Stefanie
Uredat†
a,
Aditi
Gujare†
b,
Jonas
Runge†
a,
Domenico
Truzzolillo
b,
Julian
Oberdisse
*b and
Thomas
Hellweg
*a
aDepartment of Physical and Biophysical Chemistry, Bielefeld University, Universitätsstr. 25, 33615 Bielefeld, Germany. E-mail: thomas.hellweg@uni-bielefeld.de
bLaboratoire Charles Coulomb (L2C), University of Montpellier, CNRS, 34095 Montpellier, France. E-mail: julian.oberdisse@umontpellier.fr
First published on 26th December 2023
The formation and properties of smart (stimuli-responsive) membranes are reviewed, with a special focus on temperature and pH triggering of gating to water, ions, polymers, nanoparticles, or other molecules of interest. The review is organized in two parts, starting with all-smart membranes based on intrinsically smart materials, in particular of the poly(N-isopropylacrylamide) family and similar polymers. The key steps of membrane fabrication are discussed, namely the deposition into thin films, functionalization of pores, and the secondary crosslinking of pre-existing microgel particles into membranes. The latter may be free-standing and do not necessitate the presence of a porous support layer. The temperature-dependent swelling properties of polymers provide a means of controlling the size of pores, and thus size-sensitive gating. Throughout the review, we highlight “positive” (gates open) or “negative” (closed) gating effects with respect to increasing temperature. In the second part, the functionalization of porous organic or inorganic membranes of various origins by either microgel particles or linear polymer brushes is discussed. In this case, the key steps are the adsorption or grafting mechanisms. Finally, whenever provided by the authors, the suitability of smart gating membranes for specific applications is highlighted.
Typical applications are based on the controllable semi-permeability of membranes, allowing opening or closing of passages (“gating”) using external control parameters. For instance, stimuli-responsive membranes have emerged as a promising technology in wastewater remediation, offering enhanced control and efficiency in contaminant removal.1 Stimuli-responsive membranes have also gained significant interest in the field of gas and other separation processes like distillation, adsorption, extraction, and crystallization due to their ability to control selectively gas transport and segregation properties.2 One of the most covered targets is the separation of carbon dioxide (CO2) from gas mixtures, especially in the context of mitigating greenhouse gas emissions and addressing climate change. Also, CO2 may be used as a stimulus.3–5 Yet another important application is drug delivery, with control of release induced by, e.g., local heating.6 As a last example, one may also make use of the change in optical properties as one approaches phase transitions, like cloud points, or of other changes in optical activity controlled by temperature.7
Stimuli-responsive polymer chains are often the basic unit providing smartness, i.e. their conformational changes provide control over gating by external stimuli. The gating properties of smart membranes, which may be free-standing or supported by some substrate depend on both the molecular properties of the polymer, in particular its swelling, and on the membrane geometry. The same polymer may, e.g., inhibit the passage of some solute through pores in the substrate by swelling and thereby filling the pore, or allow the passage to some other solute across its swollen, less concentrated structure in an all-smart membrane. In the present review, we attempt to highlight wherever known if the system possesses a “positive” or “negative” gating effect, as illustrated in Fig. 1(a). Here “positive” means that increasing the temperature (which is the most common control parameter) opens the gates, and vice versa. A possible mechanism based on pore size has been discussed already 15 years ago by Alem et al.,8 see Fig. 1(b).
Two stimuli have been extensively studied in the literature, temperature and pH. Concerning control of polymer swelling by temperature, the existence of a lower critical solution temperature (LCST), or an upper one (UCST), or possibly both, governs the solubility of the polymer in the solvent. The most investigated temperature sensitive polymer exhibiting a LCST close to body temperature (>33 °C) is the poly(N-substituted acrylamide) family (like pNIPAM), with variations extending typically between poly(N-n-propylacrylamide) (21 °C) and poly(N-isopropylmethacrylamide) (44 °C), depending moreover on deuteration.9,10 Other related polymers are poly(N,N′-diethyl acrylamide) exhibiting a LCST in the range 26–35 °C.6 Another, widely explored family is caprolactam, for instance poly(vinylcaprolactam) (pVCL) with a LCST in the range of 32–34 °C.11 If microgels are employed, the most common primary (internal) crosslinker is N,N′-methylenebisacrylamide (BIS).12–15 However, also other cross-linkers were already used e.g. different methacrylamides,16 divinylbenzene17 or cleavable cross-linkers.18
The reference polymer pNIPAM, e.g., has been proposed as micro-actuator, in particular with linear swelling properties for certain microgel architectures.9 that can be employed in tunable coatings to trigger the adsorption/desorption of biological cells.19–21 A similar application based on chains (as opposed to microgel particles) focusing on proteins has been proposed by Ulbricht and Yang.22 Besides the monomer chemistry, the network connectivity also impacts macroscopic properties, and thus possibly gating. For instance, the control of mechanical properties by crosslinking has been highlighted in recent work by Kim et al.23 in which the authors synthesized thin hydrogels where entanglements greatly outnumber crosslinks. Such hydrogels enable transmission of tension through the network, while the sparse crosslinks prevent the polymer chains from disentangling. In this case, the large number of entanglements favors a more ductile/less brittle behavior under stress, leading to higher toughness and fatigue resistance.
