MODELING OF ELECTROMAGNETIC HEATING, COOLING AND PHASE-TRANSFORMATIONS DURING SURFACE HARDENING OF STEELS

Citation
A. Jacot et al., MODELING OF ELECTROMAGNETIC HEATING, COOLING AND PHASE-TRANSFORMATIONS DURING SURFACE HARDENING OF STEELS, Journal de physique. IV, 6(C1), 1996, pp. 203-213
Citations number
20
Categorie Soggetti
Physics
Journal title
ISSN journal
11554339
Volume
6
Issue
C1
Year of publication
1996
Pages
203 - 213
Database
ISI
SICI code
1155-4339(1996)6:C1<203:MOEHCA>2.0.ZU;2-N
Abstract
A comprehensive micro-macroscopic model of the continuous hardening of 3d-axisymmetric steel components by induction heating has been develo ped. At the macroscopic scale, the Maxwell and heat flow equations are solved using a mixed numerical formulation : the inductor and the wor kpiece are enmeshed with finite elements (FE) but boundary elements (B E) are used for the solution of the electromagnetic equations in the a mbient air. This method allows the inductor to be moved with respect t o the workpiece without any remeshing procedure. The heat flow equatio n is solved for the workpiece using the same FE mesh. For the thermal boundary conditions, a net radiation method has been implemented to ac count for grey diffuse bodies and the viewing factors of the element f acets are calculated using a ''shooting'' technique. The boundary cond ition associated with the water spraying below the inductor is deduced ,from the inverse modelling of temperatures measured at various locati ons of a test piece. These macroscopic calculations of induction heati ng have been coupled to a microscopic model describing the solid state transformations that occur during both heating and cooling. From the local thermal history, the evolutions of the various phase fractions a re predicted from TTT-diagrams using an additivity principle. A micro- enthalpy method has been implemented in the heat flow calculations in order to account for the latent heat released by the various transform ations. At each time step the local properties of the material, in par ticular its magnetic susceptibility, are updated according to the new temperatures and magnetic field. The results of the simulation are com pared with experimental cooling curves and hardness profiles.