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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 />

� Fe content<br />

Chapter 4. Nitri<strong>de</strong> Dispersion Strengthened Steels<br />

The concentration of Fe into the <strong>par</strong>ticles has the opposite behaviour than the<br />

concentration of Ti and N (Figure 4.23 (a)). The highest level is measured in as-milled<br />

samples (~45 at.%), the lowest in pow<strong>de</strong>rs annealed at 850 and 1000°C (~5at.%), and an<br />

intermediate constant value (~30-35%) is measured in samples heat treated at 600, 700 and<br />

hot extru<strong>de</strong>d state.<br />

It is worth mentioning that, the fraction of Fe in Ti-N rich <strong>par</strong>ticles can be non-zero. As<br />

an example, it is suggested, that in the case of <strong>nano</strong>sized precipitates, thermodynamic barrier<br />

for nucleation may be lowered by increasing concentration of matrix atoms in the precipitates<br />

[19, 20]. However, this effect is less pronounced for <strong>par</strong>ticles reaching <strong>la</strong>rger sizes (advanced<br />

growth stage and coarsening). This could exp<strong>la</strong>in that be biggest <strong>par</strong>ticles (observed in<br />

samples annealed at 850 and 1000°C) contain only few percents of iron. The presence of few<br />

percents of iron in nitri<strong>de</strong>s is already reported elsewhere [17]. However, in all analyzed<br />

states, the measured Fe concentration is higher than the maximum value compatible with the<br />

interpretation of SANS data.<br />

Local magnification effects [12,13] could be at the origin of this slight discrepancy (~30-<br />

35at.% of Fe according to APT and less than 20 at.% according to SANS). Mo<strong>de</strong>lling of field<br />

evaporation of high-field <strong>nano</strong><strong>par</strong>ticles in MA NDS matrix (section ΙΙ.4. (d) of the Chapter<br />

2), shows that when radius of <strong>nano</strong><strong>par</strong>ticle exceed 1 nm, the composition in the core is not<br />

affected by trajectory aberrations. However, as already said in the case of Cr atoms, even if<br />

the mo<strong>de</strong>l reproduce qualitatively the experimental artefacts, it could un<strong>de</strong>restimate their<br />

intensity and spatial extension because all the input <strong>par</strong>ameters are not known (e.g. field<br />

evaporation of N and Ti insi<strong>de</strong> a nitri<strong>de</strong>) and because it is possible that some mechanisms are<br />

not consi<strong>de</strong>red (e.g. poor conductivity of nitri<strong>de</strong>s). In addition, when measuring the<br />

composition, by introducing a small box insi<strong>de</strong> <strong>par</strong>ticle, it is not possible to clearly <strong>de</strong>fine the<br />

limit between the area containing Fe actually present in the <strong>par</strong>ticle, and Fe introduced by<br />

over<strong>la</strong>p. In or<strong>de</strong>r to estimate the actual level of Fe, concentration profiles were drawn through<br />

Ti-N rich <strong>par</strong>ticles with Rg > 2.5 nm in all samples (except as-milled one, where <strong>nano</strong><strong>par</strong>ticle<br />

with Rg=2.2 nm was studied). On the profiles, the level of Fe observed in the core of Ti-N<br />

rich <strong>par</strong>ticles is in the range 10 to 20 at % in case of <strong>par</strong>ticles annealed at 600 and 700°C as<br />

well as in hot extru<strong>de</strong>d states. Smaller content of Fe (~5 at.%) is <strong>de</strong>tected in <strong>par</strong>ticles after<br />

157

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