| Literature DB >> 30018213 |
Abstract
Biomimetic membranes are attracting increased attention due to the huge potential of using biological functional components and processes as an inspirational basis for technology development. Indeed, this has led to several new membrane designs and applications. However, there are still a number of issues which need attention. Here, I will discuss three examples of biomimetic membrane developments within the areas of water treatment, energy conversion, and biomedicine with a focus on challenges and applicability. While the water treatment area has witnessed some progress in developing biomimetic membranes of which some are now commercially available, other areas are still far from being translated into technology. For energy conversion, there has been much focus on using bacteriorhodopsin proteins, but energy densities have so far not reached sufficient levels to be competitive with state-of-the-art photovoltaic cells. For biomedical (e.g., drug delivery) applications the research focus has been on the mechanism of action, and much less on the delivery 'per se'. Thus, in order for these areas to move forward, we need to address some hard questions: is bacteriorhodopsin really the optimal light harvester to be used in energy conversion? And how do we ensure that biomedical nano-carriers covered with biomimetic membrane material ever reach their target cells/tissue in sufficient quantities? In addition to these area-specific questions the general issue of production cost and scalability must also be treated in order to ensure efficient translation of biomimetic membrane concepts into reality.Entities:
Keywords: aquaporin; biomedicine; biomimetic; energy-conversion; sensing; separation
Year: 2018 PMID: 30018213 PMCID: PMC6161077 DOI: 10.3390/membranes8030044
Source DB: PubMed Journal: Membranes (Basel) ISSN: 2077-0375
Figure 1Two popular design concepts for biomimetic separation membranes [13]: (A top) a matrix of vesicles with reconstituted aquaporin proteins embedded in an immobilizing material (yellow) (e.g., polyamide) constitutes the selective layer formed on top of a substrate layer (blue) (e.g., polysulfone). (A bottom) a monolayer with the protein (red) directly embedded in a host membrane (orange) formed on top of a substrate layer (blue). (B) scanning electron micrograph of the design in (A). Scale bar 1 µm. The design in (A top) have also recently been used for creating membranes based on immobilized imidazole quartets [15].
Figure 2(A) Principal diagram of BSSC based on bR/purple membranes immobilized on TiO2 spheres (red) which are deposited on a fluorine-doped tin oxide (FTO) conducting glass. This acts as the working electrode with an FTO surface covered with aluminium (Al) or platinum (Pt) as counter electrode. A redox electrolyte (e.g., based on I−/I2−) is encapsulated between the FTO slides. The photon induced photocurrents arises from excitation of bR leading to electrons being injected into the FTO working electrode. The maximal output (VOC) is determined by the difference between the Fermi level and redox level. (B) Photo-current/photo-voltage (I/V) relation. VOC: open circuit voltage; ISC: short circuit current (at VOC = 0). VMP: voltage at maximal power output PMAX. IMP current at PMAX. The ratio between the yellow area and orange area defines the fill factor (FF), see also Table 1.
Performance data for selected BSSCs.
| BSSC Substrate | Cell Area | Short Circuit Current | Open Circuit Voltage | Illumination Intensity j | Efficiency | Fill Factor | Ref |
|---|---|---|---|---|---|---|---|
| A [cm2] | ISC [A/m2] | VOC [V] | P [W/m2] | H [%] | FF - | ||
| bR-TiO2 g | 0.5 | 0.9 | 0.35 | 400 | 0.002 a | 0.24 b | [ |
| bR-TiO2 h | <2 | 2.3 | 0.22 | 600 | 0.03 c | 0.67 d | [ |
| bR-TiO2 e | 0.25 | 10 | 0.53 | 1000 | 0.35 | 0.66 | [ |
| bR-TiO2 e | 0.25 | 2.8 | 0.52 | 1000 | 0.09 | 0.62 | [ |
| bR-TiO2 f | 0.25 | 2.1 | 0.53 | 1000 | n.a. | n.a. | [ |
| bR-TiO2 e | 0.25 | 4 | 0.5 | 1000 | 0.11 | n.a. | [ |
| bRu-TiO2 e | 0.25 | 2.1 | 0.53 | 1000 | 0.11 | n.a. | [ |
| (bRu + bR)-TiO2 e | 0.25 | 4.5 | 0.57 | 1000 | 0.16 | 0.62 | [ |
| Cu-2-α-oxymesoisochlorin | 1.0 | 90 | 0.52 | 1000 | 2.6 | 0.7 b | [ |
| N719 (Di-tetrabutylammonium cis-bis(isothiocyanato)bis(2,2′-bipyridyl-4,4′-dicarboxylato)ruthenium(II))-TiO2 e | 0.25 | 90.5 | 0.77 | 1000 | 5.9 | - | [ |
a: calculated from Figure 11 in [59] using a linear approximation of the VOC-ISC relationship. b: FF = (VOC·ISC)Pmax/VOC(max)·ISC(max). [74]. c: η = VOC(max)·ISC(max)·FF/Pincoming [74]. d: approximated by eye from Figure 11 in [69]. e: with Pt-coated FTO glass as counter electrode. f: with C-coated FTO glass as counter electrode. g: with Al-coated FTO glass as counter electrode. h: nanotube arrays. i: Pt as counter electrode. j: white light illumination. 1: Table 1 is by no means exhaustive, but serves to provide exemplary values for ISC, VOC, FF, and η in biomimetic systems allowing for direct comparison with conventional photovoltaic cells.
Figure 3Examples of thermo-responsive nano-carrier designs with biomimetic membrane coatings where the basic mechanism of action is to induce a local temperature increase by near-infrared laser illumination to >43 °C which leads to hyperthermal tissue (tumor) destruction. (A) Red blood cell mimicking carrier for delivering paclitaxel (PTX) using 808 nm laser irradiation which is captured by the membrane embedded DiR dye molecule. The ensuing thermal energy triggers a DPPC phase transition and core destruction, resulting in the release of the chemotherapy medication PTX [89]. (B) Cancer cell mimicking carriers for delivering the diagnostic dye indocyanine dye. By utilizing binding molecules from cancer cell membranes adhesion to homologous cancer cells can be achieved while the DPPE-PEG prevents phagocytosis non-specific binding to serum proteins resulting in tumor accumulation of the nano-carrier. Irradiation at 780 nm results in energy absorption in ICG and thermal destruction of the tumor [90]. (C) Macrophage-camouflaged carrier where macrophage proteins provide molecular recognition with tumor proteins and the Au-coated silica core allows for energy absorption at 808 nm leading to thermal tumor destruction [91].