Molybdenum accumulation at ferrite: Austenite interfaces during isothermal transformation of an Fe-0.24 pct C-0.93 pct Mo alloy |
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Authors: | E S Humphreys H A Fletcher J D Hutchins A J Garratt-Reed Jr" target="_blank">W T ReynoldsJr H I Aaronson G R Purdy G D W Smith |
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Affiliation: | (1) the Begbroke Science Park, Oxford University, OX1 3PH Oxford, United Kingdom;(2) Outokumpu Stainless Ltd., Sheffield, United Kingdom;(3) the Department of Materials, Oxford University, UK;(4) Present address: the Center for Materials Science and Engineering, Massachusetts Institute of Technology, 02139 Cambridge, MA;(5) the Department of Materials Science and Engineering, Virginia Polytechnic Institute and State University, 24061 Blacksburg, VA;(6) Department of Materials Science and Engineering, Carnegie Mellon University, 15213 Pittsburgh, PA;(7) School of Physics and Materials Engineering, Monash University, 3800 Victoria, Australia;(8) the Department of Materials Science and Engineering, McMaster University, L8S 4L7 Hamilton, ON, Canada |
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Abstract: | A scanning transmission electron microscope (STEM) technique was used to measure Mo concentrations at ferrite:austenite (α:γ) interfaces in an Fe-0.24 pct C-0.93 pct Mo alloy partially transformed at 650°C, 630°C, and 610°C. These concentrations
were quite small at 650°C, which is just below the bay temperature of the time-temperature-transformation (TTT) curve for
the initiation of ferrite formation. There were larger concentrations at 630°C, a temperature at which transformation stasis
(incomplete transformation) occurred. Concentrations at 610°C were intermediate between the values observed at 650°C and 630°C.
The average accumulation at the latter temperatures increased appreciably as a function of transformation time. After each
heat treatment, there was considerable variation in Mo accumulation from one α:γ interface to another and, to a lesser extent, from one region to another along the same interface. These higher Mo concentrations
were deduced to have developed largely through volume diffusion of Mo, mainly through ferrite, to interfaces whose ledgewise
growth had been interrupted by growth stasis. (Mo2C precipitation at α:γ boundaries occurred only at the end of growth stasis.) It appears that only a very small amount of Mo segregation is needed,
probably at specific interfacial sites, in order to produce growth cessation. Growth kinetics anomalies of this kind continue
to provide the best evidence available for the operation of a coupled-solute drag effect.
This article is based on a presentation given in the symposium “The Effect of Alloying Elements on the Gamma to Alpha Transformation
in Steels,” October 6, 2002, at the TMS Fall Meeting in Columbus, Ohio, under the auspices of the McMaster Centre for Steel
Research and the ASM-TMS Phase Transformations Committee. |
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