Solidification and cast structures
Most pure metals grow with a smooth, rounded solid–liquid interface, whereas Si and Bi tend to grow bounded by flat crystal faces (facets). Which is the correct guide to explain this difference?
- AThe higher the melting point, the harder it is for interface atoms to move, and every substance melting above about 1000 °C grows with facets
- BThe lower the thermal conductivity, the harder it is for latent heat to escape from the interface, and locally overheated faces become facets
- CThe larger the entropy of fusion (ΔSf/R greater than about 2), the flatter the interface is on the atomic scale, giving facets
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Answer: C. The larger the entropy of fusion (ΔSf/R greater than about 2), the flatter the interface is on the atomic scale, giving facets
In Jackson's theory the roughness of the interface is set by α ≈ ΔSf/R, the entropy of fusion divided by the gas constant. For most metals α is about 1, so the interface is atomically rough and atoms can attach anywhere, and growth proceeds continuously with a small undercooling (non-faceted). For Si, α is large at about 3.6, the interface is atomically flat and atoms can attach only at steps, so the crystal grows bounded by facets and needs a larger undercooling. It is not the melting point that decides this; iron, with a melting point of about 1540 °C, is non-faceted. Thermal conductivity is not a main factor in the shape either. The plate-like eutectic Si in Al-Si alloys is also a result of the faceted growth of Si.
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