>98.5 MgSO
Cellulose-base (CA) membranes have been developed and commercialized for more than 60 years. In 1955, cellulose acetate membranes were prepared and introduced by Reid et al. using acetone as the solvent [ 28 ]. The general synthesis process of CA membrane is called phase inversion method: cellulose triacetate is first dissolved in an organic solvent or solvent mixture to form a casting solution. Then the solution is coated on a flat or tubular support. Finally, the support is immersed in a non-solvent bath, where polymer coagulation occurs and a CA membrane forms. Although CA membranes made by Reid at al. had good selectivity, the water permeability was extremely low and could not be used for practical applications. In 1963, Loeb et al. invented the first efficient RO membrane: cellulose diacetate (CDA) membrane. CDA membranes had much higher flux compared to CA membranes but were prone to biological attack [ 29 ]. The invention of CDA membranes accelerated the development of cellulose triacetate (CTA) membranes, which had slightly stronger thermal, chemical, and biological stabilities [ 30 ]. With asymmetric morphologies, cellulose-based membranes have anisotropic structures, consisting of an upper skin layer on a porous sublayer [ 31 ]. Both the skin layer and porous sublayer have identical chemical composition. The filtration performance of CA membranes depends on the degree of acetylation. For instance, CA membrane with 40 wt% acetate and a 2.7 degree of acetylation had a salt rejection between 98% and 99% [ 32 ]. Higher acetylation will result in higher selectivity but lower water permeability. CA membranes are stable in pH range 4–6. In acidic and basic feed solutions, hydrolysis reaction will happen and lower the selectivity.
Though membranes with better separation performances and comparable costs were fabricated, some studies were reported to improve CA membranes. Chou et at. found dispersing silver nanoparticles on CA membrane surface would increase its biological stability while maintain the permeability and salt rejection [ 33 ]. Coating phospholipid polymer on CA membrane during phase conversion resulted in a fouling-resistant membrane with high water flux [ 34 ]. A small percentage of mineral fillers such as aluminum oxide improved the compaction resistance of CA membranes remarkably [ 35 ]. During the past four decades, thin-film composite (TFC) membranes, whose permeability and rejections surpass those of CA membranes, have dominated the market. However, CA membrane still exists due to its overall exceptional chlorine resistance, which depends on several parameters such as polymer type, synthesis procedure, and pH of feed solution. Since feed water disinfection is a necessary step in RO and NF installations and chlorine is the most common choice of disinfectants, it is important to have chlorine-tolerant membranes for water treatment. Table 2 shows effects of various processing methods on chlorine resistance. Current research mainly focuses on modifications of TFC membranes for chlorine resistance improvement.
Effects of various processing methods on chlorine resistance.
Membrane | Processing Method | Performance Evaluation | Reference |
---|---|---|---|
Cellulose acetate | Blending with polyethersulfone and polyethylene glycol | Such blended membranes had higher porosity (permeability) and chlorine tolerance compared with virgin cellulose acetate membranes. | [ ] |
Sulfonated poly | Made with high fluorine contents | Sulfonated-fluorinated poly membranes displayed long-term stability (>30 days) under high acidic chlorine condition. | [ ] |
Aromatic polyamide | Adding 0.1–1 wt% multi-walled carbon nanotubes | The carbon nanotube based polyamide membranes had good selectivity and longer lifetime during desalination process. | [ ] |
Sulfonated poly | Membranes were prepared by direct copolymerization method | Water permeability and contact angle remained unaffected when exposed to high level of chlorine and wide range of pH (4–10). | [ ] |
Cellulose triacetate | Adding sodium hexametaphosphate (SHMP) as masking agent | SHMP inhibited oxidation degradation of cellulose triacetate membranes by chlorine. | [ ] |
Sulfonated cardo poly | Extra layer of formaldehyde-cross-linked polyvinyl alcohol was coated on membrane surface | The coated layer improved NaCl rejection from 91.2% to 96.8% and the membrane showed better chlorine resistance in RO operation. | [ ] |
Polyamide | Membrane synthesized by interfacial polymerization of -phenylethylenediamine and 1,3,5-benzenetricarbonyl trichloride | When immersed in NaOCl solution, the membrane exhibited higher chlorine tolerance than a commercial polyamide membrane. | [ ] |
TFC membranes were invented by Cadotte in the 1970s, but were not widely used until the second half of the 1980s [ 43 ]. Polyamide (PA) membranes were developed by Hoehn and Richter and had good water purification performance. The main drawback of PA membranes was susceptibility to free chlorine attack [ 44 ]. After development of TFC membranes, it was found the PA TFC membranes had outstanding separation performance as well as better chlorine resistance. As shown in Figure 3 , the structure of a PA TFC membrane consists of a thin selective barrier layer on a porous support [ 45 , 46 , 47 ]. The support has a microporous structure (UF membrane), providing mechanical strength and high water flux, and the barrier layer has a function of ion separation. Compared with CA membranes, which can only be made from linear, soluble polymers, TFC membranes have more desirable characteristics. Many materials (linear and crosslinked polymers) and approaches can be used to synthesize or modify the porous support and barrier layer individually to optimize the thermal and chemical stabilities, permeability, salt rejections, etc. Many papers focus on improving TFC membranes for RO applications have been published. On the other hand, the manufacturing cost of TFC membranes is higher than that of CA membranes since at least two membrane fabrication steps are needed: synthesis of microporous support followed by synthesis and deposition of barrier layer on microporous support.
Thin-film composite membrane structure.
The porous support plays an important role in providing mechanical strength to withstand high pressure during RO and NF processes. Meanwhile to form a defect-free barrier layer, the surface of the support needs to be uniform and smooth. Polysulfone is one of the most significant microporous supports for TFC membranes [ 48 ]. The surface pore size of polysulfone support ranges from 1.9 nm to 15 nm, with a surface porosity up to 16% [ 49 , 50 ]. The selectivity generally increases with decreasing pore size [ 51 ]. Since polysulfone shows good structural stability in a wide pH range, barrier layers made from highly acidic or alkaline precursors can be coated on polysulfone substrates. The disadvantages of polysulfone include poor weatherability, low chlorine resistance, and prone to stress cracks. Adding nanoparticles and applying new preparation methods are two main approaches to improve polysulfone supports. A chlorine-resistant TFC membrane can be made by metalation sulfochlorination of polysulfone [ 52 ]. Plasma treatment on polysulfone support results in the exhibition of hydrophobicity, which optimizes chlorine resistance and water permeability [ 53 , 54 ]. In addition to polysulfone, CA, polyimide, polypropylene, polyketone and polyethylene terephthalate (PET) have also been used as porous supports [ 55 , 56 , 57 , 58 ]. A hydrolyzed PA CA membrane has been fabricated and the covalent bond between porous CA support and selective PA barrier layer indicates a chemical stable structure. This membrane exhibits a NaCl rejection up to 97% [ 58 ]. In addition, TFC membranes synthesized by heat and plasma treatments using electrospun nanofibers as supports showed remarkable filtration performance [ 59 ]. Yoon et al. have prepared a PA TFC membrane using polyacrylonitrile (PAN) nanofibrous scaffold as porous support. The experimental result showed the PA PAN composite membrane has similar sulfate rejection rate (98%) but 38% higher water permeability compared to commercial NF membranes (NF270) [ 60 ]. Several recent studies focus on the effect of support pore size on barrier layer formation and water purification performance, but there have been no consistent conclusions so far [ 61 , 62 ].
Most selective barriers of TFC membranes are synthesized by interfacial polymerization, which occurs at an interface between two immiscible monomers/solvents [ 63 , 64 ]. Once a layer forms at the interface, solvents from both sides cannot pass through it and therefore the reaction stops, producing a membrane thinner than 200 nm ( Figure 4 ). Heat treatment is necessary since interfacial polymerization happens at elevated temperature. The purification performance of TFC membranes is primarily determined by barrier layer, which is affected by solvent type and concentration, curing condition and temperature. Table 3 summarizes precursors for preparing TFC membranes by interfacial polymerization method for water purification in recent studies. Due to their good mechanical property and outstanding rejection ratio, TFC membranes are used in a large number of purification tasks, especially in desalination. The main problem associated with TFC membranes is their flux and salt rejection decrease gradually as a result of fouling, particularly in treating with wastewater containing bacteria and nutrients. According to Mansourpanah et al., TFC membranes with antifouling property can be prepared by grafting functional groups or adding hydrophilic additives on membrane surface through radiation or plasma treatment [ 65 ]. The altered barrier layer becomes smooth, hydrophilic and has similar surface charge as foulants. Therefore the interaction between contaminants and membrane surface is reduced. It is also found that TFC membranes blended with polyacrylamide and polymethacrylic acid exhibit biofouling resistance [ 66 ]. Deposition of natural hydrophilic polymers such as sericin would increase surface hydrophilicity of TFC membranes, and improves selectivity and fouling resistance [ 67 ]. Another drawback of TFC membranes is poor chlorine resistance. During water purification process, chlorine (frequently used as disinfectant) changes the hydrogen bounding in TFC membranes, resulting in performance decay [ 68 ]. Thus, it is essential to increase chlorine resistance of TFC membranes. A chlorine-resistant TFC membrane has been invented by Yao et al. by secondary interfacial polymerization method to eliminate the interaction between unreacted amino groups and free chlorine [ 69 ]. Experimental results indicated TFC membranes blended with layered double hydroxides (LDHs) have high porosity and hydrophilicity, exhibiting superior chlorine resistance and anti-fouling capacity [ 70 ]. Similar studies focus on enhancing chlorine resistance of TFC membranes by incorporating additives are available in literature [ 71 , 72 , 73 ]. From a technique perspective, methods such as atomic layer deposition (ALD) controls membrane thickness precisely through sequential surface reactions [ 74 ]. Hydrophilic selective barriers synthesized using this technology have excellent fouling and chlorine resistance.
Mechanism of interfacial polymerization.
Monomers and performance evaluation for thin-film composite (TFC) membranes prepared by interfacial polymerization method.
