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Forgeabilité des aciers inoxydables austéno-ferritiques

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

Appendices 177<br />

Appendix A: Post processing-analysis of the raw data of<br />

the plane strain compression tests<br />

A.1 Specimens measurements<br />

The undeformed and deformed specimens were measured as <strong>des</strong>cribed in Figure A. 1.<br />

a) b)<br />

Figure A. 1. Schematic diagram of a testpiece; a) before and b) after testing, and approximate dimensional<br />

measurement positions.<br />

For the thickness, the measurements were averaged over five readings. In the breadth direction the<br />

average was weighted towards the central measurement, with this being counted twice during the<br />

calculation. The cold final measurements were then used to calculate the hot final measurements of<br />

the specimen using eq A.1:<br />

hh h f � h f ( T�<br />

T0<br />

� �<br />

)<br />

eq A.1<br />

where hh is the hot thickness, hf is the deformed cold thickness, α is the thermal expansion coefficient,<br />

T the deformation temperature and T0 is room temperature.<br />

A.2 Breadth spread, origin and machine compliance corrections<br />

It was impractical to use a specimen geometry for which the tool width was not a significant factor of<br />

the specimen breadth. This led to lateral spread of the specimen and uncertainty in the contact area<br />

when the stress was applied. An ‘instantaneous’ breadth was empirically defined following the test, to<br />

take into account the changing contact area between the tools and the specimen.

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