We start with a short outline of general properties in Section II. Review articles with a similar scope have been published by Liu et al.24 in 2016 and more recently by Pan et al.25 in 2023, highlighting different types of responsiveness, and how the positive and negative gating with the different stimuli works. We propose here to review very recent contributions together with some of the older but groundbreaking articles. Section III of this review will be devoted to the discussion of “all-smart” membranes, and Section IV to “functionalized porous” membranes. Section III is further divided into two subsections where we discuss secondary crosslinking and deposition techniques. Analogously, Section IV is also divided in 2 subsections on the fabrication of porous membranes and their subsequent functionalization. In all cases, examples mostly in view of gating applications will be provided, differentiating where-ever possible “positive” from “negative” gating properties as illustrated in Fig. 1. These sections will be followed by a conclusion which also gives some outlook with respect to future research and promising new ideas.
The synthesis of stimuli-responsive polymer chains themselves is outside the scope of the present review. The reader is probably aware that usually either controlled radical (or living) polymerization, or free radical precipitation-polymerization is described in the literature.32–38 In the following two sections, two different approaches to the formation of smart polymer-based gating membranes are discussed. First, in Section III, the formation of an “all smart” membrane is targeted, either as a polymer macrogel, or as polymer gel obtained from previously synthesized microgel particles. As already mentioned in the introduction, the crosslinked state of the polymer chains is of primary importance, in particular for “all smart” membranes. Crosslinked membranes are obtained by covalently binding individual chains and make volume spanning networks via crosslinking coupling reactions.39 The latter normally lead to random network structures, as they have been studied by scattering techniques applied to macrogels.40,41 These structures cannot fully self-optimize themselves due to permanent and rigid primary crosslinking to absorb or release very high content of solvent. On the other hand, the additional external crosslinking of already internally crosslinked microgel particles offers the possibility to optimize features like mechanical strength and swelling. We call “secondary crosslinking” this additional chemical crosslinking step in the case of microgel particles which are already internally crosslinked, often using BIS. Several of these protocols, e.g. based on photocrosslinking,18,42 or with chemical crosslinking using glutaraldehyde in presence of primary amines on the chain,43,44 will be also reviewed. The requirement on the secondary crosslinker is that it is incorporated in the primary polymer network without inducing any crosslinking, while this is triggered later in the membrane preparation process.
Secondly, in Section IV, we discuss the functionalization of porous non-stimuli responsive membranes by stimuli-responsive polymer as proposed in the literature. This functionalization relies on a grafting or adsorption step, and usually leads to the formation of a stimuli-responsive brush. The supporting membranes of smart coatings are often non-crosslinked glassy polymers45,46 or carbon nanotube grids,47 with high mechanical strength. These porous support membranes can also be woven tissues, or non-woven substrates made of fibers obtained e.g. by electrospinning. Non-woven porous functionalized membranes are known to be abrasion and heat resistant, and show high flexibility and elasticity.48 Moreover, they have been proposed for applications in filtration49 and enzyme immobilization.50 The membrane optimization in response to the external stimulus may be complicated by both the difficulty in obtaining a homogenous coating on the sub-nanometric scale, and the typical lack of responsiveness of the glassy polymer scaffold of the membrane.
