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Nonlinear Finite Element Analysis of Concrete Structures

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- 97 -<br />

where the same notation as in the previous section is applied<br />

(i.e. the prime (') indicates that reference is made to the<br />

local R'Z'-coordinate system, and index b indicates that reinforcement<br />

bars are considered). Moreover, r* is the global radial<br />

distance <strong>of</strong> the centre <strong>of</strong> the reinforcement element, t is the<br />

thickness and d is the length, cf. fig. 2. In eq. (26) the matrix<br />

1/ is given by eq. (5) while the initial stress vector a'<br />

takes different forms depending on the reinforcement type.<br />

For tangential reinforcement, cf. fig. 1 a), we have<br />

ob<br />

0<br />

or (4.3-27)<br />

where a is given by eq. (3-19). For RZ-reinforcement, cf. fig.<br />

lb), we have<br />

a ob<br />

0<br />

0<br />

(4.3-28)<br />

where a again is given by eq. (3-19). For membrane reinforcement,<br />

cf. fig. 1 c), we have<br />

'ob<br />

'ol<br />

'o2<br />

(4.3-29)<br />

where ø . and a _ are given by eq. (3-12) , i.e. the stress a ,<br />

is directed in the R*-direction while a 2 is the tangential<br />

stress«<br />

Transformation <strong>of</strong> the force vector F' , from the local coordia<br />

o<br />

nate system to the global coordinate System and subsequent transformation<br />

<strong>of</strong> these forces located at the nodal points A, B and C<br />

<strong>of</strong> fig. 2 to the nodes <strong>of</strong> the involved triangular element follow

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