Nonlinear Finite Element Analysis of Concrete Structures
Nonlinear Finite Element Analysis of Concrete Structures
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