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Final solidification, centre segregation and precipitation phenomena in continuously cast round billets
Author(s) -
Jacobi Hatto,
Wünnenberg Klaus
Publication year - 1997
Publication title -
steel research
Language(s) - English
Resource type - Journals
eISSN - 1869-344X
pISSN - 0177-4832
DOI - 10.1002/srin.199701787
Subject(s) - solidus , materials science , metallurgy , necking , shrinkage , homogenization (climate) , nucleation , composite material , thermodynamics , alloy , biodiversity , ecology , physics , biology
Archimedes’ principle was applied to strand lengths of up to 14 m of round 177 mm diameter billets to determine cavity volume V (in cm 3 /m) for a series of tubemaking steels. Under steady state casting conditions, V depends primarily on the chemical composition and solidification behaviour of the steels. Averages ranged up to in an extreme case (bearing steel; v C = 2.0 m/min). Stopping the strand and abrupt lowering of withdrawal speed made it possible to artificially induce individual shrinkage cavities with peak values of V = 45 cm 3 /m. In the round mould, subsequent necking of the liquid crater is initiated in this process. Whisker‐like and icicle‐like dendrites can be observed in horizontally formed macroscopic shrinkage cavities. The liquid crater is broken off by periodic bridging (the mini‐lingot model). As permeability decreases, the bridges deflect downward in a U‐shape under the ferrostatic load. The residual inter‐dendritic melt is squeezed out in this plastic deformation process. Some bridges ultimately break. This interpretation is based on comprehensive CMA studies and concentration maps. Cores taken from the centre of a strand of bearing steel were submitted to various heat treatments between 1100 and 1350°C. Homogenization occurs below solidus ( T < 1225°C). Carbides dissolve and sulfides become globular. Spatial segregation, on the other hand, increases, above solidus. In the extreme case at 1350°C/30 h, the residual melt at the grain boundaries migrates practically completely from the surface zone to the centre of the cylindrical sample (40 mm diameter). The propellent forces for this macro‐heterogenization are provided by the activity gradient from the cylindrical surface to the centre and minimization of interface energy γ/I.

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