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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 1.Bibliography<br />

II.2. Ferritic/Martensitic (F/M) steels<br />

These materials offer more advantages and are potential candidates for SFR c<strong>la</strong>ddings as<br />

well as for other Gen IV <strong>de</strong>signs [14,15]. Commercial ferritic/martensitic steels based on 9-<br />

12%Cr exhibit the highest swelling resistance in com<strong>par</strong>ison with austenitic steels (Figure<br />

1.5). This low swelling response appears to be a generic property of ferritic alloys [20,21]. In<br />

addition these materials have high thermal conductivity and low thermal expansion. A<br />

limitation to the use of ferritic–martensitic steels is their creep resistance at temperatures<br />

(400-600°C) <strong>de</strong>sired in the Gen IV systems. One approach to extend the range of operation<br />

temperatures of F/M steels is reinforcing the F/M <strong>la</strong>ttice by stable dispersion of <strong>nano</strong><strong>par</strong>ticles.<br />

II.3. Nano-reinforced steels<br />

One example of such <strong>nano</strong>-reinforced steels may be Oxi<strong>de</strong> Dispersion Strengthened steels<br />

(ODS). These materials are presently achieve increasing attention and currently consi<strong>de</strong>red as<br />

c<strong>la</strong>dding materials for SFR and several types of Gen IV systems [22,23].<br />

These materials show remarkable properties due to high <strong>de</strong>nsity (~10 23 to ~10 24 m -3 ) of<br />

<strong>nano</strong>metre scale oxi<strong>de</strong> <strong>par</strong>ticles (1-10 nm in diameter) dispersed in Fe-Cr matrix. These <strong>nano</strong>-<br />

oxi<strong>de</strong>s are found to be extremely resistant to coarsening (even during ageing at 900°C for<br />

times up to 3000 h [24,25]). They act as i) obstacles to dislocation motion [26], providing<br />

high creep strength in the range of interest [27–30] for SFR application and ii) sinks for<br />

radiation induced point <strong>de</strong>fects, providing good radiation resistance [31–34].<br />

Properties of such ODS steels strongly <strong>de</strong>pend on microstructure that requires close<br />

control over <strong>nano</strong><strong>par</strong>ticles <strong>de</strong>nsity, size, interfacial properties, etc.<br />

E<strong>la</strong>boration way, influence of chemical composition and e<strong>la</strong>boration <strong>par</strong>ameters on final<br />

microstructure, as well as study of <strong>nano</strong>-oxi<strong>de</strong>s will be discussed in next section.<br />

III. E<strong>la</strong>boration process of ODS<br />

ODS steels are usually produced by complex pow<strong>de</strong>r metallurgy technique: mechanical<br />

alloying (MA). This process is a dry, high energy ball-milling process, where elemental or<br />

pre-alloyed pow<strong>de</strong>rs (Fe, Cr etc…) are milled together with oxi<strong>de</strong> dispersoid and<br />

subsequently mechanically homogenized [31–35]. After MA the pow<strong>de</strong>r is consolidated by<br />

pow<strong>de</strong>r metallurgical processes, as Hot Isostatic Pressing (HIP) or Hot Extrusion (HE). Then<br />

10

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