Several secondary crosslinking techniques exist, either based on electron or UV irradiation, or on chemical reactions, for instance of glutaraldehyde with amines. We introduce the different crosslinking methods first in Section III.1, before discussing the deposition protocols and the resulting membranes below. For the deposition step, any physical (adhesion for dip-coating, centrifugation for spin-coating) or physico-chemical force (i.e., self-assembly or interfacial techniques based on selective solvents or incompatible moieties) may be used. Examples of membranes obtained by different deposition protocols are discussed in Section III.2.
UV crosslinking is considerably easier to use, and less radiation damage is produced. Typical UV-sensitive monomers are benzophenone and its derivatives.53 Such photoinitiators (PIs) can be classified into type I and type II PIs.54 Type I PIs dissociate after irradiation forming two radicals. Type II PIs need a co-initiator because they undergo photoreduction.
When photosensitive monomers such as 2-hydroxy-4-(methacryloyloxy)–benzophenone (HMABP) are added into a microgel polymer system, the secondary crosslinking can be obtained with UV light irradiation. Dirksen et al.18,42 synthesized BIS-crosslinked poly(NIPAM-co-HMABP) microgels and spin coated a silicon wafer with the microgel. Freestanding membranes made of 2–3 layers of the original microgels were achieved after irradiation of the sample with UV light. They performed temperature-dependent resistance measurements and could show a switch in resistance at the VPTT of the microgel.
As one can see in Fig. 3(a), the resistivity increases abruptly with temperature, and the system displays thus a negative gating effect. If a degradable crosslinker such as 2,2′-(bisacrylamino)diethyl disulfide (BAC) is used instead of BIS, the gating behaviour can be inverted if the cross-linker is cleaved with a solution of 1,4-dithiothreotol (1 mM) after membrane formation (Fig. 3(b)) by maintaining the stability of the membranes.18 This allows switching from a negative to a positive gating effect.
The contribution by Sabadasch et al.55 shows that the UV cross-linked smart membranes can be loaded with nanoparticles (here palladium) that can be used in catalytic applications. The free-standing photo-crosslinked membranes were deposited on a nylon mesh to achieve higher mechanical stability (see Fig. 4). Such supported nanoparticle – membrane hybrids allow easy separation from the reaction medium and recycling of the catalyst. Such membranes might also be useful in microfluidic lab-on-a-chip applications. However, this still remains to be explored. Also, the thermo-response of the membranes was not yet exploited to achieve better control of the reaction.
The crosslinking mechanism of primary amines introduced by copolymerization with glutaraldehyde is different from most other crosslinking reagents. In particular, it is not based on the simple mechanism of Schiff base linkages on both ends of the glutaraldehyde. In parallel with the crosslinking reaction, the polymerization of glutaraldehyde via aldol condensation may take place, enabling the formation of links between particles.56
Swelling properties of membranes capable of gating may also be generated with non-synthetic polymers. For example, Tokarev et al.57 prepared a highly porous alginate membrane. A thin film of sodium alginate and diamine-PEG film was spin-coated on a wafer. Scanning probe microscopy measurements confirmed a phase separation of the two monomers. By addition of calcium ions, ionic crosslinking of alginate was induced. Afterwards, the membrane was formed by rinsing with water to elute the diamine-PEG. The membrane thickness was controlled by the concentration of the casting solution. The membrane was stable below pH 8 and showed pH-dependent swelling in the range going from pH 2 up to pH 6. Similar to thermo-responsive membranes a sharp swelling transition was observed between pH 4 and 5 with an inflection point of 4.6. The inflection point was in the range of the reported pKa of alginate. The pores of the membrane were found to be fully closed at pH values of 4.6 and higher.
Still et al.44 used the evaporating drop method which is drying the mixture of microgel with the secondary crosslinker (e.g. glutaraldehyde) and dry on a substrate to fabricate a freestanding temperature-sensitive membrane made of p(NIPAM-co-AEMA), where the comonomer is 2-aminoethyl methacrylate. Fig. 5 shows the so obtained freestanding membrane on the right. At higher temperatures the membrane shrinks and becomes darker due to its higher density: the light transmittance can thus be controlled, with a negative gating effect. On the left, the reversible change in size with temperature is shown.
