What is Non-equilibrium Cooling?
During a rapid cooling, the precipitated solid molecules in the liquid have not diffused uniformly, resulting in non-uniform concentration of solid molecules in the crystallisation.
- Phase Change at temperatures not at phase diagram boundary lines
- nucleation, growth and transformation rates as a function of time (not temperature)
Martensite:
Formed when when Austenite is rapidly cooled (e.g. quenched)
Fast cooling prevents Carbon diffusing out of Iron (can’t form Fe3C)
Pearlite:
Alternating layers of ferrite (α) and cementite (Fe3C)
Formed during slow cooling
Forms Body-Centred Tetragonal crystal structure. Elongated BCC
Most real world cooling scenarios are not fully at equilibrium
Martensite is a ‘supersaturated’ solution
Forms needle shaped grains and transformation occurs almost instantaneously
Austenite is denser than martensite → net volume increase → causing internal stresses that may cause crack
Tempered Martensite
Heat treatment that enhances ductility and toughness of martensite.
Heating martensite to a temperature below the eutectoid for a specific time period.
Normally between 250℃ to 650℃.
Temperature raise allows C to diffuse and form Fe₃C. (Has ⍺ and Fe₃C phases).
BCT transforms to BCC.
As hard and strong as martensite, but with enhanced ductility and toughness.
Bainite
Formed when autensite is cooled past a critical temperature (e.g. 727℃).
Bainite consists of needle-like particles, cementite (Fe3C) in a ferrite matrix.
The transformation begins with nucleation of ferrite plates (displacive growth) at the autensite boundaries.
The temperature becomes high enough that Carbon diffuses out of the lattice and the FCC structure transforms into a BCC structure.
Eventually cementite precipitates in the remaining austenite layers between the ferrite platelets.
Time - Temperature Transformations
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