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a) b - École Polytechnique de Montréal

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Reignier et al.(Reignier, et al., 2003) studied the effect of different factors on the composite<br />

droplet formation. They showed the influence of elasticity on composite droplet formation by<br />

introducing the dynamic interfacial tension term taken from VanOene(Vanoene, 1972) in the free<br />

energy mo<strong>de</strong>l <strong>de</strong>veloped by Guo et al.(Guo, Packirisamy, et al., 1997), and <strong>de</strong>veloped new<br />

equations for the interfacial free energies in conditions of dynamic mixing:<br />

Equation 2-35.<br />

Equation 2-36.<br />

Equation 2-37.<br />

2 ⎡ Ri<br />

⎤ 2 ⎡ Ri<br />

( ∑ Aγ<br />

) = 4πR<br />

γ + ( N − N ) + 4πR<br />

γ + ( N − N )<br />

i<br />

⎢<br />

⎣<br />

2 ⎡ Re<br />

⎤ 2 ⎡ Ri<br />

( ∑ Aγ<br />

) = 4πR<br />

γ + ( N − N ) + 4πR<br />

γ + ( N − N )<br />

i<br />

ij B+<br />

C<br />

ij B<br />

C<br />

⎢<br />

⎣<br />

2 ⎡ Re<br />

⎤ 2 ⎡ Ri<br />

⎤<br />

( ∑ Aiγ<br />

ij ) C = 4πRe<br />

⎢γ<br />

CA + ( N1,<br />

C − N1,<br />

A ) ⎥<br />

+ 4πRi<br />

⎢γ<br />

BC + ( N1,<br />

B − N1,<br />

C ) ⎥⎦<br />

B<br />

e<br />

i<br />

⎣<br />

BA<br />

BA<br />

Normal stress differences for the phases A, B, and C are referred to by N1, γ ij is the interfacial<br />

tension between the components i and j, and the internal and external radius of the core-shell<br />

droplets are shown by Ri and Re, respectively. Reignier et al.(Reignier, et al., 2003) indicated that<br />

the viscosity ratio estimated at a constant shear stress rather than at a constant shear rate is<br />

accurate to study the effect of viscosity ratio on the morphology because shear stress is more<br />

continuous at the interface between the dispersed phase and the matrix phase.<br />

The effect of molecular weight of phases on the encapsulation process was<br />

investigated(Reignier, et al., 2003). The equilibrium morphology for HDPE/low molecular<br />

weight PS/low molecular weight PMMA illustrates that PS encapsulates PMMA (Figure 2-6a).<br />

When components were replaced by high molecular weight PS and high molecular weight<br />

PMMA, an inversion in encapsulation occurred and PMMA encapsulated PS (Figure 2-6b). They<br />

related this discrepancy to the high viscosity of PS that does not allow PMMA to be<br />

encapsulated. Finally, consi<strong>de</strong>ring all the observations, they conclu<strong>de</strong>d that interfacial energy<br />

reduction is the main driving force controlling encapsulation effects and that the viscosity ratio<br />

and the absolute viscosity have little influence on encapsulation phenomena in composite<br />

droplets.<br />

6<br />

6<br />

6<br />

1,<br />

B<br />

1,<br />

B<br />

1,<br />

A<br />

1,<br />

A<br />

⎥<br />

⎦<br />

⎥<br />

⎦<br />

⎦<br />

i<br />

i<br />

⎢<br />

⎣<br />

⎢<br />

⎣<br />

⎣<br />

CA<br />

CB<br />

6<br />

6<br />

6<br />

1,<br />

C<br />

1,<br />

C<br />

1,<br />

A<br />

1,<br />

B<br />

28<br />

⎤<br />

⎥<br />

⎦<br />

⎤<br />

⎥<br />

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