29.06.2013 Views

a) b - École Polytechnique de Montréal

a) b - École Polytechnique de Montréal

a) b - École Polytechnique de Montréal

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

where μ is the chemical potential of component i, ni is the number of moles, Ai is the interfacial<br />

i<br />

area, and γ ij is the interfacial tension between components i and j. Thus, the phase structure of a<br />

polymer blend can be predicted by comparing the Gibbs free energies of the different structures.<br />

In their work on a HDPE/PS/PMMA blend, numerous conditions were assumed to simplify the<br />

study such as equal value of the first term of the equation for all types of morphology. For<br />

further simplification, they assumed that numbers of droplets of minor phases were equal to each<br />

other, which lead to a big error.<br />

The second term is simplified further and rewritten as:<br />

Equation 2-32.<br />

Equation 2-33.<br />

Equation 2-34.<br />

1 1 2<br />

1<br />

3<br />

( ∑ Aγ<br />

) = ( 4π<br />

) 3 ⎡ n 3 x γ + n 3γ<br />

⎤(<br />

3V<br />

)<br />

i<br />

1 1<br />

2<br />

1<br />

3<br />

( ∑ Aγ<br />

) = ( 4π<br />

) 3 ⎡ n 3 ( 1+<br />

x)<br />

γ + n 3γ<br />

⎤(<br />

3V<br />

)<br />

i<br />

( ) ( ) ( ) 3<br />

1 1 2<br />

1<br />

2<br />

2<br />

3 3 3<br />

3<br />

3<br />

∑ Aγ<br />

= 4π<br />

⎡ n x γ + n ( 1+<br />

x)<br />

γ ⎤ 3V<br />

i<br />

ij<br />

ij<br />

ij<br />

B+<br />

C<br />

B<br />

C<br />

C<br />

B<br />

where Vi is the volume fraction of phase I,<br />

V<br />

V<br />

C<br />

⎢⎣<br />

⎢⎣<br />

⎢⎣<br />

B<br />

B<br />

B<br />

AB<br />

BC<br />

AB<br />

C<br />

C<br />

AC<br />

C<br />

⎥⎦<br />

BC<br />

c<br />

⎥⎦<br />

2<br />

3<br />

AC<br />

⎥⎦<br />

c<br />

24<br />

B x = , nB and nC are numbers of particles of B and<br />

C phases. The most stable morphology is predicted by calculation of the values of ( ∑ Aγ )<br />

which correspond to the value of the Gibbs energy of mixing.<br />

Obviously, the Harkins equation and the Guo mo<strong>de</strong>l are purely thermodynamic equations in<br />

which some other factors influencing the morphology, such as rheological parameters, have not<br />

been consi<strong>de</strong>red. Although in measuring interfacial tensions of polymer pairs by various methods<br />

such as the breaking thread and pen<strong>de</strong>nt drop, viscosities of the components are taken into<br />

account, the effect of elasticity is still neglected. In the method <strong>de</strong>veloped by Guo to calculate the<br />

free energy compared to Harkins equation, concentration of components is also contributed to<br />

<strong>de</strong>termine the kind of morphology as well and it is more modified. Researchers use both the<br />

spreading coefficients and the minimal free energy surface mo<strong>de</strong>l to predict the morphologies of<br />

polymer blends (Guo, Gvozdic, et al., 1997; Guo, Packirisamy, et al., 1997; Hara & Sauer, 1998;<br />

Hobbs, et al., 1988; Horiuchi, Matchariyakul, Yase, & Kitano, 1997; Nauman & He, 2001;<br />

i<br />

2<br />

3<br />

ij<br />

c

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!