Relationship between substructure resistance and gas separation

DOI: 10.1021/ie00056a024. Publication Date: August 1991. ACS Legacy Archive. Cite this:Ind. Eng. Chem. Res. 30, 8, 1837-1840. Note: In lieu of an abst...
1 downloads 0 Views 523KB Size
Znd. Eng. Chem. Res. 1991,30,1837-1840

1837

Relationship between Substructure Resistance and Gas Separation Properties of Defect-Free Integrally Skinned Asymmetric Membranes Ingo Pinnau and William J. Koros* Department of Chemical Engineering, The University of Texas at Austin, Austin, Texas 78712 Integrally skinned asymmetric membranes consist of an ultrathin skin layer supported by a microporous substructure. Optimum membrane properties are obtained if the skin layer is defect-free and its thickness is minimized. A series resistance model shows that the minimum desirable skin thickness of defect-freeintegrally skinned asymmetric membranes having the intrinsic selectivity of the membrane material is limited by the resistance of the microporous substructure. Asymmetric membrane substructures show selectivities essentially equal to those predicted by Knudsen flow. However, pressurenormalized fluxes of substructures can vary by several orders of magnitude. Model calculations reveal that the pressure-normalized flux of the fast-permeating gas component through the substructure has to be -10 times higher than that of the component through the skin layer to achieve at least 90% of the intrinsic selectivity of the membrane material. The validity of the model is demonstrated for defect-free asymmetric polycarbonate and polyimide membranes. These considerations become increasingly important as higher performance polymeric materials are employed in membrane separation applications.

Back p ound Integrally skinned asymmetric membranes are made by a phase inversion process (Kesting, 1985). The resulting asymmetric membranes generally consist of a thin skin layer supported by a microporous substructure. It is generally believed that the gas transport properties of asymmetric membranes are predominantly determined by the resistance of the skin layer (Strathmann et al., 1971; Haraya et al., 1986). Therefore, most developments in the optimization of asymmetric membranes focused mainly on the minimization of the skin layer thickness. However, it is very difficult to prepare simultaneously ultrathin (skin-layer thickness