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Nonlinear Finite Element Analysis of Concrete Structures

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- 15 -<br />

- the criterion proposed by the writer (1977) . This criterion<br />

corresponds to a smooth and convex surface It will be considered<br />

in more details later and it is implemented in the<br />

finite element program.<br />

- the classical Coulomb criterion with tension cut-<strong>of</strong>fs. This<br />

criterion is also implemented in the finite element program<br />

and an evaluation will be postponed until the previously<br />

mentioned criteria have been compared mutally and together<br />

with some representative experimental results.<br />

As mentioned above we will in the first place disregard the Coulomb<br />

criterion with tension cut-<strong>of</strong>fs. The coefficients involved<br />

in the criteria considered are calibrated by some distinct strength<br />

values, for instance, uniaxial compressive strength a (a > 0),<br />

uniaxial tensile strength a. (a > o), etc. In some proposals<br />

such a calibration was already partly carried out leaving only<br />

a few strength values to be inserted by the user, while others<br />

need more strength values. Noting that all coordinate systems<br />

considered here are normalized by a , the applied strength values<br />

are shown in the following table.<br />

Table 2.1-1: Strength values used to calibrate coefficients in<br />

the failure criteria.<br />

V a c<br />

a ,/a<br />

eb' c<br />

£/ø p /a-<br />

' c c c<br />

Vo c<br />

p fc /a c<br />

Reimann-Janda (1965, 1974)<br />

Willam and Warnke (1974)<br />

Chen and Chen (1975)<br />

Cedolin et al. (1977)<br />

Ottosen (1977)<br />

0.08<br />

0.08<br />

0.08<br />

1.15<br />

1.15<br />

-3.20 2.87<br />

-3.20 1.80<br />

a : uniaxial tensile strength (a > o) , a : uniaxial compressive<br />

strength (a > o), a . : biaxial compressive strength (a . > o) .<br />

The additional strength values applied in the Willam and Warnke<br />

criterion are chosen to fit the experimental data <strong>of</strong> fig. 2.

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