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70<br />

Valério da Silva Almeida & João Batista de Paiva<br />

6 BEM-FEM COUPLING<br />

The BEM and FEM are coupled by representing the surface forces of the soil<br />

given in Eq. (18) as reactions between the contact elements of the superstructure-soil<br />

interface. Ideal friction conditions will also be admitted, without allowing for any relative<br />

displacement between the two media. Provided the reactions of the FEM are<br />

expressed by forces already integrated into the domain and transformed into<br />

equivalent nodal forces in each element, the surface forces of the soil can be<br />

expressed by nodal parameters distributed in the element. Hence, coupling requires<br />

transforming the surface forces into equivalent concentrated forces or vice-versa.<br />

In the present paper, the former transformation is given priority. This approach<br />

is presented accordingly.<br />

The approach developed up to this stage will be applied to the case of<br />

transverse loading, although it can be extended to the other two directions. Figure 2<br />

shows the transverse surface forces and the equivalent nodal forces.<br />

Figure 2 - Equivalent surface and nodal forces<br />

In Fig. 2, g i , g j and g k represent the surface forces at vertices i, j and k of a<br />

generic element, while F<br />

i, Fj<br />

and F k<br />

represent the equivalent nodal forces at the<br />

respective nodes.<br />

The work due to the external load in the element’s transverse direction can be<br />

expressed as:<br />

∫<br />

T = g x , x ) ⋅ w(<br />

x , x ) dA<br />

e<br />

A<br />

( 1 2 1 2<br />

(21)<br />

where ( x , )<br />

w and A are, respectively, the transversal displacement field in the<br />

1 x 2<br />

element domain and the area of the element. When the variation of the displacement<br />

field is assumed to be linear, one has:<br />

w = wξ<br />

+ +<br />

(22)<br />

i 1 wjξ2<br />

wkξ3<br />

Cadernos de Engenharia de Estruturas, São Carlos, v.9, n. 38, p. 63-82, 2007

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