Self-assembly in bulk or at interfaces is an elegant way to form thin, nanostructured polymer membranes. Several techniques relying on the physico-chemical preference of certain molecules (or moieties, in particular blocks of block copolymers) for solvents have been used in the past, in most cases however not for smart membranes. Molecular monolayers, e.g., may be spread at the air–water or oil–water interface. Ahmed et al.59 employed amphiphilic diblock copolymers that have been cross-linked in both monolayer at the air–water interface and bilayer assemblies. Similarly, El-Haitami et al.60 proposed a method to obtain ultrathin membranes with good mechanical properties by in situ synthesis at the air–water interface of a 2D semi-interpenetrating polymer network. Very recently, Coppola et al.61 fabricated in situ a polymer membrane, simply by injecting drops of polymer solutions at the oil–water interface.
Self-assembly as mechanism of nanostructure formation is based on the preference of certain blocks of a block copolymer to regroup in the bulk, and thus form organized supramolecular structures. Cetintas et al.62 present fully reversible thermo-responsive nanoporous membranes fabricated by self-assembly and non-solvent induced phase separation (NIPS) of polystyrene-poly(N-isopropylacrylamide) (PS-b-pNIPAM) block copolymers. The sudden replacement of a good solvent of both blocks by a selective solvent, i.e. non-solvent for one of the blocks, triggers a microphase separation leading to a porous system after drying. A variety of PS-b-pNIPAM block copolymers were synthesized by reversible addition-fragmentation chain transfer (RAFT) polymerization and the reaction conditions were optimized. The target copolymers featured: (1) a thermo-responsive pNIPAM block, (2) a majority PS fraction, and (3) a well-defined high molecular weight, which are requirements for successful fabrication of free-standing responsive membranes using NIPS. The resulting membranes exhibited a worm-like cylindrical morphology with interconnected nanopores. These membranes exhibit a positive gating effect, as the permeability for water increases with temperature, and is reversible. Polymer phase separation and self-assembly have been exploited also very recently by Willott and co-workers63 to obtain pH-sensitive symmetric porous microfiltration membranes and asymmetric dense nanofiltration membranes, where the degree of responsive behavior could be tuned by the degree of cross-linking.
A more conventional method for obtaining thin layers of microgels is spin coating.64–66 This technique has been extensively used to produce membranes without stimuli-responsiveness. For instance, Kang et al.67 describe the fabrication and characterization of large-scale (>2 cm in diameter) free-standing ultrathin PDMS membranes. Thangawng et al.68 report a method for making ultra-thin PDMS membranes as thin as 70 nm. On the other hand, Cors et al. have produced stimuli-responsive microgel monolayers by spin-coating which proved to have a thermal response equivalent to the one of the individual primary microgel particles in suspension.9 Such layers, however, had not yet undergone secondary crosslinking, and could be redissolved in water.
Thermo-sensitive triblock copolymers have also been deposited by spin-coating, taking advantage of their spontaneous self-assembly in bulk. Nykanen et al.69 describe the synthesis of temperature-responsive polystyrene-block-poly(N-isopropyl-acrylamide)-block-polystyrene triblock copolymers, PS-b-pNIPAM-b-PS, their self-assembly and phase behavior in bulk. Moreover, they have demonstrated the formation of thermoresponsive membranes from these block copolymers. Composite membranes for separation studies were prepared by spin-coating thin films of this triblock copolymer on top of meso/macroporous polyacrylonitrile support sheet. The permeability was measured as a function of temperature using aqueous mixture of PEG with several well-defined molecular weights. The permeability showed a temperature switchable on/off behavior, where higher permeability is obtained below the transition temperature of pNIPAM, i.e. the system presents a negative gating effect. The molecular cutoff limits for the PEG molecules are surprisingly low, between 108 and 660 g mol−1.
Other block copolymer systems can also be used. Tang et al., e.g., used a selective solvent to form nanopores with a diameter of 5 nm in spin-coated symmetric triblock copolymer layers based on methacrylates and polystyrene.70 The authors produced a poly(ethylene glycol methyl ether methacrylate)-b-PS-b-poly(ethylene glycol methyl ether methacrylate) (PMENMA-b-PS-b-PMENMA) mesoporous size-selective layer attached to a polyvinylidene fluoride macroporous supporting layer. The PMENMA covers the pores and its LCST in water can be tuned by the number of ethylene glycol units. Water permeability experiments showed that a higher flux of water passes through the membranes at temperatures above the LCST, suggesting that the pore sizes are temperature controllable and that the gating effect is positive. The T-dependent size selectivity of the membranes was also investigated and a strong size-discrimination in particle permeation was found, however based on a gradual temperature response.
