Abstract The austenite-pearlite phase transition in steels occurs over a large range of temperatures and gradually in time. According to the Scheil's additivity rule, in plain steel for any prescribed temperature evolution T(t), at any time t the fraction F(t) of transformed austenite is characterized by the condition ∫ t 0 dξ τ[T(ξ), F(t)] = 1 where τ(T, F) is a prescribed positive function. An interpretation of this law is here proposed and its properties are studied. At lower temperatures the remaining austenite is partially transformed into martensite; the transformed fraction depends on the temperature but not on time. At these temperatures, the austenite-pearlite and the austenite-martensite transformations are coupled. The austenite-pearlite transformation by continuous cooling of an initially austenitic body is then studied, taking account of recalescence and of heat diffusion. A variational formulation is given and an existence result valid for both quenching and normalization is stated. Finally a stable numerical discretization scheme is proposed.
[1]
E. Scheil,et al.
Anlaufzeit der Austenitumwandlung
,
1935
.
[2]
John W. Cahn,et al.
Transformation kinetics during continuous cooling
,
1956
.
[3]
J. K. Brimacombe,et al.
Mathematical model of heat flow and austenite-pearlite transformation in eutectoid carbon steel rods for wire
,
1981
.
[4]
J. Lions,et al.
Inequalities in mechanics and physics
,
1976
.
[5]
J. Christian,et al.
The theory of transformations in metals and alloys
,
2003
.
[6]
M. Avrami.
Kinetics of Phase Change. II Transformation‐Time Relations for Random Distribution of Nuclei
,
1940
.
[7]
J. Brimacombe,et al.
Kinetics of austenite-pearlite transformation in eutectoid carbon steel
,
1983
.