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OS-C501

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Offshore Standard DNV-<strong>OS</strong>-<strong>C501</strong>, November 2013<br />

Sec.4 Materials - laminates – Page 47<br />

.<br />

200<br />

E<br />

II<br />

FAILURE<br />

E<br />

0 + 90<br />

E 0 + PARTIALLY DAMAGED 90<br />

S<br />

T<br />

R<br />

E<br />

S<br />

S<br />

100<br />

E 0 + TOTALLY DAMAGED 90<br />

STRAIN AT ONSETT<br />

OF MATRIX CRACKING<br />

0<br />

0.0<br />

0.5<br />

1.0<br />

1.5<br />

2.0<br />

Figure 4-1<br />

Example of a stress strain curve of a 0/90 laminate<br />

STRAIN<br />

2.8.4 The strain to failure transverse to the fibre direction is identical to the strain at onset of matrix cracking.<br />

2.8.5 The strain to failure (rupture) of the laminate is the strain to failure of the fibres.<br />

2.8.6 The remaining ply properties can be calculated with laminate theory and considering [2.3].<br />

2.8.7 For properties with matrix cracking, see Sec.4 [9].<br />

2.9 Experimental measurement of ply shear properties<br />

2.9.1 The shear properties of a ply are typically non-linear. In order to perform a linear analysis an initial nondegraded<br />

shear modulus should be defined.<br />

2.9.2 For a strength analysis initial, undamaged shear modulus may be defined as the secant modulus between<br />

0 and any point on the non-linear stress strain curve as long as:<br />

— only nonlinear deformation, but no matrix cracking is observed in the experiments<br />

— the point is below 80% of the failure strength<br />

— the point is below 50% of the strain to failure<br />

An example is given in Figure 4-2.<br />

F A IL U R E<br />

S h e a r<br />

S tre s s<br />

G<br />

1 2<br />

G 1 2 a t fa ilu re<br />

G 1 2 a t 9 0 % o f fa ilu re lo a d<br />

0<br />

0 .0<br />

Figure 4-2<br />

Example of a shear stress strain curve<br />

S h e a r s tr a in<br />

2.9.3 For deflection calculations the modulus should be secant modulus at the maximum design shear stress<br />

and all requirements of [2.9.2] should be fulfilled.<br />

2.9.4 The remaining properties can be calculated by laminate theory and considering [2.3].<br />

2.9.5 For properties with matrix cracking or non-linear deformations, see Sec.4 [9].<br />

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