Current Opinion in Solid State and Materials Science 7 (2003) 407–412
Supercritical fluid applications in polymer nanocomposites David L. Tomasko *, Xiangmin Han, Dehua Liu, Weihong Gao Department of Chemical Engineering, The Ohio State University, Columbus, OH 43220, USA Received 6 October 2003; received in revised form 14 October 2003; accepted 14 October 2003
Abstract Supercritical fluids have been used to synthesize and foam a variety of polymer nanocomposite materials. There have been significant advances in developing and characterizing nanoscale structures and using supercritical fluids to alter properties at the nanoscale. In this work we summarize these advances and discuss foam properties generated using supercritical carbon dioxide as well as relevant fundamental properties of the system. Ó 2003 Elsevier Ltd. All rights reserved. Keywords: Nanocomposite; Supercritical; Carbon dioxide; Foam adsorption; Rheology
Major recent advances Nanoscale reinforced polymeric materials (aka polymer nanocomposites) provide an opportunity for combining the features of supercritical fluids with traditional polymer processing. Recent work emphasizes reducing the domain size of the dispersed component to achieve true nanoscale features. Advances include surface modification to exfoliate nanoclays, controlled synthesis in confined matrices, and better understanding of the role of supercritical CO2 in rheology and interfacial properties.
1. Introduction The Ôtop down’ approach to nanotechnology signifies the modification of microscale processing techniques to produce nanoscale features. Much of the recent work in using supercritical fluids (SCFs) for polymer composite materials falls into this vein and is the primary focus of this review. The term polymer nanocomposite is broadly defined to include a material consisting of two immiscible phases of which one is a polymeric material and one is present as a dispersed phase (or domain) with a nanoscale feature in at least one dimension. For example, the seminal work from Toyota R&D [*1,2] dem*
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onstrated a nanoclay platelet dispersed in a polymer matrix to improve the mechanical properties of the composite material. The nanoclay is a layered silicate which can be exfoliated into platelets with nanometer thickness and aspect ratios on the order of 103 . The application of supercritical fluids to the preparation of composites is through one of two approaches: in-situ polymerization of the dispersed phase in a SCFswollen polymer matrix, or dispersive mixing of the nanoscale phase into the polymer matrix using the SCF to reduce the matrix viscosity and/or nucleate nanoscale bubbles in the material. While the basic feasibility of the in-situ processes were demonstrated in the mid-1990s [**3,*4,**5,6], recent work has concentrated on reducing the dispersed phase domain size and isolating the nanoscale features in the composite materials.
2. In situ polymerization for polymer/polymer and polymer/inorganic composites In situ processes for producing nanocomposites apply a two-step procedure. Initially, the polymer substrates are infused with the precursor reactants dissolved in the SCF and then a reaction is induced (typically thermally) to generate a new dispersed phase. The SCF functions as a swelling agent for the polymer to enhance diffusion, a solvent for the precursor reactants and byproducts, and nonsolvent for the reaction products. The resulting nanoparticle or nanophase products are restrained from agglomerating by the polymeric continuous phase.
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2.1. Polymer/inorganic nanocomposites In order to obtain desired metal nanoparticles, the organometallic precursors have to be carefully selected or even synthesized to give acceptable solubility in the supercritical phase and easy reduction to pure metal. High thermal decomposition temperatures of the precursors can limit the range of suitable matrix polymers. The advantage of these systems is the relative ease of obtaining dispersed nanoparticles. Even in the initial reports using this technique, platinum particles of <50 nm were produced. Subsequent efforts have produced copper, silver, and iron nanoparticles in a variety of matrices [*7,8]. A practical polymer/inorganic hybrid device would need controllable long-range order of nanoscale metal domains over bulk dimensions. A clever approach is to use a SCF to pressure tune block copolymer selfassembly, where one polymer phase contains a functional group selectively bound to a metal precursor and then acts as a nanoscale template [**9,*10]. A key to this approach is the proper CO2 interaction with and control over the co-polymer self-assembled structures. 2.2. Polymer/polymer nanocomposites Applying a similar technique to produce polymer/ polymer nanocomposites is slightly more challenging due to the larger size of the product (polymer chain vs. atomic metal cluster) and higher mobility of the product due to stronger interactions with the matrix phase. In polymer/polymer nanocomposites several recent advances have been made to confine the polymerized phase to the nanoscale domain and characterize the dispersion more quantitatively. Recent progress demonstrates polymer blends and interpenetrating networks via SCCO2 (mainly polystyrene-based) [11,*13,14–16], some with nanoscale dispersed domains. The advance of note is the convincing demonstration that crystalline domains (or lamellae) in the matrix phase template the polymerization and maintain the dispersion of an amorphous nanophase [**17,**18].
