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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 />

Table 3.8. Chemical compositions of Fe-Cr rich phase measured by APT in ODS mo<strong>de</strong>l<br />

alloy. In total, the matrix composition is measured on three different pow<strong>de</strong>r grains.<br />

LAWATAP measurements in p<strong>la</strong>ces indicated on Figure 3.9, corresponds to 1-7 analyses.<br />

Matrix measurements are also performed for two LATAP analyses. In one (shown on Figure<br />

3.6), matrix composition is calcu<strong>la</strong>ted by simi<strong>la</strong>r way and corresponds to 8-11 analyses. In<br />

second one (shown on Figure 3.3), the composition is calcu<strong>la</strong>ted for Fe-Cr rich phase and<br />

corresponds to 12 analyse. For com<strong>par</strong>ison the nominal composition is also reported. The<br />

composition is calcu<strong>la</strong>ted in accordance to assumption that O2 ions located at 32 amu.<br />

Standard <strong>de</strong>viations are 2σ. The values are in at.%.<br />

Elements Fe Cr Si Mn W C Y Ti O<br />

Nominal (at.%) Bal. 7.45 - - - - 4.8 11.0 7.1<br />

1 88.7 9.9 0.04 0.33 0.22 0.08 0.11 0.32 0.70<br />

2σ 0.9 0.9 0.06 0.17 0.14 0.08 0.10 0.17 0.25<br />

2 90.3 7.7 0.16 0.31 0.15 0.08 0.39 0.08 0.80<br />

2σ 1.6 1.5 0.22 0.31 0.22 0.16 0.35 0.16 0.50<br />

3 89.9 7.2 0.24 0.33 0.24 0.06 0.24 0.34 1.5<br />

2σ 1.5 1.3 0.24 0.28 0.24 0.12 0.24 0.29 0.59<br />

4 90.2 8.6 0.19 0.18 0.13 0.03 0.11 0.10 0.36<br />

2σ 0.6 0.6 0.09 0.08 0.07 0.03 0.07 0.06 0.12<br />

5 90.1 8.6 0.19 0.26 0.25 0.05 0.07 0.08 0.35<br />

2σ 0.6 0.6 0.09 0.10 0.10 0.04 0.05 0.05 0.12<br />

6 90.9 8.2 0.22 0.27 0.14 0.04 0.01 0.01 0.28<br />

2σ 0.5 0.5 0.09 0.10 0.07 0.03 0.02 0.02 0.10<br />

7 90.7 8.1 0.10 0.16 0.18 0.02 0.09 0.08 0.54<br />

2σ 0.6 0.5 0.60 0.08 0.08 0.03 0.06 0.06 0.15<br />

8 86.4 10.1 0.22 0.22 0.22 0.04 0.39 0.33 1.50<br />

2σ 2.3 2.0 0.31 0.31 0.31 0.42 0.38 0.39 0.81<br />

9 88.6 9.4 0.37 0.16 0.19 0.11 0.06 0.22 0.80<br />

2σ 0.9 0.8 0.17 0.11 0.12 0.09 0.07 0.13 0.25<br />

10 88.8 8.70 0.38 0.25 0.47 0.09 0.09 0.12 1.18<br />

2σ 1.9 1.7 0.38 0.30 0.42 0.20 0.20 0.21 0.67<br />

11 85.1 11.7 0.22 0.43 0.11 0.22 0.01 0.40 1.70<br />

2σ 2.3 2.1 0.30 0.43 0.22 0.30 0.01 0.41 0.85<br />

12 89.5 9.5 0.27 0.15 0.16 0.13 0.01 0.05 0.05<br />

2σ 0.2 0.2 0.03 0.02 0.02 0.02 0.01 0.01 0.01<br />

Mean 89.7 8.85 0.20 0.23 0.19 0.07 0.08 0.12 0.48<br />

2σ 0.23 0.22 0.03 0.04 0.04 0.02 0.03 0.03 0.06<br />

As it can be seen in Table 3.8, the matrix concentration is different from the nominal one.<br />

A significant lower amount of Ti, O and Y are measured. Si, Mn, W and C are also <strong>de</strong>tected.<br />

In the Fe-Cr-rich phase, Fe varies from 85.1 to 90.9 at.% and Cr from 7.2 to 11.7 at.%.<br />

Fluctuations of Y, Ti and O elements are also observed from one p<strong>la</strong>ce to another. As an<br />

example, smaller amounts of Ti, Y and O are measured in box number 5 and 6 located far<br />

from Y-Ti-O rich phases in com<strong>par</strong>ison to boxes 1, 2 and 3 located closer (see Figure 3.9). In<br />

general, the Ti, Y and O concentrations vary from 0.01 to 0.40 at.%, 0.01 to 0.39 at.% and<br />

0.05 to 1.7 at.%, respectively. It must be mentioned that Y and O are almost immiscible in bcc<br />

iron (their equilibrium solubility limits are 0.029 at.% [12] and 0.06 [13] respectively at<br />

102

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