Finally, microgels made of NIPAM and acrylic acid have been deposited by spin-coating on silicon wafers coated with three layers, first n-octyltrichlorosilane and then poly(octadecene-alt-maleic anhydride), and with a cationic PEI layer on the surface. These thermo-responsive films show homogeneous and dense deposition in the swollen state. They also show the same behavior in their collapsed state but only at higher pH, as smaller size promotes higher packing efficiency and pH 7 or 10 makes the particles charged and results in efficient binding to the cationic PEI surface.71 Monolayer deposition of such films has been obtained by S. Schmidt et al.64 where poly(NIPAM-co-acrylic acid) microgel films were deposited on the PEI layer on silicon wafers. A stable monolayer was obtained at lower pH (pH = 2), while above pH 5, most of the material is desorbed because of the enhanced repulsion between the like-charged particles. Also thermoresponsive poly(NIPAM-co-styrene) microgel films with styrene as a comonomer to introduce amphiphilicity were deposited on glass cover slip by the same technique, spin coating, for application in cell growth and detachment.72
Carbon nanotubes have also been proposed as support for smart functionalization, taking advantage of their exceptional mechanical properties.75 Due to the rather small diameter and the high aspect ratio, carbon nanotubes offer a high surface area for smart functionalization, typically by “grafting-onto” reactions of preformed polymer chains, while “grafting from” is also possible.
Inducing phase separations in polymer solutions is a common way of producing pores. Porous polysulfone membranes were prepared via non-solvent induced phase separation (see Section III.2) with an anionic flocculant based on acrylamide and sodium acrylate (PASA), varying the PASA concentration and the temperature of the coagulation bath.76 With increasing PASA concentration an increase of viscosity was observed. This lowered the solvent-non-solvent exchange rate resulting in formation of a sponge-like membrane without macrovoids at 60 °C. Membrane permeability and fouling parameters were then studied showing impact of the PASA content. The authors attribute the improvement of the antifouling performance to the higher hydrophilization of the surface of the skin layer and a higher absolute zeta potential compared to the membrane without PASA, preventing the adsorption of foulants.
Inorganic support membranes can be obtained by various techniques. Spray-coating, e.g., has also been used to fabricate microporous membranes, however usually on supports, and as far as we are aware, not containing stimuli-responsive parts. A novel fabrication method based on spray coating was developed to produce a membrane supported on self-made macroporous silicon carbide (SiC) supports for gas purification.77 In another contribution, micro-filtration membranes were prepared on macro-porous plate alumina supports.78 Ceramic suspension was obtained by dispersing α-Al2O3 powder in an aqueous solution containing polyvinyl alcohol (PVA), polyvinyl pyrrolidone (PVP), polyacrylic acid and glycerol. Then the effects of annealing conditions on the membrane morphology, pore size distribution, as well as the permeation and binding strength were investigated.
If one is interested in having pores not only of controlled size, but also with a given orientation, then anode aluminum oxide membranes (AAO) membranes are the material of choice. Feng et al. showed that AAO pores can be functionalized to make the membrane responsive.79 Similarly, organic substrates with oriented channels have also been used,80 or track-etched gold-covered arrays of parallel capillaries which have been subsequently functionalized by Lokuge et al.81
Wessling and co-workers73 developed further the approach initiated by Stamm.84 Thermo-responsive PVCL microgels were immobilized on an inorganic membrane made of silicon carbide and carbon. The microgels are adsorbed on the surface by electrostatic attraction and hydrophobic interactions. Applying voltage to this conducting membrane increases the temperature and permeability, the system thus displays a positive gating effect. These membranes also show reversibility and a stable on–off switch. In Fig. 6 the temperature dependent dead-end permeation is shown for 3 consecutive heating and cooling cycles. A power of 30 W m−1 was applied to heat the membrane above the VPTT. The response of permeation to temperature changes is very direct due to the fast reaction of microgels to temperature changes.91
Hollow-fiber membranes made of poly(ethersulfone) (PES) have also been modified by adsorbing microgels to make them thermoresponsive micro- and ultrafiltration membranes. These PES membranes were coated with PVCL-based microgels by dynamic adsorption process. The microgels conserve their thermoresponsive behavior after adsorption on the PES membrane therefore showing complete reversibility with change in temperature.92 As a result, the complete retention of humic acid was obtained at low T, whereas the membrane became permeable at high T, evidencing a positive gating effect. Immobilisation of charged pNIPAM-co-acrylic acid microgel, on hollow-fiber PES membrane has also been studied. The acrylic acid comonomer was used to incorporate charge on the microgels, the main focus being on their behavior with the porous PES membrane.93
