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Forgeabilité des aciers inoxydables austéno-ferritiques

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

106 Chapter IV. STRAIN PARTITIONING<br />

After the fabrication of the microgrid, a low magnification-high resolution picture (4096x4096 pixels)<br />

was obtained by SEM, covering large areas before deformation (0.25mm²). Secondary electron con-<br />

trast was used. The best matching of the homologous points by image correlation requires generating<br />

an optimal contrast on the SEM pictures. In other words, the picture must involve the entire 256-grey<br />

level histogram and must not be centered on a few grey levels. Furthermore, the grey values do not<br />

exceed the 0 and 255 boundaries in order to avoid saturation in the white or black field. A testing pro-<br />

cedure consists in plotting the grey level histogram and to check its spreading. If the spreading is not<br />

acceptable, it will be changed by adjusting the brightness and contrast. Some examples of acceptable<br />

engraved microgrids are given in Figure IV.8.<br />

a) b)<br />

Figure IV.8. Examples of good microgrid high resolution pictures before deformation; a) equiaxed<br />

morphology; b) Widmanstätten morphology.<br />

As highlighted previously, the most critical step in the modified microgrid method is the engraving step.<br />

The main difficulties are summarized below.<br />

(i) Duplex stainless steels are two-phase material, and in general, the micro-etching prin-<br />

ciple consists in dissolving one phase and not the other one. To engrave microgrids in<br />

both phases requires finding a solution which could etch ferrite as well as austenite.<br />

The 40%-aqueous nitric acid electro-etching solution was that which gave the best re-<br />

sults.<br />

(ii) As can be seen in Figure IV.9.a, the microgrid appears to be more defined in the aus-<br />

tenite compared to the ferrite. This was due to the etching used to reveal the phases<br />

prior the application of the modified microgrid technique. The etchant used for this<br />

purpose affects the ferrite and not the austenite. As a consequence when a uniform<br />

layer of resin was deposited on the surface, the resin on the top of the ferrite is<br />

thicker. Figure IV.9.b shows a schematic cross section of the material close to the sur-<br />

face and the layer of resin on it. When an electron beam of constant intensity and di-<br />

ameter scans the surface, the resin on top of the austenite is burnt all the way through

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