3. Polymer/clay nanocomposites prepared in supercritical CO2 Using clay as filler, two idealized nanocomposites are possible: intercalated and exfoliated. Intercalation results from the penetration of polymer chains into the interlayer region of the clay with preservation of the ordered layer structure. Exfoliation involves extensive polymer penetration and crystallite delamination, with the individual nanometer-thick silicate platelets are randomly dispersed in the polymer matrix. Exfoliated
nanocomposites usually provide the best property enhancement due to the large aspect ratio and surface area of the clay. Depending on the polymer, intercalated and exfoliated polymer/clay nanocomposites can be obtained by means of either mechanically compounding or in-situ polymerization [19,**25]. However, none of these means is easy and straightforward. Therefore, the use of SCFs to both pretreat/delaminate silicate layers and to reduce melt viscosity is an attractive means of generating wellexfoliated polymer/clay nanocomposites for certain systems. Manke et al. [*26,27] recently patented two methods to produce PP/clay nanocomposites by the assistance of SCCO2 . The essential characteristic of the process is saturation of the clay followed by rapid depressurization to forcibly exfoliate the platelets with the expanding CO2 . A similar procedure was applied in extrusion foaming to make clay nanocomposites of high-density polyethylene (HDPE) and poly(trimethyleneterephthalate) (PTT) using SCCO2 [28]. Thirty-three percent increase in the typical clay d-spacing was realized for HDPE/clay nanocomposites with the assistance of SCCO2 , while a 10% increase was observed for PTT/clay nanocomposites.
4. Foaming Foaming comes naturally in SCF processing of polymers and there are several ways in which it is an active research area for nanocomposites. One is exploring the interaction of CO2 with surface-treated nanoparticles to influence composite foam properties and a second is the preparation of nanoporous polymers with well defined open pore structure with novel applications as low-k dielectrics, separation membranes, and drug delivery devices. 4.1. Nanocomposite foams with CO2 Compared to conventional micron-sized filler particles used in the foaming process, the extremely fine dimensions, large surface area, and intimate contact between particles and polymer matrix may greatly alter cell nucleation and growth. Nam et al. [29,30] foamed polypropylene/clay nanocomposites and showed that biaxial flow during cell growth induces the alignment of clay particles along the cell boundary. Han et al. [31,*32,33] prepared both intercalated and exfoliated polystyrene/nanoclay composites by mechanical blending and in situ polymerization respectively. The composites were then foamed by using CO2 as the foaming agent in an extrusion foaming process. The addition of a small amount of intercalated nanoclay greatly reduces
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Fig. 1. Influence of clay surface modification on the polystyrene foam cell morphology: (a) clay surface is modified by a polystyrene (PS) polymer containing one methacrylic group; (b) clay surface is modified by poly(methyl methacrylate) (PMMA) with a cationic ammonium head group. The scale bar is 50 lm.
