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a) b - École Polytechnique de Montréal

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where the number of segments of the two polymers are represented by M1 and M2, and Vs is the<br />

volume of the segments(Scott, 1949).<br />

2.1.2 Immiscible Polymer Blends<br />

Most polymer blends are immiscible, showing phase-separated mixture. Morphology of<br />

multiphase polymer blend materials can be controlled by controlling the interfacial chemistry<br />

and the microstructure. Three parameters <strong>de</strong>termine the properties of these multiphase materials:<br />

properties of the component polymers, interaction and adhesion between phases and<br />

morphology(Utracki, 1998). The properties of multiphase materials are strongly <strong>de</strong>pen<strong>de</strong>nt on<br />

their phase morphology. Controlling parameters on morphology of polymer blends inclu<strong>de</strong><br />

composition of phases, kinematic or rheological properties (elasticity and viscosity), processing<br />

conditions (shear stress, processing temperature,…), and the most important one which is a<br />

thermodynamic parameter: the interfacial tension of the pair of phases(Favis, 2000; Steinmann,<br />

Gronski, & Friedrich, 2001). Thermodynamics of interfaces <strong>de</strong>fines the interfacial tension<br />

between two phases as the area <strong>de</strong>rivative of the surface free energy per unit area of an interface.<br />

Equation 2-11.<br />

Equation 2-12.<br />

⎛ G ⎞<br />

⎜<br />

∂<br />

γ ⎟<br />

ij = and<br />

⎜ A ⎟<br />

⎝ ∂ ij ⎠<br />

⎛ F ⎞<br />

⎜<br />

∂<br />

γ ⎟<br />

ij =<br />

⎜ A ⎟<br />

⎝ ∂ ij ⎠<br />

T , P,<br />

n<br />

T , V , n<br />

where G is the Gibbs free energy, F is the Helmholtz free energy of the whole system, and Aij is<br />

the interfacial area between phases i and j.<br />

There are different ways to measure interfacial tension of two polymers, including theoretical<br />

methods such as Antonoff’s rule(Antonoff, 1942; Antonoff, 1907), the Good and Girifalco<br />

equation(Girifalco & Good, 1957; Good & Girifalco, 1964), and harmonic mean equation, and<br />

experimental methods such as the breaking thread, pendant drop, and sessile drop methods.<br />

12

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