In Situ Bulk Observations and Ab Initio Calculations Revealing the Temperature Dependence of Stacking Fault Energy in Fe–Cr–Ni Alloys
Benjamin Neding, Oleg I. Gorbatov, Jochi Tseng, Peter Hedström
Abstract
Abstract The dependence of stacking fault energy ( $${\gamma }_{\text{SFE}}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>γ</mml:mi> <mml:mtext>SFE</mml:mtext> </mml:msub> </mml:math> ) on temperature in austenitic Fe–Cr–Ni alloy powders was investigated by in situ high energy synchrotron X-ray diffraction and ab initio calculations in the temperature range from − 45 °C to 450 °C. The X-ray diffraction peak positions were used to determine the stacking fault probability and subsequently the temperature dependence of γ SFE . The effect of temperature on the diffraction peak positions was found to be mainly reversible; however, recovery of dislocations occurred above about 200 °C, which also gave an irreversible contribution. Two different ab initio -based models were evaluated with respect to the experimental data. The different predictions of the models can be explained by their respective treatment of the magnetic moments for Cr and Ni, which is critical for the alloy compositions investigated. Ab initio calculations, taking longitudinal spin fluctuations (LSF) into consideration within the quasi-classical phenomenological model, predict a temperature dependence of $${\gamma }_{\rm SFE}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>γ</mml:mi> <mml:mi>SFE</mml:mi> </mml:msub> </mml:math> in good agreement with the experimentally evaluated trend of increasing γ SFE with increasing temperature: $$\left|\Updelta {\gamma }_{\rm SFE}/\Updelta T\right|=0.05 {\text{mJ}} {\text{m}}^{-2}/{\text{K}}.$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mfenced> <mml:mi>Δ</mml:mi> <mml:msub> <mml:mi>γ</mml:mi> <mml:mi>SFE</mml:mi> </mml:msub> <mml:mo>/</mml:mo> <mml:mi>Δ</mml:mi> <mml:mi>T</mml:mi> </mml:mfenced> <mml:mo>=</mml:mo> <mml:mn>0.05</mml:mn> <mml:msup> <mml:mtext>mJm</mml:mtext> <mml:mrow> <mml:mo>-</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:msup> <mml:mo>/</mml:mo> <mml:mtext>K</mml:mtext> <mml:mo>.</mml:mo> </mml:mrow> </mml:math> The temperature effect on γ SFE is similar for all three investigated alloys: Fe–18Cr–15Ni, Fe–18Cr–17Ni, Fe–21Cr–16Ni (wt pct), while their room temperature $${\gamma }_{\rm SFE}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>γ</mml:mi> <mml:mi>SFE</mml:mi> </mml:msub> </mml:math> are evaluated to be 22, 25, 20 mJ m −2 , respectively.