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Late stages of spinodal decomposition

Now, we turn our attention to late stages of spinodal decomposition. Since the phase separation in binary mixture is intrinsically a nonlinear phenomenon, a number of nonlinear theories have been put forward on the basis of statistical consideration, notably the LBM (Danger, Baron k Miller) (H) and BS (Binder k Stauffer) (12) theories. Both theories predicted the power law scheme rather than the exponential growth of the structure... [Pg.278]

Fig. 12. Plot of the scaled structure factor F(x) in the late stage of spinodal decomposition for an A/B binary blend as a function of the reduced scattering vector x [71]... Fig. 12. Plot of the scaled structure factor F(x) in the late stage of spinodal decomposition for an A/B binary blend as a function of the reduced scattering vector x [71]...
Siggia E (1979) Late stages of spinodal decomposition in binary mixtures. Phys Rev A20 595-605... [Pg.552]

Siggia, E.D. (1979) Late stages of spinodal decomposition in binary mixtures, Phys. Rev. A 20, 595. Cook, H.E. (1970) Brownian motion in spinodal decomposition, Acta Metall. 18, 297. [Pg.165]

Fig. 3.35. Structure development during the late stages of spinodal decomposition observed for a PS/PBrxS-(l l) mixture. Micrographs were obtained during annealing at 200°C (< Tc = 220°C) for 1 min (left), 3 min (center) and 10 min (right) [17]... Fig. 3.35. Structure development during the late stages of spinodal decomposition observed for a PS/PBrxS-(l l) mixture. Micrographs were obtained during annealing at 200°C (< Tc = 220°C) for 1 min (left), 3 min (center) and 10 min (right) [17]...
Fig. 3.36. Light scattering curves obtained for a PB (M = 5.8 10 )/PIP (M = mixture during the late stage of spinodal decomposition at the indicated temperatures top] curves for 45 °C and 60 °C are shifted by constant amounts in vertical direction). Each curve contains measurements for different times and these superpose exactly. Time dependence of the interfacial area per unit volume, O12, in agreement with a power law O12 t, as indicated by the straight line with slope -1 bottom). Data from Takenaka and Hashimoto [24]... Fig. 3.36. Light scattering curves obtained for a PB (M = 5.8 10 )/PIP (M = mixture during the late stage of spinodal decomposition at the indicated temperatures top] curves for 45 °C and 60 °C are shifted by constant amounts in vertical direction). Each curve contains measurements for different times and these superpose exactly. Time dependence of the interfacial area per unit volume, O12, in agreement with a power law O12 t, as indicated by the straight line with slope -1 bottom). Data from Takenaka and Hashimoto [24]...
Figure 5.11 t(a) Schematic representation of (ill) interphase and local scale (b) LS and SANS the hierarchical structures that develop during profile in the late stage of SD for a DPB/HPI the late stage of spinodal decomposition (SD) sample. Reproduced with permission from (i) global, (II) asymptotic (or interface), and Reference [89]. [Pg.173]


See other pages where Late stages of spinodal decomposition is mentioned: [Pg.155]    [Pg.156]    [Pg.62]    [Pg.266]    [Pg.278]    [Pg.354]    [Pg.19]    [Pg.24]    [Pg.36]    [Pg.19]    [Pg.417]    [Pg.64]    [Pg.343]    [Pg.353]    [Pg.663]    [Pg.57]    [Pg.183]    [Pg.188]    [Pg.34]    [Pg.129]    [Pg.519]    [Pg.613]    [Pg.75]    [Pg.188]    [Pg.114]   
See also in sourсe #XX -- [ Pg.278 , Pg.279 ]




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