Monomer A | Monomer B | Performance Evaluation | Reference |
---|---|---|---|
Ethylenediamine | Cyclodextrins | Membrane had a water flux up to 28 L/m h (LMH) and good antifouling properties with flux reduction <20%. | [ ] |
Piperazine | 1,3,5-Benzene-tricarbonyl trichoride | High salt rejection (98% for Na SO and 97.5% for MgSO ) with enhanced water permeability. | [ ] |
-Phenylenediamine | Trimesoyl chloride | Membrane exhibited large free volume, high water flux, and low reverse salt flux. | [ ] |
Hexylene glycol | 1,3,5-Benzene-tricarbonyl trichoride | Both flux stability and fouling reversibility improved for Ca modified membranes. | [ ] |
1,3-Phenylenediamine | 1,3,5-Benzene-tricarbonyl trichoride | Membranes with two PA layers showed much higher flux and selectivity than commercial TFC membranes. | [ ] |
Piperazine | 2,4,6-Trischlorosulfonylphenol | Membrane had a flux of 13.98 LMH and good rejections for CuSO and H SO . | [ ] |
Polyallylamine | 1,3-Benzenedisulfonyl chloride | Membrane was positively charged and had selectivities greater than 90% for heavy metal ions. | [ ] |
-Phenylenediamine | 1,3,5-Triformylphloroglucinol | Membrane presented a stable rejection to Congo red of 99.5% and a high flux up to 50 LMH. | [ ] |
-Aminoethyl piperazine propane sulfonate | Trimesoyl chloride | Compared with pristine membrane, the flux increased by 82% while the NaCl rejection remained above 98%. | [ ] |
Pentaerythritol | Trimesoyl chloride | Membrane had a high rejection of Na SO (98.1%) but a low water flux of 6.1 LMH. | [ ] |
Although ceramic/inorganic RO and NF membranes have only been studied for 30 years and are in early stage of commercialization, their encouraging performance, as exemplified in Table 4 , offers great potential for water purification. In this section, two classes of ceramic membranes made from different inorganic materials are discussed.
State-of-the-art inorganic RO and NF membranes for water purification.
Membrane. | Application | Salt Rejection (%) | Flux/Permeability | Reference |
---|---|---|---|---|
γ-Al O | Desalination | 97.1 Fe , 90.9 Al , 85 Mg , 84.1 Ca , 30.7 Na , 27.3 NH | 17.4 LMH/bar | [ ] |
PVA-Al O | Dye wastewater treatment, Desalination | 96 Congo red dye 3 NaCl | 25 LMH | [ ] |
CMS-Al O | Desalination | 93 NaCl | 25 kg m h , 3.5 wt% NaCl, 75 °C | [ ] |
Al O (FAS grafted) | Desalination | >99.5 NaCl | 19.1 LMH, 2 wt% NaCl, 80 °C | [ ] |
TiO | Desalination | 99 NaCl | 6 kg m h , 10 wt% NaCl, 75 °C | [ ] |
ZrO | High salinity water treatment | >90 PEG 1000 68, 24.92 wt% NaCl | 13 LMH/bar | [ ] |
TiO -ZrO | Radioactive waste treatment | 99.6 Co , 99.2 Sr , 75.5 Cs | 40 LMH/bar | [ ] |
SiO | Desalination | 99.5 NaCl | 6.6 kg m h , 3.5 wt% NaCl, 22 °C | [ ] |
SiO | Desalination | 99.6 NaCl | 9.5 kg m h , 3.5 wt% NaCl, 22 °C | [ ] |
CoO-SiO | Desalination | 99.7 NaCl | 7.7 kg m h , 3.5 wt% NaCl, 22 °C | [ ] |
Ax-GO | Desalination | 99.9 NaCl | 19.7 kg m h , 3.5 wt% NaCl, 90 °C | [ ] |
CNT-rGO | Drinking water purification | 97.3 Methyl orange | 20–30 LMH/bar | [ ] |
TiO -GO | Dye wastewater treatment | >97 Organic dyes | 89.6 LMH/bar | [ ] |
APT-GO | Dye wastewater treatment | ~100 Rhodamine blue | 13.3 LMH, 7.5 mg L RhB | [ ] |
MoS | Dye wastewater treatment | 100 Methylene blue | 135.3 LMH/bar | [ ] |
YSZ | Dye wastewater treatment | >98 NaCl | 28 LMH/bar | [ ] |
Compared to polymeric membranes, inorganic membranes offer higher chemical stability and stronger mechanical properties. Metal oxides such as alumina, zirconia, and titania form an important class of ceramic membranes. Conventionally, a RO metal oxide membrane has an asymmetric structure consisting of a thick macroporous (>50 nm) support, an intermediate mesoporous (2–5 nm) layer, and a thin selective (<1 nm) top layer. A NF metal oxide membrane has similar structure as RO metal oxide membrane but contains no selective top layer [ 101 , 102 , 103 ]. The most widely used approach for preparing metal oxide ceramic membranes is sol-gel method, which converts precursor solutions into solid membranes in four steps: precipitation reaction first happens between hydrolyzed precursors, followed by a peptization reaction in which precipitation transforms into a colloid sol. The stable sol is then coated on a porous support and gelates during drying. Finally high temperature sintering is applied to the membrane to optimize mechanical properties and pore structure [ 8 , 89 ]. In order to make homogeneous membranes with less defects, colloidal particles are dispersed uniformly in the solvent by stabilizers such as nitric acid, ethanolamine (MEA) and triethylenetetramine (TETA) [ 104 , 105 , 106 ]. Since complex fabrication process of multi-layered membranes as well as expensive precursor materials indicating high manufacturing cost, simplified synthesis method and use of cheap materials will reduce the production cost and accelerate the development and commercialization of ceramic membranes.
One of the most widely studied inorganic membranes is alumina membrane, which has an average pore size of 2–5 nm (MWCO of 3000–1000 Da) and is commonly used in NF systems or as an intermediate layer in RO membranes [ 107 ]. Alumina membranes with pore size smaller than 1 nm has been made, but showed low permeability (5 LMH/bar) and cannot be used for industrial purposes [ 8 ]. Wang el al. have prepared a supported γ-Al 2 O 3 hollow fiber membrane with a mean pore size of 1.61 nm that demonstrates a high water permeability of 17.4 LMH/bar [ 85 ]. This membrane exhibits good selectivity for multivalent ions such as Ca 2+ (84.1%), Mg 2+ (85%), Al 3+ (90.9%) and Fe 3+ (97.1%), but very low retention of monovalent ions such as NH 4 + (27.3%) and Na + (30.7%). Recent studies focus on surface modification of alumina membrane to further improve its purification performance. For instance, a mixed matrix carbon molecular sieve (CMS) and α-Al 2 O 3 membrane fabricated by vacuum-assisted impregnation method has a water flux up to 25 kg m −2 h −1 and a salt rejection between 93% and 99% when tested using 3.5 wt% NaCl (seawater) at 75 °C [ 87 ]. Ren et al. changed the surface of a porous alumina membrane from hydrophilic to hydrophobic by fluoroalkylsilane (FAS) grafting, resulting in a water flux of 19.1 LMH and salt rejection over 99.5% [ 88 ]. Such outstanding salt retention and water permeability hold promise for practical desalination applications. In addition to surface modification, using cheap precursor materials provides both economic and environmental benefits. Researchers have used Al 2 O 3 hollow fiber supports and coal fly ash, a byproduct of coal burning, to synthesize Al 2 O 3 -NaA zeolite membranes successfully. The Al 2 O 3 -NaA zeolite membrane has been used to treat wastewater containing lead ions (Pb(Ⅱ), 50 mg L −1 ) and possesses a Pb(Ⅱ) removal rate of 99.9% [ 108 ].
Zirconia and titania are other popular materials for ceramic membranes. In sol-gel method, zirconium alkoxides are often used as precursors to prepare zirconia sols [ 109 , 110 ]. However, some zirconium alkoxides such as zirconium propoxide is water-reactive, which could produce agglomerates rather than stable nanoparticles. Therefore at the beginning few laboratories had successfully synthesized zirconia membranes. In 1998, Garem et al. discovered that adding 13 mol% magnesium would enhance the chemical and thermal stabilities of zirconia sols [ 111 ]. Since then many stabilizers have been investigated for preparing zirconia membranes. Glycerol has been introduced into the sol-gel process to make ZrO 2 NF membranes for treating high-salinity wastewater. More specifically, glycerol binds to the surface of ZrO 2 nanoparticles as a capping agent and prevents phase transformation during calcination. The crack-free ZrO 2 NF membrane exhibits a permeability of 13 LMH/bar and approximately 68% rejection rate when filtering NaCl solutions with mass fraction up to 24.92% [ 90 ]. Lu et al. have used zirconium salts and titanium alkoxides as sol-gel precursors to prepare a TiO 2 -doped ZiO 2 NF membrane [ 91 ]. The addition of Ti 4+ suppresses zirconia phase transformation, narrows the pore size distribution and increases the specific surface area. This membrane has high water permeability above 35 LMH/bar with a MWCO of 500 Da, and simulated retention rates of 99.6% for Co 2+ and 99.2% for Sr 2+ , indicating its attractive potential for radioactive wastewater treatment. Compared with alumina and zirconia membranes, the surface pore size and phase composition of titania membranes can be controlled by synthesis procedure. Anatase is the most preferable crystal form of titania due to its exceptional stability and narrow pore size distribution. A TiO 2 membrane with a pore diameter of 4 nm has been fabricated successfully by gentle heat treatment and remained stable in various solutions (brackish water, sea water and brine water) for over 350 h [ 89 ].
In addition to traditional metal oxide membranes, composite membranes made of two or more metal oxides is a current research focus. For example, a bilayer membrane containing a TiO 2 layer on top of a ZnAl 2 O 4 layer has been prepared and evaluated. It has been proved that compare to single layer membrane made from 50 mol% TiO 2 and 50 mol% ZnAl 2 O 4 with similar pore size, the bilayer membrane which has opposite surface charges could increase the electric interactions between membrane pores and filtered ions, and therefore produces a higher salt rejection, especially for divalent salts [ 112 ]. Another example of inorganic composite membranes is CoO-SiO 2 membrane synthesized by Elma et al. for desalination applications [ 94 ]. The effects of cobalt addition (up to 35 mol%), feed solution concentration (0.3–7.5 wt% NaCl), and operation temperature (22–60 °C) on purification performance were investigated systematically. Experimental results showed the volume fraction of silica mesopores increases with cobalt concentration, and with over 99.7% NaCl retention rate at all times, the highest water flux of 20 kg m −2 h −1 was achieved for 0.3 wt% feed solution at 60 °C. Furthermore, a series of studies confirm that silica membranes blended with cobalt oxide exhibit not only excellent desalination performance but also robust structures compared to single-element SiO 2 membranes [ 92 , 93 ].
