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Etude par Sonde Atomique Tomographique de la formation de nano ...

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tel-00751814, version 1 - 14 Nov 2012<br />

Chapter 3. Oxi<strong>de</strong> Dispersion Strengthened Steels<br />

hot extru<strong>de</strong>d state) incorporation, whereas just slight enrichment in Y is observed (~2 times<br />

higher for both annealed and hot extru<strong>de</strong>d state). As it will be shown below, this can be linked<br />

with the fact that Y is the slowest diffuser. In addition, some <strong>par</strong>t of Y (36% owing to APT) is<br />

located in Y-O rich <strong>nano</strong>clusters just after mechanical alloying step.<br />

c) Formation mechanism of <strong>nano</strong><strong>par</strong>ticles in ODS steel<br />

Different <strong>formation</strong> mechanisms of <strong>nano</strong><strong>par</strong>ticles have been <strong>de</strong>tailed in Chapter 1<br />

(Section ΙΙΙ.3 (c)). In present case, <strong>nano</strong>metric <strong>nano</strong><strong>par</strong>ticles are observed in the ODS steel<br />

just after mechanical alloying step.<br />

Consi<strong>de</strong>ring the materials that have been studied in this work, a <strong>formation</strong> mechanism for<br />

oxi<strong>de</strong> <strong>nano</strong>clusters could be suggested. Mechanical alloying results in: a) dissolution of Y2O3<br />

initial oxi<strong>de</strong> inducing supersaturation of Y and O in the matrix (64 and 72 % of Y, O<br />

respectively) and b) <strong>formation</strong> of Y-O-enriched aggregates. These Y-O enriched phases could<br />

contain some amount of Ti (up to 1.6±0.5 at.%). However, the origin of YO-rich aggregates is<br />

still not clear. Two possibility can be consi<strong>de</strong>red: (i) they are produced by the direct<br />

trans<strong>formation</strong> (un<strong>de</strong>r ball milling conditions) of Y2O3 oxi<strong>de</strong> towards Y-O-rich phases or (ii)<br />

complete dissolution of Y2O3 occurs first and then Y-O-rich phase nucleates. Since Y2O3 is<br />

very stable oxi<strong>de</strong> (heat of <strong>formation</strong> of - 1907 kJ.mol -1 [9]), milling time and intensity of<br />

industrial attritor may not be sufficient fully dissolve it in Fe-Cr matrix. From this point, the<br />

hypothesis that MA results in only a <strong>par</strong>tial dissolution of original Y2O3 pow<strong>de</strong>r seems to be<br />

probable. Ten<strong>de</strong>ncy of Y2O3 to amorphization during ball milling process has been wi<strong>de</strong>ly<br />

<strong>de</strong>monstrated [17–19].<br />

Subsequent annealing or hot extrusion, results in significant <strong>de</strong>pletion of matrix in Y, O<br />

and Ti, whereas <strong>nano</strong><strong>par</strong>ticles become more enriched. Y-O <strong>nano</strong><strong>par</strong>ticles in as-milled state,<br />

act as nuclei for the <strong>formation</strong> of the <strong>nano</strong>-oxi<strong>de</strong> <strong>par</strong>ticles. Y, O and Ti are incorporated to<br />

these nuclei, resulting in their enrichment. After annealing or hot extrusion, most of Ti and Y<br />

are located into <strong>nano</strong><strong>par</strong>ticles. The schematic representation of <strong>nano</strong><strong>par</strong>ticles <strong>formation</strong> is<br />

summarized in Figure 3.17.<br />

125

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