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OS-C501

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

Sec.9 Structural analysis – Page 154<br />

do not allow values for all three parameters to be specified, one should generally use the measured values for<br />

G and ν, and let the E value be calculated (from the formula above) by the program. In that case the shear<br />

response of the core will be described accurately. However, in particular applications, in which core shear<br />

effects are negligible and axial stresses/strains are crucial, correct E values shall be applied.<br />

Guidance note:<br />

For many core materials experimentally measured values of E, G and ν are not in agreement with the isotropic<br />

formula:<br />

---e-n-d---of---G-u-i-d-a-n-c-e---n-o-t-e---<br />

10.2.3 Anisotropic core shall be described with 4 elastic constants in a 2-D analysis, i.e. E x , E z , G xz, ν xz .<br />

10.2.4 Anisotropic core shall be described with 9 elastic constants in a 3-D analysis, i.e. E x , E y , E z , G xy , G yz ,<br />

G xz , ν xy , ν yz , ν xz .<br />

10.3 2-D non-linear failure analysis<br />

E<br />

G =<br />

2 (1 + ν )<br />

10.3.1 If the through thickness stresses or the through width strains are insignificant, see [10.1.3], a 2-D<br />

progressive analysis may be carried out.<br />

10.3.2 At the beginning of the analysis, the analyst shall use non-degraded material properties.<br />

10.3.3 All displacement calculations shall be based on time-dependent material properties related to, e.g.,<br />

naturally or environmentally degradation during service life.<br />

10.3.4 For an undamaged sandwich structure, the following stresses and load shall typically be calculated:<br />

σ , , and .<br />

face σ τ<br />

core core Pcr<br />

Guidance note:<br />

Example: Transverse loading case for an open beam.<br />

Stresses shall be calculated as follows:<br />

σ<br />

σ<br />

Mz<br />

=<br />

D<br />

face<br />

E face<br />

Mz<br />

=<br />

D<br />

core<br />

E core<br />

Identically for a box beam:<br />

τ<br />

core<br />

=<br />

T<br />

D<br />

⎡<br />

⎢ E<br />

⎣<br />

face<br />

t<br />

face<br />

2<br />

d<br />

+<br />

E<br />

2<br />

core<br />

t<br />

core<br />

4<br />

2<br />

⎤<br />

⎥<br />

⎦<br />

σ<br />

Mz<br />

=<br />

D<br />

face<br />

E face<br />

τ =<br />

bd<br />

4 I<br />

2<br />

N<br />

in N-direction, and<br />

τ<br />

core<br />

=<br />

( 2 b + d )<br />

8I<br />

2<br />

d<br />

N<br />

in direction perpendicular to<br />

N.<br />

10.3.5 For given loading conditions, stresses and strains shall be calculated and failure criteria shall be<br />

checked.<br />

10.3.6 Any failure of the face material shall be modelled the same way as for monolithic laminates according<br />

to Sec.4 and Sec.9 [2].<br />

10.3.7 If core failure of type ductile or plastic occurs due to core yielding (in tension or compression), E core *<br />

shall be set equal to the secant modulus at the corresponding σ level; G core * shall be proportionally reduced by<br />

the same amount. If σˆ is reached, E core and G core shall be reduced to 0 (default value) or to positive values<br />

core<br />

as described in [10.3.11].<br />

DET NORSKE VERITAS AS

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