In spite of prominent outcomes of metal oxide RO and NF membranes, certain shortcomings such as raw material cost and membrane thickness have hindered their commercialization for water purification. These issues can be overcome by further reducing the membrane thickness or exploring other cheap materials that have great chemical and thermal stabilities. Membranes that have strong surface charges in aqueous environment are also attractive.
In recent years, ordered mesoporous materials (OMMs) have attracted increasingly research interests in addressing water pollution and water shortage problems [ 113 , 114 ]. Among all kinds of OMMs, ordered mesoporous carbons (OMCs) such as carbon nanotubes (CNTs) and graphene possess important properties including large specific surface area, highly uniform structure with tunable pore size and strong atomic bonds, thus have been selected as promising candidates for wastewater treatment applications [ 115 , 116 , 117 ]. As one of fullerene derivatives, CNTs are cylindrical molecules composed of rolled-up graphite sheets with diameter ranges from 1 nm to several centimeters [ 118 ]. Based on the layers of graphite sheets, CNTs can be further classified into single-walled carbon nanotubes (SWCNTs), double-walled carbon nanotubes (DWCNTs) and multi-walled carbon nanotubes (MWCNTs). For water desalination and purification applications, CNTs can be fabricated into standalone membranes or incorporated with other materials in many formats. An investigation of a highly stable and electrochemically active membrane made solely of CNTs, which could find significant applications in chemical and biological wastewater treatment, was undertaken by Sadia et al. [ 119 ]. Such CNTs membrane maintained a phenol removal rate over 85% for 4 h with an average oxidation rate of ~0.059 mol h −1 m −2 when operated with H 2 O 2 . Since water molecules can transport through CNTs structure without much impedance, some CNTs membranes used in RO systems with outstanding salt rejections as well as high water permeabilities have been reported [ 120 , 121 , 122 ]. On the other hand, the incorporation of CNTs into polymeric or inorganic matrix makes it possible to modify membrane properties and further improve surface hydrophilicity, fouling resistance, structural stability and salt retention. Yang et al. have confirmed a polyvinyl alcohol (PVA) based carboxylic MWCNTs membrane synthesized by interfacial adhesion method has better thermal stability and separation performance than a PVA membrane without carboxylic MWCNTs [ 123 ]. This PVA/C-MWCNT membrane exhibits a water flux of 6.96 kg m −2 h −1 and a NaCl rejection of 99.91% at 22 °C. In the work conducted by Peydayesh et al., hyperbranched polyethyleneimine modified MWCNTs were incorporated into polyethersulfone matrix to form a positively charged NF membrane, which had a average pore size of 0.81 nm and an enhanced water flux of 75.7 LMH [ 124 ]. The hybrid membrane showed superior retention rates for heavy metals (i.e., 99.06% for Zn 2+ , 94.63 for Ni 2+ , and 93.93% for Pb 2+ ) and antifouling property due to effective membrane surface charge and hydrophilicity, respectively.
Despite advantages of CNTs, drawbacks such as high cost and low selectivity for certain ions (arsenate, arsenic, and sodium) have limited their commercialization [ 118 ]. Graphene, a cost-effective two-dimensional carbon allotrope that consists of a monolayer of carbon atoms arranged in hexagonal lattice, has been found to be a highly permeable and selective material for water purification processes [ 125 , 126 ]. Since water flux across a membrane is inversely proportional to the membrane thickness, single-atom-thick graphene offers an opportunity for exceptional permeability and efficient energy utilization [ 127 ]. Pure graphene has a closely packed structure which is impermeable to gas and liquid molecules. Therefore to improve permeability and ion selectivity defects or functional groups must be generated designedly. Nanoporous graphene can be fabricated either by electrochemical modification of pristine graphene or by growth on supports from different chemical reactions [ 128 ]. The most commonly applied techniques to generate nanosized pores on graphene structure include high-temperature oxidation, ultraviolet (UV) ozone treatment and plasma etching [ 129 , 130 , 131 ]. Sub-nanometer-sized pores on monolayer graphene have been created successfully for nanofiltration and desalination applications [ 132 ]. During synthesis process, small defects were first introduced by ion bombardment and further enlarged by oxidative etching. The experimental results revealed that the separation mechanisms of the porous graphene membrane at short and long oxidation periods are electrostatic repulsion and streric size exclusion, respectively. Graphene oxide (GO), chemically converted from graphene nanosheets, has oxygen functional groups such as hydroxyl and epoxy which enable it to have better water dispersibility than graphene [ 133 , 134 ]. Nair et al. invented a GO membrane consisting of closed-packed GO sheets that only allow water molecules to travel through and concurrently hinder the motion of other species [ 135 ]. Similarly, Zhao et al. designed a free-standing GO membrane in which the GO sheets are crosslinked by Ca 2+ from Congo red dye [ 136 ]. More specifically, this GO membrane with tunable interlayer spacing was prepared by facile and thermal reduction methods using hot pressing method. Accompanied by relative high water permeability (17.1 LMH/bar), the resulting membrane showed excellent removal rates for heavy metal ions (i.e., 98.6% for Cu 2+ , 97.2% for Pb 2+ , 99.1% for Cd 2+ and 97.2% for Ni 2+ ). Although there have been many breakthroughs and exciting achievements for porous graphene and GO membranes in water filtration, special synthesis techniques for large-area porous membranes and fabrication reproducibility remain challenges towards commercialization.
Mixed matrix membranes (MMMs), a currently popular area of research, are made by incorporating inorganic fillers into organic matrices. Although TFC membranes have excellent salt removal performance, there is a trade-off between permeability and selectivity. The main advantage of MMMs is to combine the low manufacturing cost, outstanding selectivity and high packing density of polymeric materials with long-term stabilities, high mechanical strength and regeneration capability of ceramic materials. One type of MMMs is a polymeric membrane blended with inorganic nanoparticles, which can be prepared by dispersion crosslinking, interfacial polymerization, or dip coating. Inorganic fillers that have been investigated for this purpose include titania, zeolite, silica, alumina, etc., and experimental results indicate the addition of inorganic nanoparticles alter the polymeric structures and effect the transportation of molecules through membrane pores [ 137 , 138 , 139 , 140 , 141 ]. Therefore it is not surprising that small inorganic nanoparticles would improve the water purification performance of organic membranes. Titania is widely used in anti-fouling coating due to its photocatalytic property. Kim et al. studied the influence of TiO 2 fillers on the properties of carboxylate groups functionalized TFC membranes and found the carboxylate groups help the adsorption of titania on TFC membrane surface, which result in very good anti-biofouling properties, especially under UV excitation [ 142 ]. Such a hybrid RO membrane also has stable surface structure since no significant loss of titania particles was observed after being tested for 168 h [ 143 ]. Researchers also recognized the addition of zeolite and silica nanoparticles increases the surface roughness, contact angle, and water flux [ 144 , 145 ]. NaA zeolite nanoparticles are the first successfully synthesized zeolite particles with low contact angle (<5°) and RO ranged pores (~0.5 nm) [ 146 ]. MMMs prepared with NaA zeolite fillers by interfacial polymerization method have many outstanding properties, that is, more negatively charged and hydrophilic surface with increasing zeolite content, enhanced water permeability, and better water purification performance [ 147 ].
Composite membrane synthesized from carbon-based materials and organic materials is another type of MMMs. Majumder et al. reported a polystyrene membrane incorporated with MWCNTs which have an average diameter of 7 nm [ 148 ]. The MWCNTs were grown and aligned by catalytic chemical vapor deposition (cCVD) method, followed by spin coated on polystyrene matrix to seal gaps between CNTs. The tips of MWCNTs were opened by plasma etching approach, and the water flux of the synthesized composite membrane was 4–5 orders of magnitude higher than that calculated from Hagen-Poiseuille theory, indicating macroscale hydrologic mechanism. On the other hand, some researchers explained the ultra-high water flux was due to the formation of a layer of water molecules along MWCNTs walls, which reduce the friction significantly when bulk mater molecules come through [ 149 ]. Furthermore, to simplify the complex fabrication steps of MMMs, a patient has been published recently about dispersing 0.8 nm diameter CNTs into cross-linking solutions during the formation of polymeric membranes, so that the CNTs can be embedded into the organic barrier layer on top of microporous polyethersulfone support [ 150 ]. After being functionalized by octadecylamine, tests were performed on membranes made with and without CNTs to demonstrate the improved water flux generated by CNTs pathways. Experimental results showed the flux of membrane containing CNTs was approximately twice as much as that without CNTs (44 L m −2 day −1 bar −1 compared with 26 L m −2 day −1 bar −1 ), and MMMs with CNTs also had a slightly better salt rejection (97.7% compared with 96.2%). Even though MMMs combine the benefits of both polymeric and ceramic membranes, they are difficult to study since the interface between various materials may have unwanted structure and certain great materials become insoluble in each other. In addition, studies on MMMs with larger surface area are necessary before developing manufacturing apparatus for large-scale production.
