

5 0.000 0.000 -6.642 0.000 0.000 -6.626<br />

Table 2. Numerical example: Displacements (in).<br />

6Concluding Remarks<br />

This chapter has offered a complete consistent numerical formulation for the structural<br />

analysis of prestressed hyperelastic Saint Venant-Kirchoff membranes. Two<br />

structural loading steps can be considered successively: in the first, the prestressing<br />

loads are transferred to the structure whereas in the second, in service loads such<br />

as live loads or wind load arise. By taking into account this approach, an initial

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