Bell et al.43 used the pore-covering method to obtain a temperature sensitive membrane. They first synthesized microgels with a hard core and a fuzzy shell. The core was wider than the pores of the porous substrate made of PES. The microgel deposition was performed by a constant flow of dilute microgel suspension in a specially-designed 3D-printed dead-end module with a filter membrane area of 4 cm2, producing SX-membranes (single crosslinked). In a second experiment they chemically crosslinked the so obtained microgel layers with flowing ammonium persulfate and N,N,N′,N′-tetra-methyl-ethylenediamine-solution through the membrane, achieving a secondary or double crosslinking (DX). These authors then carried out temperature-dependent resistance measurements and provided evidence for a difference between the SX- and DX-membrane. For example, the DX-membrane showed no compression effect in contrast to the SX-membrane. The compression was used to create more densely packed multilayers, which could be fixed in this state with chemical crosslinking. The SX-membranes desorbed from the membrane surface, when there was no more pressure/flux applied, while the DX-membrane remained intact on the surface. The higher temperature induced higher resistivity, i.e. this system possessed a negative gating effect.
Friebe and Ulbricht83 reported grafted pNIPAM via Atom Transfer Radical Polymerization (ATRP) in the pores of a track-etched PET membrane. They observed a significant reduction in the water permeability of the grafted membranes compared to untreated ones. Further, a thermo-responsive gating is achieved due to the thermo-responsive behavior of pNIPAM. The water permeation is strongly reduced below the LCST of pNIPAM because the polymer brush is swollen and blocks the membrane pores. ATRP grafting allows controlled functionalization in terms of layer thickness, thereby controlling the pore diameter and thus the gating effect in a more efficient manner as illustrated in Fig. 7. Functionalization of the porous materials in such a controlled manner could be further used for development in drug release and microfluidic applications.
In an already mentioned article which nicely illustrates the possible mechanisms of gating, Alem et al.8 grafted pNIPAM via ATRP on a track-etched PET membrane. They analyzed the gating functionality of the membranes with conductivity measurements. For membranes with an initial pore diameter of 330 nm the conductivity increased above the LCST of NIPAM: The polymer brush collapsed and the membrane pore was not blocked anymore: a positive gating effect was observed. For membranes with an initial pore diameter of 80 nm the conductivity decreased above the LCST of NIPAM, and a negative gating effect was found. These authors proposed two different types of water permeation control mechanisms depending on the initial pore diameter (see Fig. 1): for small pores the pNIPAM layer on the membrane surface is thicker compared to the pore diameter and the pNIPAM layer inside the pores. Thus, above the LCST the polymer collapses and is forming a hydrophobic “cork” blocking the membrane pores.
Finally, it is worth mentioning the recent work by Ding et al., which represents a macroscopic and thus visual illustration of gating with temperature.94 The authors reported the fabrication of wood-based smart gating membranes exhibiting reversible and stable pore opening/closing under heating/cooling stimuli. The fabrication included pretreatment of a polar wood scaffold with methacrylic anhydride, followed by in situ polymerization of pNIPAM to fill the pores with thermoresponsive hydrogels. The thermoresponsive smart gating wood membrane pores close below LCST and open above LCST of pNIPAM (Fig. 8(a)–(c)), showing therefore positive gating.
Stimuli-responsive polymers can be modified by functionalization inducing changes in membrane wetting behavior. Wetting is a property of a surface which reflects the equilibrium between the interfacial forces acting along the boundary line separating the surface, the liquid deposited on it, and the surrounding fluid. This equilibrium can be tuned by modifying the hydrophobicity of a polymer anchored on the surface. The article by Zhang et al. describes the fabrication of pNIPAM functionalized carbon nanotube-based smart membranes.75 Nanofiber composite membranes with switchable superwettability are obtained by carbon nanotubes (CNTs) adsorption onto electrospun polyurethane (PU) nanofibers (non-woven). This structure is subsequently functionalized with pNIPAM. The authors show that pNIPAM enhances the interfacial interaction between CNTs and PU nanofibers without sacrificing the flexibility of the membrane. As a result, the membrane can be either oil- or water-permeable, at high and low temperatures, respectively. Depending on the substance to be blocked or not, the system thus represents a positive gating effect (for oil), and a negative one (for water).
