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Nonlinear Finite Element Analysis of Concrete Structures

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- 86 -<br />

at point A, B and C are given by<br />

U A<br />

V A<br />

a b<br />

U B<br />

V B<br />

(4.3-1)<br />

u c<br />

where index b in general indicates that a reinforcement bar is<br />

considered. The points A, B and C are the nodal points <strong>of</strong> the<br />

reinforcement element and the vector eL" contains therefore the<br />

nodal displacements. In accordance with the triangular element<br />

concept, we work with a linear displacement field i.e.<br />

u' = a, + a 2 r' + a- z'<br />

V<br />

= a 4 + a 5 r' + a g z'<br />

To determine the constants a, a 6 the displacement values<br />

at point A(r' = z' -= 0), B(r' = d, z' = 0) and C(r' = 0, z' = d) ,<br />

i.e., the nodal points, are applied. I-- follows that<br />

u' =<br />

V =<br />

U A +<br />

V Å +<br />

* < U B<br />

* < V B<br />

u^)r' + ^(uv£)r'<br />

+ Js(v^<br />

u A )z'<br />

"A>« 1 (4.3-2)<br />

The corresponding reinforcement strains <strong>of</strong> interest are<br />

£ R<br />

3u'<br />

e ' =<br />

u<br />

—(u'cosa - v'sino)<br />

(4.3-3)<br />

RZ<br />

3u' . 3v'<br />

3z' 3r»

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