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Transformation induced within the neighbor grain by the plate impinging on the grain boundary is denominated "intergrain autocatalysis". From the above one can infer that martensite autocatalysis results from the relaxation of transformation strains. Sympathetic nucleation and slip accomplish that. The former mechanically relaxes the shear-component of the shape-strain, promoting variant-selection.

The Theory of Transformations in Metals and Alloys

Complementary relaxation by slip introduces a thermally-activated dependence in the autocatalysis. Slip may become predominant when the austenite plasticity so permits, e. It is worthy of note that in polycrystalline materials the austenite grain boundaries may become a hindrance to the transformation uniformity by limiting the size of the martensite units, as well as foster the intergrain-autocatalysis that spreads the transformation over the austenite grains.

To cope with the typically fast transformation rate, we used a formalism that bears experimentally perceived aspects of the autocatalysis during the martensite spread. At martensite transformation temperatures a large driving force for austenite to martensite is available. However, owing to the peculiarities of martensite nucleation only a relatively small number of nuclei per unit of volume are normally available for nucleation of the so-called primary plates.

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To promote further transformation and therefore to achieve a larger decrease in Gibbs free energy, the martensite transformation "finds a way" resorting to autocatalysis to increase the number of potential nucleation sites from which new martensite plates form. Some specific conclusions are:. The intragrain transformation relates to the auto-accommodation of transformation strains, thence it has a mechanical aspect.

The stress-assisted intergrain autocatalysis depends on thermal activation. This indicates that the intergrain autocatalysis is hindered at low temperatures. Thence, the autocatalysis provides further environments for martensite nucleation than are distinct than provided by the pre-existent austenitic sites. In a classical view, that is equivalent to admitting the autocatalytic nucleation sites with a distinct potency-distribution. The austenite grain boundaries have multiple effects in the martensite transformation, by fostering martensite nucleation, by limiting the size of the martensite units and by contributing to the intergrain autocatalysis spread-events.

The authors are grateful to Prof. Kahl Zilnyk for providing the micrograph used in Fig. Theory of Transformations in Metals and Alloys. Oxford: Pergamon Press; Isothermal martensite formation at sub-zero temperatures. Heterogeneous Nucleation of the Martensite Transformation. On the entropic nucleation barrier in a martensitic transformation. Philosophical Magazine.

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Acta Materialia. Incubation times and entropy barriers in martensitic kinetics: Monte Carlo quench simulation of strain pseudospins.


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Burst phenomenon in the martensitic transformation. Transactions AIME. Rate of propagation of martensite. Metallographic study of influence of austenite grain-size on martensite kinetics. Acta Metallurgica. Formation sequence of plates in isothermal martensite transformation. Materials Research. The mechanism of the martensite burst transformation in Fe-Ni single crystals. Metallurgical and Materials Transactions A. Practical Applications of Quantitative Metallography. STP Philadelphia: ASTM; Measurement of particle sizes in opaque bodies.

A computer-assisted analysis of the spread of martensite-transformation. Materials Science and Engineering. Microstructural path analysis of athermal martensite. Scripta Materialia. Reaction kinetics in processes of nucleation and growth.

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The Journal of Chemical Physics. The statistics of crystal growth in metals. Microstructural descriptors and the effects of nuclei clustering on recrystallization path kinetics. Formal analysis of isothermal martensite spread. Isothermal martensite: the austenite grain-size and the kinetics of "spread". Materials Science and Technology. Initial nucleation kinetics of martensite transformation.

Journal of Materials Science. Phase-field modeling of displacive phase transformations in elastically anisotropic and inhomogeneous polycrystals. Nucleation of isothermal martensitic transformation. Distributed-activation kinetics of heterogeneous martensitic nucleation. Kinetics of anomalous multi-step formation of lath martensite in steel. Thermally activated martensite: its relationship to non-thermally activated athermal martensite. Hoboken: Wiley; Nucleation and growth of a single martensite particle.

Cambridge: Massachusetts Institute of Technology; Spread of transformation and plate dimensions of isothermally formed martensite. Materials Science and Engineering: A. The dimensions of isothermally formed martensitic plates in a Fe-Ni-Mn alloy. This is an Open Access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Services on Demand Journal. Background It is well-known that the initiation of the martensitic transformation in high Ni Fe-Ni-C alloys demands significant super-cooling to reach the martensite start temperature, M S , frequently signaled by a transformation-burst, heat-rise and sonic-emission 7.


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  • Experimental Details The material preparation is duly described in the referenced papers, so that they were not detailed here for brevity sake. Analytical Model The fast transformation-rate is a handicap to study the evolution of a martensitic transformation.

    Phase Transformations in Metals and Alloys, Second Edituion

    Discussion Tables 1 - 2 show that the number density of the martensite units, N VM , are orders of magnitude higher than the calculated number density of initial martensite nucleation events, n V , as might be expected. Acknowledgements P. References 1 Christian JW. UFSCar - Dep. In general, n atomic orbitals in this case the six Na 3s orbitals will generate n molecular orbitals with n-1 possible nodes.

    In Chapter 2, we showed that the energy versus internuclear distance graph for a two hydrogen atom system has a low energy level and a high energy level corresponding to the bonding and antibonding molecular orbitals, respectively. These two energy levels were well separated from each other, and the two electrons in H 2 energetically prefer the lower energy level. If more atoms are introduced to the system, there will be a number of additional levels between the lowest and highest energy levels. In band theory, the atom chain is extrapolated to a very large number - on the order of 10 22 atoms in a crystal - so that the different combinations of bonding and anti-bonding orbitals create "bands" of possible energy states for the metal.

    In the language of physics, this approach of building the bands from discrete atomic orbitals is called the "tight-binding" approximation.

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    The number of atoms is so large that the energies can be thought of as a continuum rather than a series of distinct levels. A metal will only partially fill this band, as there are fewer valence electrons than there are energy states to fill. In the case of Na metal, this results in a half-filled 3s band.

    Nearly free electron model. In metals, the valence electrons are delocalized over many atoms.

    by J.W. Christian

    The total energy of each electron is given by the sum of its kinetic and potential energy:. This potential holds the valence electrons in the crystal but, in the free electron model, is essentially uniform across the crystal. Electron wavelength and wavenumber.


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    • What are the consequences of this model for band theory? For a hypothetical infinite chain i.