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Nonlinear Finite Element Analysis of Concrete Structures

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- 98 -<br />

exactly the same lines as the transformations <strong>of</strong> the feme vector<br />

F* . caused by temperature stresses and dealt with in the<br />

previous section. Therefore an expression similar to eq. (22)<br />

holds, i.e..<br />

i» _ni '-'T* ^"T —V ~•<br />

or<br />

o<br />

A B C o_r><br />

o<br />

(4.3-30)<br />

where F<br />

is the equivalent nodal force vector due to reinforcement<br />

at the nodes <strong>of</strong> the involved triangular element. The index<br />

r indicates that reinforcement is considered. As given previously<br />

the matrix S<br />

is described by eq. (4.2-4) where the coordinates<br />

<strong>of</strong> point A are applied. The matrices N and IL, are<br />

_ B t.<br />

given similarly. The matrix L is given by eq. (14) and F" ,<br />

by eq. (26). °<br />

To reduce computer time it is convenient to give a closed form<br />

_m _<br />

expression for the term L<br />

trivial matri>. multiplications we obtain:<br />

Tangential reinforcement:<br />

F' . present in eq. (30). After<br />

I T<br />

F'<br />

ø b<br />

. = -irdt cr<br />

o<br />

o<br />

1<br />

0<br />

1<br />

0<br />

0<br />

0<br />

where o is expressed by eq. (3-19).<br />

RZ-reinforcement:<br />

-cosa<br />

-sina<br />

rV T F<br />

51<br />

°o<br />

b = -2iTr*t a<br />

cosa<br />

sina<br />

0<br />

0

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