Membrane Gas Separation


Part II  Nanocomposite (Mixed Matrix)



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206. Membrane Gas Separation

Part II 
Nanocomposite (Mixed Matrix) 
Membranes 



Membrane Gas Separation Edited by Yuri Yampolskii and Benny Freeman
© 2010 John Wiley & Sons, Ltd

Glassy Perfl uorolymer – Zeolite 
Hybrid Membranes for Gas 
Separations
Giovanni Golemme 
a,b
, Johannes Carolus Jansen 
b
, Daniela Muoio 
a
, Andrea Bruno 
a

Raffaella Manes 
a
, Maria Giovanna Buonomenna 
a
, Jungkyu Choi 
c

and Michael Tsapatsis 
c


a
 Universit à della Calabria, Dipartimento di Ingegneria Chimica e dei Materiali, and INSTM 
Consortium, Rende, Italy
 
b
 Istituto per la Tecnologia delle Membrane, ITM - CNR, Rende, Italy
c
 University of Minnesota, Department of Chemical Engineering and Materials Science, 
Minneapolis, USA
6.1
Introduction 
Commercial polymeric membranes are cheap, but very often not suffi ciently permselec-
tive. For any given gas pair, polymers typically show high selectivities with modest 
permeabilities, or high permeabilities coupled with reduced selectivities, so that in a 
selectivity vs. permeability log – log plot all polymers fall below a so - called upper bound 
line [1] . On the other hand, inorganic membranes are often very permselective, easy to 
clean, thermally and chemically resistant, but are usually expensive, brittle, diffi cult 
to be prepared in a reproducible way, and are typically characterized by a low surface -
to - volume ratio in modules which, in turn, affects industrial applications (increased dead 
volume, need of larger compressors) and therefore translates into higher investment and 
running costs. 
Mixed - matrix membranes (MMMs), also referred to as hybrid membranes, contain a 
separating layer made of a continuous phase (usually a polymer) embedding a second


114
Membrane Gas Separation
dispersed phase, the chemical nature of which is different. They represent a viable 
opportunity for enhancing the separation capabilities of polymeric membranes for gas 
separation (GS). The combination of two materials with different gas diffusivity and 
solubility, in fact, allows a combination of high permselectivity of the fi ller (e.g. carbon 
molecular sieves, zeolites, inorganic particles) with an ease of production of polymeric 
membranes [2] . 
In general, the preparation of defect - free MMMs is not an easy task, especially dealing 
with rigid fi llers in glassy polymers. In fact, the poor adhesion between the two phases 
can produce voids at the interface and preferential paths for the diffusing species, which 
spoil the selectivity of the composite membrane [3] . This problem is particularly severe 
for Hyfl ons AD and Tefl ons AF, high free volume, amorphous and glassy perfl uoropoly-
mers with interesting GS properties for hydrocarbon mixtures, for the sweetening of 
natural gas and for the N 
2
/CH 
4
separation [4] : the well - known diffi culty of sticking 
anything on the surface of perfl uorinated polymers, such as polytetrafl uoroethylene, can 
be rationalized by considering their very low solubility parameters [5] . In fact, in the 
literature the only composite membranes based on amorphous glassy perfl uoropolymers 
are made of dispersions of non - porous nano - sized amorphous SiO 
2
in Tefl on AF 2400 
[6] and AF 1600 [7] . SiO 
2
nanoparticles in Tefl ons AF interfere with the packing ability 
of the polymer and increase the amount of free volume. The increase in the permeability 
of large, condensable molecules exceeds the one of small molecules, thereby decreasing 
the intrinsic size selectivity of the polymer: as a consequence, a selectivity reversal for 
the n - butane/CH 
4
pair takes place above a 18 wt % SiO 
2
content in Tefl on AF 2400 [6] . 
The dispersion of suitable porous fi llers inside such polymers offers a new degree of 
freedom for improvement of their permselectivity, by enhancing the solubility selectivity 
and/or the mobility selectivity or, in the limiting case, the sieving capabilities of the 
zeolites. The main goal of this work is to demonstrate that porous fi llers can be effectively 
dispersed in amorphous glassy perfl uoropolymers. Silicalite 

1, the siliceous form of 
ZSM - 5 (structure topology MFI) [8] , has a three - dimensional channel structure with 
straight channels of 5.4 – 5.6 Å along the b axis and zigzag channels of 5.6 Å in the ac
plane. The zigzag channels connect subsequent layers of straight channels. There were 
several reasons for choosing it as the porous fi ller: fi rst, because this zeolite is hydrophobic 
and, unlike zeolites containing aluminium, its pores do not absorb signifi cant amounts of 
moisture; secondly, because it can be easily prepared in a wide range of sizes and shapes; 
and fi nally, because the sorption and mobility data of several gases and vapours in it are 
already available in the literature. 
Several mixed matrix membranes made of silicalite - 1 crystals of different size and 
shape embedded in Tefl on AF 1600, Tefl on AF 2400 and Hyfl on AD 60X have been 
prepared. The gas permeation properties of the membranes have been tested with pure 
gases, and some experiments with n - C 
4

10
/CH 
4
mixtures have also been carried out on 
silicalite - 1/Tefl on AF 2400 membranes.

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