The ‘
Umklappen’ which is the process of the formation of one martensite (α') needle, takes place in an extremely short time. This process, therefore, must be adiabatic and needs no diffusion of atoms, that is, no change of composition, consequently, when the austenite (γ) is cooled from point X (Fig. 2 and 3). it passes through point C' where the transformation would occur if it were isothermal, and yet the state does not change before the temperature falls to point K, where the entropy of γ is equal to that of α' of the same internal energy.
Moreover since the
Umklappen is accompanied by the internal stress which needs some energy (W), it does not take, place even when K is reached, But it does for the first time when U is reached at which the internal energy of γ is larger by the amount W than that of α'.
The larger the stre_??_s is, the lower the temperature of U. Hence the so-called Ar'', point should coincide with the temperature of U of the α' needle having the smallest W, the existence of the temperature range of the transformation as is observed is due to the preserce of α' needles of various values of W. In the case of an extraordinary high cooling velocity, the super-cooling of point U may occur, although it does not occur in the case of the ordinary quenching. The degree of the super-cooling depends upon the activation energy for
Umklappen Q', which has the different value for each α' needle in general.
This phenomenon also therefore. broadens the range of the transformation temperature.
Thus the nature of α' formation is markedly different from that of the growth-process as in the case of the super-cooled A
3 or Ar' transformation. It is to be concluded that the Ae'' line has no direct relation to the extension of α side line of A
3 transformation (GPA) in the Fe-C equilibrium diagram.
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