An important application of membranes is therefore (ultra)filtration. The permeation of solvent and solutes depends crucially on the physico-chemical state of the internal membrane surface. Controlling adsorption or desorption of, e.g., proteins, is fundamental to designing efficient filtering membranes. Ulbricht and Yang22 used benzophenone as photo-initiator to crosslink different systems of acrylamide, acrylic acid and BIS with UV light, which are adsorbed/entrapped on a porous polypropylene substrate coated with benzophenone as photoinitiator. They obtained polymer brushes on the substrate which they used to bind more lysine reversibly to the substrate surface in comparison to the unmodified membrane.22
In another contribution, Li et al. grafted pNIPAM via ATRP in the pores of AAO membranes.95 They analyze the gating functionality of the membrane by the permeation of vitamin B12. They observe a strong increase of permeability by heating above the LCST of pNIPAM, due to the collapse of the blocking polymer layer. This system thus displayed a positive gating effect. Moreover, the thermo-responsive switching of the gates was preserved for three consecutive closed-opened cycles. Very recently, Lee et al.96 reported for a similarly prepared AAO-g-pNIPAM membrane a decrease in resistance with increasing temperature due to the positive gating effect.
As already mentioned, Lokuge et al.81 grafted pNIPAM brushes on a gold-coated nanocapillary array membrane (NCAM) via ATRP to control the thickness of the pNIPAM brushes. They investigated the flow of dextran of different molecular weight through different pore size NCAMs with different pNIPAM brush thicknesses. Below the NIPAM LCST the dextran flow through the NCAM was inhibited due to brush swelling, while above the LCST dextran could flow through the NCAM. This behavior evidences a positive gating effect. These authors were thus able to produce a thermoresponsive molecular gate. Fig. 9 shows the dextran concentration on one side of the membrane measured by UV-spectroscopy, while the other side is a dextran reservoir. Each time the temperature is above the LCST, the gates open and the dextran concentration increases further, while it stays constant when the gates are closed below the LCST.
Most of the effects have been characterized by permeation experiments. In some cases, microscopic observation allowed evidencing pore opening or closing. Given the fundamental question of how the pores are really closed, we think it would be of interest to go further towards microscopic characterization, which in the field of polymer physics is often performed by scattering techniques. Indeed, grazing-incidence, reflectometry, or small-angle scattering of neutrons or X-rays would give access to polymer conformations as a function of the external stimulus, which could then be correlated with permeation experiments. We have found only limited use of these techniques in the literature, and it is hoped to see more applications of these techniques in the future.
One of the key questions which arises when reviewing the most recent contributions is if it is “better” to use temperature-sensitive individual polymer chains (e.g. as smart pore coating), or deposit larger microgel particles and possibly crosslink them together (“all smart”). While the discussion is still open, we note that microgel particles have the advantage of being visible via microscopy at the single-building block scale of the membrane. Moreover, their degree of smartness can be tuned by internal crosslinking. One can imagine, e.g., that tuning the ratio between primary and secondary crosslinking “tightens” the network between two limiting cases, the one of strong particles loosely connected, and the inverse, a strong percolating network filled with fuzzy particles, each case having a different temperature response due to the different degrees of hydrophobicity of each crosslinker. Also, their larger and controllable size can be used to design both “pore covering” and “pore filling” mechanisms. Last but not least, their larger size can be used to prepare membranes with larger pores, and thus higher throughput when the gates are open, while retention is already high with a single microgel layer. On the other hand, da Silva showed that one can get good variation of the flux (and low flux) by grafting individual pNIPAM chains on 5-micron pores, which is highly promising.80
It appears that although continuous progress has been made in the field over the past years, future work should couple fundamental understanding with improved gating properties. This may include better permeation when pores are open, allowing for higher fluxes, while efficiently blocking flux when closed. One can also imagine adding functions to the gating membranes, like embedded catalytic particles (see Sabadasch et al.55) which could favor a desired reaction, like decomposition of some pollutant during filtering. Given the many possible applications, in particular those related to environmental issues (decontamination, waste-water treatment, controlled catalytic reactions…), we are looking forward to following new adventures in this field.
Footnote |
† These authors have contributed equally to the review article. |
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