Solidification and cast structures
Which statement about constitutional supercooling, which causes an initially planar solid–liquid interface to become uneven in directional solidification of an alloy, is correct? Take an alloy with k < 1.
- ARejected solute lowers the liquidus temperature at the interface, and it rises with distance, so if the actual temperature gradient is small the liquid ahead falls below its liquidus temperature
- BSolute in the liquid ahead of the interface is absorbed into the solid and depleted, raising the liquidus temperature, so the larger the temperature gradient the more easily the liquid ahead becomes supercooled
- CA negative temperature gradient, with temperature falling from the interface into the liquid, arises from the latent heat of solidification, and this thermal undercooling destabilizes the interface only in alloys
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Answer: A. Rejected solute lowers the liquidus temperature at the interface, and it rises with distance, so if the actual temperature gradient is small the liquid ahead falls below its liquidus temperature
With k < 1, solute rejected at the interface piles up ahead of it, so the liquid at the interface is enriched and its liquidus temperature is lower. Away from the interface the concentration returns to the original C₀, so the liquidus temperature rises with distance. If the actual temperature gradient G is smaller than this gradient of the liquidus temperature, a layer of liquid below its liquidus temperature, that is, supercooled liquid, forms ahead of the interface. This is constitutional supercooling, and because small bumps on the interface grow toward the more supercooled side, the planar interface breaks down. The liquid ahead becomes enriched, not depleted, and a larger temperature gradient makes constitutional supercooling less likely. Thermal undercooling from a negative temperature gradient is a separate phenomenon that does not depend on solute and occurs in pure metals as well.
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