Although the water purification market has been occupied by polymeric membranes for more than 10 years, research and development activities in polymeric membranes are reaching the bottleneck and many industries still use traditional TFC membranes such as PA membrane which was introduced nearly 40 years ago. Despite expansions of TFC membranes and related techniques, it is time to upgrade RO technology to a new height or develop another cutting-edge technology for water purification. Addition of functional materials such as inorganic fillers, lyotropic crystals, CNTs, MWCNTs, and aquaporins can optimize the water flux and/or salt rejection, but the high cost issue associated with synthesis and blending these materials needs to be addressed before scale-up production and commercialization [ 151 , 152 ]. Meanwhile, new models are needed to predict the performance of composite membranes. Traditional polymeric RO and NF membranes are commonly modeled based on extended Nernst-Planck equation, which needs to be modified for carbon-based MMMs [ 153 ]. Recent models applied to calculate water flux and salt rejection of charged membranes for aqueous electrolyte solutions are listed in Table 5 . For organic membranes blended with CNTs, CNTs can be simplified as circular cylinders, the fluid transport of which can be modeled using Hagen-Poiseuille equation. The flow through pores outside the CNTs and within the polymeric matrix can still be studied by extended Nernst-Planck model concerning dielectric exclusion since the dielectric constants for feed water, CNTs and organic matrix are different and electrostatic interactions will happen between ions in feed solution and polarization charges formed along the boundary of various dielectric media [ 154 ]. Assuming that the CNTs are distributed uniformly in polymeric base, the predicted model for such MMMs is likely to be extended Nernst-Planck formula plus an additional Hagen-Poiseuille term. Both terms are re-written according to their corresponding concentration before addition. The modeling of MMMs with GO fillers is more complicated and depends on the insertion direction: if GO is blended vertically into organic membrane like CNTs, similar equation of CNTs MMMs can be used for GO MMMs; If GO is added horizontally, the tortuosity factor in the extended Nernst-Planck equation needs to be revised due to the fact that the ion transport path inside GO is different from that in polymeric matrix. Additionally, since the functional groups located on the surface of GO (types of functional groups are determined by synthesis method, precursor materials, etc.) can react with ions in fluid and form complexes, the flux and permeability may change with time, indicating possible process-model mismatch. On the other hand, advanced techniques including rapid thermal processing (RTP) and nanorods fabrication enable the generation of defect-free membranes for water treatment applications. In addition to the use of new materials and leading-edge technologies, membrane diameter also plays an important role in enhancing filtration performance. Membranes with large surface area could reduce capital cost and energy consumption by approximately 15% [ 68 ]. Furthermore, different water treatment plants have specific difficulties to overcome. For instance, low recovery rate of seawater, disposal of brine and high capital cost are the biggest challenges that nowadays desalination plants confront. Tarquim et al. have developed a method to minimize produced brines, which results in good recovery rate, but more research and equipment are needed to reduce brine disposal [ 155 ]. Moreover, integration of traditional synthesis process with renewable energy may make green fabrication of nanocomposite membranes possible.
Recent models for transport of aqueous electrolytes through charged membranes.
Suitable Retention Mechanisms | Model | Model Evaluation | Reference |
---|---|---|---|
UF | Irreversible thermodynamic model | The model can be used to predict the performance for single electrolyte solution but not for mixed electrolyte solutions. | [ ] |
RO/UF | Extended Nernst-Planck model | Single-ion rejection calculated from the model matched with that obtained from irreversible thermodynamic model, and there is little difference between mixed-ion rejection and experimental data. | [ ] |
NF | Solution-diffusion-electromigration model | Easily modeled chloride and sulfate selectivities with transmission coefficient simplified to zero. | [ ] |
RO | Merten and Lonsdale transport model | The model gave concentration polarization corrected salt transport coefficients whose effects were significant at high feed pressures. | [ ] |
RO/NF | Donnan steric pore model and dielectric exclusion | Dielectric exclusion was considered as the primary effect when analyzed mass transfer of electrolytes and neutral solutes. | [ ] |
NF | Coupled series-parallel resistance model | This model was developed specifically for organic solvents permeating through ceramic membranes and a good fit to experimental data was obtained for different solvents. | [ ] |
RO/NF | Pore blockage-cake filtration model | Model had similar results and coefficient of determination as Faridirad model, but with lower Akaike information criteria values. | [ ] |
The excellent filtration performance of inorganic membranes, as stated in Table 4 , indicates the capacity of ceramic membranes for most water purification applications, and the low acceptance of inorganic membranes in the past is because of the sheer dominance of polymeric RO and NF membranes in large-scale water treatment systems. Recent research on preparation of advanced inorganic membranes such as free-standing CNTs membranes and interlayer free membranes enables efficient filtration process with better purification performance and lower facility cost [ 8 , 162 ]. According to Weschenfelder et al., the operation expense and total cost of a water treatment plant using ceramic membranes with a flow rate of 2 m/s and water recovery rate of 95% are US $0.23/m 3 and US $3.21/m 3 , respectively [ 163 ]. Similar to polymeric membranes, the development and manufacturing costs of ceramic membranes remains a significant problem for their industrialization. For example, although there have been rapid growth and development for CNTs and MWCNTs membranes in laboratory-scale, the commercial applications of carbon-based membranes are ongoing in a low pace due to the high cost of synthesizing CNTs and MWCNTs. Thanks to recent advancements in fabrication technology including cCVD, large-scale synthesis of high-quality CNTs economically is achievable. However, the reproducibility and feasibility of these methods for making membranes are in doubt. For traditional metal oxide membranes, high cost of supports is a challenging issue for commercialization. Current research focuses on studying alternative inorganic membranes made from cheaper or waste materials such as coal fly ash to reduce the manufacturing investment.
Tremendous amount of effort has been made to overcome the clean water scarcity and nanotechnology is a strong candidate with fast development. Study and commercialization of polymeric RO and NF membranes started in the early 1960s. So far the water desalination market is dominated by two kinds of membranes: cellulose-based (CA) membranes and thin-film composite (TFC) membranes. The most representative products such as TS40, TS80 and AD-90 were developed more than 30 years ago and due to their low manufacturing costs and high salt rejections, no major change has been made since then. New research directions for barrier layers in TFC membranes include improvement of fouling resistance as well as chemical and thermal stabilities. Meanwhile microporous supports can be optimized to increase the mechanical strength and permeability.
Inorganic RO and NF membranes have been studied in lab scale for water purification since the 1980s. The most representative ceramic membranes are metal oxide membranes and carbon-based membranes. The main synthesis method for metal oxide membranes is sol-gel technique, which needs further optimization to control the particle size and distribution. The performance of mixed matrix membranes (MMMs) made with both organic and inorganic nanomaterials is excellent, yet they are too expensive compared with other membranes. Hence it is important to realize the economic competitiveness of MMMs, as well as their potential applications. While nanotechnology is leading the way in developing RO and NF membranes for water purification, there are still technical and scientific problems that need to be solved before more benefits can be realized. Despite the challenges to be overcome, it is highly possible that ceramic membranes will be commercialized and industrialized in water purification and desalination fields in the near future.
This research received no external funding.
The author declares no conflict of interest.
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npj Clean Water volume 5 , Article number: 10 ( 2022 ) Cite this article
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Water contamination due to environmental conditions and poor waste management in certain areas of the world represents a serious problem in accessing clean and safe drinking water. This problem is especially critical in electricity-poor regions, where advanced water purification methods are absent. Here, we demonstrate that titanium dioxide nanowires (TiO 2 NWs)-based photocatalytic filters assisted only with sunlight can efficiently decontaminate water. Moreover, interweaving TiO 2 NWs with carbon nanotubes (CNTs) leads to the formation of a TiO 2 NWs/CNTs composite material and offers an additional water decontamination channel, that is of pasteurization with the visible part of the solar emission spectrum. Our results demonstrate that this nanoporous filter can successfully intercept various types of microbial pathogens, including bacteria and large viruses. In addition, photo-catalytically generated reactive oxygen species (ROS) on the surface of the TiO 2 NWs/CNTs-based filter material under exposure to sunlight contribute to an efficient removal of a broad range of organic compounds and infective microbes. A pilot study also yielded encouraging results in reducing traces of drugs and pesticides in drinking water.
Introduction.
Universal access to clean and safe drinking water is essential for life. Since 1990 in emerging countries, the quality of water has remarkably improved due to economic growth and technological progress. Yet, even nowadays, numerous locations throughout the world are constantly exposed to risks of contamination and still suffer from the lack of sanitary infrastructure. According to the World Health Organization (WHO) [ 1 ], at least 1.8 billion people, mainly in rural areas, consume water that is contaminated with feces. According to the United Nations Children’s Fund (UNICEF), an estimated number of 1,800 children die every day (diarrhea) because of unsafe water supply [ 2 ]. WHO reports that by 2040, a large portion of the world will endure water stress in relation to the dramatically insufficient drinking water resources. For this reason, the same source predicts a global crisis regarding universal access to clean and safe drinking water.
This problem may prove to be especially acute in countries where sanitary infrastructure is not at place or disrupted (e.g., at remote, rural or war-affected areas), as well as in electrical energy-disadvantaged communities, where running advanced purification methods is not feasible. Under such circumstances, people are forced to drink water contaminated by feces, parasites, life-threatening harmful bacteria, viruses, etc. These pathogenic species could be of various nature, like, e.g., Escherichia Coli , Salmonella , Cryptosporidium , or Hepatitis A , which could cause not only stomach pain, fever, headache, painful diarrhea and fatigue, but even death, as in the case of Legionella Pneumophila infection. It is then important to find a simple and efficient way to eliminate them to provide clean, safe and affordable drinking water in a cost-effective manner.
One of the possible solutions would be to make use of the photocatalytic water treatment by combining sunlight with nanoscale forms of titanium dioxide (TiO 2 ). In fact, this approach for water decontamination has been extensively investigated since 1985 [ 3 , 4 , 5 , 6 , 7 , 8 ]. TiO 2 is a wide-band gap semiconductor, which efficiently absorbs the ultra-violet (UV) part of the sunlight spectrum. For typical photocatalytic applications, due to their large specific surface area, the nano-sized forms of TiO 2 , e.g., TiO 2 nanoparticles (TiO 2 NPs) or TiO 2 nanowires (TiO 2 NWs), are of particular importance. The electron-hole pairs induced by the absorbed UV photons diffuse to the surface of TiO 2 NPs or TiO 2 NWs, where, in contact with water and oxygen molecules, reactive oxygen species (ROS) are produced. In the aquatic environment this photocatalytic mechanism generates various kinds of ROS, the most important of which are: hydroxyl radical (OH . ), superoxide radical anion (O 2 .− ), hydrogen peroxide (H 2 O 2 ), and singlet oxygen ( 1 Δ g ) [ 9 ]. In turn, ROS formed on the surface of photo-excited TiO 2 NPs, before they decay, can readily attack and react with organic contaminants and pathogens, if there are any in the immediate vicinity.
