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Forgeabilité des aciers inoxydables austéno-ferritiques

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tel-00672279, version 1 - 21 Feb 2012<br />

Appendices 185<br />

� The local transformation gradient at a given grid intersection p is computed as the average of<br />

the true local gradient over a small volume � p around the grid intersection. The chosen vo-<br />

lume is a cylinder with its axis orthogonal to the surface of the sample, height e arbitrarily<br />

small, and a polygonal upper surface � p whose vertices are neighbours of the considered<br />

grid intersection (see Figure B.1). Let � � p be the boundary of� p , S�p its area and n�p its<br />

normal. � p� is the lower surface of the cylinder.<br />

Considered micro-grid intersection<br />

Neighbour micro-grid intersection<br />

Then, eq B.5 gives:<br />

Surface of the sample<br />

1<br />

F p F � � x�<br />

n<br />

�p<br />

V<br />

F<br />

� �<br />

�p<br />

��p<br />

Figure B.1. Averaging volume for local strain computation [98].<br />

� � �<br />

� � � � �<br />

� ���<br />

� � � � �<br />

� ���<br />

�<br />

��<br />

��<br />

� xde<br />

xds<br />

xds<br />

1 e<br />

p p<br />

ndl<br />

p<br />

S p e<br />

e<br />

p<br />

ds<br />

p n<br />

With e tending to 0, one gets then:<br />

F<br />

since x is continuous.<br />

� � xds<br />

�<br />

1 � �p<br />

�<br />

� ���<br />

x�<br />

ndl�<br />

� �p�<br />

S�p<br />

� �n<br />

��p<br />

�p<br />

�<br />

��<br />

��<br />

p n<br />

�<br />

�<br />

,<br />

�<br />

eq B.7<br />

. eq B.8<br />

, eq B.9

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