cell size and increases cell density. Once exfoliated, the nanocomposite exhibits extremely high cell densities and even smaller cell size. Compared with unmodified polystyrene foams, the nanocomposite foams exhibit higher tensile modulus, improved fire retardance, and better barrier properties. Recently, Zeng et al. [**25,34] further manipulated the foam cell morphology by adjusting the interaction between CO2 and the clay surface. The clay was exfoliated by an in situ technique grafting PMMA onto the surface using then the modified clay was extrusion blended with polystyrene. This clay exhibited a much higher nucleation efficiency than the one whose surface was modified by polystyrene with a single methacrylic group linker (Fig. 1). A strong affinity between CO2 and the carbonyl group may reduce the gas–particle interfacial tension, which would lead to the reduction in nucleation free energy and a large increase of nucleation rate. Several other researchers also mention the potential applications of nanoclays in various polymer processing operations, including foaming [35–39]. 4.2. Nanometer sized foams with CO2 To reduce the cell size in polymer foams from micrometer to sub-micrometer is nontrivial requiring both a very high nucleation rate and a truncated cell growth stage. In practice, cell sizes of several hundred nanometers have been achieved with a few reports in the sub-100 nm range. Generally this involves working with high Tg materials and using an increase in temperature to initiate foaming without exceeding the Tg of the native polymer. All of these nanofoams are produced by batch processes that limit the size of products. Materials studied include PMMA [40–42], poly(ether sulfone) (PES) and poly(ether imide) (PEI) [43,44], a blend of polysulfone and polyimide [*45], and a series of polyimides for ultralow-k dielectrics [46,47]. A different nanostructured ‘‘foam’’, layered polymers with nanoscale gaps, was created by Zhang and Handa [48]. Polystyrene beads or films were compressed together
first to introduce weak chain-entanglements at the interfaces. After saturation with CO2 , the polymer was heated and layered structures with nanoscale interlayer gaps were formed due to the nucleation and expansion of CO2 in the weak chain-entanglement regions.
5. Role of SCF at polymer/clay interface 5.1. Rheology In many of the applications discussed above the supercritical fluid acts primarily as a diluent/swelling agent for the polymer phase, solvent for monomers or reactants, and a blowing agent to produce foams. During the dispersion of nanoparticles in a polymer matrix, or during the formation of nanofoam bubbles, the viscosity of the polymer/gas system plays a pivotal role. As a result, increased attention has been given to understand the rheological properties of polymer/gas melt or solution systems. In general, viscosity is observed to decrease as CO2 is dissolved into various polymers. Once the nanometer-sized fillers are dispersed in the polymer matrix, the rheological behavior becomes more complex due to synergetic effect of nanofillers and CO2 . Interesting developments include the shear viscosity change of intercalated nanocomposites of PS/montmorillonite (MMT) nanoclay with and without CO2 [*49]. This work observed that the melt viscosity of polystyrene in the presence of CO2 actually decreased with the addition of nanoclay filler in contrast to the typical increase with filler concentration (Fig. 2). They suggest this may be an interfacial effect wherein CO2 concentrations are enhanced at the polymer/clay interface causing a different structure in the polymer phase near the clay nanoparticles. Secondly, Flichy et al. [**50] used a rotational viscometer, a drag-driven device, to study the effect of CO2 on the rheology of poly(propylene glycol) (PPG) and suspensions of nanoporous silica with PPG. This is one of the first published accounts of high pressure stress rheometry.
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Hocker et al. predicted isotherms in one-dimensional slit-pores of different widths [**54]. In their work, the adsorption ‘‘hump’’ shows up in meso- and macropores, but not in micropores (<2 nm width). In fact, they show that the ‘‘hump’’ in the adsorption isotherm is not correlated with a 3-layer micropore but is fit only with the inclusion of a 30 layer macropore ascribed to the clay binder in their zeolite material.
Shear viscosity (Pa.sec)
3500 10 1/sec 20 1/sec 30 1/sec
3000
2500
2000
1500
6. Conclusions 1000 0.0%
2.5%
5.0%
7.5%
10.0%
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Fig. 2. Effect of montmorillonite clay (20A) concentration on viscosity of polystyrene (PS) containing 3 wt% CO2 .
The rheological properties of nanocomposites with or without CO2 are far from well understood and are receiving increasing attention from researchers. Elastic and viscous moduli, extensional viscosity, and the time dependent behavior are awaiting further study, and depend to a large extent on the design of the rheometer. These properties will improve understanding of the principles behind the dispersion of nanoparticles and the interaction between nanoparticles and the polymer matrix.
