Abstract
Liquid droplets of three commercial Fe-Ni–based alloys were undercooled to different temperatures by electromagnetic levitation and quenched. Discontinuous changes in the grain size and microstructure as a function of melt undercooling (ΔT) were observed in all three alloys. At ΔT < 80 K, fine, equiaxed grains with a substructure consisting of spherical elements were observed. In the range 80 K < ΔT < 155 K, the microstructure consisted of colonies of columnar dendrites. The colonies were two orders of magnitude larger than the equiaxed grains reported at lower ΔT. At ΔT > 155 K, the equiaxed grains with a substructure of spherical elements returned. The critical undercoolings at which the microstructural transitions occur (ΔT * 1 = 80 K and ΔT * 2 = 155 K) show good agreement with those for similar binary systems. The results were successfully described by calculating the time needed for breakup of the primary dendrites as a function of ΔT and comparing this to the time during which the sample temperature is above the solidus due to recalescence.
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Acknowledgments
The authors thank H.-G. Lindenkreuz for performing the quenching experiments, B. Bartusch for the DSC measurements, and Dr. P.K. Galenko (DLR Köln) for helpful discussions. Financial support for this work was provided by the European Space Agency under the MAP, Project No. AO 99-101.
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Manuscript submitted April 24, 2008.
Appendix I
Appendix I
Calculation Parameters
Parameter (Unit) | P36 | M50 | M79 | Source |
---|---|---|---|---|
x (at. pct) | Fe-34.85Ni-0.7C | Fe-48.17Ni-0.09C | Fe-84.11Ni-0.1C | |
k Fe-Ni | 0.944 | 0.988 | 0.98 | [27]** |
k Fe-C | 0.174 | 0.205 | 0.205 | [28]** |
m l(Fe-Ni) (K/at. pct) | −1 | −0.15 | 0.65 | [27]** |
m l(Fe-C) (K/at. pct) | −16.9 | −17.8 | −17.8 | [28]** |
T l (K) | 1750 | 1733 | 1727 | DSC* |
T s (K) | 1726 | 1710 | 1702 | DSC* |
ΔH f (J/g) | 304 | 322 | 311 | DSC* |
C pliq at T l (J/g/K) | 0.76 | 0.75 | 0.74 | [27]** |
C psol at RT (J/g/K) | 0.68 | 0.68 | 0.67 | [27]** |
ρ liq at T l (gcm−3) | 7.55 | 7.55 | 7.55 | [29]† |
ρ sol at RT (gcm−3) | 8.1 | 8.25 | 8.7 | |
α liq at T l (m2/s) | 4.92 × 10−6 | 4.88 × 10−6 | 4.86 × 10−6 | [29]† |
η liq at T l (mPas) | 0.75 | 0.74 | 0.71 | [30]** |
D liq (m2/s) | 6 × 10−9 | 6 × 10−9 | 6 × 10−9 | assumed |
V DF (m/s) | 3 | 3 | 3 | assumed |
V D (m/s) | 25 | 25 | 25 | assumed |
d o (m) | 8.52 × 10−10 | 7.84 × 10−10 | 7.89 × 10−10 | calculated |
μ K (ms−1 K−1) | 1.01 | 2.95 | 1.095 | calculated |
ε c (pct) | 2 | 2 | 2 | assumed |
a 1, a 2, σ 0 | 0.3, 0.1, 30 | 0.3, 0.1, 30 | 0.3, 0.1, 30 | assumed |
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Woodcock, T., Shuleshova, O., Gehrmann, B. et al. Microstructural Transitions in Commercial Fe-Ni–Based Soft-Magnetic Alloys Quenched from Undercooled Liquid Droplets. Metall Mater Trans A 39, 2906–2913 (2008). https://doi.org/10.1007/s11661-008-9635-x
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DOI: https://doi.org/10.1007/s11661-008-9635-x