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Nonlinear Finite Element Analysis of Concrete Structures

Nonlinear Finite Element Analysis of Concrete Structures

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- 83 -<br />

the "embedded" concept where reinforcement can be located arbitrarily<br />

within the concrete elements. Assuming consistent displacements<br />

for reinforcement elements and concrete elements the<br />

displacements and thereby the response <strong>of</strong> the reinforcement can<br />

be described by the nodal displacements <strong>of</strong> the concrete element.<br />

The advantage is that reinforcement can be located at will but<br />

assumption <strong>of</strong> perfect bond is inhersnt in the approach. In the<br />

present report this latter consideration for reinforcement is<br />

employed. A quite similar formulation was given by Zienkiewicz<br />

et al. (1972), but the present concept "n its original form and<br />

the corresponding procedures in the finite element program were<br />

given by Tingleff (1969, 1973).<br />

Figure 1 illustrates how the discrete reinforcement bars are<br />

smeared out to equivalent "shells" possessing volumina and stiffness<br />

characteristics identical to those <strong>of</strong> the bars. This means<br />

that all three elements can be treated in the same way except<br />

for their different stiffness characteristics. In general all<br />

three types <strong>of</strong> reinforcement will therefore be referred to as<br />

bars.<br />

In addition to the in-plane forces <strong>of</strong> the bar, transverse forces,<br />

i.e., dowel forces, may develop as a result <strong>of</strong> cracking. Relative<br />

displacements parallel to a crack plane result mainly in local<br />

bending <strong>of</strong> the bar as well as local crushing <strong>of</strong> the concrete in<br />

the vicinity <strong>of</strong> the bar. Such crushing <strong>of</strong> the concrete might be<br />

simulated by suitable link elements which, however, is beyond<br />

the possibilities <strong>of</strong> the present approach. Local bending <strong>of</strong> a bar<br />

could in principle be considered, but this would require knowledge<br />

<strong>of</strong> the displacement fields <strong>of</strong> two subsequent triangular<br />

elements. As a result nodal points are coupled that generally do<br />

not interact. This coupling would in general almost double the<br />

band width <strong>of</strong> the equation system thereby increasing the computer<br />

time inadmissibly, at least for the equation solver used here.<br />

The only possibility to deal with dowel action, therefore, is to<br />

consider the shear stiffness <strong>of</strong> the bar. The corresponding shear<br />

forces that might be present in RZ- and membrane reinforcement<br />

are shown in fig. 1. This approach to consider dowel action is<br />

evaluated in sections 5.1 and 5.3 and it is shown there that

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