The literature now demonstrates the ability to use SCFs for controlled synthesis and processing of composite materials with nanoscale features. Novel combinations of chemistry, polymer architecture, and CO2 thermodynamics are yielding unique structures and processes. Fundamentally, a direct correlation between adsorption in nanopores, rheology of nanocomposites, and final properties of composite materials has yet to be drawn although this is only a matter of time. Polymer nanocomposite systems are drawing significant attention from many different angles and there will be much more progress in the next few years. From this short review it is clear that supercritical fluids will play an important role in the development of manufacturing processes at the nanoscale.
5.2. Adsorption Another fundamental area relevant for nanocomposite research is the behavior of CO2 confined in nanoscale systems. Recent results show that supercritical fluids (CO2 in particular) exhibit unique behavior in nanoscale systems including pores and films. This behavior most often manifests itself near the critical point of CO2 where the isothermal compressibility is at its highest. Sirard et al. showed using ellipsometry that the swelling of thin films of PMMA undergoes an anomalous maximum near the critical point of CO2 [**51]. The high compressibility of CO2 at these conditions results in concentration inhomogeneities near the surface of the film that are of such a magnitude that they only affect observable properties in nanoscale films (thicknesses up to 325 nm were studied). Swelling in bulk PMMA does not exhibit a maximum. A second, related phenomenon is the Ôhump’ in the excess adsorption isotherms on activated carbons and zeolites near the critical point of CO2 [52,*53]. This behavior is also related to the highly compressible state but is difficult to analyze because molecular model parameters necessary to capture the magnitude of the Ôhump’ require an unrealistic number of CO2 layers in the pore (more than can physically fit). For example,
Acknowledgements The authors gratefully acknowledge financial support from the National Science Foundation through grants EEC-0223592 and DMI-0200324 and from the donors of The Petroleum Research Fund, administered by the American Chemical Society.
References The papers of particular interest have been highlighted as: * of special interest; ** of outstanding interest. [*1] Usuki A, Kojima Y, Kawasumi M, Okada A, Fukushima Y, Kurauchi T, Kamigaito O. Synthesis of nylon 6–clay hybrid. J Mater Res 1993;8:1179–84, One of the papers that ignited the flurry of research in polymer nanocomposites. Data show improved mechanical properties over pure polymer. [2] Usuki A, Kawasumi M, Kojima Y, Okada A, Kurauchi T, Kamigaito O. Swelling behavior of montmorillonite cation exchanged for x-amino acids by e-caprolactam. J Mater Res 1993;8:1174–8. [**3] Watkins JJ, McCarthy TJ. Polymerization in supercritical fluidswollen polymers: a new route to polymer blends. Macromol-
D.L. Tomasko et al. / Current Opinion in Solid State and Materials Science 7 (2003) 407–412
[*4]
[**5]
[6]
[*7]
[8]
[**9]
[*10]
[11]
[12]
[*13]
[14]
[15]
[16]
[**17]
[**18]
