Abstract

In this article, the influences of cooling rate on the microstructure evolution and liquid–liquid phase separation behavior of Cu–16.2Fe–4.5 P immiscible alloys were systematically investigated. With the cooling rate changing from 1580 K/s to 30 K/s, Cu–16.2Fe–4.5 P metallic samples were still composed of Cu, Fe2P, Fe3P and Cu3P phases according to XRD analyses. With the cooling rate as 1580 K/s, it was observed that Fe–P particles as secondary phase exhibited nearly spherical shape with a uniform dispersion in Cu-rich matrix, which was attributed to the suppressed Marangoni convection and Stokes motion. As the cooling rate decreasing to 30 K/s, an evolving core-shell structure in this alloy was observed to be formed due to the relatively sufficient liquid separation occurrence. Furthermore, it was found that a Fe2P layer was formed to be encapsulated secondary phase, in which Fe3P and Cu particles were also examined. In addition, the microstructure evolution mechanism of Cu–16.2Fe–4.5 P alloys with different cooling rate was also applied.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call