Thus, due to the high specific surface area of nano-sized photocatalytic particles, their efficient photo-generation of ROS, as well as large contact surface and direct interactions, the photocatalytic systems based on nanoparticle forms of TiO 2 provide a powerful disinfecting strategy against waterborne microorganisms and pathogens [ 10 , 11 ]. However, despite the significant potential and many advantages of such an approach, no operational photocatalytic sunlight-driven titania-based devices have been elaborated up to date. The current situation can be explained in part by the technical complications, which are directly related to the nanoparticle form of titania. More specifically, in slurry-type reactors, after completed photocatalytic cycles, it is difficult to collect and recycle TiO 2 NPs (20–100 nm in size), which are dispersed in suspension containing the pollutants.
To overcome this problem, different techniques of immobilization of TiO 2 NPs on various types of substrates have been developed [ 12 , 13 ]. However, TiO 2 NPs immobilized in the form of compact thin films and porous coatings usually reveal mechanical and structural instabilities, because the powdery deposits tend to detach and fall apart exposed to the action of even weak friction and shear forces.
In this regard, here, we report the design and characterization of a highly efficient and durable photocatalytic water filter, which is based on a nanocomposite material consisting of titanium dioxide nanowires (TiO 2 NWs) and carbon nanotubes (CNTs).
The device has a very simple (planar) configuration, in which the contaminated water passes through a multi-layered filter material, the pathogens are trapped on the filter surface, whereas the UV component of the sunlight, being strongly absorbed by TiO 2 NWs, generates ROS. Therefore, in addition to the mechanical retention of pathogens, the photo-triggered ROS attack and kill diverse range of pathogenic species, including bacteria and germs, thus leading to even more efficient water decontamination. Furthermore, implementation of CNTs in the herein developed composite contributes to enhancing the photocatalytic action under exposure to sunlight [ 14 , 15 ]. Especially, electrically-conducting CNTs absorb a broad spectrum of the sunlight radiation, which heats up the filter material and thus provides an additional channel for water disinfection via pasteurization [ 16 , 17 ].
To further improve the photocatalytic properties of the composite filter material elaborated herein, we have also proposed to combine the TiO 2 NWs/CNTs composite with gold nanoparticles (AuNPs). The issue of incorporation of AuNPs into the structure of the filter material and its influence on the resulting photocatalytic properties is discussed in a more complete manner in the final part of this study (Summary).
In brief, this study reports a tailored synthetic method to prepare a solar water purifier, its basic active components, as well as its thorough characterization in terms of photo-generation of ROS––towards the removal of a wide spectrum of toxic chemicals and pathogens from drinking water.
General concept of the tio 2 nws/cnts nanocomposite-based water purification filter.
As mentioned above, the essential building elements of the herein elaborated nanoporous photocatalytic filter material are TiO 2 NWs and CNTs. A simple representation of the working principle of this TiO 2 NWs/CNTs nanocomposite for water filtration is shown in Fig. 1 .
a A representative selection of microorganisms, which could contaminate the drinking water. They are trapped at the surface of the TiO 2 NWs/CNTs composite - based filter. The sketches of the pathogens are shown on the same scale as the filter material, except for the Hepatitis A virus, the diameter of which is of 24 nm. b The principle of ROS generation at the surface of TiO 2 NWs upon UV illumination. Since the lifetime of ROS (OH . , H 2 O 2 and O 2 .− ) is short, the volume of action is also indicated. Incorporation of CNTs into the TiO 2 NWs/CNTs nano-construct efficiently separates electron-holes pairs photo-generated within TiO 2 NWs, thus reducing their recombination rate and consequently increasing the efficiency of photocatalysis. (The scalebar in a) is 1 μm).
In particular, thanks to its nanoporous structure, the composite filter material efficiently retains waterborne microbial pathogens (a typical few of them are schematically depicted in Fig. 1a ). Moreover, the filter paper decontaminates the polluted water through the action of ROS, which are photo-catalytically generated under the influence of the UV component of sunlight on the TiO 2 NWs surface due to their direct contact with water and oxygen molecules [ 18 ] (Fig. 1b ).
When it comes to the function played by CNTs in the TiO 2 NWs/CNTs nanocomposite material developed by us, it is generally accepted that the presence of CNTs enhances the photocatalytic effect in two ways. Specifically, numerous reports have shown that CNTs in combination with either TiO 2 NPs or TiO 2 NWs can act as electron acceptors to more effectively separate charges photo-generated within TiO 2 nanostructures and thus significantly improve the photocatalytic properties of such constructs [ 14 , 15 ]. In addition, the broadband absorption of solar radiation leads to heating of the filter material, thereby allowing photo-thermal disinfection of water [ 16 , 17 ]. Indeed, we show that the herein elaborated combination of TiO 2 NWs with CNTs, gave a considerable improvement in the functioning of the filter material.
High resolution TEM images of the individual nano-structural components, that is of a single TiO 2 NW and a single CNT, are shown in Fig. 2a, b , respectively. For the practical implementation of numerous variants of the filter material, a large-scale production of both TiO 2 NWs and CNTs was develop in our laboratory. The detailed description of the large-scale synthesis routes of TiO 2 NWs can be found in ref. [ 19 ]. and in the U.S. patent ‘Titanium oxide aerogel composites’ filed by us [ 20 ].
a , b HR TEM images of the essential individual nano-structural components of the composite filter material, i.e., a single TiO 2 NW and a single multiwalled CNT, respectively. The length of both nanoelements can reach several micrometers (The scalebars are 10 nm).; ( c ) Photos of selected samples of TiO 2 NWs-based filter paper with various wt% contents of CNTs, which alters their transparency (the diameter of the filter paper disc is of 20 mm); d Characteristic SEM image of the filter paper (The scalebar is 5 μm is 5b, ( e ) Photo of large area filter papers synthesized from pure TiO 2 NWs (front) and containing 1 wt% content of CNTs (grayish). (The scalebar is 10 cm).
In short, the first step of the synthesis yields titanate (H 2 Ti 3 O 7 ) nanowires, which recrystallize into anatase TiO 2 NWs during the subsequent heat treatment process. While using this technological approach, in our laboratory conditions we were able to produce an amount of ~0.3–1.0 kg of TiO 2 NWs per day in a single synthesis cycle. However, it is worth mentioning that prospective industrial production would not be subject to such quantitative restrictions.
The mass production of CNTs was accomplished by a process of catalytic chemical vapor deposition (CVD) performed in an inclined rotary tube furnace operating in continuous mode [ 21 ]. As explained in Methods, the overnight synthesis produced ~1.2 kg of CNTs.
The above-described high-efficiency synthesis processes of both nano-structural components, i.e., TiO 2 NWs and CNTs, allowed us to fabricate photocatalytic filtering papers with large surface areas. To this end, TiO 2 NWs and CNTs were mixed in different proportions in order to optimize the filter’s performance in terms of water sterilization. Subsequently, the corresponding mixtures were processed by doctor blading into films of various thicknesses, ranging from 2 μm up to 300 μm. The thin layers obtained this way could easily be detached from the hydrophobic support material. After air drying at 120 °C and calcination in vacuum at 600 °C, a phase transformation from titanate to anatase was achieved. It is worth mentioning here that that the calcination process fuses TiO 2 NWs together, thus leading to the formation a thin filtering membrane with a tightly compact structure, which, in normal use (i.e., under standard volume flow-rates), does not release nano-structural ingredients. In short, the technology developed herein made it possible to produce freestanding, flexible thin filtering papers with large surfaces, which, depending on their thickness, could even be transparent. Examples of such thin disc-shaped filtering membranes (50 μm thick, 20 mm in diameter), with various wt% contents of CNTs, are shown in Fig. 2c .
The surface appearance of the filter is shown in an SEM image in Fig. 2d , while the large surface area (~0.3 m 2 ), self-standing filter papers used for the fabrication of the solar-thermal water purification prototype are displayed in Fig. 2e , for pure TiO 2 NWs (white) and with 1 wt% content of CNTs (grayish).
The large area filter paper made it possible to fabricate a prototype of a solar-thermal water purification system (Fig. 3a ). For this purpose, a freestanding 30 μm thick filter paper with dimensions of 37.5 cm × 28.0 cm was positioned and fixed between two 1.5 mm thick borosilicate glass windows. In our design, borosilicate glass was chosen because of its low absorbance in the UV range. The water inlet and outlet were placed on the opposite diagonal sides of the device (Fig. 3 b). The stacked assembly was sealed and mechanically secured by a rectangular aluminum frame. For receiving the highest photon flux, the sun-facing surface area of ~0.1 m 2 could easily be positioned at an optimal angle ( θ ) with respect to solar radiation. The total internal volume of the device was estimated to be of 200 ± 50 ml.
a Photograph of the device (with a visible random mirror image of the surroundings on the outer glass surface of the filter) and ( b ) the sketch of the cross-section of the prototype. The flow-rate through the device depends on the water pressure through the difference in elevation levels between the contaminated water tank and the clean water outlet (symbolically marked as height, h). The orientation of the device can easily be adjusted to an optimal angle (Θ) with respect to solar radiation; ( c ) Temperature of the solar-thermal device when exposed to the sun. The limit temperatures are of 52.2 and 52.9 °C for the fit curves for the infrared camera and for the thermocouple, respectively. The inset shows the infrared image of the prototype at one temperature point during its exposure to sunlight; ( d ) Purified water volume flowing through the device as a function of time for three values of h: 75, 120 and 160 cm. The rectilinear slopes of the plots confirm the dependence of the volume flow-rate on h according to the Pascal’s law.
The possibility of efficient heating of the influent water due to the photo-thermal effect is also an important attribute of the developed filtering device. In our opinion, this functional property is related to the presence of CNTs in the structure of the filtering layer. Absorbing a broad spectrum of sunlight, these carbon nanowires with a metallic character heat up the filter and water in its immediate vicinity, thus enabling sterilization by elevated temperatures. In particular, temperatures of the order of 50 °C could be attained inside the prototype after approximately 1 h. of exposure to solar radiation (during a sunny afternoon on June 11th in Lausanne, Switzerland). To illustrate the thermal characteristics of the prototype, temperature was measured with both a thermocouple (on the surface of the device) and an infrared camera. The corresponding time dependencies of the device temperature exposed to the sun radiation for about 60 min are shown in Fig. 3c . It is worth mentioning that no forced water flow was used in this experiment. Therefore, the outcome of this experiment reflects the maximum potential temperature that the device can attain under similar meteorological conditions.
