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Rasmus ÿstergaard forside 100%.indd - Solid Mechanics

Rasmus ÿstergaard forside 100%.indd - Solid Mechanics

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Interface Fracture Toughness of Sandwich Structures 451<br />

By superimposing a stress field corresponding to an intact sandwich loaded<br />

by the moment M3 and the force P3 we arrive at a reduced problem<br />

where the singular stress components at the crack tip are as in the original<br />

problem. The superposition is illustrated in Figure 3. The relations between<br />

the reduced load parameters M and P and the original loads, Pn, Mn,<br />

n ¼ 1 ...3 are<br />

P ¼ P1 þ C1P3 þ C2M3<br />

h<br />

M ¼ M1 þ C3M3,<br />

where C 1, C 2, and C 3 are constants only dependent on elasticity and<br />

geometry. The constants are to be found in closed form in appendix C.<br />

This result is important since we now only have to determine the singularity<br />

in terms of G and for all combinations of P and M instead of all<br />

combinations of Pn, Mn, n ¼ 1 ...3.<br />

(a)<br />

(b)<br />

(c)<br />

P 1<br />

P 2<br />

P 3<br />

P<br />

P<br />

M 1<br />

M 2<br />

M 3<br />

M<br />

M *<br />

d<br />

Figure 3. By super imposing the stress field in (b) on the stress field in (a) the situation in<br />

(c) is found, where M ¼ Ph þ M and is given in the appendix.<br />

M 3<br />

M 3<br />

P 3<br />

P 3<br />

ð7Þ

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