Unformatted text preview: ys positive).
Forming a surface always raises the energy.
G=V*Gv+ sigma*A = r^3 + r^2
When r is small (r<1), free energy is positive. When r is big(r>1), free energy is negative.
When the temperature difference from the transformation temperature is small, the driving
force of nucleation is also small. Thus, the activation energy/barrier is bigger and the rate is
nucleation limited. If the temperature difference is large, nucleation is easier due to a bigger
driving force. Thus, the barrier is smaller and nucleation is easier, so the rate is growth
If the upper arrow cools material, the final microstructure contains nuclei of Beta
almost exclusively in the grain boundaries of alpha.
It is easier to nucleate on grain boundaries. The barrier to nucleation is the formation of
surface energy but at grain boundaries, it wipes out some of the interfacial energy of the
already existing grains.
If the system is cooled slowly from the alpha phase, it allows enough time for the diffusion of
beta particles. Thus, the beta diffuses to the boundaries...
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This note was uploaded on 01/26/2014 for the course ENG 45 taught by Professor Stephenmorris during the Fall '12 term at Berkeley.
- Fall '12