An important parameter of the filtering system is its flow-rate ( Q ), defined as the purified water volume ( V ) passing through the device per unit time ( t ), i.e., Q = V / t . This volume flow-rate is usually described the Darcy’s law [ 22 ], which states that the fluid flow-rate through a filtration device is directly proportional to the corresponding pressure gradient, that is: Q = κA Δp / μL where Q [ m 3 ∙ s −1 ] is the volume flow-rate, κ [ m 2 ] is the permeability of the medium, A [ m 2 ] is the filter area, Δp [ Pa ] is the pressure drop across the filter membrane of thickness L [ m ], and μ [ Pa ∙ s ] is the viscosity of the fluid.
The drop of pressure across the filtering device can be varied by changing the vertical separation between the polluted water tank and the filter outlet, in accordance to the Pascal’s law: Δp = gρh , where g is the gravitational constant, ρ stands for the fluid density and h abbreviates the vertical separation distance (height). For the meaning of the symbols see Fig. 3b . The measured dependencies of the water volume flowing through the device as a function of time for three values of h : 75, 120 and 160 cm is shown in Fig. 3d . Qualitatively, the Darcy’s law is satisfied, although for higher h values, there might be some pressure loss, since V versus h is not strictly linear. As can be seen, even this small surface area filter can supply ca . 2.0 liters of decontaminated water per day.
The photo-catalytic efficiency of the filtering composite material prepared in this work was checked for a broad spectrum of potential targets, ranging from small molecular compounds to bacteria. In particular, for characterization of the photocatalytic generation of ROS the following methods were implemented: electron spin resonance (ESR), optical spectroscopy and standard microbiological bacteria survival tests. In addition, for measuring the variation of minute concentrations of molecules, such as drugs and pesticides in water, mass spectrometry (MS) coupled with high-performance liquid chromatography (HPLC) was applied.
To confirm the efficient photocatalytic generation of ROS in an aqueous environment by the TiO 2 NWs/CNTs-based filtering composite material, ESR in combination with spin-trapping was employed. Specifically, a stable nitroxide radical, 4-Hydroxy-2,2,6,6-tetramethylpiperidine-1-oxyl (TEMPOL), was used as a target molecule for the photo-generated ROS, i.e., OH ∙ and O 2 .−∙ radicals [ 20 , 23 ]. The ESR-active TEMPOL is a water-soluble antioxidant, which reportedly acts as a superoxide dismutase (SOD) mimicking agent [ 24 , 25 ].
The reactive pathways of TEMPOL with ROS have been reported to introduce structural changes at the 1- and 4-positions of this nitroxide molecule, for O 2 − and OH ∙ radicals, respectively [ 26 ]. Acting in concert, these structural changes induce the decay of the ESR-active TEMPOL, as well as lead to the concurrent formation of another ESR-active radical, the 4-oxo-TEMPO (TEMPONE).
In aqueous solutions, both TEMPOL and TEMPONE reveal easily detectable ESR spectra, which are characteristic for NO-centered radicals bearing one unpaired electron ( S = 1/2). Specifically, the corresponding ESR signals consist of three well-resolved features resulting from the 14 N atom-related hyperfine splitting ( I = 1). Due to the differences in the hyperfine splitting constants, A 14 N , and the spectroscopic g -factors values, being of 17.1 G/2.0057 and 16.1 G/2.0056, for TEMPOL and TEMPONE, respectively, these two nitroxide radicals can be very easily distinguished [ 27 ].
The principle of the ESR experiment allowing for an indirect detection and evaluation of photo-catalyzed ROS, with using TEMPOL as a target molecule, is shown schematically in Fig. 4a . In particular, the diagram in this figure depicts the two most important reaction pathways related to the attack of O 2 − and OH ∙ radicals on TEMPOL, thus leading to the ESR-silent TEMPOL-hydroxylamine (TEMPOL-H) and the ESR-active TEMPONE, respectively.
a Principle of oxidative stress evaluation with using a stable nitroxide radical, TEMPOL. The reducing/oxidative action of the photo-generated ROS deprives the TEMPOL molecule of spin and makes it ESR-silent. Through a competing process, the OH ∙ radical attacks the TEMPOL molecule at the 4-position and converts it to another ESR-active nitroxide, TEMPONE. b The ROS-inducted progressive decay of the ESR signal of TEMPOL is accompanied by the occurrence of the ESR signal of TEMPONE, as observed over 120 min time under exposure to UV-A. c Time-evolutions of the ESR signal intensities of TEMPOL monitored at the entrance and outlet of the TiO 2 NWs/CNTs––based photocatalytic filter.
Considering the course of the ESR signals of TEMPOL and TEMPONE as a function of time, it seems clear that their time-evolutions confirm the presence of ROS, but with divergent dependencies. In particular, as a function of time, the ESR signal intensities of TEMPOL and TEMPONE, gradually decay and increase, respectively.
Typical results of ROS detection by means of ESR using TEMPOL as a molecular target are shown in Fig. 4b . Specifically, it can be seen that for the generation of ROS by TiO 2 -based photo-catalyst, after a prolonged illumination with UV-A light, the ESR signals of TEMPOL and TEMPONE clearly decrease and increase, respectively. Note that only the low-field hyperfine components of the ESR spectra of TEMPOL and TEMPONE are shown in Fig. 4b .
During this experiment, both sides of the filtering device were illuminated by a UV-A light source, which was operating at the wavelength of 367 nm with the power intensity of ~1–3 mW/cm 2 .
To check the efficiency of the prototype in photo-generation of ROS when exposed to sunlight, the samples for ESR measurements were taken regularly over an extended period of time from the inlet and outlet of the filter (see Fig. 3b ). Before staring the experiment, the upper tank of the device was filled with the volume of two liters of 400 μM aqueous solution of TEMPOL.
Changes in the intensities of the ESR spectra during the filter’s exposure to sunlight were assessed by comparing the double integrals of the corresponding ESR signals acquired sequentially as a function of time (for more details see METHODS).
The corresponding plots of the ESR signal intensities monitored at the entrance and outlet of the prototype filtering device over ~2.5-h. period of exposure to sunlight, during the sunny early afternoon of April 6 th in Lausanne, Switzerland, are displayed in Fig. 4c . As shown, the ESR signal intensity of TEMPOL decreases strongly with time after its passage through the filter, which is the consequence of the ROS-induced damage. It is worth mentioning that the simultaneous creation of the ESR-active TEMPONE compensates to a relatively small extent the herein observed overwhelming decay of the paramagnetic TEMPOL. In fact, as mentioned before, both these processes confirm the divergent mechanisms of ROS-mediated actions on the same target molecule (TEMPOL). Thus, this observation validates the final conclusion that TiO 2 NWs/CNTs-based composite is very efficient in generating ROS and the accompanying oxidative stress on its surface.
The colorful dye, methyl orange (C 14 H 14 N 3 NaO 3 S, abbreviated as MO) is often used as a model organic pollutant for evaluation of the ROS generation efficiency and the oxidative stress conditions in various environments [ 28 , 29 , 30 ]. The usefulness of MO for this type or research is due to the fact that the ROS-mediated damage to MO reduces its strong absorption band at 464 nm. In particular, under the influence of photo-oxidative stress, the MO molecules undergo the successive stages of hydroxylation, demethylation and oxidation, which result in photo-bleaching and, ultimately, complete loss of color. The corresponding changes in the molecular structure of the dye can be associated to its concentration and easily be monitored by the changes in the dye’s absorbance ( A ), according to the Beer–Lambert law expressed as A = ε l c, where ε is the molar attenuation coefficient, l is the optical path, and c is the MO concentration.
In this experiment, MO dissolved in distilled water (Millipore), with an initial concentration c 0 = 20 mg/mL was poured into Petri dishes (90 mm in diameter and 15 mm height) containing the test samples in the form of discs (50 mm in diameter) at their bottom. For the purpose of exposure to UVA light, a UV spot light source, LC-8 Lightingcure™ ( λ exc = 365 nm, 16 mW/cm 2 , from Hamamatsu Photonics (Japan), was used. The photocatalytic activity of the herein developed composite material based on TiO 2 NWs/CNTs was tested, as well as two reference materials: a commercial standard photocatalyst, TiO 2 NPs (Degussa P25), having similar specific surface area (~40 m 2 /g), and a nano-structured aluminum oxide (Al 2 O 3 ).
The photodegradation of the dye and the corresponding changes in its concentration were monitored by measuring the characteristic MO absorbance peak at 464 nm with a UV–Vis spectrophotometer, Varian Cary 50, Agilent (USA). In order to obtain the time dependencies, small aliquots (2.5 mL) were taken every 10 min from Petri dishes and transferred to the cuvettes of the UV–VIS spectrophotometer.
All these test measurements were performed under static conditions, i.e ., without flow or mixing/stirring the MO solution in Petri dishes. As shown in Fig. 5a , the filter paper elaborated herein is twice as efficient as the P25 itself.
a The normalized concentration (c/c 0 ) of MO versus UVA illumination time in the presence of the TiO 2 NWs/CNTs filter (red dots). The herein monitored MO degradation efficiency was compared to that of P25 TiO 2 NPs (Degussa) deposited on an anodic aluminum oxide (Al 2 O 3 ) membrane (gray circles) and also compared to the efficiency of the same anodic Al 2 O 3 membrane without any coverage (black dots); For illumination with UVA, a UV spot light source (λ exc = 365 nm, 16 mW/cm 2 ), model LC-8 Lightingcure™ (Hamamatsu Photonics, Japan) was implemented; ( b ) After the first passage through the TiO 2 NWs/CNTs photocatalytic filter, both micropollutants slightly desorb, which coincides with starting of UV-A illumination (due to thermal desorption). For subsequent passages, however, the photo-generated ROS take over and destroy these harmful molecules.
It has been shown that CNTs in combination with other semiconducting nanomaterials, such as, e.g., TiO 2 NPs or zinc oxide NPs (ZnONPs), substantially reinforce the photo-catalytic efficiency of composite photo-catalytic materials [ 31 ]. In particular, it has been demonstrated that the presence of CNTs in theses composite materials enhances their photocatalytic efficiencies through increased total active surface area and electrical conductivity [ 32 ]. Therefore, in the presence of CNTs, these contributions increase lifetimes of the photo-generated electron-hole pairs generated by semiconducting nanomaterials, thus improving their overall photo-catalytic performance [ 16 ].
