OS-C501
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Offshore Standard DNV-<strong>OS</strong>-<strong>C501</strong>, November 2013<br />
Sec.5 Materials – sandwich structures – Page 80<br />
Table 5-3 Mechanical static properties for core materials (Continued)<br />
Mechanical parameter Unit Reference in Appendix D<br />
yz<br />
core non-linear Core shear stress normal to the core plane [N/mm 2 ]<br />
(or MPa)<br />
Fracture toughness<br />
G Ic core Mode-I (opening) critical strain energy release rate [N/m] [D.2.5]<br />
G II core Mode-II (shearing) critical strain energy release rate [N/m] [D.2.5]<br />
2.2.7 The static data for adhesive materials are the following:<br />
for measurement method<br />
[D.2.4] for balsa<br />
[D.2.3] for other materials<br />
σ ∧ t<br />
Table 5-4 Mechanical static properties for adhesive materials<br />
Mechanical parameter Unit Reference in Appendix D<br />
for measurement method<br />
In-plane elastic constants<br />
E adhesive linear Modulus of elasticity of adhesive in the linear range [N/mm 2 ]<br />
(or MPa)<br />
[D.3.2] or [D.3.3]<br />
E adhesive non-linear Modulus of elasticity of adhesive at the failure point [N/mm 2 ] [D.3.2] or [D.3.3]<br />
(or MPa)<br />
G xy adhesive linear In plane shear modulus of adhesive in the linear range [N/mm 2 ] [D.3.4]<br />
(or MPa)<br />
G xy adhesive non-linear In plane shear modulus of adhesive at the failure point [N/mm 2 ]<br />
(or MPa)<br />
[D.3.4]<br />
ν xy adhesive Major Poisson’s ratio of adhesive [-] [D.3.2] or [D.3.3]<br />
In-plane strain to failure<br />
adhesive Adhesive tensile strain at failure point [D.3.2]<br />
ε ∧ t<br />
In-plane strength<br />
σ ∧<br />
σ ∧ t<br />
σ ∧<br />
xy<br />
adhesive Adhesive flatwise tensile strength [N/mm 2 ]<br />
(or MPa)<br />
adhesive Adhesive tensile strength [N/mm 2 ]<br />
(or MPa)<br />
adhesive Adhesive shear strength [N/mm 2 ]<br />
(or MPa)<br />
2.3 Relationship between strength and strain to failure<br />
2.3.1 For material exhibiting a brittle type (type-I) of failure and a linear elastic behaviour up to ultimate failure<br />
then, E = σ/ε.<br />
2.3.2 For material exhibiting a ductile or plastic type of failure (respectively type-II and -III), the linear<br />
relationship shall be used up to the upper bound of the linear elastic limit. Material properties listed in Tables<br />
B1 and B2 pertaining to this regime are called linear.<br />
2.3.3 Beyond the upper bound of the linear elastic limit, a different modulus shall be used; this one shall<br />
represent the elastic behaviour related to the range of the stress-strain curve. Material properties, listed in Table<br />
5-3 and Table 5-4 and pertaining to this regime, are called non-linear. In most cases, it is convenient to use a<br />
linear secant modulus to describe the material.<br />
2.3.4 When the stress-strain relationship can not be established for non-linear range, a non-linear analysis shall<br />
be carried out.<br />
2.4 Characteristic values<br />
[D.3.3]<br />
[D.3.2]<br />
[D.3.4]<br />
Fracture toughness<br />
G Ic adhesive Mode-I (opening) critical strain energy release rate [N/m] [D.2.5] or [D.4.2]<br />
G IIc adhesive Mode-II (shearing) critical strain energy release rate [N/m] [D.2.5] or [D.4.2]<br />
2.4.1 Characteristic values shall be used for all strength values in this standard. The procedure to obtain<br />
characteristic values is given in Sec.4 [2.4].<br />
2.4.2 For most core materials the coefficient of variation (COV) of the test specimens is relatively independent<br />
of the specimen size. However, for some materials, like balsa, the COV varies with specimen size. This<br />
variation should be considered in the analysis.<br />
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