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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

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