Micropollutants, such as drug residues, pesticides, maintenance products, hormones, or cosmetics, contaminate drinking water worldwide and may have a long-term toxic effect on living organisms and the ecosystem [ 33 , 34 , 35 ]. In this regard, we also examined whether our photocatalytic filter was able to reduce their concentrations. To this end, the Central Environmental Laboratory of EPFL prepared a “cocktail” of nine micropollutants (five drugs, three pesticides and one maintenance product: atrazin, carbamazepin, diclofenac, mecoprop, metolachlor, bezotriazol, lomeprol, gabapentin, metformin). They were dissolved in 5 L of distilled water, representing a concentration of hundreds nanograms per liter (ng/L). After each passage through the filter, the micropollutants were separated by high-performance liquid chromatography (HPLC), and various bands were analyzed with mass spectrometry (MS). Figure 5b shows the results of the successful removal of two selected micropollutants, i.e., gabapentin (painkiller) and metformin (drug for diabetes).
The first passage performed in the dark (sampling 1) showed a global decrease in concentrations of both gabapentin (blue trace) and metformin (red trace), that can be attributed to the adsorption of a certain part of the compounds on the filter surface. Specifically, as can be seen in Fig. Fig. 5 b, the concentrations of both compounds decreased by ~25% during the 1st sample run. This downward trend in the concentration of both chemicals was partially stopped during the 2nd sampling period. The herein observed inhibition of the filtration process and the accompanying slight increase in the concentration of both chemicals may be related to thermal desorption. Actually, it also coincides with the beginning of exposure of the filter to illumination with UVA light (365 nm, 1 ÷ 3 mW/cm 2 ). However, during the next sampling runs (samplings 3 and 4), a small drop in concentrations of both micropollutants was observed, what can be attributed to the ROS-mediated photo-decomposition (see Fig. 5b ). This small, though measurable change might be due to very low concentrations of gabapentin and metformin, and their relatively short residence time under flow conditions within the volume where ROS are photo-generated (see Fig. 1b ). An additional argument supporting this rather minor effect of micropollutant photodegradation can also be related the very low power density of the incident UVA radiation in this experiment. Although the observed decrease in concentration is slight, it nevertheless suggests the potential of the herein developed TiO 2 NWs/CNTs-based photocatalytic filter for the removal of micropollutants from water.
The capability of the device to filter out germs from water was verified using the Colilert and Quanti-Tray method [ 36 , 37 ]. This is a standard method to indicate the sanitary quality of water, e.g., the evidence of fecal contamination with coliform bacteria, with special emphasis on E. coli . In practical application of this method, the enzymatic activity of coliform bacteria metabolizes two nutrient-indicating molecules, i.e., ortho-nitrophenyl-β-D-galactopyranoside (ONPG) and 4-methyl-umbelliferyl-β-D-glucuronide (MUG). More specifically, in the general case of the presence of coliform group bacteria, the metabolized ONPG turns the colorless water into yellow, whereas in the specific case of the presence of E. coli , MUG renders the aqueous milieu fluorescent upon UV illumination. In this approach, the enumeration of coliforms and E. coli in water samples is performed using so-called colony-forming units (CFU).
The tested water sample was taken from the river La Chamberonne (passing nearby the laboratory). Prior to performing the contamination test, an aliquot of 1 ml of this water was 100 times diluted with distilled water. Next, before and after passing through the filter, the water was mixed with the Colilert reagent, poured into Quanti-trays and incubated at 35 °C for 24 h. The results are shown in Fig. 6a . The Quanti-tray containing the untreated water turned completely yellow and became also fluorescent under UV light (not shown), while the Quanti-tray with the filtered solution did not change color. Moreover, as can be seen in the upper portion of Fig. 6a , all the cells of the Quanti-tray containing the untreated water are yellow, thus confirming the contamination with coliform bacteria at the level higher than 200 CFU/100 ml. In contrast, the assessment of the Quanti-tray containing the treated water (lower portion of Fig. 6a ), points to the contamination level well below 1 CFU/100 ml.
a The presence of coliform bacteria in the 100 times diluted river water is indicated by the yellow color of the Quanti-tray (upper part of the image), whereas the colorless Quanti-tray confirms that no bacteria passed through the TiO 2 NWs/CNTs filter (lower part of the image); ( b ) The bacterial inactivation performance of the TiO 2 NWs/CNTs filter upon UVA and visible light illumination as compared to the control surface of the humid Teflon filter. After 30 sec of illumination with UVA light and after more than 300 sec when exposed to visible light, the concentrations of bacteria are below the detection limit. Inset: schematic representation of the experiment showing the location of the bacteria-containing spots on the filter’s surface.
Thus, the Colilert and Quanti-Tray procedure confirmed the efficiency of the TiO 2 NWs/CNTs-composite-based filter for the mechanical removal of waterborne pathogens, including E-coli bacteria. This high filtration efficiency can be attributed to the small cut-off size of the filter pores (<1 μm).
Below we show that apart from the mechanical retention of pathogens, the photocatalytic properties of the herein developed filter material also allow for their complete deactivation. To this end, a second microbiological test was performed. Specifically, we employed the conventional plate count technique, in which, similarly to the previously discussed Colilert and Quanti-Tray test, CFU units are taken into account to estimate the number of viable microorganisms in the sample [ 37 ].
The E. coli bacteria survival was measured under three conditions: (i) deposited on TiO 2 NWs/CNTs filter and illuminated with UV light (at 365 nm with power density of 16 mW/cm 2 ), for time intervals of 20, 60, 100 and 180 sec; (ii) deposited on the same filter, but illuminated with daily sun light extended up to 600 sec; and iii) deposited on Teflon substrate, illuminated by the UV and visible lights for the corresponding time intervals - as control measurement. In all cases, the starting E. coli concentration was 2*10 8 CFU/mL.
From the suspensions prepared that way, 5-μL aliquots were taken, dropped on the filter surface and exposed to illumination with UVA light. After each illumination run, the filter fragments were placed in Eppendorf tubes containing physiological salt and then rinsed for 60 min. This treatment allowed to the dead E. coli to be removed and to enter the survived cells back into solution. Next, serial dilutions were prepared from the solution containing cells and 10 μL aliquots of each dilution were spread onto cultivation agar in Petri dishes. Subsequently, they were incubated at 37 °C for 24 h. The enumeration of bacteria per mL (CFU/mL) was extrapolated from the colonies counted at the appropriate spots for TiO 2 NWs filter, and the survival rate could be established. The results shown in Fig. 6b superbly demonstrate the antibacterial activity of the TiO 2 NW/CNTs filter. Already, after 60 sec of UVA light exposure the number of survived bacteria drops below the detection limit (red trace in Fig. 6b ). Even after exposure for 30 sec to UVA light, the damaged bacteria could be noticed in the SEM image (not shown) . A direct impact of high energy UV photons can damage the E. coli bacteria as shown in the control experiment on the wet Teflon filter surface, but the corresponding decrease in their number is non-comparable with that of the TiO 2 NWs-based photocatalytic filter.
It is also worth mentioning that in the experiment described above, the time scale in which E. coli inactivation occurred was much shorter than for any other tests of light-dependent oxidative stress conducted herein. The rapid photo-inactivation of E. coli observed in this experiment can be attributed to the fact that the bacteria were trapped on the filter surface, thus being in the immediate range of ROS photo-generated by immobilized photocatalyst particles. In addition, the entire experiment was carried out under static conditions (without water flow). Therefore, the photo-catalytically induced ROS, before their disappearance, had a better chance of reaching the bacteria. This is in contrast to other experiments, in which photodegradation of waterborne chemical compounds, such as TEMPOL or MO, was observed under flow conditions.
The apparent differences in photo-deactivation rates of adsorbed bacteria and water-soluble chemicals can then be associated to the limited volume of action of ROS generated mainly at the filter surface. Specifically, both the small volume of the direct ROS-mediated deactivation (symbolically represented by the bluish cylinder in Fig. 1b ) and dynamic conditions of water flow led to the observed reduction in photocatalytic deactivation efficiency of waterborne chemicals.
Furthermore, another interesting observation is the fact that that exposure only to sunlight exerts a profound sterilizing impact and significantly eliminates E. coli bacteria. This sterilizing effect is related, in part, to the UV component of the sunlight spectrum, which induces photocatalytic damage to bacteria, as well as to pasteurization due to the increased temperature of the filter material containing CNTs in its structure (see Fig. 3d ). Regardless of the contributions of the above-mentioned mechanisms, the photo-thermal water filter developed in this work seems to be an interesting proposition for large-scale applications, allowing for effective water purification in the absence of specific infrastructures. The device, using solely sunlight, exerts a sterilizing effect by destroying microbial pathogens, such as bacteria or even viruses, thus rendering the polluted water safe and drinkable.
We have reported a simple approach to filter and purify water, which is based on the herein developed thermo-photocatalytic composite material, TiO 2 NWs/CNTs, and is using solely sunlight as a source of energy. The filter can efficiently entrap, degrade and eliminate waterborne pathogens, including bacteria, viruses and worms. Furthermore, it has also proven efficiency in photocatalytic decomposition and neutralization of waterborne organic micropollutants, such as drugs, pesticides and detergents.
In the filtering device constructed in this work, the sunlight-mediated disinfection of waterborne pathogens occurs due to the combined action of photo-generated ROS and thermal pasteurization, i.e., the respective contributions of photocatalytic properties of TiO 2 NWs and photo-thermal input of CNTs, resulting from their strong absorption in broad optical spectral range.
A small prototype of the water-filtering device with surface of 0.3 m 2 can supply 2 L/day of decontaminated water, which could be easily scaled up by increasing the filter surface. The great advantage of this device is that it is cost-effective, thermally stable, chemically inert, and capable of promoting oxidation of organic compounds via photo-catalytic generation of ROS. We believe that this simple method could be a good solution for drinkable water-stressed areas.
