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Volumen II - SAM

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Table 2: Interface equilibrium concentration in different Zr alloys at [1100, 1200, 1250]°C<br />

C β/β+α β/β+α β/β+α β/β+α<br />

Cα/α+β α/α+β<br />

Cα/α+ α/α+ox α/α+<br />

T°C<br />

Zy-4<br />

(wt frac) (at. frac)<br />

Zr-O<br />

((((wt frac)<br />

Zy-4<br />

(wt frac) (at. frac)<br />

Zr-O<br />

(wt frac)<br />

Zy-4<br />

(wt frac) (at.frac)<br />

Zr-O<br />

(wt frac)<br />

1100<br />

TC<br />

C-K<br />

0.0031<br />

0.0038<br />

0.0174<br />

0.0213<br />

0.0040 0.0162<br />

0.0212<br />

0.0854<br />

0.1099<br />

0.0152 0.0684 0.2943 0.0702<br />

1200<br />

TC<br />

C-K<br />

0.0048<br />

0.0057<br />

0.0279<br />

0.0316<br />

0.0061 0.0209<br />

0.0248<br />

0.1086<br />

0.1267<br />

0.0198 0.0698 0.2998 0.0715<br />

1250<br />

TC<br />

C-K<br />

0.0058<br />

0.0068<br />

0.0322<br />

0.0376<br />

0.0071 0.0228<br />

0.0265<br />

0.1175<br />

0.1344<br />

0.0218 0.0705 0.3021 0.0721<br />

Kinetic data set<br />

Experimental diffusion profiles from [1], determined by microprobe analysis, allow to locate with adequate<br />

precision the α/β interface at different temperatures. Then, an adequate set of input kinetic parameters for<br />

Zy-4 has been chosen in the [1100-1250]°C temperature range in order to reproduce the α/β interface<br />

position at each diffusion time (Table 3).<br />

Table 3: Diffusion coefficients in αZr, βZr and ZrO2 at 1100, 1200, 1250°C<br />

T°C Dα (cm 2 /s) Dβ (cm 2 /s) Dox (cm 2 /s)<br />

1100 2.48x10 -8 8.44x10 -7 3.99x10 -7<br />

1200 8.50x10 -8 1.55x10 -6 9.21x10 -7<br />

1250 1.48x10 -7 2.05x10 -6 1.35x10 -6<br />

Comparison of EKINOX simulations with experimental oxygen profiles<br />

The diffusion profiles in α and β phases of Zy-4 are presented in the [1100-1250]°C temperatures range<br />

(Fig.4.) These profiles have been simulated using EKINOX and TC for Zy-4 values from Table 2 and<br />

kinetics parameters given in Table 3. The experimental data are partially taken from [1].<br />

The simulation profiles are in the experimental quoted errors (around 1x10 -2 atomic fraction). The shape of<br />

the experimental oxygen diffusion profile obtained at 1200°C for the longest oxidation times is due to α(o)<br />

incursions in prior-β. Additionally, the determination of the experimental equilibrium concentration at the<br />

α/ox interface is quite difficult. Considering these points, simulations are in good agreement with<br />

experimental data.<br />

Oxygen concentration (at. fraction)<br />

0,3<br />

0,25<br />

0,2<br />

0,15<br />

0,1<br />

0,05<br />

1100°C<br />

0<br />

0 100 200 300 400 500 600<br />

Distance (µm)<br />

467s - Experimental<br />

467s - Simulation<br />

117s - Experimental<br />

117s - Simulation<br />

Oxygen concentration (at.fraction)<br />

0,30<br />

0,25<br />

0,20<br />

0,15<br />

0,10<br />

0,05<br />

0,00<br />

0 100 200 300 400 500 600<br />

Fig. 4. Comparison of experimental and calculated O diffusion profiles in Zy-4 at 1100, 1200 and 1250°C.<br />

The choice of adequate kinetic variables in α phase is significant for the simulation. Finally, the Arrhenius<br />

plot presented in Fig.5, determined from adjusted EKINOX diffusion parameters (Table 3), can be expressed<br />

T[K]<br />

as follows:<br />

D [cm 2 /s]<br />

1E-6<br />

1E-7<br />

1E-8<br />

1200°C<br />

Distance (µm)<br />

1520 1480 1440 1400 1360<br />

0,00066 0,00069 0,00072<br />

1 / T [K -1 ]<br />

1429s - Simulation<br />

1500s - Experimental<br />

520s - Simulation<br />

500-600s - Experimental<br />

187s - Simulation<br />

~ 200s - Experimental<br />

55s - Simulation<br />

~ 50-60s - Experimental<br />

Fig.5. Arrhenius diagram of O diffusion in αZr<br />

1320<br />

Oxygen concentration (at. fraction)<br />

0,3<br />

0,25<br />

0,2<br />

0,15<br />

0,1<br />

0,05<br />

1250°C<br />

0<br />

0 100 200 300 400 500 600<br />

Distance (µm)<br />

120s - Experimental<br />

120s - Simulation<br />

309s - Experimental<br />

309s - Simulation

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