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Extra resources for à ост Кристаллоь / Rost Kristallov / Growth of Crystals: Volume 11
The initial nucleation occurred at large helicoidal dislocations, not at smaller dislocations. These experimental difficulties made it impossible to establish where the nucleation occurred (on edge or screw dislocations), and also where the precipitate of the second phase developed. (c) Precipitate Growth In the stage shown in Fig. 5, new particles of the thickened phase are formed, as at a and b, which are absent in Fig. 4. Figures 4 and 5 together show that there is also a change in the disposition of the dislocations at this stage.
Ya. 1. Frenkel', The Kinetic Theory of Liquids [in Russian], Izd. AN SSSR, Moscow (1959). J. B. Zeldovich, Acta Physicochim. URSS, 18:1 (1943). D. Bahat, J. Mater. , 4:847 (1969). R. Kaishev, Bull. Bulg. Set. ), 1:100 (1950). R. Becker, Annal. Physique, 32:128 (1938); D. Turnbull, In: Impurities and Defects [Russian translation], Metallurgizdat, Moscow (1960), p. 141. M. L. Lyubimov, Glass-Metal Joints [in Russian], Gosenergoizdat, Moscow (1957). B. Routh, Glass in Electronics [Russian translation], Sov.
In that case, (2), (6), and (lla) give the activity for a given melt as (12) Here f3o/2Y characterizes the chemical and structural factors (for ~a = 0); the substrate activation is defined by the second term in (12). Figure 2 has been constructed in accordance with (2) with the ~a for Graham glass and the various metals mentioned above, which serves to explain the above series in q, (Table 1). An interesting point is that the chemically less active metals in Fig. ; with y = 100 ergs/cm2 for Au, Rh, Ir, we get from (12) that f30 = 163 ergs/cm2 , while for Ag, Cu, Pd, and Pt we get that f30 is 186 ergs/cm2.