As an outlook, to further improve the photocatalytic properties of the composite filtering material elaborated in this work, we also propose a few of possible improvements. The first could be the incorporation of gold nanoparticles (AuNPs) into the TiO 2 NWs/CNTs-based composite fabric, as shown in Fig. 7a, b . In this regard, earlier studies have shown that AuNPs exhibit enhanced photon absorption properties and can be used to efficiently generate local heating upon illumination through photo-induced resonant plasmons [ 38 ]. Therefore, composites consisting of the photoactive TiO 2 and AuNPs can be conveniently employed as plasmonic photocatalysts, enabling a number of important reactions to occur with high efficiency and under minimal light exposure [ 39 , 40 , 41 ]. Although the exact underlying mechanisms are still not well understood, this direction of improvement of the composite material seems to be promising. In particular, the expected improvement in photocatalytic composite material also incorporating AuNPs is related to the plasmonic effect, which works for the whole spectral range of sunlight.
a TEM images of a large assembly of the TiO 2 NWs/AuNPs composite (the scalebar is 200 nm), and ( b ) Enlarged image fragment selected from the image shown in ( a ) (the scalebar is 5 nm); ( c and e ) SEM images of the filter material without and with surface structuring, respectively (the scalebar is 2 μm). d Two distinctly different optical responses upon visible light illumination of non-structured (left) and structured (right) versions of the filter material (the scalebar is 10 mm).
A second route for improvement could be the surface structuring of the filter, in order to better trap and conduct the incident light into the bulk of the material, since, as mentioned before, both ROS generation and the resulting water pasteurization are proportional to the illuminated volume. In general, the question of more efficient light trapping is very vivid in photovoltaics in order to improve the light-matter interaction within the device’s photo-active layer and thus to enhance the solar cell efficiency. One way of achieving this is through elaboration of periodic light trapping structures. Recently, numerous such structures have been developed, including nanowires [ 42 ], nanoparticles [ 43 ], gratings [ 44 , 45 ], and many more. In particular, gratings could be designed to diffract the incident light at the TiO 2 –air interface at angles bigger than the critical angle (depending on the grating periodicity), so that most of the potentially scattered or reflected energy could be returned to the photo-active filter layer. It has previously been shown that such surface structuring results in an effective enhancement of the optical path length and better light absorption [ 45 ].
In this regard, in Fig. 7c–e , we show that it is possible to fabricate the TiO 2 NWs/CNTs filter to have a grating pattern structure on its surface. Specifically, the SEM images of the as-deposited filter on a flat and lithography-modified substrate surfaces are shown in Fig. 7c, e , respectively. The grating pattern structure can easily be recognized on the surface of the filter material deposited on the lithography-engineered substrate. Moreover, as shown in Fig. 7d , these two surfaces have distinctly different optical responses, due to the enhanced light interference on the surface with the grating pattern.
Further optimization of structuring of the filter surface as well as exploration of its advantageous properties are the subjects of forthcoming studies related to the TiO 2 NWs/CNTs filter material.
TiO 2 nano-powder with size distribution of 20–50 nm (Nanoshell LLC) was dissolved in a base solution of NaOH (Merck), and heated up to 70 °C and exposed to turbulent mixing. In a time-window of 1–24 h a high fraction of mesoporous titanates was formed with a jelly-like appearance. By centrifugation the (H 2 Ti 3 O 7 ) NWs were separated from the reaction residues and transformed into anatase TiO 2 NWs by heat treatment at 600 °C (ref. [ 20 ]). The specific surface of TiO 2 NWs is in the 150 m 2 /g range.
The continuous production method of CNTs implemented in this work was based on chemical vapor deposition (CVD) performed in an inclined rotary tube furnace [ 21 ]. This approach overcomes the limited capacity and scalability of more frequently used fixed bed reactors [ 46 , 47 ]. The furnace used here was equipped with a quartz tube with a diameter of 80 mm. During the CVD deposition process, the catalyst (bimetallic Fe 2 Ni catalytic particles on CaCO 3 supporter) was continuously introduced into the reaction tube with an endless screw placed at the end of the catalyst container. Acetylene and argon were fluxed at 10 L/h and 80 L/h, respectively. The material was purified by dissolving the catalyst and the support in a 1.5 M hydrochloric acid. Subsequently, MWCNTs were filtered, washed with distilled water, and dried at 120 °C overnight. A production rate of about 1.2 kg per day was achieved. The specific surface of CNTs 700 m 2 /g rage.
The mean pore size distribution of the filters was characterized by polystyrene dispersion of 1.97 μm , 870 nm , 530 nm and 110 nm particles of concentration of 13.7 mg/L, which were passed through the filter. Due to intrinsic absorbance and the light scattering of polymer colloid particles, the dispersion has a characteristic absorbance spectrum. Therefore, comparing the initial spectra with the filtered solution spectra yields information about the concentration and retention ability.
The light intensities were measured with the optical intensity handheld meter ML9002A (Anritsu). The silicone-based detector measured the total power incident onto the 9 mm-diameter circular surface of the probe.
Thermal images were captured with the FLIR ONE infrared camera. It measured the intensity of infrared light (7.5 μm < λ < 14 μm) emitted by the objects in the field of view of the camera over an area of 160 by 120 pixels to compute their temperature. In the limit of sensibility of −20 °C to 120 ̊ the temperature resolution was of 0.1 °C.
The water sample/nutrient-indicator mixture was introduced into a Quanti-Tray (array of plastic reservoirs) and sealed with IDEXX Quanti-Tray Sealer. The sealed tray was placed in an incubator at 44.5 ± 0.2 °C for 18 h. The numbers of positive wells (yellow color) were translated into the Most Probable Numbers by a table provided with the trays.
Evaluation of viable coliforms and E. coli in water samples was performed using the so-called colony-forming units (CFU) method. The CFU method is generally accepted for the evaluation and assessment of viable microorganisms, as well as for testing the impact of antimicrobial techniques and substances under various experimental conditions.
The initial concentration of E. coli bacteria used in this study was of 2–10 8 CFU/ml. All manipulations with the bacteria were performed using clean, sterile equipment, including pipette tips and Eppendorf tubes, solidified agar media, Petri dishes, and the bacterial cell spreader. To expose the E. coli bacteria in control experiments to UVA light, a UVA-light spot source, LC-8 Lightingcure™ (λ = 365 nm, 16 mW/cm 2 ) from Hamamatsu Photonics (Japan) was used. In experiments aiming at characterizing the disinfecting potential of the filter material based on the TiO 2 NWs /CNTs nanocomposite, E. coli bacteria deposited on this filter were exposed to sunlight.
The ESR experiments were carried out at room temperature using a cw-ESR X-band spectrometer, Bruker EleXsys E500 (Bruker BioSpin GmbH, Karlsruhe, Germany), equipped with a high-Q cylindrical cavity (Model ER 4122 SHQE). Water with 400 μM concentration of TEMPOL was passed through the filter and exposed to sunlight (as shown in Fig. 3 ) over a period of ~2.5 h. Small aliquots of about 20 μL were taken both before and after the filter at regular time intervals, transferred into 0.7 mm ID and 0.87 mm OD glass capillary tubes (VitroCom, NJ, USA), with a sample height of ca . 30 mm, and sealed on both ends with Cha-seal (Tube sealing compound, Chase Scientific Glass, Rockwood, TN, USA). The typical instrumental settings were: microwave frequency ~9.4 GHz; microwave power 0.633 mW; magnetic field sweep 120 G; magnetic field modulation frequency 100 kHz; magnetic field modulation amplitude 0.5 G; time constant 10.24 ms; spectral resolution 2048 points; conversion time 40.96 ms; resulting magnetic field sweeping time 84 s; two scans were accumulated per one trace. To evaluate the number of spins in the individual samples, the respective ESR spectra were double-integrated using a software tool (OriginPro2019) and the obtained signal intensities were compared with the intensity of the reference signal (400 μM TEMPOL).
Methyl orange solution (MO) with an initial concentration of 20 mg/L was poured into Petri dishes containing the test samples in the form of discs (50 mm in diameter) at their bottom. For the purpose of exposure to UVA light, a UV spot light source, LC-8 Lightingcure™ (λ exc = 365 nm, 16 mW/cm 2 ), from Hamamatsu Photonics (Japan), was used. The photodegradation of the dye and the corresponding changes in its concentration were monitored by measuring the characteristic MO absorbance peak at 464 nm with a UV–Vis spectrophotometer, Varian Cary 50, Agilent (USA). In order to obtain the time dependencies, small aliquots (2.5 mL) were taken every 10 min from Petri dishes and transferred to the cuvettes of the UV–VIS spectrophotometer.
The data that support the findings of this study are available from the corresponding author upon reasonable request.
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E.H. gratefully acknowledges the Global Water Award of the United Arab Emirates, the Swiss-South African collaboration grant, and the support of the Karl Zeno Schindler Foundation. We would also like to thank Lenke Horváth and Rita Smajda, for their assistance in the early stage of the experiments.
Present address: Stavropoulos Center for Complex Quantum Matter, University of Notre Dame, Indianapolis, IN, USA
Laboratory of Physics of Complex Matter, Ecole Polytechnique Fédérale de Lausanne, Lausanne, Switzerland
E. Horváth, J. Gabathuler, G. Bourdiec, E. Vidal-Revel, M. Benthem Muñiz, L. Rossi, A. Sienkiewicz & L. Forró
Central Environmental Laboratory, Ecole Polytechnique Fédérale de Lausanne, Lausanne, Switzerland
M. Gaal, D. Grandjean & F. Breider
ADSresonances Sàrl, CH-1028, Préverenges, Switzerland
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E.H. was the project leader and synthesized the materials. L.R. did the electron microscopy. J.G. worked with the prototype and characterized the filter paper with G.B., E.V.-R. and M.B.-M. The micropollutant test was performed by M.G., D.G. and F.B. The ESR measurements were done by A.S. who has participated in the paper writing. L.F. is the team leader and wrote the paper. All authors approved the manuscript.
Correspondence to E. Horváth or L. Forró .
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Horváth, E., Gabathuler, J., Bourdiec, G. et al. Solar water purification with photocatalytic nanocomposite filter based on TiO 2 nanowires and carbon nanotubes. npj Clean Water 5 , 10 (2022). https://doi.org/10.1038/s41545-022-00157-2
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