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76<br />
Valério da Silva Almeida & João Batista de Paiva<br />
Note that taking into account the soil’s rigidity throughout its depth represents a<br />
significant alteration in the displacement values of the soil-raft-building system, since<br />
the relative differences between cases b and c are about 50% (see Fig. 7). This<br />
influence proves more relevant than the consideration of the position of the<br />
indeformable layer, since the relative difference of displacements between cases a<br />
and b is in the order of 20%.<br />
Figure 8 shows the diagrams of bending moments of M<br />
x<br />
along the raft’s BB<br />
2<br />
cut. The variations of these bending moments for the different cases also proved<br />
similar to those presented by the fields of displacement. For these moments, the<br />
average differences between cases b and c and between a and b are, respectively,<br />
52% and 13%.<br />
Figure 9 shows the values of the stresses ( σ<br />
33<br />
) that are mobilized in the area of<br />
contact between soil and raft in the AA cut. The contact stresses also show similar<br />
results in the various cases, the most significant variation occurring between cases b<br />
and c, with a mean value of 33%.<br />
From table 4 it can be noted that, when the soil’s deformability is taken into<br />
account, the columns’ normal values are more closely distributed around the average,<br />
i.e., there is a more uniform redistribution of forces because the mobilisation of the<br />
soil-raft-building system occurs jointly.<br />
Carga permanente<br />
Ação de vento<br />
3 m<br />
r = 10.L<br />
2 m<br />
Radier<br />
h = η L R<br />
36 m<br />
t R<br />
Ω 1<br />
Ω 2<br />
L R<br />
= 20 m<br />
Radier<br />
M t<br />
F x2<br />
F x1 A x 1<br />
x 2<br />
3 m 14 m<br />
5 m 10 m<br />
5 m<br />
Ω 3<br />
Base indeslocável<br />
Edifício de múltiplos andares<br />
Caso a<br />
Caso b<br />
Caso c<br />
Caso d<br />
Limite da superfície discretizada<br />
do semi-espaço<br />
E Ω= E Ω = E Ω= 100 MPa E 3E Ω = 3/2 E Ω = E = 90<br />
1<br />
2 Ω 3/2 E = 3 E = E = 90<br />
1<br />
Ω= E<br />
2 3<br />
Ω = E Ω= 100 MPa<br />
1 2 3<br />
3<br />
Ω 1 Ω 2 Ω 3<br />
η=50 η =1 η =1 (η = η = 3/8η) η =1 (η = η = 3/8η)<br />
Ω<br />
Ω<br />
Ω2<br />
3<br />
Ω2<br />
3<br />
a)<br />
b)<br />
Cadernos de Engenharia de Estruturas, São Carlos, v.9, n. 38, p. 63-82, 2007