ecules 1994;27:4845–7, Initial demonstration of polymer/polymer blends via the SCF swelling technique. Watkins JJ, McCarthy TJ. Polymer/metal nanocomposite synthesis in supercritical CO2 . Chem Mater 1995;7:1991–4, Initial demonstration of polymer/metal nanocomposites. Platinum nanoparticles <50 nm in PMP. Watkins JJ, McCarthy TJ. Polymerization of styrene in supercritical CO2 -swollen poly(chlorotrifluoroethylene). Macromolecules 1995;28:4067–74, Detailed study showing specifics of the in situ polymerization technique. Watkins JJ, McCarthy TJ. Chemistry in supercritical fluidswollen polymers: direct synthesis of metal/polymer nanocomposites. Polym Mater Sci Eng 1995;73:158–9. Said-Galiyev E, Nikitin L, Vinokur R, Gallyamov M, Kurykin M, Petrova O, et al. New chelate complexes of copper and iron: synthesis and impregnation into a polymer matrix from solution in supercritical carbon dioxide. Ind Eng Chem Res 2000;39:4891–6, Recent extension of polymer/metal nanocomposites to include copper and iron chelate complexes. Nazem N, Taylor LT, Rubira AF. Metallized poly(etherether ketone) films achieved by supercritical fluid impregnation of a silver precursor followed by thermal curing. J Supercrit Fluids 2002;23:43–57. Brown GD, Watkins JJ. Carbon dioxide-dilated block copolymer templates for nanostructured materials. In: Materials Issues and Modeling for Device Nanofabrication Materials, Research Society Symposium Proceeding, vol. 584; 2000. p. 169–74. Demonstration of polymer/metal nanocomposites via swollen block copolymers with emphasis on long range order of the dispersed phase. Brown GD, Watkins JJ. Preparation of nanocomposites by selective metallization in CO2 -swollen cylindrical diblock copolymers templates. Polymeric Materials Science and Engineering 2001;84:130–1, Use of CO2 to control domain sizes in self-assembled block copolymers therefore limiting product sizes. Li D, Han B, Liu Z. Grafting of 2-hydroxyethyl methacrylate onto isotactic poly(propylene) using supercritical CO2 as a solvent and swelling agent. Macromol Chem Phys 2001;202: 2187–94. Li D, Han B, Liu Z, Zhao D. Phase behavior of supercritical CO2 /styrene/poly(ethylene terephthalate) (PET) system and preparation of polystyrene/PET composites. Polymer 2001;42: 2331–7. Li D, Liu Z, Han B, Song L, Yang G, Jiang T. Preparation of nanometer dispersed polypropylene/polystyrene interpenetrating network using supercritical CO2 as a swelling agent. Polymer 2002;43:5363–7, Demonstration of a cross-linked IPN using the SCF technique. Liu Z, Song L, Dai X, Yang G, Han B, Xu J. Grafting of methyl methacrylate onto isotactic polypropylene film using supercritical CO2 as a swelling agent. Polymer 2002;43:1183–8. Liu Z, Wang J, Dai X, Han B, Dong Z, Yang G, et al. Synthesis of composites of silicon rubber and polystyrene using supercritical CO2 as a swelling agent. J Mater Chem 2002;12:2688–91. Liu Z, Dong Z, Han B, Wang J, He J, Yang G. Composites prepared by the polymerization of styrene within supercritical CO2 -swollen polypropylene. Chem Mater 2002;14:4619–23. Caskey TC, Lesser AJ, McCarthy TJ. In situ polymerization and nano-templating phenomenon in nylon fiber/PMMA composite laminates. J Appl Polym Sci 2003;88:1600–7, Demonstrates templating by crystalling nylon fibers and shows the potential for SCF application in traditional thermoset composite processes. Zhang J, Busby AJ, Roberts CJ, Chen X, Davies MC, Tendler SJB, et al. Preparation of a poly(methyl methacrylate)/ultrahigh molecular weight polyethylene blend using supercritical carbon dioxide and the identification of a three-phase structure: an
[19] [20] [21]
[22]
[23]
[24]
[**25]
[*26]
[27]
[28]
[29]
[30]
[31]
[*32]
[33]
[34]
[35]
[36]
[37]
[38]
411
