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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- 71 -<br />
Here r is the mean radius <strong>of</strong> the element and, as previously<br />
mentioned, the matrix B is evaluated at the centroid <strong>of</strong> the triangle.<br />
The index T denotes the transpose <strong>of</strong> a natrix. Body forces<br />
b due to gravity in the direction <strong>of</strong> the Z-axis may be dealt with<br />
in the program, i.e..<br />
b = 0<br />
b r<br />
Using eq. (4.1-21) and eq. (4) we obtain<br />
F. = I N '<br />
T b dV = N T L 2TT<br />
b J<br />
r<br />
m<br />
A<br />
el.vol<br />
2irr<br />
m<br />
Ab„<br />
Z<br />
where the matrix N is evaluated at the centroid <strong>of</strong> the triangle.<br />
Nodal forces due to prescribed discrete point forces P located<br />
within the element are given by eq. (4.1-22) and eq. (4), i.e.,<br />
- =T -<br />
F = I N P<br />
P<br />
(4.2-13)<br />
where the summation extends over the number <strong>of</strong> discrete point<br />
forces P and where the matrix N is evaluated at the location <strong>of</strong><br />
the point force in question. Nodal forces due to prescribed<br />
traction forces t are given by eq. (4.1-23) and eq. (4), i.e.<br />
; t - f « T t ds<br />
S - area <strong>of</strong><br />
the element<br />
and nodal forces due to temperature expansion are given by eq.<br />
(4.1-24), i.e.<br />
l<br />
• I<br />
D é dV<br />
o<br />
= B T 5 e 2Trr A<br />
o m<br />
el.vol