After steel sheets (0.37wt%Si) pre-electroplated with a thin layer of pure Fe were immersed in molten zinc for various time, the change in the microstructure of the galvanized coating on the steel and the change of α-Fe/Γ interface were studied. The EDS (energy dispersive sepectroscopy) results show that excessive silicon accumulates on the surface of the steel substrate due to the low solubility of silicon in the Γ layer after the Fe layer is depleted by the increasing growth of the compound layers. With the movement of α-Fe/Γ interface towards the substrate by the Fe/Zn reaction, silicon-rich α-Fe peels off from the substrate and breaks into particles. The particles, much like an inert marker in a Kirkendall effect experiment, move towards the δ layer through the Γ layer because silicon-rich α-Fe can not be adsorbed in the Γ layer. On reaching the δ/Γ interface,the particles quickly dissolve in the δ layer, and accelerate its growth, resulting in the gradual disappearance of the Γ layer. At the same time, the normal coating is quickly changed into coatings typical of reactive steels as silicon dissolved in the δ layer soon diffuses toward the ζ layer. A similar process may happen in the initial stage of galvanizing reactive steels on a small scale, although it is hard to be observed.
参考文献
[1] | R W Sandlin .[J].Wire Wire Products,1941,16:28. |
[2] | X P Su;N Y Tang;J M Togurp .[J].Canadian Metallurgical Quarterly,2001,40(03):377. |
[3] | J Mackowiak;N R Short .[J].International Metals Reviews,1979,24:1. |
[4] | J Foct;P Perrot;G Reumont .[J].Scripta Metallurgica et Materialia,1993,28:1195. |
[5] | G Reumont;P Perrot;J Foct .[J].Journal of Materials Science,1998,33:4759. |
[6] | J Foct;P Perrot;G Reumont.Proc,17th Int Galva Conf[M].Paris:European General Galvanizing Association,1994:1. |
[7] | W D Schulz;P Schubert;M Thiele.Proc,20th Int Galva Conf[M].Amsterdam:European General Galvanizing Association,2003:61. |
[8] | M S Kozdras;P Niessen .[J].Metallograghy,1989,22:253. |
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