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Nonlinear Finite Element Analysis of Concrete Structures

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- 72 -<br />

where the B-matrix is given by eq. (7) and evaluated at the centra<br />

<strong>of</strong> the triangle while D and é are given by eqs. (10) and<br />

troid<br />

(11).<br />

4.2.2. Cracking in the concrete element<br />

Suppose now that tensile cracks according to the clacking criteria<br />

<strong>of</strong> section 2.1.4. initiate within the element. The present<br />

section deals with the corresponding modifications in the finite<br />

element approach <strong>of</strong> the concrete triangular axisymmetric element.<br />

Due to rotational symmetry only two types <strong>of</strong> cracks can exist,<br />

namely radial cracks where the crack plane follows a radial<br />

plane and circumferential cracks where the crack plane forms a<br />

rotational symmetric surface. These two types <strong>of</strong> cracks are il-<br />

Circumferential cracks<br />

Fig. 4.2-2: Type <strong>of</strong> cracks in an axisymmetric structure.<br />

lustrated in fig. 2. In addition, combinations <strong>of</strong> these cracks<br />

are possible namely: a radial crack together with a circumferential<br />

crack, two circumferential cracks with different directions<br />

<strong>of</strong> the crack planes and finally these last named two circumferential<br />

cracks together with a radial crack.<br />

When a crack forms then in principle a discontinuous displacement<br />

field results. However, this can be represented only in the<br />

finite element approach either by forcing the cracks to follow<br />

the boundary <strong>of</strong> the elements and then introducing new nodal<br />

points along these boundaries so that separation can occur, or<br />

by allowing the cracks to propagate through the elements and then<br />

define new elements and nodal points so that representation <strong>of</strong>

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