atomic force microscopy study. Macromolecules 2002;35:8869– 77, A single-step method to prepare composites templated by crystalline domains. Excellent development of AFM technique to analyze morphology. Lan TK, Padmananda D, Pinnavaia, Thomas J. On the nature of polyimide–clay hybrid composites. Chem Mater 1994;6:573. Okada AU, Arimitsu. The chemistry of polymer–clay hybrids. Mater Sci Eng, C: Biomim Mater, Sens Syst 1995;C3:109–15. Kojima Y, Usuki A, Kawasumi M, Okada A, Fukushima Y, Kurauchi T, et al. Mechanical properties of nylon 6–clay hybrid. J Mater Res 1993;8:1185–9. Zeng C, Lee LJ. Poly(methyl methacrylate) and polystyre/clay nanocomposites prepared by in-situ polymerization. Macromolecules 2001;34:4098–103. Wang H, Zeng C, Elkovitch M, Lee LJ, Koelling KW. Processing and properties of polymeric nano-composites. Polym Eng Sci 2001;41:2036–46. Svoboda P, Zeng C, Wang H, Lee LJ, Tomasko DL. Morphology and mechanical properties of polypropylene/organoclay nanocomposites. J Appl Polym Sci 2002;85:1562–70. Zeng C, Han X, Lee LJ, Koelling KW, Tomasko DL. Polymer/ clay nanocomposite foams prepared by using carbon dioxide. Adv Mater 2003;15(20):1743–7, Novel study showing the effect of clay surface treatment on resulting foam morphology. Extremely high cell densities and small cell sizes observed. Manke CW, Gulari E, Mielewski DF, Lee EC-c. System and method of delaminating a layered silicate material by supercritical fluid treatment, 6,469,073 B1, 2002. Interesting patent showing a SCF based technique to exfoliate clay. Mielewski DF, Lee EC-c, Manke CW, Gulari E. System and method of preparing a reinforced polymer by supercritical fluid treatment, 2002/0082331 A1, 2002. Garcia-Leiner M, Lesser AJ. Polymer–clay nanocomposites prepared in supercritical carbon dioxide. ACS Div Polym Mater: Sci Eng 2003;88:92–3. Nam PH, Okamoto M, Maiti P, Kotaka T, Nakayama T, Takada M, et al. Biaxial flow-induced alignment of silicate layers in polypropylene/clay nanocomposite foam. Nano Letters 2001;1:503–5. Nam PH, Maiti P, Okamoto M, Kotaka T, Nakayama T, Takada M, et al. Foam processing and cellular structure of polypropylene/clay nanocomposites. Polym Eng Sci 2002;42: 1907–18. Han X, Zeng C, Lee LJ, Koelling KW, Tomasko DL. Processing and cell structure of nano-clay modified microcellular foams. San Francisco, CA: SPE-ANTEC; 2002. p. 1915–9. Han X, Zeng C, Lee LJ, Koelling KW, Tomasko DL. Extrusion of polystyrene nanocomposite foams with supercritical CO2 . Polym Eng Sci 2003;43:1261–75, One of the first studies on extrusion foaming of nanocomposites and evaluation of properties. Han X, Zeng C, Lnee LJ, Koelling KW, Tomasko DL. Extrusion of polystyrene foams reinforced with nano-clays. Nashville, TN: SPE-ANTEC; 2003. p. 1732–6. Zeng C, Han X, Lee LJ, Koelling KW, Tomasko DL. Structure of nanocomposite foams. San Francisco, CA: SPE-ANTEC; 2002. pp. 1504–8. Wilson PS. Structural foam composite having nano-particle reinforcement and method of making the same, WO0037242, 2000. Fibiger RF, Barger MA, Suh KW, Tung HC, Liang W, Mackey GA, Schomaker JA. Nanocomposite articles and process for making, WO0047657, 2000. Steeman PAM, Voets PEL, Van EMA. Extruded nanocomposite moulded part comprising at least a polycondensate and a nano-filler and a process for its production, WO0118107, 2001. Strauss W, Ranade A, D’Souza NA, Reidy RF, Paceley M. Effect of montmorillonite on formation of polystyrene foams
412
[39]
[40]
[41]
[42]
[43]
[44]
[*45]
[46]
[47]
