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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

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