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Composite Materials Research Progress

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Optimization of Laminated <strong>Composite</strong> Structures… 89<br />

4<br />

∑ t i ≤ 4<br />

i=<br />

1<br />

(8.3)<br />

0. 001 ≤ θ i ≤ 180 i = 1,<br />

2<br />

0. 001 t ≤ 10<br />

i = 1,<br />

2<br />

≤ i<br />

where j is the number of the load case. This problem is solved by resorting the its bound<br />

formulation (Olhoff, 1989) including here 5 design variables (2 orientations, 2 thicknesses<br />

and the multi-objective factor β) and 7 constraints:<br />

1<br />

min β<br />

2<br />

1 T<br />

ε(<br />

j)<br />

Aε(<br />

j)<br />

2<br />

TW ( j)<br />

( i , ti<br />

)<br />

4<br />

∑ t i<br />

i=<br />

1<br />

0. 001 ≤ i ≤<br />

0. 001 ≤ i ≤ 10<br />

≤ β<br />

2<br />

j = 1,<br />

2<br />

θ ≤1<br />

i , j = 1,<br />

2<br />

(8.4)<br />

≤ 4<br />

θ 180 i = 1,<br />

2<br />

t i = 1,<br />

2<br />

The results are reported in Figure 8.10 for the different values of k. The solution is<br />

obtained when the relative variation of the design variables at 2 successive iterations is lower<br />

than 0.01. It is seen that a large number of iterations is needed to reach the optimum when<br />

MMA is used. GCMMA converges in a lower number of iterations. As for mono-objective<br />

problems, SAM is the most effective optimization method.<br />

+ MMA<br />

o GCMMA<br />

Δ SAM<br />

Maximum strain energy density (N/mm)<br />

4<br />

3<br />

2<br />

1<br />

0<br />

0 2 4 6 8<br />

80<br />

60<br />

40<br />

20<br />

Number of iterations<br />

0<br />

0 2 4 6 8<br />

Load parameter k Load parameter k<br />

Figure 8.10. Variation of the strain energy density and number of iterations needed to reach the solution<br />

as a function of the parameter k.

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