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a) b - École Polytechnique de Montréal

a) b - École Polytechnique de Montréal

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Addition of a low concentration of HDPE to the system leads to the encapsulation of HDPE<br />

droplets in a highly continuous PS network resulting in a bi-continuous/dispersed phase<br />

morphology and a slight reduction of PS continuity(point b in Figure 6-11). A further increase of<br />

HDPE phase generates a tri-continuous morphology(type II) where the coalescence of HDPE<br />

droplets forms a continuous phase of HDPE in highly continuous PS (point c in Figure 6-11).<br />

Note that at point c for the 30/30/40 HDPE/PS/PMMA blend, the continuity level of PS is<br />

lowered to 68% Such a <strong>de</strong>crease in the continuity level is attributed to the entrapment of some<br />

parts of the PS phase in the PMMA network. Point d indicates the expected drop in continuity<br />

after the formation of the type I tricontinuous structure at point e. At point e, the 82% HDPE<br />

volume fraction corresponds to the 50/10/40 HDPE/PS/PMMA blend. This type I tri-continuous<br />

structure with a PS continuity of 76% represents the case where 50% HDPE and 40% PMMA<br />

form a co-continuous structure with a thin PS layer situated at the HDPE/PMMA interface.<br />

Finally, replacing all the PS with HDPE results in a (60%HDPE matrix/40%PMMA dispersed<br />

phase) blend (point f in Figure 6-11).<br />

Local maximum continuity of 78% is obtained for 48/12/40 HDPE/PS/PMMA blend from Figure<br />

6-11. The most important observation for scheme a, where the PMMA concentration is held at<br />

40%, is that due to the thermodynamic limitations of spreading, the system is never able to form<br />

PS droplets even at a very low concentration of PS. PS always spreads between HDPE and<br />

PMMA in or<strong>de</strong>r to separate those two components. Thus even the smallest amount of PS in<br />

scheme a) presents a layer structure as opposed to droplets.<br />

In scheme (b), from Figure 6-10, the concentration of the PS phase is kept constant at 10%<br />

volume fraction and the concentration ratio of the two other phases changes. In Figure 6-12, the<br />

continuity of the PS phase following Scheme b is examined as a function of the % concentration<br />

of HDPE in (HDPE plus PMMA) where HDPE plus PMMA always equals 90% in the ternary<br />

blend with PMMA. Thus, 100% HDPE refers to the 90%HDPE/10%PS blend, while 50% HDPE<br />

in Figure 6-12 refers to the 45%HDPE/10%PS/45%PMMA blend. This scheme allows for the<br />

study of the effect of the composition of the inner phase(HDPE) and the outer phase(PMMA)<br />

on the morphology of the middle phase(PS). It is interesting to note that in this case, the PS<br />

continuity curve is almost symmetric. At 0% HDPE, the continuity of PS is zero due to the<br />

presence of PS droplets within the matrix of PMMA(point a in Figure 6-12).<br />

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