D.L. Tomasko et al. / Current Opinion in Solid State and Materials Science 7 (2003) 407–412 using supercritical CO2 . Nashville, TN: SPE-ANTEC; 2003. p. 1812–6. Strauss W, Ranade A, D’Souza NA, Reidy RF, Paceley M. Preparation and characterization of supercritical CO2 processed polystyrene nanocomposite foams. In: Advancing Materials in the Global Economy––Applications, Emerging Markets and Evolving Technologies, Book 1. International SAMPE Symposium and Exhibition, vol. 48; 2003. p. 1171–80. Handa YP, Zhang Z. A new technique for measuring retrograde vitrification in polymer–gas systems and for making ultramicrocellular foams from the retrograde phase. J Polym Sci: Part B: Polym Phys 2000;38:716–25. Handa YP, Zhang Z, Wong B. Solubility, diffusivity, and retrograde vitrification in PMMA-CO2 , and development of sub-micron cellular structures. Cell Polym 2001;20:1–16. Siripurapu S, DeSimone JM, Spontak RJ, Khan SA. Generation of nanoporous thin polymer films via foaming with carbon dioxide. Preprints of Symposia, vol. 48. American Chemical Society, Division of Fuel Chemistry; 2003. p. 262–3. Krause B, Sijbesma HJP, Munuklu P, Van der Vegt NFA, Wessling M. Bicontinuous nanoporous polymers by carbon dioxide foaming. Macromolecules 2001;34:8792–801. Krause B, Kloth M, Van der Vegt NFA, Wessling M. Porous monofilaments by continuous solid-state foaming. Ind Eng Chem Res 2002;41:1195–204. Krause B, Diekmann K, van der Vegt NFA, Wessling M. Open nanoporous morphologies from polymeric blends by carbon dioxide foaming. Macromolecules 2002;35:1738–45, A clear, systematic study of foaming conditions to produce nanoporosity in films of polymer blends. Krause B, Koops G-H, Van der Vegt NFA, Wessling M, Wubbenhorst M, Van Turnhout J. Ultralow-k dielectrics made by supercritical foaming of thin polymer films. Adv Mater 2002;14:1041–6. Krause B, van der Vegt NFA, Wessling M. New ways to produce porous polymeric membranes by carbon dioxide foaming. Desalination 2002;144:5–7.
[48] Zhang Z, Handa YP. Polymer mica: layered polymer with nanometer sized interlayer gaps. J Mater Sci Lett 2003;22:135– 7. [*49] Wingert MJ, Han X, Zeng C, Li H, Lee LJ, Tomasko DL, Koelling KW. Rheological changes in CO2 impregnated polystyrene reinforced with nanoclays. SPE-ANTEC: Nashville, TN; 2003. p. 986–90. Demonstrated synergistic effect of clay and CO2 on the rheology of polystyrene based nanocomposites. [**50] Flichy NMB, Lawrence CJ, Kazarian SG. Rheology of poly(propylene glycol) and suspensions of fumed silica in poly(propylene glycol) under high-pressure CO2 . Industrial & Engineering Chemistry Research, in press. New high pressure rotational rheometer demonstrated with CO2 and silica suspensions in oligomeric PPG. Excellent analysis of swelling and surface chemistry effects. [**51] Sirard SM, Green PF, Johnston KP. Spectroscopic ellipsometry investigation of the swelling of poly(dimethylsiloxane) thin films with high pressure carbon dioxide. J Phys Chem B 2001;105:722–66, Excellent study showing the effect of high compressibility near the critical point on the swelling behavior of thin films. [52] Chen JS, Wong DSH, Tan CS, Subramanian R, Lira CT, Orth M. Adsorption and desorption of carbon dioxide onto and from activated carbon at high pressures. Ind Eng Chem Res 1997;36:2808. [*53] Humayun R, Tomasko DL. High resolution adsorption isotherms of supercritical carbon dioxide on activated carbon. AIChE J 2000;46:2065–75, High resolution data clearly demonstrating the anomalous adsorption behavior near the critical point in a porous material. [**54] Hocker T, Rajendran A, Mazzoti M. Measuring and modeling supercritical adsorption in porous solids. Carbon dioxide on 13X zeolite and on silica gel. Langmuir 2003;19:1254–67, Very good experimental and modeling study showing the anomalous maximum in adsorption near the critical point. Model results show that multilayers in the clay binder are responsible for most of the observed maximum.