suggests that the crystalline phase can be attributed to the increase in gas diffusivity
in crystalline and liquid crystalline polymers.
Figure 8 presents the relationship between gas diffusivity and solubility in crystalline
and liquid crystalline polymers, with the amorphous data for comparison (Kanehashi
and Nagai 2005). Gas permeability is a product of the solubility and diffusivity, as
shown in Eq. 1. Compared with solubility, the gas diffusivities in crystalline, liquid
crystalline, and glassy amorphous polymers are widely distributed. For example, O 2
diffusivity varies from 3.90 Â 10
À9 to 6.70 Â 10
À7 for glassy amorphous polymers,
1.10 Â 10
À9 to 1.37 Â 10
À6 for crystalline polymers, and 6.20 Â 10
À11 to
7.65 Â 10
À7 cm
2 s
À1 for liquid crystalline polymers. Oxygen solubility varies from
0.15 to 1.44 for amorphous polymers, 0.00680 to 0.190 for crystalline polymers, and
0.00480 to 0.177 cm
3 (STP) (cm
3 atm)
À1 for liquid crystalline polymers. These results
suggest that the permeability of non-condensable gases, such as O 2 and N 2 , in
crystalline, liquid crystalline, and glassy amorphous polymers depend more on diffusivity rather than on solubility. Gas solubility in crystalline and liquid crystalline
polymers shows lower values, and diffusivity shows higher values than that in glassy
amorphous polymers at the same gas permeability (Fig. 8). Thus, the gas transport
behavior in crystalline and liquid crystalline polymers can be different from glassy
amorphous polymers. This difference is attributed to the presence of crystal structures
assuming they follow similar solution/diffusion mechanisms. Therefore, gas transport
properties in crystalline and liquid crystalline polymers could be strongly affected by
the crystal structure parameters, such as crystal size and distribution.
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19 Gas Permeation and Barrier Properties of Liquid Crystalline Polymers
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