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Composite Materials Research Progress

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40<br />

&22 [MPa]<br />

& & [MPa]<br />

& & [MPa]<br />

-4000 -3000 -2000 -1000-50 0 1000 2000<br />

T300/5208<br />

N5208<br />

Jacquemin Frédéric and Fréour Sylvain<br />

50<br />

-150<br />

-250<br />

-350<br />

& 11 [MPa]<br />

-500 -400 -300 -200 -100 0 100<br />

-100<br />

T300/5208<br />

N5208<br />

100<br />

50<br />

-250 -200 -150 -100 -50 0 50<br />

T300/5208<br />

N5208<br />

σ 22 [MPa]<br />

& 22 [MPa]<br />

200<br />

100<br />

0<br />

-200<br />

-300<br />

-400<br />

-500<br />

0<br />

-50<br />

-100<br />

& & &[MPa]<br />

σ 33 [MPa]<br />

& & [MPa]<br />

-4000 -3000 -2000 -1000-50 0 1000 2000<br />

AS4/3501<br />

3501-6<br />

50<br />

-150<br />

-250<br />

-350<br />

σ 11 [MPa]<br />

200<br />

-500 -400 -300 -200 -100 0 100<br />

AS4/3501<br />

3501-6<br />

σ 22 [MPa]<br />

0<br />

-200<br />

-400<br />

100<br />

50<br />

-250 -200 -150 -100 -50 0 50<br />

AS4/3501<br />

3501-6<br />

σ 22 [MPa]<br />

Figure 5. Examples of macroscopic and local (matrix only) stress failure envelopes of T300/5208 and<br />

AS4/3501-6 plies.<br />

5.3.2. Observations on Predicted Results and Discussion<br />

According to the identification procedure described in subsection 5.2.3, an infinite number of<br />

I I I I<br />

macroscopic stress states sets { σ a , σ b , σ c , σ d } can be considered for the determination<br />

I<br />

of the researched microscopic failure envelope strength coefficients. Actually, σ c only may<br />

I<br />

a<br />

I<br />

b<br />

I<br />

d<br />

vary whereas σ , σ and σ are fixed by the macroscopic ultimate stresses<br />

of the considered composite structure (see the first raw of Table 7). Several tests were<br />

0<br />

-50<br />

-100<br />

I<br />

Y ,<br />

/<br />

I<br />

Y ,<br />

I<br />

S

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